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only that the author(s) didn't take a sample soon enough. The three studies using RF fields
are not directly comparable as seen in Table 5-3, and no general conclusion is possible.
5.3. EFFECTS ON TRANSCRIPTION, TRANSLATION, AND CELL TRANSFORMATION
5.3.1. Extremely Low Frequency Electromagnetic Fields
Goodman and her collaborators have published a number of papers in which cellular
transcription was induced in gnat (Sciara coprophila) larval salivary glands following exposure
to ELF fields. Goodman et al. (1983) exposed salivary glands to pulsed magnetic fields in 0.5
milliliters (mL) of Schneider's Drosophila medium in petri dishes between a pair of 10-cm by
10-cm Helmholtz aiding coils oriented vertically, producing a magnetic field parallel to the
bottom of the petri dish. The glands (still attached to the larval bodies) were exposed to either
repetitive single pulses (single 380-microsecond pulses of 15 mV amplitude repeated at 72 Hz)
or to repetitive pulse trains [5-millisecond pulse trains of 200-microsecond pulses (also 15 mV
amplitude) repeated at 15 Hz]. The rate of change of the magnetic field was about 0.1
G/microsecond (0.01 mT/microsecond) for the pulse trains and 0.05 G/microsecond (0.005
mT/microsecond) for the single pulses. The authors measured transcription in three ways: (1)
nascent RNA chains attached to specific chromosome regions were identified by
autoradiography; (2) nick translation using deoxyribonuclease I to identify transcriptionally
active chromatin regions; and (3) RNAs of various size classes were isolated and analyzed for
changes in the pattern of tritiated uridine incorporation. At 15 and 45 minutes of exposure to
the single pulse field, there was a specific increase in RNA transcription in most of the bands
and interband regions of the chromosomes. At 30 minutes, exposure transcription was about
at the control rate. Nick translation showed some "hot spots" of transcription at 45 minutes of
exposure. The pulse-train field led to a gradual increase in transcription up to 45 minutes of
exposure but not to the level reached by the single pulse exposure. Effects of both types of
fields decreased after 60 minutes of exposure. Isolation of RNA on sucrose gradients showed
a fourfold increase in total RNA but an 11 -fold increase in the mRNA size class at 15- and
45-minute exposures to single pulse fields. All size classes of RNA were at control levels after
15 minutes of exposure to pulse-train fields, but after 45 minutes, the levels of all RNA size
classes had increased.
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Goodman and Henderson (1986), using the same test system just described, compared
the effect of wave shape on transcription induction. The magnetic fields were generated with
10 x 10 cm Helmholtz aiding coils orientated vertically. The authors used a 72-Hz sine wave
(0.8 mV positive amplitude, 1.15 mT peak magnetic field, rate of change of field was 0.5 T/sec,
induced electric field at a radius of 2 cm was 5 x 10"3 V/m) and a 72-Hz repeating single pulse
(380-microsecond positive pulse width, 4.5 microseconds negative spike, 3.5 mT peak
magnetic field, rate of change of field was 9200 mT/second, induced electric field at a radius of
2 cm was 9.2 x 10"2 V/m). Autoradiographs of the salivary gland chromosomes, particularly
the X chromosome, showed similar induction of transcription for both EM field types. The
grain patterns were consistent with induction of mRNA gene sites and suggested that
enhanced transcription was occurring at sites normally active at this stage of larval
development. Analysis of RNA on sucrose gradients showed increased incorporation of
tritiated uridine into size classes consistent with processed and unprocessed mRNA (6-10 S
and 20-25 S). When the sine wave frequency was raised to 222 Hz (0.37 mT) or 4400 Hz
(0.018 mT) a similar pattern of induction resulted but to a lesser degree. The relative
transcriptional activity of the 6-10 S size class was inversely correlated with frequency.
Goodman et al. (1987) did a more detailed analysis of grain count distribution over the X
chromosome of Sciara after exposures to 72-Hz single pulse, pulse train, or sinusoidal EM
waves as described in the previous two papers. In addition to enhanced transcription at
normally active sites, they also found transcription occurring at sites not detectably active in
control cells. The response was qualitatively the same with the three different fields but the
sinusoidal and single pulse fields were' more effective than the pulse train field.
Goodman and Henderson (1988), again using the S. coprophila salivary gland system,
reported altered polypeptide synthesis following exposure to ELF fields of various waveforms
and frequencies. Table 5-4 summarizes the exposures used.
The polypeptide patterns obtained by two-dimensional gel electrophoresis were
qualitatively and quantitatively different for each type of exposure and different from control
and heat-shocked cells; however, conclusions about specific effects of the different types of
exposure are not possible. Individual proteins were not identified, and it is not possible to
ascribe the observed effects to either the electric field or the magnetic field. No conclusions
could be made concerning any possible effect of frequency.
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TABLE 5-4. CHARACTERISTICS OF ELECTROMAGNETIC FIELDS TESTED
Frequency
(Hz)
72
15
1.5
72
60
Positive
induced
amplitude
(mV)
15
14.5
2.5
0.8
0.8
Positive
duration
(Msec)
380
200
250
Burst
width
(msec)
5
30
Negative
space
(Msec)
28
10
Negative
spike
(Msec)
4500
24
4
Peak
magnetic
field
(mT)
3.5
1.9
0.38
1.1
1.5
Electric
field
(V/m)
9x10'3
9x10'3
1.5x10'3
5x10"*
5x10"*
An effect of magnetic fields has also been shown on the lac operon system by Aarholt et
al. (1982). In this system the beta-galactosidase gene is under control of the lac operon and is
normally repressed by a represser protein. If the dynamic equilibrium between synthesis and
degradation of the represser protein is changed, changes in rate of synthesis of beta-
galactosidase should be seen. The authors exposed the bacteria to a 50-Hz square wave
magnetic field varying from 0 to 0.7 mT and measured beta-galactosidase synthesis. The rate
of synthesis was quite dependent on field strength; it started to decrease at 0.27 mT, was less
than one-third of the control rate at 0.30 mT, then increased to the control rate by 0.32 mT.
The rate remained at the control level until the field intensity reached about 0.51 mT when the
rate began to increase, reaching more than twice the control rate at 0.54 mT. The rate fell
sharply beyond 0.56 mT and returned to the control rate again at 0.58 mT. The field strength
effect on synthesis rate was strongly dependent on cell concentration. The field strength
dependence was seen at 1.5 x 107 celis/mL (the lowest cell concentration reported), remained
constant until about 3 x 107, increased to its greatest level between 3.6 x 107 and 5.0 x 107
cells/mL, and disappeared above 1 x 108 cells/mL The effect is maximum when the
intercellular distance is about 30 m and is no longer present when the intercellular distance is
less than 20 ju.m. The mechanism of the observed effects in not understood; however, based
on the work reported in this paper and on work by others cited in this paper, the authors
speculate that the effect involves the represser protein rather than the DMA.
The following comment is not intended as additional proof of a transcription-inducing
potential of ELF fields but is intended to show that this is a rapidly developing area and
additional peer-reviewed publications should soon be available. A number of meeting
abstracts and presentations have appeared in the past year showing transcriptional changes
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in cells (including human and other mammalian cells) exposed to ELF electromagnetic and
magnetic fields. Oncogenes are among the genes induced.
5.3.2. Radiofrequency Electromagnetic Fields
Cell transformation has also been demonstrated following microwave exposure. This
subject is included here on the assumption that the transformed phenotype results ultimately
from altered gene expression.
Balcer-Kubiczek and Harrison (1 985) presented what they considered to be evidence for
microwave carcinogenesis in vitro. Their conclusion was based on an observed synergistic
effect of pulsed 2.45-GHz microwaves (120 pulses/second, 83-microsecond pulse width,
SAR = 4.4 W/kg) and x-rays on the frequency of malignant transformation of C3H/10T1/2
mouse embryo cells. The synergistic effect was seen only if the cells were treated with the
tumor promotor 12-O-tetradecanoylphorbol-13-acetate (TPA) following exposure. A similar
experiment was done with benzo[a]pyrene instead of x-rays, but no TPA treatment was given.
Temperature of the cell cultures during microwave exposure (37.2 ą 0.1° C) was controlled by
immersing the culture flasks in a constant-temperature water bath, but as discussed
previously, the effective temperature at localized intracellular sites may be higher than the
average culture temperature. Cells were irradiated with microwaves for a total of 24 hours,
either continuously in the presence of 2.5 to 12.5 M benzo[a]pyrene or with an interruption
after 6 hours to allow for exposure to 1 .5 - 6 Gy of 1 00 kV (peak) x-rays. Following exposure
to x-rays, some cultures received 0.1 micrograms per milliliter (^ug/mL) TPA. Results of the
transformation studies are given in Table 5-5. No results are given on induction of cell
TABLE 5-5. EFFECT OF MW IRRADIATION ON TRANSFORMATION FREQUENCY(x 103) IN C3H/10T1/2
MOUSE EMBRYO FIBROBLASTS
Treatment
X-ray only
X-ray + MW
X-ray + TPA
X-ray + MW + TPA
BP only
BP + MW
1.5Gy
0.31
0.40
1.80
6.0
4.5 Gy
2.9
2.9
5.1
8.2
OGy
10.0
10.3
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transformation by microwaves alone or by microwaves plus TPA, obvious experiments when
the authors conclude that the microwave effect is at the initiation phase. Microwave exposure
alone reduced the plating efficiency by about one-half compared to sham-irradiated controls,
while TPA alone increased the plating efficiency by about 40%. TPA addition to
microwave-exposed cells raised the plating efficiency somewhat over that seen after
microwaves alone. The authors speculate that the results were due to a membrane effect with
secondary DMA damage or to an effect on DMA repair, these effects being partially reversed by
TPA, allowing some cells to express the transformed phenotype that would otherwise have
died.
A follow-up study was published by Balcer-Kubiczek and Harrison (1989) to further clarify
the suggestion made in the 1985 study that microwaves alone may act as an initiator of
neoplastic transformation in vitro or interfere with repair of damage caused by other
carcinogens. Exposures of mouse C3H/1OT1/2 cells in culture to 2.45-GHz microwaves
pulsed at 120 pulses per second with an 83-microsecond pulse width for 24 hours, (SAR =
4.4 ą 0.8 W/kg at the cell monolayer) were as given in the previous experiment. Microwaves
alone, without post-irradiation TPA, or TPA alone, produced no transformed foci in the cell
cultures; however, post-irradiation treatment with 0.1 fig TPA/mL led to a significant increase in
transformation frequency over the control level. Therefore, the conclusion is that microwaves,
as used in this experiment, act as an initiator in a two-stage transformation assay. Unlike the
previous study, there was no effect on plating efficiency by any treatment.
5.3.3. Summary
Several experiments by Goodman and colleagues have shown that pulsed and sinusoidal
magnetic fields in the ELF frequency range between 1.5 and 222 Hz have the ability to affect
the transcription (or gene expression) of information from DNA to mRNA in gnat (Sciara
corprophila) larval salivary glands and the translation of the mRNA message into protein
synthesis in the same system. The effect on gene expression is mainly one of enhancing the
activity of genes that are already active at that stage of larval development, but new sites were
also induced by the field. The protein synthesis experiments showed the induction of different
patterns of molecular weight distribution for each of the waveforms used. Exposure of
Escherichia coli bacteria to a 50-Hz square wave magnetic field resulted in a complex
intensity-dependent enhancement and inhibition of the synthesis rate of a specific protein
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known to be under the control of the lac operon and normally repressed by a represser
protein.
Exposure to 2.45-GHz RF radiation pulsed at 120 pulses per second followed by treatment
with the phorbol ester TPA has induced the transformation to malignancy of the mouse
C3H/10T1/2 cell line (Balcer-Kubiczek and Harrison, 1989). In this system the modulated RF
radiation is acting like an initiator in a traditional two-stage cancer promotion protocol in this
cell line.
5.4. CALCIUM EFFLUX FROM BRAIN TISSUE
A rapid change in calcium concentration is essential in many physiologic, metabolic, and
cellular processes (e.g., regulation of nerve membrane excitability, release of neurotransmitter
substances from presynaptic nerve terminals, mitochondrial function, the action ,of cyclic
nucleotides in controlling cellular activity, and the initiation of cell proliferation and tumor
promotion). According to Adey (1988a), alterations in calcium efflux have been demonstrated
with low frequency EM fields, with low frequency electric fields, with combined low frequency
EM and static magnetic fields, and with RF fields amplitude-modulated at low frequencies.
Calcium-ion (Ca++)efflux from brain tissue, sensitive to electric currents applied to brain
tissues in vitro, has been used as a biochemical marker to study the biological effects of EM
fields.
Most studies on calcium efflux have used cerebral tissue. Blackwell and Saunders (1986)
reviewed the effects of low-level RF and microwave radiation on brain tissue and animal
behavior and concluded that there is some evidence for effects of low level EM radiation on
Ca+ + exchange in nervous tissue, but they noted that many experiments reporting positive
effects have been criticized. Examples of calcium efflux studies are presented in the following
section.
5.4.1. Extremely Low Frequency Fields
Bawin and Adey (1976) examined the effect of ELF fields on calcium efflux from chick
cerebral hemispheres, chick striated muscle, and cat cerebral cortex. The tissues, maintained
at 36° C during the experiment, were labelled in vitro with 45Ca++. "Sets" of 10 brain tissues
were exposed for 20 minutes to weak ELF sinusoidal electric fields of 1, 6,16, 32, or 75 Hz
with electric gradients at each frequency of 5,10, 56, or 100 V/m; 50 muscle samples were
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exposed to a 16-Hz, 20 V/m field. Controls consisted of sham-treated samples. The samples
were assayed for radioactivity and the data were smoothed by the removal of counts more
than 1.5 standard deviations away from the mean before statistical evaluation.
The results of these experiments suggested that ELF fields inhibited calcium release from
cerebral tissue and the pattern of inhibition indicated the existence of frequency and amplitude
"windows." In the chick brain, the maximum reduction (p<0.01) occurred at frequencies of 6
and 16 Hz with field gradients of 10 V/m. In the cat tissue, significant reduction in 45Ca+ +
efflux occurred at 6 Hz (p<0.05) and 16 Hz (p<0.01) with 56 V/m gradients. Muscle tissues
were unaffected by field conditions that induced changes in 45Ca+ + efflux from brain tissue.
This study (Bawin and Adey, 1976) has been criticized, however, for the rejection of data that
were more than 1.5 standard deviations away from the mean of the exposed or sham data
before final analysis (Myers and Ross, 1981).
In contrast to the inhibition of Ca++ efflux observed at 16 Hz by Bawin and Adey (1976),
Blackman et al. (1982) demonstrated an enhancement in Ca++ efflux at 16 Hz, but with
different exposure conditions. Bawin and Adey had exposed the samples to an oscillating AC
electric field with only a small magnetic component, whereas Blackman et al. (1982) used an
AC electromagnetic field. Blackman et al. (1985a) tested the hypothesis that the differences in
calcium efflux were due to the AC magnetic component present in the system. The exposure
system consisted of a transmission line exposure chamber in which the electric and magnetic
fields were perpendicular to each other and oriented in the horizontal plane. To expose
samples to an AC electromagnetic field under altered local geomagnetic field (LGF)
conditions, a DC magnetic field was generated by a pair of Helmholtz coils which were placed
around the transmission line. The coils produced a uniform magnetic field within the exposure
chamber that was parallel to the local vector of the geomagnetic field, which was inclined at
85° from the horizontal plane. One of the major findings of the study was that a 15-Hz signal,
effective in inducing a change in calcium efflux when the LGF was 38 tesla (T), was rendered
ineffective when the LGF was reduced to 19 T. Changes in the LGF also rendered ineffective
signals effective. Blackman et al. (1985a) concluded that the AC magnetic component was
essential for the efflux enhancements observed in their laboratory.
Blackman et al. (1985b, 1988b) examined frequency-dependent exposure regions that had
been identified for the efflux of Ca+ + from brain tissue of newly hatched chickens (Gallus
domesticus). The frequency dependence of calcium efflux from the brain preparations (32
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chicks/exposure) was first tested using nine different EM fields, ranging from 1 to 120 Hz [LGF:
0.38 G (0.038 mT), 85° N (inclination of the magnetic field to the horizontal plane of the AC
electric and magnetic components)] (Blackman et al., 1985b). Two effective frequency
regions, one at 15 and 16 Hz and the other between 45 and 105 Hz, were identified. The two
frequency regions were not the same size, and the investigators decided to further
characterize the frequency dependence using higher frequencies (Blackman et al., 1988b).
Thirty-eight frequencies, ranging from 1 to 510 Hz (with a static magnetic field of 0.038 mT at
85° inclination), were tested using 28 to 32 chicks per exposure. The samples were exposed
in a transmission line exposure chamber to crossed electric [15.9 volts root-mean-square per
meter (Vrms/m)] and magnetic [73 nanotesla root-mean-square (nTrms)] fields. Cerebral
hemispheres from newly hatched chickens were removed, halved, and labelled in vitro with
45Ca++. Half of the halved hemispheres were exposed or sham-exposed to the field for 20
minutes. The other half (controls) were incubated for 20 minutes outside the exposure
chamber. The radioactivity in the control sample was used to normalize the radioactivity in the
paired-treated sample to adjust for possible influences caused by differences in sex, age, and
brain mass among the animals, and in the specific activity of the labelling solutions.
When the differences in mean efflux values between exposed and sham-irradiated samples
were compared, there were no discernable patterns of response as a function of frequency.
However, calculation at each frequency of the p-value which combines the difference between
the means of the exposed and sham-exposed groups with the variance of each group
provided the investigators with a basis for hypothesizing the existence of three
frequency-dependent patterns of calcium efflux in the data. One pattern occurred between 15
and 315 Hz, one occurred at 60, 90, and 180 Hz (but not at 300 Hz), and one occurred at 405
Hz. The authors speculated on mechanisms that could be responsible for EM field-induced
changes in calcium-ion efflux, focusing on the initial transduction of electromagnetic energy
into a small physicochemical change. Assuming that the LFG determines the frequencies that
are effective in the transduction step, magnetic resonance mechanisms, either nuclear
magnetic resonance or electron paramagnetic resonance, which operate through the
oscillating magnetic field and require an LGF, are the leading candidates. In nuclear magnetic
resonance, the oscillating magnetic field acts on nuclei with magnetic moments. The
interaction between the time-varying magnetic field and nuclear magnetic moments naturally
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found in biological systems provides the basis for nuclear magnetic resonance imaging
(Blackman et al., 1988b).
Another mechanism, the simple Lorentz-force interaction, in which an oscillating electric
field, or an electric field induced from an oscillating magnetic field, causes charged species to
move in an LGF, was considered as a possible explanation for the pattern of significant results
observed at 60, 90, and 1 80 Hz. The authors state that the usefulness of this model is
hampered by the absence of a known chemical entity that would explain the specific observed
frequencies and LGF field strength.
In a different type of study, Blackman et al. (1 988a) tested the effects of ELF on
field-induced Ca++ efflux in brain tissue of a developing organism. Fertilized eggs of Gallus
domesticus were exposed in a parallel plate apparatus consisting of one ground plate
between two energized plates. During their 21 -day incubation period, the eggs were exposed
continuously to either 50- or 60-Hz sinusoidal electric fields at an average intensity of 1 0
Vrms/m. The LGF in the egg exposure apparatus was 40 microtesla (fiT) (0.04 mT) with an
inclination of 55° N. The ambient 60-Hz magnetic field was less than 70 nanotesia (nT). The
entire apparatus was mounted on a pivot which allowed the eggs to be automatically tilted
through 66° once an hour.
The chickens were removed from the exposure apparatus within 1 .5 days after hatching
and their brains were removed, separated along the midline, and labelled for 30 minutes at 37°
C with radioactive Ca+ +. The assay consisted of a test and a control. A tube containing one
of the brain halves of a pair was placed in the exposure chamber at 37° C (treated sample),
and the tube containing the other brain half was placed in a water bath at 37° C for the
20-minute exposure period (control sample). The samples that had been exposed to either 50
or 60 Hz during incubation were exposed for 20 minutes to either 50- or 60-Hz EM fields at
average values of 15.9 Vrms/m and 73 nTrms (in an LGF of 38 fiT, 85°N to the horizontal plane
of the AC electric and magnetic components). Exposure took place in a transmission line
exposure chamber. Efflux of radioactive Ca+ + from the brains of the treated and control
groups was then measured by standard procedures. The ratios of counts per minute in the
treated (exposed) samples were compared to those of the control samples.
The brains from chicks exposed to 50-Hz fields during incubation and exposed to 60-Hz
fields in vitro exhibited increased calcium efflux (40%, p<0.01 , Bonferroni-adjusted t-tests).
The brains from chicks exposed to 60 Hz during incubation and to 60 Hz in vitro did not. The
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brains from chicks exposed to 60-Hz fields during incubation were not affected by either 50- or
60-Hz fields. The investigators concluded that exposure of the developing chick to ambient
power-line-frequency electric fields, at levels typically found inside homes, can alter the
response of brain tissue to field-induced calcium-ion efflux, but they stated that the
physiological significance of this finding for the intact organism or for other species is not
clear.
5.4.2. Modulated Radiofrequency Fields
Bawin et al. (1975) demonstrated that weak VHF fields, amplitude-modulated at brain wave
frequencies, increased calcium efflux from the isolated brain of the neonatal chick. Ten
forebrains, preincubated with 45Ca++ for 30 minutes, were used for each field condition, and
each condition was tested at least three times. Fields of 147 MHz with field intensities of 1 to 2
mW/cm2 and amplitude-modulated at 0.5 to 35 Hz (modulation depths were kept between 80%
and 90%) were applied for 20 minutes. One group of tissues was irradiated with an
unmodulated carrier wave, and controls were run in the absence of fields. The counts of
radioactivity were normalized before statistical evaluation.
Unmodulated radiations and fields modulated at 0.5 and 3 Hz produced no significant
changes in the 45Ca+ + efflux in comparison with the unirradiated controls. However, fields
modulated at frequencies ranging from 6 to 16 Hz produced a progressive increase in the
45Ca+ + efflux frorrrthe brains (p<0.05 to p<0.01), then a gradual decline in efflux at higher
frequencies. This is indicative of a "windowed" effect, dependent on a narrow band of slow
modulation frequencies.
The Bawin et al. (1975) data evaluation has been criticized by Myers and Ross (1981) for
the presentation of normalized control values, on the basis that normalization removes
important information about variation of the control data between different experimental tests
and between different experiments.
Albert et al. (1987) examined 45Ca+ + efflux from cerebral cortex tissue slices and cerebral
hemispheres that were prepared from Gallus domesticus chicks and exposed to 147-MHz RF
radiation, amplitude-modulated at 16 Hz, and applied at a power density of 0.75 mW/cm2. The
data showed that exposure had no statistically significant effect on 45Ca+ + efflux. These
results are in contrast to the increased Ca++ efflux observed by Blackman et al. (1980) using
the same frequencies. However, Blackman (1987) notes that Albert et al. (1987) tested a
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different intensity (0.75 mW/cm2) from that tested by Blackman et al. (1980) (0.83 mW/cm2),
suggesting the existence of an additional null effect intensity region. In a recent study,
Blackman et al. (1989) confirmed the existence of narrow power density ranges for the
enhancement of Ca+ + efflux from chick forebrain tissue exposed in vitro to 50-MHz RF
electromagnetic radiation (magnetic field: 0.038 mT, 60°N), amplitude-modulated at 16 Hz
utilizing a series of power densities. A statistically significant (p<0.001 to p<0.05)
enhancement of calcium ion efflux was observed at 1.75, 3.85, 5.57, 6.82, 7.65, 7.77, and 8.82
mW/cm2, while no change was observed at 0.75, 2.30, 4.50, 5.85, 7.08, 8.19, 8.66,10.6, and
14.7 mW/cm2. In other words, six windows were observed with five being in a mathematical
relationship to each other. Blackman et al. (1989) speculate that deterministic chaos is the
potential cause of the multiple intensity windows observed. This probability would extend
Fr?lich's model down to the ELF range.
Lin-Liu and Adey (1982) examined the effect of weak sinusoidally modulated microwave
fields on 45Ca++ efflux from synaptosomes undergoing continuous perfusion. Synaptosomes
are isolated subcellular neuronal elements that resemble synaptic terminals in situ. Their
membrane properties can be more easily manipulated than whole brain or tissue slices. The
synaptosomes, prepared in duplicate from the cerebri of male Sprague-Dawley rats, were
loaded with 45Ca+ + and applied to a millipore filter which was placed in the perfusion system
and perfused with Ca-free medium for 45 minutes. One of the duplicate samples served as
control and the other was exposed to the fields during perfusion. The perfusate was collected
at one minute intervals and assayed for radioactivity. The temperature was maintained at 31°
C to minimize synaptosomal autolysis. The 450-MHz field was either unmodulated or
sinusoidally amplitude modulated at 16 or 60 Hz, the unmodulated signal had a power density
of 0.5 mW/cm2 and the modulated signals had the same peak power with a modulation depth
of 75%. The electrical gradient produced by the unmodulated field was 43 V/m in air. The field
intensities used were not expected to cause significant changes in calcium efflux due to
thermal energy transfer. In the perfused, unirradiated samples, the rate of calcium efflux from
the synaptosomes showed a biphasic response, with a fast (half-time, 5 minutes) and slow
(half-time, 40 minutes) phase. The 450-MHz field modulated at 16 Hz, applied for 10 minutes
during the second phase, increased the rate constant for 45Ca+ + by 38% (p<0.01,
Mann-Whitney U test). Unmodulated or 60-Hz modulated signals were not effective.
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These results support the experiments of Bawin et al. (1975,1978) that 16-Hz
amplitude-modulated signals can stimulate the release of preincubated 45Ca++ from isolated
brain tissue.
Shelton and Merritt (1981) failed to demonstrate altered 45Ca++ efflux in rat cerebral tissue
preloaded with 45Ca++ and exposed to pulse-modulated (rather than amplitude-modulated)
microwave radiation (1-GHz carrier frequency) at various power densities (16 Hz at 0.5,1.0,
2.0, or 15 mW/cm2 or 32 Hz at 1.0 or 2.0 mW/cm2). Merritt et al. (1982) were also unable to
alter 45Ca+ + binding to brain tissue with pulse-modulated microwave radiation. Rat brain
tissue was loaded in vivo with 45Ca+ + by intraventricular injection and exposed in vitro to
pulse-modulated 1-GHz radiation (SAR, 0.29 or 2.9 W/kg) or 2.45 GHz (SAR, 0.3 W/kg) and in
vivo to 2.06 GHz (SAR, 0.12 to 2.4 W/kg). Merritt et al. (1982) suggest that because
pulse-modulated and amplitude-modulated signals [such as those used in experiments by
Bawin et al. (1975)] are quite different, the biologic effects induced by them may be different.
Dutta et al. (1984) also reported enhanced Ca++ efflux from human neuroblastoma cell
cultures exposed to RF radiation at 915 MHz, amplitude modulated at 16 Hz at certain narrow
ranges of SAR (0.05 and 1.0 mW/g). Subsequently, Dutta et al. (1989) conducted a similar
study using exposure conditions analogous to those used by Bawin et al. (1975) and
Blackman et al. (1980). Human neuroblastoma cells, labelled with 45Ca++, were exposed for
30 minutes to EM radiation at 147 MHz, sinusoidally amplitude-modulated at 16 Hz at various
SAR values (0.1, 0.05, 0.01, and 0.005 W/kg) (magnetic field: 0.016 mT, 53° inclination).
Calcium-ion efflux was also measured from the human neuroblastoma cells at 147 MHz and
various amplitude modulation frequencies (SAR, 0.05 W/kg) and from human neuroblastoma
cells and hybrid Chinese hamster-mouse neuroblastoma cell lines at 147 MHz, amplitude-
modulated at 16 Hz (SAR, 0.05 W/kg). In all cases the results for the exposed groups were
compared with those for unexposed controls. The respective findings of the three studies
were as follows: significantly enhanced 45Ca+ + efflux was observed at SAR values of 0.05
and 0.005 W/kg (p<0.001 and 0.003, respectively); significant 45Ca++ efflux from human cells
was observed at amplitude modulation frequencies of 16 and 57.5 Hz (p=0.008, and p<0.001,
respectively); and significant enhancement of 45Ca++ efflux was observed in both human and
nonhuman cell lines (p<0.001 for both). These studies show that cell lines derived from
tumors of the human central nervous system respond to modulated RF fields similar to normal
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nervous tissues or cell lines from nervous systems of chicks and cats. These results also
confirm the findings of Bawin et at. and Blackman et al.
In addition to the in vitro effects cited above, EM field-induced alterations in calcium efflux
have been observed in intact animals. Adey et al. (1982) examined the effects of weak,
amplitude-modulated microwave fields on calcium efflux from the cerebral cortex of 23 awake
cats. The cerebral cortex was exposed while the animals were under ether anesthesia and a
plastic cylinder was inserted and placed in contact with the pial surface to make a "cortical
well"; at the conclusion of surgery, ether was discontinued, and the animals were immobilized
with gallium triethiodide for calcium efflux measurements. 45Ca+ + was placed in the wells for
a 90-minute incubation, then the medium was replaced with nonradioactive solution. The
solution was completely exchanged and samples were taken for scintillation counting every 10
minutes for 3 to: 4 hours. Field exposure, initiated at intervals ranging from 80 to 120 minutes
after incubation of the cortex with 45Ca+ +, lasted for 60 minutes. For the efflux experiments,
the 450-MHz field (3.0 mW/cm2) modulated at 16 Hz (modulation depth of 85%) was applied in
an anechoic chamber maintained at 28° C, with the cats oriented at right angles to the field. At
the end of the experiment, the animals were killed with an overdose of phenobarbital, and
cortical samples were taken to measure the depth of 45Ca+ + diffusion. Sham controls were
used in this study, but sham treatment was not detailed.
The efflux of 45Ca+ + from preloaded cat cerebral cortex, not exposed to the experimental
field, followed an exponential pattern with three phases: an initial phase of rapidly declining
efflux, lasting about 10 minutes; an intermediate phase in which the slope of the efflux curve
was somewhat reduced (at 20 to 80 minutes); a third phase of gentle slope starting at about
180 minutes from the beginning of sampling and extending to about 210 minutes. The efflux
curve for the test group followed the control curve until field exposure was initiated 80 to 120
minutes after incubation of the cortex with 45Ca+ + . Following field exposure, the efflux curve
of the exposed group was interrupted by waves of increased 45Ca+ + efflux. The waves had
periods of approximately 20 to 30 minutes and were irregular in amplitude, continuing into the
postexposure period. A comparison of the control and field exposure data with calculated
predicted curves (binomial probability analysis) indicates that the field-exposed efflux curves
comprise a different population from controls at a confidence level of 0.968.
Tissue field measurements, performed in separate studies, showed a field strength of 33
V/m (0.29 W/kg) for the interhemispheric fissure. Measurement of radioactivity in cortical
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samples at the end of the study demonstrated that 45Ca+ + penetrated the tissue at the rate of
1.7 mm/hour.
5.4.3. Unmodulated Radiofrequency Fields
Three of the studies mentioned in the preceding section under Modulated RF/microwave
fields included control groups that were exposed to unmodulated fields and examined for
alterations in calcium efflux or other membrane effects. No changes in calcium efflux were
observed at any of the unmodulated frequencies tested. These studies with brief descriptions
of field conditions are as follows: Bawin et al. (1975) -147 MHz, 1 to 2 mW/cm2, 20 minutes;
Un-Liu and Adey (1982) - 450 MHz, 0.5 mW/cm2,10 minutes; Blackman et al. (1980) -147
MHz, 0.83 and 0 mW/cm2, 20 minutes.
5.4.4. Summary
The preceding studies demonstrate that calcium efflux from brain tissue was increased or
decreased by ELF fields, was decreased or not affected by modulated RF and microwave
fields, and was not affected by unmodulated RF radiation. These responses appear to be
highly dependent on specific field conditions: e.g., frequency, power density, and type of
modulation, emphasizing the complexities involved in comparing one study with another.
Although alterations in Ca+ + efflux indicate some interaction of ELF at the cell membrane, the
physiological significance of this effect is still not fully understood (Blackwell and Saunders,
1986; Blackman et al., 1988a), and a direct relationship between the effect of EM radiation on
calcium efflux and tumor induction or promotion cannot be established at this time.
The experiments of Blackman et al. (1988a) showing frequency selectivity in the calcium
efflux from brain tissue at field strengths of 16 V/m and 0.07 fiJ (crossed electric and magnetic
fields) are the only laboratory studies showing ELF effects at levels comparable to ambient
fields in residential buildings. All nonhuman effects measured in laboratory settings have
occurred at field strengths much higher than ambient levels.
Adey (1988a) proposed that in the amplification stage of transductive coupling, the initial
stimuli associated with EM oscillations elicit a highly cooperative modification of calcium
binding to the glycoproteins that protrude from the membrane surface. Adey (1988a)
suggests that the alteration in calcium binding could spread longitudinally, consistent with the
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direction of flow of extracellular currents associated with physiological activity and with
imposed EM fields.
5.5. INTRACELLULAR ENZYME RESPONSES
5.5.1. Protein Kinases
5.5.1.1. Modulated Radiofrequency Fields
Protein kinases are enzymes that phosphorylate proteins on serine, threonine, or tyrosine
residues. These catalyzed phosphoryiations have profound effects on cellular protein activity
and play a major role in the regulation of a wide range of cellular functions, including signal
transduction and cell proliferation.
Byus et al. (1984) examined the effects of modulated microwave fields on the endogenous
activities of both cAMP-dependent and cAMP-independent protein kinases of cultured human
tonsil lymphocytes. Cells were exposed in a Crawford cell exposure system to a 450-Hz field
(peak intensity, 1.0 mW/cm2), sinusoidally amplitude-modulated at various frequencies
between 3 and 100 Hz for up to 60 minutes; under the exposure conditions, no temperature
rise was detected in the culture medium. Calf thymus histone was used as a substrate for
monitoring kinase activity.
At a modulated field of 16 Hz, no change (relative to controls) was observed in cellular
cAMP-dependent protein kinase activity following 15-, 30-, and 60-minute exposures. The
same exposure condition, however, caused a 50% to 55% decrease in cAMP-independent
protein kinase activity after 15- and 30-minute exposure periods. After longer exposure
periods, 45 and 60 minutes, no detectable change in the enzyme activity was observed,
suggesting that the decrease in enzyme activity at 15 and 30 minutes was transient and
returned to control values even in the presence of continued exposure.
The cAMP-independent kinase activity was also observed to decrease when the field was
modulated at 60 Hz; however the decrease in activity, 15% at 15 minutes and 35% at 30
minutes, was less than that observed at 16 Hz. Again, as in the case with 16-Hz fields, a
60-minute exposure period at 60 Hz produced no decrease in activity, suggesting a transient
effect.
Experiments were also carried out to determine if other modulated frequencies caused
changes in lymphocyte kinase activity. Exposing lymphocytes for 30 minutes to modulated
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frequencies of 3, 6, 80, and 100 Hz or unmodulated 450-Hz carrier caused no apparent
decrease in cAMP-independent cellular kinase activity compared to unexposed controls.
Decreases in kinase activity were observed only at 16, 40, and 60 Hz with the largest decrease
occurring at 16 Hz.
This study clearly demonstrates a "windowed" effect for both time and modulation
frequency in the microwave-induced decrease of lymphocyte cAMP-independent protein
kinase activity. The significance of these results is unclear, however. It is not known, for
example, what specific kinase (or kinases) was affected in this study. The authors of the study
state that".. .our data offer no insight into the real biological effect of these fields upon
lymphocyte function in particular, or upon the general state of the immune system." Although
the significance of the results are unclear, it should be emphasized that any effect on protein
kinase activity of the magnitude observed in this study would be expected to have significant
effects on cellular activity because of the major role played by kinases in the control of cellular
function. For example, the attenuation of cellular responsiveness (termed desensitization)
following plasma membrane receptor activation is known to be controlled in some signal
transduction systems through receptor phosphorylation by specific kinases. Any unwarranted
decrease in the activity of one of these kinases, therefore, could cause perturbations in the
signal system by allowing the receptor to be "on" for a longer period than appropriate. The
B-adrenergic receptor is an example of a plasma membrane receptor which is known to be
desensitized via phosphorylation by a specific cAMP-independent protein kinase (Benovic et
al., 1989).
5.5.2. Ornithine Decarboxylase Activity
The enzyme ornithine decarboxylase (ODC) is the controlling enzyme in polyamine
biosynthesis and is affected by a wide variety of hormones and growth factors active at the cell
surface (reviewed by Byus et ai., 1987); the activity of ODC can change rapidly and markedly
in response to extracellular signals. ODC activity is elevated in all rapidly growing cells
including transformed or cancer cells, and is increased by phorbol ester tumor-promoting
compounds (reviewed by Byus et al., 1987). The following studies examined the effects of ELF
and modulated RF and microwave fields on ODC activity in established cell lines.
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5.5.2.1. Extremely Low Frequency Fields
Byus et at. (1987) investigated the effects of a low-energy 60-Hz field on ODC activity in
human lymphoma GEM ceils, mouse myeloma cells (P3), and Reuber H35 hepatoma cells.
The exposure conditions were designed to allow the cell cultures to be physically isolated from
any possible products of electrolysis at the carbon electrodes following field exposure. GEM
and P3 cells were tested in suspension culture in a series of tissue culture flasks connected by
tubing filled with agar gel. During field exposure a small current [368 microamperes(^A)] was
passed through the flasks. This current produced an electric field of 10 millivolts per
centimeter (mV/cm) (1 V/m) in the suspension. This field was uniform over 80% of the area of
the culture flask. The cultures were exposed to the field for 1 hour, and ODC activities were
compared to those of sham-exposed control cultures at time points ranging from 0 to 4 hours
after exposure.
A 1-hour exposure to the 60-Hz EM field with an intensity of 10 millivolts per centimeter
[mV/cm (1 V/m) produced a threefold increase in ODC activity in human lymphoma GEM cells
immediately after exposure. The activity continued to increase for 1 hour after exposure to a
level fivefold greater than control cultures, then returned to control levels within 2 to 4 hours of
exposure. P3 cells, exposed in the same apparatus to the 60-Hz field for 1 hour, exhibited no
increase in ODC activity immediately after field exposure, but did show a two- to threefold
increase in activity during the 1- to 2-hour period following exposure; the activity had returned
to normal by 3 hours.
Reuber H35 hepatoma cells were exposed to the 60-Hz field for one hour in monolayer
culture in square Petri dishes connected by agar bridges. This system was developed to
obtain greater uniformity in current distribution using low field intensities [0.1-10 mV/cm (0.01-1
V/m)]. Since the resistivity of the culture medium is 50 ohm-cm, the current densities
corresponding to these electric fields are 2 to 200^A/cm2. ODC activity in the field-exposed
cultures was compared to that of sham-exposed cultures 1, 2, and 3 hours after exposure.
The response of the H35 cells was not a typical logarithmic dose-response relationship
between field strength and degree of ODC induction. Exposure of the cells at an intensity of
10 mV/cm (1 V/m), to a 60-Hz field for 1 hour elicited an increase in ODC activity of nearly 50%,
which returned to control level by 1 hour after exposure. The ODC activity was only slightly
increased by the 5.0-mV/cm (0.5 V/m) field, was not increased by a 1-mV/cm (0.1 V/m) field,
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but was increased 30% by the much smaller field of 0.1 mV/cm (0.01 V/m). These data were
not analyzed statistically. In addition, the H35 cells were exposed continuously to the 60-Hz
[10 mV/cm (1.0 V/m)] field for 2 and 3 hours. The 2-hour exposure had no effect on enzyme
activity and the 3-hour exposure actually decreased activity in comparison to controls. At no
time during the 1- to 3-hour exposures did the temperature of the medium change by more
than 0.1° C.
The authors' major conclusion from these experiments is that 60-Hz EM fields, similar in
type and intensity to those found in the environment, increase the activity of the enzyme ODC
inside the cell (Byus et al., 1987). The investigators could not explain the heterogeneity of
response between the different cells. They also did not attempt to explain why the response
induced by 0.1 mV/cm was as large as at the highest field (10 mV/cm) while only background
rates were observed at 5.0 and 1.0 mV/cm.
As we have shown in Section 1.2 of this document, typical domestic 60-Hz fields of 0.1 pT
and 33 V/m produce internal currents and electric fields on the order of 10'5 //A/cm2 and 10"6
V/m. The effects produced by Byus et al. (1987) in these experiments were induced by cellular
currents of 200^A/cm2 and electric fields in the cell medium of 1 V/m. This is at least 1 million
times higher than internal currents and fields induced by ambient exposures. The authors, in
stating the similarity of their experimental conditions to background fields, referred to external
ambient fields rather than to the internal fields experienced by the cells.
5.5.2.2. Modulated Radiofrequency Fields
Byus et al. (1988) examined the effects of frequency-modulated microwave radiation and
TPA, a phorbol ester tumor-promoting agent, on ODC activity in cell cultures. The following
experiments were performed:
Reuber H35 hepatoma cells, Chinese hamster ovary (CHO) cells, and 294T melanoma
cells were exposed in circular Petri dishes in a Crawford cell exposure system, to fields
of 450 MHz, 1.0 mW/cm2, sinusoidally amplitude-modulated at 16 Hz; controls were
sham exposed;
Reuber H35 hepatoma cells were exposed to the 450-MHz fields modulated at 5,10,
16, 20, 60, or 100 Hz; controls were sham exposed;
Reuber H35 hepatoma cells and CHO cells, either exposed to the 450-MHz field
modulated to 16 Hz or sham-exposed for 1 hour, were treated immediately with TPA.
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The cultures were irradiated or sham-irradiated for 1 hour; modulation depth of the field
was maintained at 75%-85%; there were no changes in the temperature of the culture medium
between the beginning and end of exposure in any of the experiments. ODC activity was
measured at various times ranging from 1 to 5 hours after exposure to the field or after
addition of TPA. An additional experiment was performed in which DNA synthesis was
determined in H35 cells that had been irradiated with a real or sham field for 1 hour and
treated with TPA.
In all three cell types a 1-hour exposure produced a notable (up to 50%) increase in ODC
activity when compared with unexposed cultures. ODC activity remained elevated in the
field-exposed Reuber H35 and CHO cell cultures for more than 3 hours following removal from
the field, but persisted for only 1 hour in the 294T melanoma cell cultures.
In the experiment in which the Reuber H35 hepatoma cells were exposed to the various
modulated 450 MHz fields, modulation frequencies of 60 and 100 Hz failed to alter ODC
activity in cultures to the field for 1 hour, whereas the modulation frequency of 16 Hz caused a
50% increase in enzyme activity. ODC activity was also increased at modulation frequencies
of 10 and 20 Hz, but to a lesser degree.
The effect of the modulated microwave radiation on the induction of ODC by phorbol
esters (TPA) was also tested in Reuber H35 cells and CHO cells. ODC activity, which is known
to be stimulated by TPA, was further stimulated in H35 and CHO cells which were previously
exposed for 1 hour to the 450-MHz field modulated at 16 Hz before treatment with TPA. This
effect was most evident in the H35 cells 4 and 5 hours after addition of TPA (-13% increase),
and in CHO cells 3, 4, and 5 hours after addition of TPA (-50% increase). A1-hour exposure
to the same field did not alter either sham-control DNA synthesis or TPA-stimulated DNA
synthesis, as measured by [3H]thymidine incorporation, indicating that the increase in ODC
activity is not an effect secondary to the stimulation of cell division.
Byus et al. (1988) noted that brief exposure of the cells to the EM field altered their
responsiveness to TPA. TPA has been shown to have a specific cellular receptor which, when
activated, becomes associated with the plasma membrane. This phorbol ester receptor has
been identified as a calcium and phospholipid-dependent protein kinase and given the
designation, protein kinase C. Protein kinase C, which is a cAMP-independent enzyme, has
been implicated in the regulation of a variety of cellular events, including modulation of
receptor functions for the major classes of hormones, adenylate cyclase activity, induction of
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ornithine decarboxylase, and the induction of cell proliferation (reviewed by Byus et al., 1988).
The results of this study are consistent with the idea that protein kinase C may be a target for
low energy EM fields, leading sequentially to a variety of altered intracellular events (Byus et
al., 1988).
5.5.3. Summary
In an examination of modulated microwave fields on cellular protein kinase activity in
human lymphocytes, Byus et al. (1984) demonstrated a "windowed" effect (for both time and
frequency) for the microwave-induced decrease in cAMP-independent protein kinase activity.
(No effect was observed on cAMP-dependent protein kinase activity.) The maximum decrease
in activity (50%-55%) was observed at 16 Hz with lesser amounts of decrease at 40 and 60 Hz;
temporally, the decrease in activity was maximum after 15- to 30-minute exposures, and by 60
minutes the activity returned to normal. This microwave-mediated decrease in protein kinase
activity may have important implications for hormone receptor function and the regulation of
cell proliferation.
The studies of Byus et al. (1987,1988) have also shown that ELF and low energy
amplitude modulated microwave fields can increase ODC activity in various cell types.
Maximum ODC induction occurred in the range of 10 to 20 Hz, corresponding to the
frequency-dependent responses in brain tissue CA+ + efflux, both for low frequency fields and
for RF fields modulated at low frequencies (Bawin and Adey, 1976; Bawin et al., 1975).
Byus et al. (1988) also demonstrated a potentiation by modulated fields of TPA-stimulated
ODC activity in cultured cells.
5.6. PARATHYROID HORMONE AND THE PLASMA MEMBRANE
Collagen is synthesized by osteoblasts and represents 90% of the organic matrix of bone
(Rosen and Luben, 1983). Collagen synthesis in cultured rat bones can be increased by
treatment with insulin and glucocorticoids, and can be decreased by parathyroid hormone
(PTH) and 1,25-dihydroxyvitamin D3 (reviewed by Rosen and Luben, 1983). It appears that
collagen may be important in the calcification of bone matrix (Bloom and Fawcett, 1969). Low
energy EM fields pulsed at frequencies of 10 to 90 Hz are used to stimulate the healing of
chronically ununited fractures in humans (Luben et al., 1982). The mechanisms of action of
these fields, thought to be triggered at the cell membrane, have been studied in vitro with an
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isolated osteoblast-like cell line (MMB-1) and whole bone, using collagen synthesis and other
end points as markers (Luben et al., 1982; Rosen and Luben, 1983; Cain and Luben, 1987).
In bone cells, PTH and osteoclast-activating factor (OAF), both acting through cell
membrane receptors, stimulate both the activation of adenylate cyclase to form cAMP and
inhibit collagen synthesis (Cain and Luben, 1987; Rosen and Luben, 1983). Vitamin D3 also
inhibits collagen synthesis, but via a cytoplasmic rather than a membrane receptor.
5.6.1. Extremely Low Frequency Fields
Luben et al. (1982) exposed cultured cranial bone from 3-day-old mice and MMB-1 cells (a
line developed from primary cultures of mouse cranial bone cells) to EM fields similar to those
used clinically to stimulate the healing of bone fractures, and then examined the responses of
the cells to PTH, OAF, or vitamin D3 (Table 5-6). The tissues and cells were exposed, in
incubators, to two pulsed fields of approximately 20 G (2.0 mT). One field, "single pulse,
patient" (SPP), consisted of a continuous train of single pulses at a frequency of 72 Hz. Each
pulse had an initial component 325 seconds long, with a drop of 20% between the peak of the
rising phase and the onset of the falling phase. The falling phase had an overshoot of
opposite polarity with a typical peak amplitude 20% of the initial deflection. The other field,
"pulse train, patient" (PTP), consisted of bursts of pulses produced at a 4-kHz rate, each burst
lasting 5 microseconds and being repeated at a 15-Hz rate. The initial pulse was 200 seconds
long, and it was followed by a deflection of opposite polarity lasting 18.5 microseconds and
limited in amplitude to 20% of the initial deflection. The magnetic fields for both SPP and PTP
induced electrical gradients of ~1.0 mV/cm (0.1 V/m) around a 1 -cm loop in the spatially
TABLE 5-6. EFFECTS OF FIELDS ON cAMP ACCUMULATION IN BONE CELL MONOLAYERS
Agent
None
PTH
PTH
PTH
OAF
OAF
Dose
ng/mL
10
30
100
1
10
cAMP.
No Reid
2.1 ą 0.3
5.7 ą 0.8a
8.3 ą 1.0a
11.6ą 1.8a
9.3 ą 0.9a
13.8+ 2.1a
Dmol per 106 cells (% no field, aaent control*
SPP Reid
3.1 ą 0.6
3.3 ą 0.4 (58%)
4.1 ą 0.8 (49%)
5.3 ą 0.5a(46%)
4.2 ą 0.6 (45%)
5.6 ą 0.7(41%)
PTP Reid
2.3 + 0.5
2.6 ą 0.4(46%)
3.5 ą 0.6 (42%)
4.9 ą 0.8a(42%)
3.3 ą 0.5 (35%)
4.3 ą 0.8a(31%)
Significantly different from control (no field), p<0.05. Paired t tests indicated no significant differences be-
tween effects of SPP and PTP fields at any dose.
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homogeneous portion of the field between the coils; the peak extracellular current density in
homogeneous conducting electrolytes would be ~1.0/Wcm2.
The cells were exposed for 12, 72, or 90 hours in the fields, then were removed and treated
with either PTH, OAF, or 1,25-dihydroxyvitamin D3. Assays were performed for cAMP
accumulation, adenylate cyclase activity, and/or collagen synthesis. In addition, total
adenylate cyclase catalytic units in the membrane were assessed by activation with fluoride.
(In this assay, MMB-1 cells were grown in the presence or absence of the SPP field for 72
hours and then removed; cell layers were disrupted to prepare membranes for adenylate
cyclase assay and the membranes were treated in the absence of fields with either PTH or 1
millimolar (mM) sodium fluoride, and the amount of cAMP formed was determined by
radioimmunoassay.) The controls were treated with (1) no agent, no field (shielded); (2)
agents, but no field; (3) no agent, but fields. In the assays for cAMP accumulation, adenylate
cyclase activity, and collagen synthesis, no statistically significant differences were observed
between the no agent, no field controls (1) and the no agent, field exposed controls (3).
The major findings of this study are as follows:
The production of cAMP by the bone cell monolayers was significantly increased
(p<0.05) in the no-field controls by PTH and OAF. This increase did not occur when
preparations were pretreated with each of the fields, particularly in the groups treated
with 100 nanograms per milliliter (ng/mL) PTH and with 10 ng/mL OAF (Table 5-6).
Neither basal nor fluoride-activated adenylate cyclase activity were altered in
membranes from cells cultured in the fields.
The inhibitory effects of PTH on collagen synthesis, as measured by the incorporation
of [3H]proline, were blocked in cells grown for 12 hours in the presence of the SPP
field. The cells were exposed only to the SPP field and only for 12 hours; labelling with
[3H]proline took place 42 to 48 hours after field exposure.
The fields had no effect on the inhibitory effects of 1,25-dihydroxyvitamin D3) thought to
act by a cytoplasmic, rather than by a membrane-dependent mechanism.
The investigators suggest that because the fields inhibited the activities of PTH and OAF
(which have membrane receptors), but did not change the activity of 1,25-dihydroxyvitamin DS
(which has a cytoplasmic receptor), the cell membrane is probably the primary site of
interaction with the EM field. The fact that PTH-activated plasma membrane adenylate cyclase
was inhibited by the field, and the fact that adenylate cyclase catalytic units in the cell
membrane and basal cyclase activity were not, suggests that the fields were not acting directly
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on the cyclase, but that they were interfering with the binding of hormone to receptor, the
ability of the hormone-receptor complex to activate cyclase, or both. The other possible target
for the fields is the coupling of the hormone-receptor complex to adenylate cyclase in the
membrane. This type of effect could be mediated either directly, by effects on the intrinsic
membrane coupling proteins or indirectly, by modification of other membrane functions (Luben
etal., 1982).
Cain and Luben (1987) conducted further in vitro studies to elucidate the biochemical
mechanisms of EM-field effects on bone healing by examining the effects of exposure to
pulsed fields on PTH-stimulated cAMP accumulation and bone resorption in mouse calvaria
(the superior portion of the cranium). In contrast to the study of Luben et al. (1982) in which
cells were exposed to the field for 12 or more hours, the cranial bones from newborn Swiss
mice in the present study were placed in culture medium and exposed to pulsed EM fields
(PEMF) of extremely low frequency for only 1 hour. The exposure system consisted of a 10-
cm x 10-cm Helmholtz coil kept in a humidified incubator at 37° C and 5% carbon dioxide; the
generator unit remained outside the incubator. The waveform parameters used in the
experiments were a positive pulse at 100 microseconds and a negative pulse of 2
microseconds, repeated at a frequency of 15 Hz. The induced magnetic field was
approximately 8 G (0.8 ml) with an electric field strength of 0.6 mV/cm (60 mV/m) and a
current density of 20/Wcm2 in the medium. The control bones were shielded during PEMF
exposure.
The investigators selected this system for its usefulness in observing early and late
responses to PTH which acts on the cell through plasma membrane receptors. The early
response to PTH can be detected as early as 1 minute after exposure to the hormone by
monitoring cellular increases in the production of cAMP. The late response, bone resorption
(monitored by release of extracellular Ca++ from the bone matrix), can be measured 72 hours
after hormone treatment.
For the cAMP assay, cranial bones were exposed to the PEMF for 1 hour and incubated
for 30 minutes in medium with 5 mM theophylline, a phosphodiesterase inhibitor, which inhibits
the breakdown of the accumulated cAMP. The bones were then treated with PTH and were
rapidly "killed" in a microwave oven. cAMP levels were measured by radioimmunoassay.
Following a 1-hour exposure to PEMF and a subsequent 30-minute incubation with
theophylline, the inhibition of PTH-stimulated cAMP accumulation was observed, similar to that
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reported by Luben et al. (1982), but more subtle. The observation was complicated by the fact
that exposure to PEMF accelerated the time course of cAMP response to PTH. cAMP levels in
field-exposed bones peaked after 3-minutes of exposure to PTH, whereas that in the
unexposed bones peaked after 5 minutes. As a result, the cAMP levels of the unexposed
bones were significantly lower (p<0.05) than those of the field-exposed bones at 3 minutes.
However, the cAMP accumulation in the field-exposed bones decreased within 5 minutes and
remained lower than the control levels throughout the 11 -minute observation period.
For the bone resorption experiments, the neonates were injected subcutaneously with
45Ca+* 72 hours before the cranial bones were removed. Following incubations of 6 to 24
hours, to equilibrate exchangeable Ca++, the bones were irradiated for 1 to 5 hours. Within
30 minutes after removal from the field, treatment with various concentrations of PTH was
begun. After preincubation and field exposure, some bones were "killed" by alternate freezing
and thawing. Those not frozen were called "live" bones. The bones were then cultured in
medium (37° C, 5% carbon dioxide) and were decalcified. The percentage of bone calcium
released during 72 hours of culture was determined by comparing 45Ca radioactivity in the
medium versus that remaining in the bones. The percent release for "dead" bones was
subtracted from the percent release of live bones. The results of the experiments were based
on pooled samples.
The main result of the bone resorption experiment was that a field exposure for 1 to 5
hours altered 45Ca++ release measured 72 hours after hormone treatment and field exposure.
At submaximal PTH doses [2.3 nanomolar (nM) and 6.9 nM], 1 - to 5-hour field exposures
inhibited bone resorption (35% and 44%, respectively), but at the maximal dose of PTH, 23 nM,
field exposures did not inhibit resorption. In the absence of PTH, basal bone resorption of
6.17% was increased to 8.66% (a 40% increase) after a 1-hour field exposure (a 5-hour field
exposure was not tested in this part of the study), but basal cAMP levels were not affected.
The investigators noted that the data from this study showing that PEMF inhibited the
hormonal action of PTH, cAMP accumulation, and bone resorption are consistent with the
hypothesis that field perturbation occurs at the membrane level.
5.6.2. Modulated Radiofrequency Fields
No data were found.
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5.6.3. Unmodulated Radiofrequency Fields
No data were found.
5.6.4. Summary
The preceding studies show that pulsed magnetic fields inhibit the hormonal action of
parathyroid hormone, which is to increase the concentration of cAMP, decrease the rate of
collagen synthesis in bone cell cultures, and increase the rate of bone resorption. This action
occurs at plasma membrane PTH receptors. These experiments indicate that pulsed magnetic
fields interfere with the signal transduction system which is mediated by the binding of PTH to
its plasma membrane receptor. Inasmuch as cell proliferation is also thought to be mediated
through the activation of multiple signal transduction systems, it is possible that ELF also has
the potential for causing changes in some of these systems and thus could have an effect on
cell growth including the growth of preneoplastic lesions and tumors.
5.7. MELATONIN AND OTHER HORMONES
In the previous section, the effects of ELF fields on parathyroid hormone-dependent
aspects of collagen synthesis were examined. Another endocrine gland, the pineal, and its
hormones have been associated with certain forms of breast and prostate cancer in humans
and with cancer induction in animals.
5.7.1. Background: Melatonin and Cancer
Various investigators have reported an association of melatonin secretion with cancer in
humans, particularly certain forms of prostate and breast cancer. Fraschini et al. (1988)
examined 254 cancer patients and found increased serum melatonin levels in 99 cases
(38.9%), decreased levels in 15 cases (5.9%), and no change in 140 cases (55.2%). Mean
serum melatonin levels were significantly higher in cancer patients compared with 98 healthy
controls (p<0.0001). Regardless of cancer type, serum melatonin levels were higher in cancer
patients compared with controls: breast and lung cancer, p<0.001; colorectal and gastric
cancer, p<0.005; soft tissue sarcoma, p<0.01; and lymphoma, p<0.025. Fraschini et al.
(1988) also observed that 66.7% of the patients whose tumors responded to chemotherapy
also exhibited increased serum melatonin levels following chemotherapy.
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Cohen et al. (1978) proposed that reduced pineal melatonin secretion may be a factor in
breast cancer risk. Bartsch et al. (1981, cited in Wilson et al., 1988) reported that women with
breast cancer had reduced urinary melatonin levels. Danforth et al. (1982) noted altered
melatonin secretion in patients with estrogen-positive breast cancer. Bartsch et al. (1985)
reported that men with cancer of the prostate had lower nocturnal melatonin levels than men
without the disease. Stevens (1987) suggested that ELF field-induced exposure in rats may
result in loss of gonadal downregulation, resulting in increased circulating estrogen levels
which may in turn stimulate mammary tissue proliferation and hence increase breast cancer
risk.
Tamarkin et al. (1981) reported that melatonin alters dimethylbenz[a]anthracene (DMBA)
mammary carcinogenicity. Fifty-day-old rats were given 15 mg of DMBA and were divided into
four groups: (1) DMBA + vehicle; (2) DMBA + daily melatonin injections (beginning at day
50); (3) DMBA + pinealectomy (at day 20); and (4) DMBA + pinealectomy + melatonin.
Group 2 had significantly fewer mammary tumors than group 1 (controls), indicating that
melatonin inhibited carcinogenesis by DMBA; group 3 had more tumors than group 1,
indicating that removal of the pineal enhanced carcinogenesis; and group 4 had fewer tumors
than groups 1 or 3, indicating that melatonin ameliorated the adverse effects of pinealectomy.
From their studies, which demonstrated that rats constantly exposed to light had increased
DMBA-induced mammary tumors, Shah et al. (1984) and Mhatre et al. (1984) concluded that
constant light from birth effectively deprives female rats of melatonin and leads to a constant
availability of estrogen and elevated circulating prolactin, which increases the turnover of the
breast epithelial cells, thereby rendering the breast tissue more vulnerable to the
carcinogenicity of DMBA. Some experiments in rodents have shown an increase in mammary
cancer on administration of estrogen and of prolactin (Henderson and Pike, 1981).
Immune and neuroendocrine functions cooperate closely to protect the organism from
external attacks (Maestroni et al., 1988). Maestroni et al. (1988) demonstrated in experimental
studies with mice that melatonin has a general "up-regulatory" effect on the immune system.
Exogenous melatonin can counteract the effect of acute stress and/or of pharmacologic
corticosterone on antibody production, thymus weight and antiviral resistance. Maestroni et
al. (1988) suggest that activation of T lymphocytes is necessary for the immuno-enhancing
and anti-stress action of melatonin.
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Melatonin can either stimulate or inhibit cell proliferation, apparently depending on dosage.
Blask and Hill (1986) have shown that physiologic levels of melatonin inhibit cancer cell
growth, while sub- and super-physiologic levels of melatonin do not. A melatonin-induced
proliferation of the erythroid- and myeloid-bone-marrow cell compartments has been observed
which apparently extends to all body cells (Di Bella et al., 1979). The growth of lung, stomach,
and breast cancers; lymphoma; and bone sarcoma were depressed with melatonin treatment;
the survival time of patients was increased and symptoms alleviated (Di Bella et al., 1979).
This treatment is potentiated by simultaneously lowering the levels of circulating growth
hormone. In vitro, melatonin exhibits oncostatic properties against certain cancer cell lines
including carcinomas and breast cancer (Blask and Hill, 1986; Rodin, 1963). Melatonin has
also been used in the treatment of leukopenia, in both chronic and acute lymphoblastic
leukemia and during antiblastic chemotherapy (DiBella et al., 1979). In contrast, there have
been other reports indicating that the pineal gland either has no effect on or stimulates the
growth of some tumors (Kachi et al., 1988).
The inconsistent results of animal studies on the pineal gland and its hormones could be
due to the dependence of pineal response on the photoperiodic environment (Reiter, 1988).
Of particular importance is the timing of the administration of melatonin, which is most effective
in pineal-intact animals when given late in the light period (Reiter, 1988).
5.7.2. Extremely Low Frequency Fields
Based on experimental evidence that shows an effect of light and ELF electric and/or
magnetic fields on pineal melatonin production, and on the relationship of melatonin to
mammary carcinogenesis, Stevens (1987) has proposed a hypothesis that the use of electric
power may increase the risk of breast cancer.
Pineal production of the hormone melatonin, which shows a distinct circadian rhythm, is
suppressed by light. The circadian rhythm is evident in blood and pineal gland levels of
melatonin: low levels in daylight and high levels at night (Tamarkin et al., 1985). Melatonin, in
turn, suppresses prolactin production by the pituitary and estrogen production by the ovary
(Mhatre et al., 1984).
If circulating levels of melatonin are reduced (by pinealectomy or constant-light exposure),
the growth of DMBA-induced mammary tumors in the rat is accelerated (see Section 5.7.1).
Stevens (1987) proposes a scheme through which long-term exposure to ELF fields may act
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as a "functional pinealectomy" and enhance mammary DMBA-induced carcinogenesis in rats
(Figure 5-1). The hypothesis is based on the idea that melatonin level affects production of
prolactin and estrogen, and that it is the action of these hormones that increases breast
cancer risk by increasing stem cell turnover. In addition, Wilson et al. (1988) propose that ELF
may also have an effect on steroid hormone-promoted prostate cancers.
Wilson et al. (1981,1986) demonstrated that melatonin production can be suppressed by a
60-Hz field. Male Sprague-Dawley rats were acclimated to a daily 14-hour light: 10-hour dark
photoperiod at 21° C and 20% to 40% relative humidity (Wilson et al., 1981). At 56 days of
age, 20 animals in electrical contact with the reference ground electrode were exposed to a
uniform, vertical 60-Hz field (field strength, 1.7 to 1.9 kV/m) in a parallel-plate exposure system.
The animals were exposed 20 hours per day for 30 days. At the end of exposure, animals
were killed in groups of 10 (5 exposed, 5 sham-exposed) at four different times during the
light/dark cycle (1400 [light], 2200 [dark], 0200 [dark], and 0800 [light] hours). All conditions
were the same for the exposed and sham-exposed animals except for the presence or
absence of the electric field. Pineal glands were removed and quick-frozen usually within 2
Chronic 60-Hz Electric Field
Pineal Gland: Reduced Melatonin Production
Ovary: Constant Estrogen
Piituitary: Constant Prolactin
I
east
I
Increased Turnover of Breast Epithelial Stem Cells at Risk
Increased DMBA Mammary Carcinogenicity
Figure 5-1. Proposed mechanism by which chronic exposure to a 60-Hz electric field may increase
dimethylbenz[ajanthracene (DMBA) -induced mammary carcinogenesis in rats.
SOURCE: Adapted from Stevens, 1987.
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minutes of death. Pineal melatonin was assayed by gas chromatography/mass spectrometry
using an internal standard and the data were analyzed by analysis of variance.
Exposed rats, killed at 0200 hours, showed a significant (p<0.05) reduction in melatonin
levels compared with control rats. During the dark phase, there was a significant increase
(p<0.01) in pineal melatonin of the sham-exposed animals, but no increase in the
field-exposed animals (p<0.20), based on the internal standard. In a duplicate experiment, the
melatonin data followed the same pattern; however, there were large variances in the data, so
the two sampling times in the dark period (2200 and 0200 hours) were combined and the
light-period sampling times (1400 and 0800 hours) were combined. Melatonin levels for
sham-exposed rats differed significantly (p<0.002) between light and dark periods; in contrast,
no significant differences were seen in melatonin levels of exposed animals between dark and
light periods (p>0.05).
In a similar study Wilson et al. (1983) reported that exposure to 60 kV/m also suppressed
the nocturnal increases in melatonin. The suppression of the normal nocturnal increase for
melatonin was consistent with a reduction in serotonin N-acetyl transferase (SNAT) activity (the
rate-limiting enzyme in the synthesis of melatonin from serotonin). Further studies, in which
rats were exposed for 3 weeks to 60-Hz, 39 kV/m electric fields, demonstrated that the time
required for recovery of the melatonin rhythm after cessation of field exposure was less than 3
days, indicating the overall metabolic competence of the pineal is not permanently
compromised by electric-field exposure (Wilson et al., 1986).
5.7.3. Modulated Radiofrequency Fields
No data were found.
5.7.4. Unmodulated Radiofrequency Fields
Elder et al. (1984) reviewed the effects of RF fields on endocrine gland function and
concluded that changes reported in hormonal activities and blood chemistry are similar to
those observed during increased thermoregulatory activity and heat stress and are generally
associated with SARs >1 W/kg. This conclusion is supported by Elder et al. (1987a, b) in an
update of the previous report (Elder et al., 1984). The endocrine effects reported by Elder et
al. (1984) appeared to have occurred in the presence of colonic temperature elevations of 0.3°
C or more.
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5.7.5. Summary
In the preceding sections, studies have been presented that demonstrate that exposure for
3 to 4 weeks to a 60-Hz ELF field suppresses the nocturnal production of melatonin in rats, but
that the overall metabolic competence of the pineal is not permanently compromised.
Studies in humans have shown increased serum melatonin levels following chemotherapy
and decreased urinary levels in some cases of breast and prostate cancer. In addition, animal
and in vitro studies have demonstrated that melatonin can inhibit tumor induction with
chemical carcinogens, can inhibit the growth of established tumors, and can enhance the
cellular immune response. The results of these studies suggest that there is a relationship
between cancer and pineal gland function. In other studies, however, melatonin has had
either no or stimulatory effects on tumor growth. Some of the inconsistencies in these studies
could probably be resolved with improved techniques for dealing with the circadian aspects of
pineal gland function.
The suppressive effects of ELF on pineal melatonin production and the general oncostatic
properties of melatonin in several endocrine-stimulated tumors provide indirect evidence for
the hypothesis that ELF exposure may be a risk factor in the growth of these tumors. Studies
that incorporate all three parameters, ELF exposure, melatonin production, and breast cancer
induction, are needed for further evaluation of this hypothesis.
In other studies, pineal neurological activity and melatonin synthetic activity were inhibited
by static magnetic fields when the orientation of the field was changed by as little as 5
degrees, a change which is only a factor of 10 higher than ambient magnetic residential fields
(Welker et al., 1983; Semm et al., 1980). These studies and the role of the retina as the
magnetoreceptor (Olcese et al., 1985; Reuss and Olcese, 1986) are discussed in greater detail
in Section 5.10.1.
5.8. GROWTH AND DIFFERENTIATION
5.8.1. Extremely Low Frequency Fields
Several studies have demonstrated a growth-enhancing effect of ELF exposures on both
normal and neoplastic cells in vitro. The stimulation of the growth of neoplastic cells is of
particular concern in the therapeutic treatment of bone fractures with ELF fields in cases where
a neoplastic lesion may be present. Because osteogenesis is thought to occur as a result of
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differentiation of osteoblasts (Akamine et al., 1985), information on the effect of ELF on cellular
differentiation is of interest.
McLeod et al. (1987) demonstrated that protein biosynthesis in neonatal bovine fibroblasts
(measured by [3H]proline incorporation into extracellular and intracellular protein) was reduced
by low frequency sine wave electrical fields. Stable low-frequency current with DC flow limited
to less than 0.1 % of the AC amplitude was provided by a programmable current source.
Current was passed through the exposure samples for 12 hours via platinum electrodes that
were separated from the bath by media bridges and convection barriers. Experiments were
performed over a range of current densities (0.1 ^wA/crn2 to 1 mA/cm2, root mean square) and
frequencies (0.1 to 1000 Hz). A frequency- and amplitude-dependent reduction in the rate of
incorporation was observed. The data indicated an optimal frequency range for the alteration
of extracellular matrix protein synthesis. Peak sensitivity was at 10 Hz, with a current density of
only 0.5/Wcm2, at which a notable reduction in protein incorporation in the matrix component
was produced. Furthermore, the response was dependent also on the orientation of the cells
relative to the direction of the applied electric field. The incorporation of radiolabel into
intracellular protein reflected the pattern seen in the extracellular matrix (no other details were
given). The investigators concluded that currents of physiological strength can stimulate a
reduction in biosynthesis and thereby may influence tissue growth, remodeling, and repair.
Whitson et al. (1986), on the other hand, applied 60-Hz, 1000 V/cm (100 kV/m) electric
fields (the authors acknowledge that a magnetic field may also be produced) to human
fibroblasts in vitro for up to 48 hours, and evaluated DNA repair and cell growth or survival. No
effects were observed on any of the parameters examined.
Akamine et al. (1985) examined the effects of a pulsed EM field (PEMF) on the growth and
differentiation of F9 cells, a clonal line of embryonal carcinoma (EC) cells. EC cells are
described as stem cells of teratocarcinoma that resemble undifferentiated cells of early
embryos. These cells can be induced to differentiate to endodermal cells in vitro by treatment
with retinoic acid.
The current was produced by a generator outside a carbon dioxide incubator connected to
two coils located inside the incubator. The coils were positioned so that the generated
magnetic component was normal to the culture surface and so that the induced electric field
becomes stronger as one moves out along a radius on the culture surface. PEMF was begun
12 hours after plating the cells, and the stimulation was continued for 84 hours. The pulse
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width was rectangular, the pulse width was 130 seconds, and the frequency was 100 Hz. The
magnetic field at the center of the field was either 1.0 G (0.1 mT) or 10.0 G (1 mT). Immediately
after exposure the cells were counted and examined for morphological changes and
biochemical assays were conducted for cellular differentiation, based on the production of
plasminogen activator and the synthesis of glycopeptides.
As evidenced by increased cell numbers, PEMF stimulated the growth of F9 cells with
retinoic acid (294% of control at 10 G, 176% of control at 1 G) and without (137% of control at
10 G, 150% of control at 1 G). Based on morphological observations, retinoic acid stimulated
cellular differentiation in 90% of the cells not exposed to the field, in 58% of the ceils exposed
to 1 G, and in 46% of the cells exposed to 10 G. Retinoic acid-stimulated cellular
differentiation was also inhibited when based on production of plasminogen activator, but not
when based on glycopeptide profiles. Thus, the PEMF promoted the growth of the embryonal
carcinoma cells in the presence and absence of retinoic acid and inhibited retinoic
acid-induced differentiation based on morphological observations and on the production of
plasminogen activator. Because field-stimulated growth of carcinoma cells was observed in
these studies, the investigators advised caution in the treatment of malignant tumors with
PEMF.
The clonogenic capacity and surface properties of two human cancer cell lines (Colo 205
and Colo 320, derived from adenocarcinomas of the colon) have been studied by Phillips et al.
(1986a, b) and Phillips and Winters (1987) using a standardized 60-Hz EM-field exposure
system. Changes in colony-formation (a measurement of proliferative capacity) of the cells
were assessed using a soft agar culture technique, and changes in surface properties were
evaluated using a monoclonal antibody binding assay, a transferrin binding assay, and cell
lysis by human NK (natural killer) cells.
Exposures to four different fields were performed concurrently in four exposure chambers.
Exposures consisted of only an electric field [E+; current density = 300 microamperes per
square meter (aA/m2 )= SO^A/cm2)] a magnetic field [M = 1.0 G, 0.1 millitesla
root-mean-square (mTrms)], combined electric and magnetic fields (E+M+; at intensities
indicated), and unexposed control (E-M-). Electric fields were produced by transfer of a
uniform current density through closed system cylindrical cell-exposure chambers that had
been filled completely with the cell suspension. A rotating magnetic field was produced using
two sets of Helmholtz coils, and the insulated glass incubator with plastic cell chamber holders
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was installed within the area of uniformity for the field. The temperature of the chambers never
varied more than 0.15° C and the temperatures of the exposure groups showed no consistent
variation.
Cells were exposed continuously for 24 hours. The cells were then removed from the
chambers and prepared for the assays. Viability was greater than 90% following field
exposure. In five out of five experiments with Colo 320 DM and in four out of five experiments
with Colo 205, cells exposed to M+ and E+M+ produced more colonies than the
sham-exposed control cells, statistically significant at the p<0.01 or p<0.05 levels
(Kruskal-Wallis nonparametric analysis of variance). The cells exposed to E+ only
demonstrated a mixed response (i.e., in some experiments, the numbers of colonies formed by
E+ cells was significantly decreased, while in others the numbers of colonies formed by En-
cells was either significantly increased or remained the same).
The changes in cell-surface properties were assessed by quantifying the binding to the
cells of monoclonal antibodies produced against Colo 205 and Colo 320 DM tumor-associated
antigens. These properties were also altered by field exposure, as evidenced by a general
increase in the expression of tumor-associated antigen in E+M+ and M+ cells. The
alterations were not as dramatic as those observed in the cloning assay, but in several cases
the increases in antibody binding were statistically significant (p<0.01 or p<0.05). The effects
on surface properties of the target cells were consistent with changes in plasma membrane
structure and function following EM-field exposures described by other investigators (Luben et
al., 1982).
Transferrin is the major iron-transport protein in the body and is an obligatory growth factor
for many cells when cultured in serum-free medium (reviewed by Phillips et al., 1986b).
Transferrin receptors are located on the cell surface, more so on the surfaces of malignant or
proliferating normal cells, than on normal nondividing cells, and the number of receptors on a
cell is inversely related to cell density. These may be the receptors for NK cells. In three
separate experiments, the number of transferrin receptors quantitated on Colo 205 cells
exposed to M+ and E+M+ fields were close to or exceeded the maximum theoretical number
of receptors determined for the cell line and were independent of ceil density. Thus, the cells
were no longer subject to the regulatory influence of cell density. E+ cells expressed fewer
transferrin receptors than were predicted on the basis of cell culture density.
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After the initial cloning assays were completed, the cells from the four groups were
transferred for maintenance in long-term culture. After 4 months, increased numbers
(approximately twofold more than E-M- controls) of transferrin receptors were still present on
E+M+ and on M+ cells, while decreased numbers (approximately one-fourth of E-M- controls)
were present on E+ cells; lysis, measured by a standard 51Cr-release assay, was decreased
approximately 70% in both E+M+ and M+ cells but was increased about 53% for E+ cells.
After 8 months in culture, the cells still exhibited an increased reproductive capacity and
increased numbers of transferrin receptors.
In summary, this study has shown that exposure of Colo 205 cells to EM fields resulted in
effects on cellular function, as evidenced by increased reproductive capacity of the cells,
particularly for cells exposed to combined electric and magnetic fields or to the magnetic field
alone. The increased proliferative response was correlated with increased numbers of
transferrin receptors (also indicative of growth potential) in ColoLT cells exposed to
electromagnetic and magnetic fields combined and to magnetic fields alone. The EM-induced
increases in transferrin receptors were also consistent with changes in cell surface properties,
as were increases in the numbers of tumor-associated antigens, and changes in susceptibility
of the cells to lysis by NK cells, especially in cells exposed to E+M+ and M+ fields. The
persistence of these effects suggest that under the conditions of these experiments, EM
exposures are capable of producing significant permanent changes in cellular structure and
function.
It has been suggested that the mechanism for the healing of nonunion bone fractures with
PEMF is related to revascularization of injured osseous structures. To test this hypothesis,
Yen-Patton et al. (1988) examined the effects of PEMF on the rate of repopulation of denuded
areas of endothelial cell monolayers and the rate of endothelial cell neovascularization in
culture. Human umbilical vein endotheiial cells and bovine aortic endothelial cell cultures were
subjected to injury-simulating denuding of a vessel wall and were then exposed, along with
uninjured controls, to the ELF. The field was generated by 22.5-cm x 22.5-cm Helmholtz coils
(waveform 200 seconds wide, shaped as a burst of 20 to 21 closely spaced events); the burst,
5 milliseconds wide, was repeated at 15 Hz, resulting in a calculated induced voltage of 1.3
mV/cm (0.13 V/m) in the tissue culture dish. The magnetic field intensity at the center of the
Helmholtz coils was approximately 1 G, and the rate of change of the magnetic field was 8.5 x
104 G/sec during field expansion and 4.3 x 105 G/sec during field collapse. Under these
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conditions, temperature changes in tissue culture media are <0.001(C (Bassett 1987, as cited
in Yen-Patton et al., 1988).
Reendothelialization was assessed by scintillation counting of live cultures that had been
incubated with tritiated thymidine for up to 96 hours, and injury response (wound healing) was
defined as the difference between thymidine incorporation of injured and uninjured cultures.
Cultures were disrupted by passaging with EDTA-trypsin and monitored for tube formation
(indicative of vascularization) at various intervals for up to 23 days.
In the presence of EM fields, there was a small but statistically significant enhancement in
growth rate of partially denuded endothelial cell monolayers as evidenced by increased
tritiated thymidine incorporation (40% response in the human cells, and 20% response in the
bovine cells). The cells exposed to the fields and entering the denuded regions were
elongated and formed a sprouting pattern, while those outside the field had a more cuboidal
morphology.
Cells that were disrupted and passaged with ethylenediamine tetraacetate-trypsin
reorganized into three-dimensional vessel-like structures after 5 to 8 hours of exposure to the
EM fields and in the presence of endothelial cell growth factor, heparin, and a component
fibronectin (protein) matrix. In the absence of EM fields, vascularization of confluent layers of
cells was observed only after long-term incubation (2-3 months). The investigators concluded
that the discrete stages of neovascularization that were observed with field exposure were
qualitatively comparable to stages of in vivo angiogenesis. With regard to carcinogenicity,
angiogenesis (possibly promoted by EM fields) is essential to neoplastic growth, as well as to
the progression of benign to malignant tumors (Folkman, 1975).
5.8.2. Modulated Radiofrequency Fields
No data were found.
5.8.3. Radiofrequency Fields
No data were found for nonthermal effects of RF fields on growth or cellular differentiation
that could be related to cancer promotion.
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5.8.4. Static Electric Fields
Becker and Esper (1981) examined the effects of electrostimulation, at levels used to
stimulate osteogenesis, on the growth of human fibrosarcoma cells (HT 1080) in culture.
Stainless steel electrodes were inserted through the side walls of two chambers of a plastic
triwell culture dish. The two wells were connected by a conducting agar bridge. The
chambers, containing coverslips, were seeded with the cells and incubated for 48 hours. A
current of 360 nanoamperes (nA) was transmitted between the two electrodes at an average
voltage of 1.1 Vfor 24 hours. The third chamber, the control, received no current. The cells
on the coverslips were fixed for counting immediately after exposure.
Cell counts revealed an approximately threefold increase in the cell population in both
experimental chambers relative to the control chambers. Unlike the McLeod et al. (1987) study
in which an AC field reduced protein synthesis, Becker and Esper (1981) used a DC field with
no AC component. These preliminary results suggest that, because the growth of human
fibrosarcoma was stimulated in this study with currents and voltages used to stimulate
osteogenesis, it would be prudent not to administer electrostimulation to patients with
suspected premalignant or malignant lesions located within the current pathway (Becker and
Esper, 1981).
5.8.5. Summary
The preceding studies show that currents of the strength used to stimulate bone repair can
stimulate alterations in biosynthesis and thereby may influence the growth, remodeling, and
repair of normal tissue. These fields also stimulated the growth of human fibrosarcoma cells
and embryonal carcinoma cells, and inhibited differentiation of embryonal carcinoma cells,
suggesting a tumor-promoting potential for ELF. The investigators in these studies advise that
caution should be exercised in the treatment of tumors with PEMF or the treatment of broken
bones with the fields in patients who also have tumors.
5.9. IMMUNOLOGIC/HEMATOLOGIC EFFECTS
The immune system is the physiological defense against a large spectrum of agents
including bacteria, viruses, fungi, parasites, toxins from organisms, miscellaneous chemical
substances, and neoplasms. Two types of effects are possible: immunosuppression and
immunopotentiation. Immunosuppression may result in an increased susceptibility to infection
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by microorganisms or to the development of tumors while immunopotentiation involves a
generalized increase in immune responsiveness such as hypersensitivity (allergy) or
autoimmunity. Impairment of the immune system could result in adverse health effects. The
immune system consists of cells that are specialized for defense, broadly classified into
lymphoid cells and phagocytic cells that produce humoral substances such as antibodies and
complement.
Assays of lymphocyte function, an important factor in cellular immunity, are used frequently
to assess immune competence. Another, less specific, indicator of immune status is the
peripheral blood cell count, particularly the lymphocyte fraction. Therefore, studies that assess
hematological effects, as well as those that assess immune status, have been included in this
section.
5.9.1. Extremely Low Frequency Fields
Fotopoulos et al. (1987), conducting an investigation of the effects on humans of exposure
to 60-Hz electric and magnetic fields, reported preliminary results of blood chemistry,
hematologic, and immunologic assays. Twelve subjects participated in four experimental
sessions, spaced 1 week apart: two sessions involved 6 hours of exposure to a 60-Hz,
9-kV/m, 16-A/m (2 x 10"2 mT) field, and two identical sessions involved exposure of humans to
a sham field. The subjects served as their own controls. The order of field presentation was
counterbalanced under double-blind conditions. Blood samples were collected in two
sessions before the exposures to establish baseline conditions and then on the days of the
experiments immediately before and after exposure to the real or sham field. Details of
exposure conditions were published elsewhere and are not available.
Expected circadian variations were observed before and after the 6-hour exposure
sessions among the hematologic, chemical, and immunologic variables studied, and many of
the variables did not exhibit significant changes under field exposure conditions compared
with sham controls. There were no significant differences in levels of calcium, glucose, uric
acid, albumin, potassium, or sodium between field-exposed and sham-exposed subjects.
However, lactic acid dehydrogenase (LDH) levels were significantly higher in the pre-exposure
compared with postexposure periods (p=0.004) on the first day but not the second day of field
exposure.
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No differences were observed in white blood cell (WBC) count, red blood cell (RBC) count,
hemoglobin (Hgb), hematocrit (Hct), mean corpuscular hemoglobin (MCH), mean corpuscular
hemoglobin concentration (MCHC), mean corpuscular volume (MCV), or platelets. The
differential cell count revealed a significant increase (p=0.043) in percent lymphocytes only on
the second day of field exposure.
There were no field effects on total T-cells, B-cells, natural killer, and suppressor cells,
based on monoclonal antibody assays, and there was no effect on cell-mediated immunity,
based on a lymphocyte blastogenesis assay using T- and B-cell-specific mitogens. However,
pre-exposure levels were significantly higher than postexposure levels on the first day of field
exposures and not on the second day. This pattern was similar to the pattern with LDH. The
increases in lymphocyte counts on the second day of exposure and decreases in T-helper cell
counts on the first day of exposure suggest that the low frequency electric and magnetic fields
used in this study could enhance certain elements of the cell-mediated immune response in
humans. The investigators consider the findings in this study to be preliminary and defer
interpretation of the results until additional work is done.
Seto et al. (1986) examined the hematologic effects of ELF fields on three generations of
Sprague-Dawley rats that were conceived, born, and raised in an electric field. The animals
(42 to 44 from each generation) were exposed to a 60-Hz, 80-kV/m, unperturbed vertical field
21 hours/day until they were approximately 120 days of age. Sham-exposed controls (42 to 44
from each generation) were conceived, born, and raised under identical conditions, but were
not exposed to the field. The cell counts for the 135 field-exposed and 135 sham-exposed rats
were analyzed statistically by multivariate analysis of variance, univariate analysis of variance,
and tests of simple effects.
Red cell parameters, which included RBC, Hgb, Hct, MCV, MCH and MCHC, were not
affected by field exposure. "Subtle" but statistically significant decreases in total white cell
counts (p=0.006), lymphocyte counts (p=0.027), and eosinophil counts (p=0.035) were
observed. The investigators commented that the observed hematologic variations related to
field exposure were similar to those observed in animals experiencing mild stress, implying
that the field (80-kV/m) could have induced the effects through stress. They further stated that
such effects are not likely to be reliably replicated by an experiment in which sample sizes
smaller than the ones in this study are used.
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Ragan et al. (1983) examined numerous hematologic and serum chemistry variables in
female Sprague-Dawley rats (10-20/group) exposed to unperturbed 60-Hz electric fields at 100
kV/m for 15, 30, 60, or 120 days. The field strength delivered by the apparatus with no animals
or cages installed was 100 kV/m. Each study was replicated once. The data underwent
rigorous statistical evaluation, and although no consistent effect of the field was detected,
statistically significant effects (using Student's t test) were observed in certain variables at
certain time points. For example, at 15 and 120 days of exposure duration the white count
was lower (p<0.02) and at 60 days it was higher (p<0.01) in the exposed as compared with
the sham-exposed groups. Lymphocyte values correlated with the total leukocyte counts.
There were no significant differences between exposed and sham-exposed rats in numbers of
neutrophils, monocytes, eosinophils, and basophils. Platelet numbers were significantly
increased (p<0.02) after 60 days of exposure, but not at other time points. Bone marrow
cellularity was increased (p<0.05) in replicate 2 at 30 days of exposure. Similar occasional
changes were seen in RBC parameters (RBC counts, Hgb concentration, RBC volume, MCV,
MCH, and MCHC) and in serum chemistry values (iron, triglycerides, alkaline phosphatase,
alpha and beta globulins). The investigators drew no definite conclusions but inferred that the
60-Hz field is of potentially low toxicity and emphasized the need for appropriate experimental
design and statistical analysis in studies of this type.
A study was conducted in which ECR-SW strain mice were exposed to a 240-kV/m, 60-Hz
field 18 to 22 hours/day, 7 days/week for a total of 4500 hours of exposure (about 32 weeks)
before they were killed for tests (Fam 1980). Ten males and 10 females were used for
complete blood counts. Statistical analysis (analysis of variance and t statistics) indicated no
differences in the blood count values of the males at the a= 0.05 level, but there was a
significant difference between the exposed females and their controls in several parameters.
For example, exposed animals had a lower white blood cell count (a = 0.0021), a lower
hemoglobin (a= 0.0104), a lower mean corpuscular hemoglobin (a = 0.024), and a higher
percentage of bands (a = 0.0143). The investigators were not certain if the effects on the
females were due to field exposure or if they were the result of lower food and water
consumption. There were no statistically significant effects on lymphocyte counts in males or
females. At the end of the study, heart, lungs, liver, spleen, kidney, and ovary or testes were
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examined microscopically. There were no histological findings that could be attributed to
exposure.
Lyle et at. (1988) tested the effects of 60-Hz sinusoidal electric fields with intensities of 0.1,
1.0, or 10 mV/cm (0.01, 0.1, or 1.0 V/m) on T-lymphocyte cytotoxicity. The field exposure
apparatus consisted of six polystyrene culture flasks positioned vertically and joined in series
by short agar bridges, with carbon electrodes in the medium of the end flasks and cell-bearing
medium in the middle four flasks. Experimental conditions included field, sham, and plastic
control (no agar bridges). Cytotoxicity was measured using the 4-hour chromium release
assay. The effector (cytotoxic) cells used in the cytotoxicity assays were of the murine
T-lymphocyte line, CTLL-1. These are normal T-Iymphocytes that are cultured in interleukin-2,
the T-cell growth factor, to stimulate growth. The target cells were an allogeneic H-2d
B-lymphoma cell line, MPC-11. The assays were performed with electric fields present only
during the 4-hour assay, and using CTLL-1 cells pre-exposed for 48 hours to the electric field.
In addition, the effects of a 48-hour field exposure on growth of the CTLL-1 cells cultured in the
presence of "optimal" growth factor concentrations (1:2 dilution) or in the presence of
suboptimal concentrations (1:32) were determined.
When the cells were exposed to the field only during the 4-hour assay, a nonsignificant 5%
decrease in cytotoxicity reaction of the CTLL-1 effectors against the target MCP cells was
observed in the field-exposed versus sham-exposed flasks. Forty-eight hours of exposure of
the effector cells to the 60-Hz, 10-mV/cm (1.0 V/m) field before the assay resulted in a 25%
inhibition of cytotoxicity (p<0.005, Student's T test), in comparison to the sham controls for
that experiment; the 1.0-mV/cm (0.1 V/m) field produced a 19% inhibition in comparison with
the sham controls for that experiment (p<0.0005); and the 0.1 -mV/cm (0.01 V/m) field
produced a 7% (nonsignificant) inhibition. The field had no effect on the proliferation of the
CTLL-1 effector cells in the presence of interleukin-2, an indication that the inhibition seen in
the 48-hour cytotoxicity study was not due to the inhibition of cell proliferation but rather to an
alteration of the mechanism for cytotoxicity itself. The investigators concluded that, under the
conditions of the study, cytotoxicity shows a dose response to a 60-Hz sinusoidal electric field
between 0.1 and 10 mV/cm, with a detection threshold that lies between 0.1 and 1.0 mV/cm.
Morris and Phillips (1982) observed no effect on the primary antibody response to keyhole
limpet hemocyanin in mice following their exposure to 60-Hz, 0.15 to 0.25 kV/m fields for 30 or
60 days, or on the mitogen stimulation response of spleen cells to B- and T-cell mitogens in
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mice exposed to the same fields for 90 or 150 days. The reason for the difference in the
results of this study and the study of Lyle et al. (1988) is not clear. The main difference in the
two studies was field strength which ranged from 0.01 to 1.0 V/m in the Lyle study and from
0.15 to 0.25 kV/m in the Morris and Phillips study. In addition, in the Lyle study, cells were
exposed in vitro, while in the Morris and Phillips study the whole animal was exposed.
5.9.2. Modulated Radiofrequency Fields
To test the effects of RF radiation on cells already challenged by a commonly encountered
viral agent, Roberts et al. (1987) assayed mitogen responsiveness after exposure of influenza
virus-infected human mononuciear leukocytes to continuous or pulse-modulated 2450-MHz RF
radiation, specific absorption rate of 4 mW/mL (4 W/kg). Mononuciear leukocytes (MNL) were
exposed or sham-exposed to influenza virus then exposed or sham-exposed to the RF
radiation as continuous waves or pulse modulated at 60 or 16 Hz. The four groups of cells
were then stimulated with the mitogen phytohemagglutinin (PHA). RF radiation exposure
caused no changes in leukocyte viability or in mitogen-stimulated DMA synthesis by human
mononuciear leukocytes infected in vitro with influenza virus when compared with sham-RF
radiation-exposed ceils.
Lyle et al. (1983) tested the effects of a 450-MHz microwave field, 1.5 mW/cm2, sinusoidally
amplitude-modulated at 60 Hz on the same allogeneic cytotoxicity system as that described
previously for the study of Lyle et al. (1988). An anechoic exposure system was used. The
chamber temperature was kept to within 0.1 degrees of 35° C throughout the 4-hour exposure
period, and the temperature within the sample well measured before and after the exposure
did not differ significantly from the air temperature. The investigators characterized the
cytotoxic response to the field with various manipulations of the procedure. The calculated
field strength in the culture fluid was in the range of 10 to 30 mV/cm (1 to 3 V/m), somewhat
higher than with the 60-Hz field tested by Lyle et al. (1988).
Cytotoxicity to the target cell (MPC-11) by the CTLL-1 line was significantly inhibited (20%,
p<0.05 to p<0.0005 for five different experiments) when the 4-hour cytotoxicity assay was
conducted in the presence of the field; similar suppression was observed when the effector
cells (CTLL-1) were exposed to the field for 4 hours before the target cells were added for the
cytotoxicity assay. The investigators attributed the suppression to an effect on the effector
cells, not the target cells. The results were similar when the cells were exposed to the field
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during only the first 2 hours of the assay (exposure during the last 2 hours produced only
partial inhibition). This suggests a preferential effect on the recognition phase of cytotoxicity.
Cytotoxicity was also assessed in two experiments 1, 4, 9, and 12.5 hours after field exposure
of the effector cells. In both experiments inhibition decreased as the time interval increased
(for experiment #1: 24% inhibition, p<0.05, during assay; 17%, p<0.025,1 hour; 14%,
p<0.025, 4 hours; 14%, p<0.05, 9 hours) and after 12.5 hours the cytotoxic inhibition was no
longer observed. The assay was then conducted after T-cells were exposed during the 4-hour
assay to various amplitude modulation frequencies (16, 40, 80, and 100 Hz). All modulation
frequencies produced suppression, but it was maximal at 60 Hz (20%).
Lyle et al. (1988) suggested that the differences in their experiments of 1988 and 1983 (the
60-Hz modulated 450-MHz microwave field of the 1983 study produced a rapid inhibition when
the 4-hour cytotoxicity assay was conducted in the presence of the field, whereas the 60-Hz
field in the 1988 study produced inhibition only after 48-hours of field exposure) could have
been due to either different characteristics of the two fields or different culture conditions
between the two sets of experiments (Lyle et al., 1988).
5.9.3. Unmodulated Radiofrequency Fields
A study of the long-term effects (including immunologic and hematologic parameters) of
RF radiation was conducted, using 14-week-old male Wistar-Furth rats (Smialowicz et al.,
1981). Sixteen animals were exposed to 970-MHz EM radiation [SAR = 2.5 mW/g (2.5 W/kg),
22 hours daily for 70 consecutive days]. The exposure system consisted of 16 individual
circularly polarized waveguides and similar nonenergized chambers served as sham-irradiated
controls. No differences were observed in the body weights, hematologic profile, or in vitro
lymphocyte responses to mitogens between the two groups. The only effects observed were
increased levels of triglycerides, albumin, and total protein which were thought by the
Investigators to be related to thermal stress.
Chou et al. (1983) examined the effects of long-term exposure to continuous wave (CW)
microwave radiation on New Zealand rabbits. Two groups of 16 animals each were exposed
to 2450-MHz fields in two experiments of 90 days each. The incident power densities of the
first and second studies were 0.5 and 5 mW/cm2, respectively. After adapting to the anechoic
chamber exposure system, eight rabbits were exposed for 7 hours daily, 5 days a week for 13
weeks, and eight were sham exposed. SARs were 5.5 W/kg in the head and 7 W/kg in the
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back at 5 mW/cm2. There were no changes in body weights, blood cell counts and
morphology, clinical chemistry parameters, protein electrophoresis, lymphocyte blast
transformation, and histology of the exposed animals in comparison with controls; and there
were no changes in the eyes of the exposed animals. The only effect, decreased food
consumption, was observed during exposure to the 5-mW/cm2 exposure.
Wright et al. (1984) studied the effects of high frequency radiation in Wistar rats and
Cynomologus and Rhesus monkeys, exposed for 28 and 24 days, respectively, 23 hours/day.
The rats were exposed to 28 MHz (125 mW/cm2) fields for 28 days and examined for
histopathologic effects or were exposed to 220 mW/cm2 for 13 days and thyroid function was
assessed. The Cynomologus monkeys were exposed to 28 MHz (25 mW/cm2) for 24 days
and examined for hematologic changes. The Rhesus monkeys were exposed to 125 mW/cm2
(28 MHz) radiation for 11 days and electrolytes were measured. There were no
histopathologic changes in the rat or hematologic changes in the monkey that could be
attributed to exposure. The rats did exhibit reduced uptake of iodine by the thyroid, reduced
levels of plasma thyroid-stimulating hormone, and reduced ratio of protein bound to
nonprotein bound iodine. However, these animals were exposed to a 220-mW/cm2 field (likely
to induce thermal changes in man), and the thyroid effects were thought to be compensatory
responses to an induced heat load.
Ottenbreit et al. (1981) examined the effects of microwaves on the colony-forming capacity
of human neutrophil precursor cells (CFU-C) in a methylcellulose culture system. Bone
marrow specimens were aspirated from children with acute leukemia in remission, or from
children with other disorders who had marrow aspirations performed for evaluation of clinical
status, or for diagnostic determinations. The cells collected from the top layer of a
Ficoll-Hypaque gradient were used for the assay. The cells were allowed to stand overnight,
were suspended in microcapillary tubes, and were exposed to 2450-MHz CW microwaves for
15 minutes in a fluid-filled waveguide irradiation system. Irradiation of the cells for 15 minutes
at 31, 62,125, 250, 500, and 1000 mW/cm2 was conducted with bath temperatures set at 37°
C for the two lowest power levels and at 7, 22, 37, and 41 ° C for the last four power ranges,
respectively. Sham-exposed controls were treated in the same way, but the microwave power
was not turned on. The cells were then cultured with 20% fibroblast conditioned medium at
37° C, 7.5% humidity. Colonies were counted on days 6 or 7, and days 12-14.
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When colonies were scored on days 6 or 7, there was no reduction in the number of
colonies formed by field-exposed cells at power levels of 31 and 62 mW/cm2. As the power
level was increased to 1000 mW/cm2, there was a corresponding reduction in the number of
colonies formed by the microwave-exposed cells (p<0.05, Student's t test, at the four highest
levels). The maximum reduction occurred at 500 and 1000 mW/cm2. At days 12-14, there was
a similar dose-dependent reduction in colony numbers. Additional experiments showed that
the effects observed were not related to temperature rise, or to the state of cell cycle, and were
irreversible. The investigators hypothesized that, because CFU-C require the addition of
exogenous stimulators for cell growth (fibroblast conditioned medium in this case), it is
possible that microwave irradiation alters the membrane receptors of CFU-C making some of
them unresponsive to the stimulation factors. In addition, the investigators suggested that the
cells from patients with leukemia or other disorders might react differently to EM radiation than
CFU-C from normal individuals. Ottenbreit et al. are currently investigating this possibility.
In a series of in vitro studies designed to characterize direct RF radiation effects on
immune function, specifically the effects of RF radiation on the immunoglobulins in solution
when bound to the lymphocyte cell surface, Liburdy and Wyant (1984) observed that RF
radiation (10 MHz; 8500 V/m, applied electric field; <0.134 W/kg, internal absorbed power; 20
V/m, internal electric field) altered the physical separation of immunoglobulin (Ig) and of
Ig-bearing T- and B-lymphocytes during liquid gel chromatography and immunoaffinity cell
chromatography, respectively. Human serum was exposed to the 10-MHz electric field during
chromatography. The gel column was placed perpendicular to the electric field surrounded by
a jacket of circulating water for conductive cooling. The temperature of the gel, maintained at
25° C, increased approximately 0.05° C during the first 15 minutes and then stabilized at
25 ą 0.01° C during the 18-hour exposure period. To further ensure that changes in the
elution profile were not from temperature increases, two chromatography separations were
performed at 24 and 26° C in the absence of RF radiation field. No alterations in the elution
pattern were detected.
The elution profiles for the three immunogolbulins examined (IgM, IgA, and IgG), were
altered by field exposure during elution, as evidenced by accelerated elution of all three peaks.
This is thought to reflect an increase in the steric resistance of Ig molecules to the gel pores.
The investigators were able to almost completely rule out the possibility that RF
radiation-induced alterations in the gel matrix could have influenced the results.
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Effects on lymphocyte separation were investigated by performing immunoaffinity cell
chromatography during exposure to 2500-MHz RF radiation (194 V/m, < 0.117 W/kg, 10
mW/cm2). This chromatography procedure separates lymphocytes based on antigen-antibody
interactions at the cell surface. Spleen cells from female Balb/c(H-2d) were fractionated at 4.0°
C over Ig-derivatized agarose beads (derived with polyclonal antibody directed against all
mouse lg+ classes) into Ig' and lg+ lymphocyte subpopulations. Because they were derived
with polyclonal antibodies directed against all mouse Ig classes, all lg+ lymphocytes were
expected to interact with the beads when no field is present. RF radiation exposures, on the
other hand, resulted in premature elution of 19% of the lg+ (B-cell) population. This premature
elution resulted in a difference in distribution among cell fractions collected and indicates an
RF radiation-induced alteration of specific Ig binding between B-lymphocyte cell surfaces and
the column. Temperature fluctuations did not exceed ą 0.03° C. Although these effects
occurred at SARs well below the recommended safety limit for humans in the United States of
0.4 W/kg, averaged over any 6-minute period, the investigators advise caution in extrapolating
from in vitro to in vivo conditions. The results do suggest alterations in the structure of
membrane-bound proteins that apparently affect receptor binding on the cell surface (Elder,
1987b).
There were two other in vitro studies in which thermal effects were carefully excluded.
Szmigielski (1975) reported that radiation at 3 GHz with a power level of 5 mW/cm2 decreased
the viability of rabbit granulocytes. Lin et al. (1979) reported that radiation of 2.45 GHz with a
power level of 60 to 1000 mW/cm2 reduced the numbers of granulocyte and macrophage
colony-forming units from preparations of mouse bone marrow.
5.9.4. Summary
5.9.4.1. Extremely Low Frequency Fields
Preliminary data from the analysis of pre- and postexposure blood samples from humans
exposed to ELF fields of 60 Hz, 16-A/m (2 x 10'2 mT) and 9-kV/m for two sessions of 6 hours
each resulted in the following observations (Fotopoulos et al., 1987): (1) no statistically
significant differences in concentrations of calcium, glucose, uric acid, albumin, potassium, or
sodium; (2) a significant decrease in lactic acid dehydrogeriase after one of the two exposure
sessions; (3) no significant differences in red and white cell blood counts, hemoglobin,
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hematocrit, mean corpuscular volume, or platelets; (4) a significant increase in the peripheral
lymphocyte count after one of the exposure sessions; (5) no significant difference in total
T-cells, B-cells, natural killer cells, helper cells, or suppressor cells, based on monoclonal
antibody assays; (6) no significant effect on cell-mediated immunity; (7) although the level of
T-helper cells is typically higher in the morning than the afternoon, the difference was
significantly larger in exposure days than days of sham exposure. Although the authors
consider the data preliminary until more work is done, they point out that these field exposures
might be enhancing the cell-mediated immune response in humans.
Seto et al. (1986) examined the hematologic effects of ELF on Sprague-Dawley rats that
were exposed to a 60-Hz, 80-kV/m, unperturbed vertical field 21 hours/day through three
generations. "Subtle" but statistically significant decreases in total white cell counts,
lymphocyte counts, and eosinophil counts were observed. Red cell parameters were not
affected by field exposure. The investigators implied that the field could have induced the
effects through stress.
In another study, no consistent effects were observed in rats exposed to unperturbed
60-Hz fields at 100 kV/m for 15, 30, 60, or 120 days (Ragan et al., 1983). In two of eight
experiments, the white count was lower and in one it was higher in the exposed compared
with the sham-exposed groups. Platelets were significantly increased after 60 days of
exposure, but not at other time points. Bone marrow cellularity was increased only in replicate
2 at 30 days of exposure. Occasional changes were also seen in red blood cell parameters
and in serum chemistry values. The authors drew no definite conclusions, but inferred that the
field had potentially a low level of toxicity.
A study was conducted in which small numbers of ECR-SW strain mice were exposed to a
240-kV/m, 60-Hz field 18 to 22 hours/day, 7 days/week for a total of 4500 hours of exposure
(about 32 weeks) before they were killed for tests (Fam, 1980). No statistical differences were
observed in the blood count values of the males at the a= 0.05 level. However, exposed
females had lower white blood cell counts, lower hemoglobin values, lower mean corpuscular
hemoglobin values, and a higher percentages of bands, all of which were statistically
significant The investigators indicated that the effects on the females could have been due to
either field exposure or decreased food and water consumption.
Morris and Phillips (1982) observed no effect on the primary antibody response to keyhole
limpet hemocyanin in mice following their exposure to 60-Hz, 0.15- to 0.25-kV/m fields, for 30
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or 60 days, or on the mitogen stimulation response of spleen cells to B- and T-cell mitogens in
mice exposed to the same fields for 90 or 150 days.
An in vitro, field strength-related suppression of murine T-lymphocyte-mediated cytotoxicity
was observed following a 48-hour exposure to 60-Hz sinusoidal electric fields at field strengths
between 0.01 and 0.1 V/m, with a threshold for significance that lay between 0.01 and 0.1 V/m
(Lyle et al., 1988). The inhibition was preferentially expressed during the early recognition
phase of the immune response. The field had no effect on the proliferation of the CTLL-1
effector cells in the presence of interleukin-2, an indication that the inhibition of cytotoxicity
was not due to the inhibition of cell proliferation but rather to an alteration of the mechanism
for cytotoxicity itself.
In conclusion, the effects of 60 Hz electric fields on immune function in vivo are small and
inconsistent when present at all. This is the overall conclusion from one human study and two
studies each in rats and mice at field strengths ranging from 0.15 to 240 kV/m. However, in
one in vitro study of a murine cytotoxic T-cell line, a 48-hour exposure to 60-Hz electric fields of
only 0.1 and 1.0 V/m suppressed the cytotoxicity of these T-cells; no effect was seen at 0.01
V/m.
T-cell cytotoxicity, important in the elimination of certain infectious agents, allograft
rejection, and tumor immunity (reviewed in Lyle et al., 1988), can be quantified in vitro with the
4-hour chromium release assay. The results of these assays have been shown to correlate
directly with in vivo anti-tumor activity. Immunotherapy trials have shown that when the
T-lymphocyte growth factor, interleukin-1, is administered with cultured cytotoxic
T-lymphocytes, cures of cancer in animals and remissions in selected patients can occur
(reviewed in Lyle et al., 1988). The suppression of T-lymphocyte-mediated cytotoxicity by ELF
has been observed in vitro only, using only one clone of cytotoxic murine rather than human
lymphocytes. These results, though limited, suggest the possibility that weak EM fields, in
suppressing the effectiveness of cytotoxic lymphocytes, could provide a growing clone of
antigenic tumor cells to develop the mass needed to overcome a continuing immune attack.
5.9.4.2. Modulated and Unmodulated Radiofrequency Fields
Studies of the effects of modulated and unmodulated RF fields on immune function have
shown responses only at intensities large enough to cause appreciable heating, with the five
exceptions noted below. This conclusion is based on studies in virus-infected human
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mononuclear leukocytes, Wistar-Furth rats, New Zealand rabbits, rats of an unknown strain,
and monkeys of an unknown strain. The exceptions are:
Lyle et al. (1988) showed that exposure to 60-Hz modulated 450-MHz RF fields inhibits
the cytotoxicity of the same mouse T-cell line in which they found to be susceptible to
60-Hz electric fields.
Ottenbreit et al. (1981) found that the colony-forming properties of neutrophil precursor
cells from childhood leukemia patients in remission are inhibited by a 15-minute
exposure to 2450-MHz unmodulated radiation at the higher power levels of 500 and
1000mW/cm2.
Liburdy and Wyant (1984) observed a change in the liquid gel elution patterns of
human immunoglobins IgM, IgA, and IgG in solution after exposure to 10-MHz RF
radiation (SAR = 0.13 W/kg). These investigators also measured changes in the
separation patterns of lymphocyte-immunoglobin complexes in an immunoaffinity cell
chromatography assay; these changes were induced by RF radiation of 2500 Hz and a
SAR of 0.12 W/kg. This study shows that the RF radiation alters the structure of
membrane-bound proteins on the lymphocyte surface.
Szmigielski (1975) showed that RF radiation decreased the viability of rabbit
granulocytes.
Lin et al. (1979) showed that RF radiation reduced the numbers of granulocyte and
macrophage colony-forming units from preparations of mouse bone marrow.
5.10. CENTRAL NERVOUS SYSTEM EFFECTS
This section examines some of the evidence that the central nervous system (CNS) is a
target for ELF and RF interactions. Reports have been published showing that alterations in
cellular morphology of brain tissue, changes in the electroencephalogram, and changes in
pineal gland melatonin and electrical activity occur in response to magnetic and electric fields.
No attempt is made here to review the literature on circadian rhythms in behavioral activity,
although the CNS is clearly involved in coordinating circadian variations in hormone levels.
5.10.1. Extremely Low Frequency Fields
Welker et al. (1983) measured the melatonin and N-acetyltransferase content of the pineal
gland in Sprague-Dawley rats before and after changes in the orientation of static magnetic
fields. The strength of the earth's magnetic field was 0.62 Oe (0.062 mT) at a 63° inclination
with respect to the horizontal plane. The animals were placed into cages with Helmholtz coils
oriented so the static field experienced by the animals could be changed to various strengths.
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The investigators found that when the field was either inverted (-63°) or changed by small
amounts (-5°, +5°, +15°), the pineal content of both substances decreased significantly. This
occurred when the field was perturbed at night (when the pineal gland is active), but not
during the day. The same group of investigators had shown earlier (Semm et al., 1980) that
the firing rate of single pineal cells decreases gradually over periods of about 72 minutes when
the vertical component of the field is increased by 0.5 Oe (0.05 mT).
In a later paper from the same laboratory, Olcese et al. (1 985) showed that this response
disappeared when the optic nerve was cut, indicating that the retina of the eye is the
magnetoreceptor. Later, they showed (Reuss and Olcese, 1986) that the response does not
occur when the optic nerve is intact in total darkness and that dim red light must be present for
the magnetic field stimulus to be effective.
The inhibition of melatonin synthesis by a change of only 5( in the orientation of a static
magnetic field of 0.062 mT = 62 ^T is an interesting finding. It is equivalent to the finding that
the introduction of a small component either perpendicular to the field of 62 sin (5) = 4.5 ju,T,
or a change in the parallel component of 62 [1-cos (5)] = 0.24/^T is sufficient to inhibit
melatonin synthesis. Ambient residential 60-Hz fields are within this order of magnitude.
The effects of long-term exposure to ELF fields on histology of nerve tissues of rabbits,
pigs, rats, and mice were examined by light and electron microscopy. (Hansson 1981 a, b;
Hansson etal.,1987).
Rabbits were exposed under two different conditions: (1) from conception to 6 months of
age, outdoors, in a 400-kV substation; they were exposed continuously to a 50-Hz electric
field, at approximately 14 kV/m; and (2) from conception to 8 months of age, in a laboratory
with a controlled environment; 14 kV/m at 50 Hz, 23 hours/day, 7 days/week (Hansson, 1981
a, b). In both situations, controls were shielded from the field (sham-exposed) in Faraday
cages or were unexposed.
The most severe effects were observed in the rabbits that were exposed outdoors in a
substation. Cerebellar tissues from exposed rabbits exhibited changes in almost all Purkinje
nerve cells examined. Nissl granules formed by clusters of granular endoplasmic reticulum
arranged in parallel that were seen in control animals had almost disappeared from tissues or
exposed animals and were replaced by lamellar bodies. These structures were in continuity
with the endoplasmic reticulum, thus reducing the surface area of endoplasmic reticulum
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exposed to the cytoplasmic matrix; the changes extended to the dendrites. The hypolemmal
cisterns normally studded along with the Purkinje cell dendrites, had vanished. In addition,
microtubules showed altered distribution and reduction in number. Filaments and
membranous structures were observed in increased frequency.
In rabbits that received 4 or more weeks of exposure postnatally, there were changes in
the glial cells of the cerebellum (and similar, but less definite ones, in the hippocampus) that
included replacement of normally slender processes with shorter, thicker more irregular ones;
the nuclei of the glial cells could be stained with S-100 antibodies, which was not observed in
the controls. (S-100 is a ligal cell marker protein that can be demonstrated ultrastructurally
with antibodies against S-100 using quantitative immunohistochemical methods.) The number
of large astrocytes in the granular layer was increased. Concentrations of S-100 in the
cerebellum and hippocampus were increased. Changes somewhat similar to these, but less
severe, were observed in the rabbits exposed under laboratory conditions, rats exposed to
fields of 50 or 60 Hz, 14 kV/m for 22-23 hours/day, in mice exposed to fields (60 Hz, 10 kV/m)
during the first 4 weeks of age, and in minipigs exposed for almost a year and a half to electric
fields (60 Hz, 30 kV/m, 20 hours/day) (Hansson et al., 1987). The investigators concluded that
long-term exposure to power-frequency electric fields induces effects on the nervous system
of exposed animals, but they did not discuss the physiological significance of the changes.
The work of Hansson (1981 a, b) has been criticized on the basis that the animals were
maintained out-of-doors under ill-controlled conditions and environmental factors other than
the field [such as noise, ozone production, and vibrations that were related to high voltage
installations (Kornberg, 1976; Michaeison, 1979, both cited in Portet and Cabanes, 1988)
could have influenced the results (Portet and Cabenes, 1988). In addition, a reduction of
growth observed in the rabbits exposed outdoors was not reported for animals exposed in the
laboratory. In similar studies, Portet et al. (1984, cited in Portet and Cabanes, 1988) did not
observe lesions in the cerebella of neonate rabbits exposed to electric fields. Experimental
details were not available.
5.10.2. Modulated Radiofrequency Fields
Electroencephalogram (EEG) changes (which consisted of enhanced low frequency
components and decreased high frequency activities) were observed in rabbits exposed to a
RF field 2 hours/day for 6 weeks at 1.2 MHz (15-Hz modulation) at levels of 0.5 to 1 kV/m
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(~1.3-2.6 W/cm2) (Takashima et al., 1979). The effects were described as nonthermal,
because the estimated current density of 0.082 mA/cm2 was below that needed to cause
noticeable thermal effects. The EEG signals were computer processed to obtain power
spectra.
5.10.3. Unmodulated Radiofrequency Fields
Webber et al. (1980) observed ultrastructural damage, apparently of a nonthermal nature
(SAR not known), in mouse neuroblastoma cells grown in culture and exposed to microwave
pulses. The cells were exposed to short pulses at high fields [1.7 to 3.9 kV/cm (170 to 390
kV/m)] from a magnetron radar transmitter with a radar modulator. The voltage pulses from
the power supply and modulating system were converted to 1-second RF pulses in a 2.7-Hz
band (330 pulses/second, 0.0335 duty cycle). The waveguide apparatus termination was
constructed for insertion of a glass slide horizontally between two section of S-band
waveguide. The coverslip carrying the cells was placed on the glass slide, with cells facing
upward. A section of waveguide that terminated in a short circuit was mounted 4.16 cm above
the slide.
The cells were (1) exposed to 1.7 kV/cm (170 kV/m) for 30 seconds, (2) exposed to 3.0
kV/cm (300 kV/m) for 60 seconds, (3) exposed to 3.9 kV/cm (390 kV/m) for 60 seconds, or (4)
not exposed to the field. To test the effects of heat on the cells, coverslips carrying the cells
were dipped into saline at the following temperatures for 30 seconds: 37, 41, 45, 50, 62, 70,
and 80° C. The cells were examined by electron microscopy after field or heat exposure.
The most striking damage observed in cells exposed to 1.7 kV/cm (170 kV/m) was in the
form of breaks in the cell and mitochondria! membranes. The cristae lost their normal pattern
and formed myelinated figures inside the mitochondria. Parts of the cell membrane were
expelled and appeared as membrane-bound sacs outside the cell surface. Exposure of the
cells to this field for 30 seconds is expected to result in a temperature rise from 37° to 41° C.
To determine if the effect was heat-related, cells were exposed to temperatures corresponding
to temperature increases induced by microwave exposure. Cells exposed to heat alone (41° C
as well as 45° C) remained viable and maintained a normal structure without any cell damage.
Cells exposed to 50° C showed considerable damage; however, the cell membranes remained
intact. Cells exposed to 3.9 kV/cm (390 kV/m) for 60 seconds were damaged severely. The
cell content was totally disorganized and the membranes had completely broken down,
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appearing denatured. However, cells heated to 62° C, the corresponding temperature for this
exposure, exhibited greater integrity of the cell membranes (including the mitochondrial and
nuclear membranes). Because of the different nature of the damage to field-exposed
compared with temperature-exposed cells, the investigators suggested that the damage could
have been due to nonthermal effects.
5.10.4. Summary
Long-term exposure of animals to moderate or high-intensity EM fields at 50 or 60 Hz
resulted in changes in the cerebellar Purkinje nerve cells that included rearrangement of the
endoplasmic reticulum and disappearance of the hypolemmal cisterns of the dendrites
(Hansson et al., 1987). Glial reactions that showed an increased concentration of S-100 in the
cerebellar hemispheres were the most consistent findings. These changes indicated that
disturbances had taken place in the interaction between plasma membrane structures and the
cytoskeletons of cells of the nervous system.
Neuroblastoma cells exposed to microwave pulses in culture exhibited ultrastructural
damage as evidenced by breaks in the cell and mitochondrial membranes (Webber et al.,
1980). The effects were apparently nonthermal.
The studies of Semm et al. (1980), Olcese et al. (1985), and their colleagues show that
changes in magnetic fields are perceived by the retina. This stimulus decreases the firing rate
of neurons in the pineal gland and inhibits its melatonin content if applied at night when the
pineal is actively secreting melatonin. The finding that the retina is able to detect changes in
magnetic fields provides a mechanism whereby the CMS function is affected by these fields.
Alterations in Ca++ efflux from nervous tissue have been described (see Section 5.3.2.1).
Blackwell and Saunders (1986) reviewed the literature on CNS effects of RF and microwave
exposure and concluded that although calcium ions play a critical role in many metabolic and
physiological processes, the significance of changes in calcium ion exchange in brain tissue
for the health and safety of people exposed to microwave and RF radiation is difficult to
determine, and that furthermore, the evidence that calcium ion exchange in living nervous
tissues is altered by amplitude-modulated RF and microwave and radiation is inconclusive
(Blackwell and Saunders 1986).
Michaelson and Lin (1987) also reviewed the effects of low-intensity microwaves on the
CNS and concluded that to date there is no convincing evidence of the existence of
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low-intensity microwave effects on the human CNS. The animal studies that are the basis for
reported effects suggest that the mechanisms for these effects involve microwave-induced
nonuniform temperature distributions and/or thermal gradients (Michaelson and Lin, 1987).
5.11. SUMMARY AND CONCLUSIONS FOR SUPPORTING EVIDENCE OF
CARCINOGENICITY
The literature on effects of EM fields on biological processes relevant to carcinogenesis
has been reviewed in this chapter. In this section, the summaries of other sections of Chapter
5 are reviewed and overall conclusions are derived to the extent possible.
5.11.1. Summary
Table 5-7 summarizes in brief phrases the effects that have been observed for each
biological process and each of the major categories of EM fields. These summary phrases
have been derived from the section summaries and text. The first observation apparent from
Table 5-7 is that the evidence for any one process is widely scattered among different types of
exposure. The scattering is even more widespread than the table suggests, since it obviously
cannot show the large variety of frequencies, intensities, and durations of exposure that have
been used within each broad class of exposure. The table demonstrates the gaps in the
current information; for example, transcription of genetic information into messenger RNA,
translation into proteins, and parathyroid hormone effects on bone cells have been studied
only with low-frequency pulsed magnetic fields. This is understandable, since this work has its
origins in the successful use of pulsed magnetic fields for clinical healing of recalcitrant bone
fractures.
The following conclusions can be made:
None of the types of time-varying fields considered in this document cause DNA
breaks, gene mutations, or sister chromatid exchanges. (Static magnetic fields with
high field strength have affected DNA in solution and have caused sex-linked recessive
lethal mutations in Drosophiia, but the significance of this effect is not known). This
lack of a DNA and gene mutation effect is expected, since these fields do not have
enough energy to break chemical bonds.
Effects on DNA synthesis have not been studied extensively enough to draw definite
conclusions. Apparently RF fields cause inhibition and ELF magnetic fields cause an
enhancement of DNA synthesis only within a limited range of frequency and intensity
windows."
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TABLE 5-7. SUMMARY OF SUPPORTING EVIDENCE FOR CARCINOGENICITY
Subject
DMA Damage:
Breaks
Repair
DMA Synthesis
Gene Mutations
Chromosome
Aberrations
Sister Chromatid
Exchange
Mitosis
Transcription
of Genes
Translation
Cell Transforma-
tion
Calcium Efflux,
Brain Tissue
Parathyroid
Hormone
Intracellular
Enzymes
Hormones
E-Relds
No breaks
No DNA repair
Delayed S phase
No effect
(1 study)
Breaks, aneuploidy
(inconsistent)
No effect
(4 studies)
Mitotic index
reduced early, but
recovers. Cell
cycle delayed
-
_
-
Inhibition Frequency
and Amplitude
"Windows"
-
ODC is induced.
Same effect
as TPA.
Inhibits night-
time melatonin
output of pineal
gland
ELF Fields
B-Relds
No breaks
Enhancement
(frequency and
intensity windows)
No effect
(2 studies)
Breaks, aneuploidy,
decondensation
(inconsistent)
No effect
(3 studies)
-
Enhanced, both
normal and newly-
induced sites (all
waveforms)
Altered pattern of
protein synthesis
-
Blocks action
of PTHatthe
cell membrane
Combined
Eand B
No breaks
~
-
-
Breaks
No effect
(2 studies)
Cell cycle
delayed
-
Enhancement
Amplitude and
frequency
"windows"
-
Modulated
RF Fields
Inhibition
No effect
(1 study)
Spark dis-
charges caused
breaks
No effect
(2 studies)
Inconsistent
(2 studies)
-
Initiation of
C3H/10T1/2
cells
Frequency
and intensity
"windows"
-
RF Fields
No damage
Inhibition
No effect
(10 studies)
Breaks,
uncoiling,
numerical
aberrations,
dicentrics
condensation
(inconsistent)
No effect
(1 study)
No effect
(1 study)
-
No effect
(3 studies)
_ Protein kinase
C inhibited.
Frequency "windows."
_
ODC is induced
-
-
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TABLE 5-7. SUMMARY OF SUPPORTING EVIDENCE FOR CARCINOGENICITY (continued)
Subject
Growth and
Differentiation
Immunological
Systems
E-Relds
Inhibits protein
synthesis in
fibroblasts
No effect in vivo
(3 studies)
Inhibits cyto-
toxicity of T
lymphocytes in
culture.
H..FRBM*
B-Relds
Inhibits differ-
entiation and
stimulates growth
of embryonal
carcinoma cells
Combined
Eand B
Increases
reproductive
capacity of
carcinoma cells
No effect in
humans
(1 study)
Modulated
RF Reids
Cytotoxicity
same as ELF.
No effect on
leukocytes.
RF Reids
No effect
in rats, rabbits,
monkeys. Celi-
immuno-
globulin
binding is
tUAVA^J
Central Nervous
System
Inhibition of
pineal activity
via retinal
magneto-
receptors
Morpho-
logical
changes in
glial and
Purkinge
cells of
cerebellum.
EEG shifts to
lower frequencies
(ELF modulation).
Disruption of mito-
chondria and cell
membranes, different
than heat damage
(radar modulation).
Chromosomal aberrations is a frequent finding for both RF and ELF fields, but it often
does not occur. In one measurement of aberrations in peripheral lymphocytes in
electrical switchyard workers, chromosome breaks occurred immediately after they
were exposed to spark discharges, but in similar populations, with no spark discharge
exposure, no aberrations occurred. This indicates that high frequencies may be more
effective than low frequencies in causing aberrations, but these conclusions are only
tentative, and specific studies are needed to address this important issue.
ELF electric and combined electric and magnetic fields have delayed the cell cycle and
caused transient reductions in the rate of cell division, but RF fields have caused no
consistent effect. ELF magnetic fields have not been tested for their effect on the
mitotic cycle, and little testing of RF has been done.
Pulsed magnetic fields of the type used for clinical bone healing have enhanced the
transcription synthesis of mRNA at genetic sites that are normally active and have
altered the molecular weight distribution of proteins synthesized with the fields present.
The protein molecular weight distribution is different with different waveforms (pulsed
versus sinusoidal) and frequencies (60 Hz vs. 72 Hz). No other type of field has been
investigated for this effect.
Cultures of the NIH C3H/IOTI/2 cells, which are widely studied systems for investigating
cell transformation from normal to malignant patterns of growth, have been shown to
undergo transformation under special conditions. Microwave 2450-MHz power,
modulated with pulses at a rate of 120 pulses per second, were administered to the
culture at intensities low enough to cause no effect. Subsequently the cells were
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treated with TPA, the phorbol ester which is known to cause promotion of
chemically-initiated cells. The cells undergo transformation under these conditions,
indicating that this pulsed microwave power has the properties of a chemical initiator of
malignant transformation. Only one experiment has shown this phenomenon, so no
conclusions can be made about whether ELF or RF fields could produce the same
effects.
The release of calcium ions from chick brain tissue into the medium surrounding the
tissue has been affected by ELF electric fields, crossed ELF electric and magnetic fields
and RF radiation modulated at the same frequencies which cause the ELF effects. The
original investigations with ELF electric fields showed an inhibition of calcium release,
whereas an enhancement of release occurred in the other experiments. This
phenomenon has not occurred in three RF studies, but magnetic ELF fields have not
been examined for this'effect. The conditions under which this occurs are very precise
and not understood. It occurs only at certain frequencies (e.g., odd multiples of 15 Hz
with some frequencies missing) with no response at frequencies between. At some
fixed frequencies, it occurs only at certain field strengths with no response below and
above this intensity "window." In at least at one of the "windows" the orientation of the
alternating magnetic field must have a component perpendicular to the static earth's
magnetic field. The crossed electric and magnetic alternating fields producing this
effect are extremely small (16 V/m electric and 73 nT magnetic field), and in the range
of ambient magnetic ELF fields in residences. With the two exceptions discussed
below all of the other effects reviewed in this document are induced by fields at least
hundreds of times higher than this. The biological significance of this phenomenon is
not clear beyond the fact that brain tissue is somehow affected by these unique field
conditions.
The effects of pulsed ELF magnetic fields on the interaction between parathyroid
hormone (PTH) and bone cells have been studied to elucidate the mechanisms of the
clinically successful bone healing ability of these fields. These fields block the
inhibitory effect of PTH on collagen synthesis by the cells, and the action of the field
occurs at the plasma membrane where the hormone binds with its membrane receptor.
The significance of this is that pulsed magnetic ELF fields can alter the chemical
signalling process between an exogenous hormone and the cellular activity induced by
the hormone. No other type of field has been tested for this effect.
The intracellular enzyme ornithine decarboxylase, which is active during cell
proliferation and DNA synthesis of most cells, is induced by ELF electric fields and by
ELF modulated RF fields in three different cell lines. Information on the effect of other
fields has not been found. The same enzyme is induced by the phorbol ester TPA, the
most actively studied chemical promoting agent. cAMP-independent protein kinase,
one of the chemical intermediates involved in this cell proliferation response, is
inhibited in human lymphocytes by modulated RF fields, with an apparent frequency
"window."
Electric ELF field exposure to rats for 20 hours per day for 30 days causes an inhibition
of the nocturnal synthesis of melatonin by the pineal gland. Information on the effect of
other fields has not been found. This finding could have great significance in
explaining the potential carcinogenicity of ELF fields, since there is a wealth of literature
describing the oncostatic properties of melatonin, not only for chemically-induced
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mammary tumors in rats, but also (according to one report) in the treatment of human
leukemia. Other experiments in rats have shown that pineal neurological activity and
melatonin synthetic activity have been inhibited by changing the orientation of the static
magnetic field through an angle of as small as 5(, a change which is only a factor of 10
higher than ambient magnetic residential fields. This implies that exposure of humans
to weak time-varying magnetic fields at night could have an inhibitory effect on pineal
melatonin synthesis. Experimental evidence to support this hypothesis is not available
Information on the effect of ELF magnetic fields and RF fields on melatonin synthesis
has not been found. ELF electric, magnetic, and combined fields of the strength used
to stimulate bone repair can also cause alterations in biosynthesis. Inhibition of protein
biosynthesis in fibroblasts, inhibition of differentiation and stimulation of growth of
embryonal carcinoma cells, and increase in the reproductive capacity of colon
carcinoma cells are all phenomenon that are induced by ELF fields and are
characteristics of malignant growth. The extent to which they occur in the whole
organism under realistic exposure conditions is not known, but these phenomena are
consistent with the suggestion of carcinogenic effects in humans and animals.
In one human study and three animal studies, exposure to ELF fields caused small but
inconsistent changes in white blood cells. Exposure of rats, rabbits, and monkeys to
unmodulated RF fields also caused small inconsistent changes. However, one
investigator working with T-lymphocytes in culture found that both ELF electric fields
and modulated RF radiation inhibit their ability to kill their normal target cells. The
reasons for this difference between the in vivo and in vitro response is not known, but it
does call into question how directly one can infer that whole animal responses can be
predicted from cell culture experiments for these effects. Information on the effect of
magnetic fields on lymphocyte function or dynamics has not been found.
Exposure to combined ELF electric and magnetic fields 23 hours/day for the first 6 to 8
months of life caused a disappearance of Missel granules and disruption of the
endoplasmic reticulum in Purkinj'e cells and a disruption of the morphology of glial cells
in the cerebellum. This occurred most severely in rabbits but also occurs to a lesser
extent in rats, mice, and mini pigs exposed for various durations. Six-week exposures
of rabbits to ELF modulated RF fields caused a downward shift in the frequency of the
electroencephalogram (EEG). The ELF modulation frequency of 15 Hz was in the
same range as the EEG frequencies that were enhanced. The finding that the intact
retina is needed for a functioning pineal gland response to magnetic fields implies that
the CNS can be a sensor for ELF fields and raises the possibility that other
neuroendocrine functions of the CNS could be affected.
5.11.2. Conclusions
The finding that several biological phenomena, which are in some way related to
postulated mechanisms of carcinogenesis, are induced by time-varying electric and magnetic
fields is far from proof that these fields are carcinogenic by themselves or that exposure to
them are risk factors for humans. There are reasons for both questioning and affirming the
relevance of each finding. One of the primary difficulties in accepting the relevance of most of
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these findings is the fact that they are induced by field strengths many times higher than the
ambient residential exposures which are hypothetically causing human cancer. Of the effects
summarized in this chapter, only three phenomena occurred under conditions similar to the
low ELF electric and magnetic fields characteristic of ambient exposure [10 V/m and 2
milligauss (mG) = 0.2^T]: (1) calcium efflux from chick brain tissue induced by crossed
electric and magnetic fields; (2) calcium efflux from chick brain tissue after exposure of the
developing embryo to electric fields; and (3) inhibition of nocturnal melatonin synthesis by
small changes in the orientation of static magnetic fields.
The above statements are made under the assumption that human carcinogenicity is
indeed caused by 60-Hz fields with a field strength on the order of 2 mG. If the causative
agent really is the internal currents induced by these ambient fields, then it is conceivable that
the higher frequency components always accompanying ambient 60-Hz fields are the relevant
aspects of exposure. If the effects are really caused by high peak fields with high frequency
components, then the phenomena observed at higher field strengths would be relevant. In
this case more of these phenomena would be relevant, but precise quantitative evaluation is
difficult to carry out, given the current degree of knowledge.
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electric fields: effects on pineal function in the rat. Bioelectromagnetics 4-293
(Erratum to Wilson et al., 1981)
Wilson, B.W.; Chess, E.K.; Anderson, LE. (1986) 60-Hz electric-field effects on pineal
melatonin rhythms: time course for onset and recovery. Bioelectromagnetics 7:239-242.
Wilson, B.W.; Lueng, F.; Buschbom, R.; Stevens, R.G.; Anderson, L.E.; Reiter, R.J. (1988)
Electric fields, the pineal gland, and cancer. In: Gupta, D.; Attanasio, A.; Reiter, R J
eds. The pineal gland and cancer. Tubingen, West Germany: Brain Research '
Promotion, pp. 245-259.
Wolff, S.; James, T.L; Young, G.B.; Margulis, A.R.; Bodycote, J.; Afzal, V. (1985) Magnetic
resonance imaging: absence of in vitro cytogenetic damage. Radiology 155:163-165.
Wright, N.A.; Borland, R.G.; Cookson, J.H. et al. (1984) Biological studies with
continuous-wave radiofrequency (28 MHz) radiation. Radiat. Res. 97:468-477.
Yao, K.T.S. (1978) Microwave radiation-induced chromosomal aberrations in corneal
epithelium of Chinese hamsters. J. Hered. 69:409-412.
Yao, K.T.S. (1982) Cytogenetic consequences of microwave irradiation on mammalian cells
incubated in vitro. J. Hered. 73:133-138.
Yen-Patton, G.P.A.; Patton, W.F.; Beer, D.M.; Jacobson, B.S. (1988) Endothelial cell response
to pulsed electromagnetic fields: stimulation of growth rate and angiogenesis in vitro
J. Cell. Physiol. 134:37-46.
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6. RESEARCH NEEDS
6.1. INTRODUCTION
In order for the Agency to evaluate the public health hazard of electromagnetic (EM) fields
and to be in a position to recommend preventive measures, more information is needed in
several areas. The research topics that need to be investigated to supply this information are
summarized as follows:
Health Hazards Evaluation
- Cancer
- Reproductive effects
- Central nervous system neuroendocrine, immunological effects
Exposure Evaluation
- Characterization of high frequency transients and harmonics of fields from electrical
power sources
.- Relative contribution of sources to total exposure
- High-voltage transmission lines
- Distribution lines to homes and industries
- Power distribution transformers
- Appliances
- Ground currents in households, industrial buildings, office buildings and
schools
- Transportation systems (e.g., electric trains)
Mitigation (exposure reduction)
- Reduction of ground currents
- Redesign of appliances
- Redesign of wiring and routing of distribution lines
- Supression of transients and high frequencies
Avoidance of hazardous sources
This section deals only with research needed for evaluation of the cancer hazard, although
we recognize that other areas also need further research.
6.2. INFORMATION NEEDS ARISING FROM THE EVALUATION IN THIS DOCUMENT
The evaluation carried out in this document has raised several unanswered questions
about the carcinogenic potential of EM fields. The major information needs that have been
identified are outlined in this section. Before these needs can be translated into a research
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program, the ongoing research that is now being carried out must be taken into account. This
is not being attempted in this section; rather, the emphasis here is on the issues about
population hazards that need to be dealt with before an evaluation of the public health hazards
and the determination of meaningful preventive measures can be made.
6.2.1. Epidemiology Research Needs
The association between cancer occurrence and exposure to either extremely low
frequency (ELF) or radiofrequency (RF) fields is not strong enough to constitute a proven
causal relationship, largely because the relative risks in the published reports have seldom
exceeded 3.0 in both childhood .residential exposures and in occupational situations. Two
possible explanations for this are: (1) our imprecise knowledge of the causal aspects of
exposure (field strength, frequency, time patterns of exposure, and synergistic factors)
prevents us from identifying exposure indices that distinguish exposed from unexposed
populations, or (2) the observed effects are actually caused by some other factor not related to
the EM-fields but which co-varies with EM-field strength. A third possible explanation is that
exposures have been too weak to produce an observable effect. This cannot be evaluated
because there is currently no reasonable basis for making predictions of the expected human
response.
To evaluate the first two possibilities, two things need to be done: (1) define job categories
in electrically-related occupations to reflect actual exposure to EM fields. These definitions
would be used as the basis for selecting cohorts for study. These studies should be designed
to investigate a variety of exposure parameters, which need to be judiciously selected using
the most recent concepts of likely mechanisms of carcinogenesis; and (2) investigate, with
improved study designs and exposure measurements, those populations that have already
showed some excess risk from EM fields or have potentially high exposures, such as military
communications and radar workers; amateur radio operators; telephone and electrical utility
workers; electric-arc welders; aluminum smelter workers; engineers, scientists, and computer
operators working with electrical equipment; people living near radio and TV broadcast
towers; users of electric blankets; and Hodgkin's lymphoma patients. In designing these
studies, special attention needs to be given to confounding variables in order to avoid an
incorrect attribution of the effects to EM fields simply as a consequence of the intense scrutiny
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given to them. More information about the risks of RF and modulated RF exposure is needed
before any conclusions can be made about either their safety or hazard.
6.2.2. Laboratory Research Needs
Both animal and in vitro studies are needed to discover the relevant exposure factors and
their interaction, to gain some understanding of the mechanisms of action, and to extrapolate
"effective doses" to the human exposure situation.
For long-term animal studies, the most obvious need is to conduct a carcinogen bioassay
with magnetic field ELF exposures. The experiment planned by the Ontario Hydroelectric
Power Company (described in Section 4.6) will be the first animal carcinogen bioassay to be
done with 60-Hz magnetic fields. It may or may not confirm the human findings and will
generate additional research topics regardless of the outcome. Since the University of
Rochester study is already examining the effect of ELF electric fields on the growth rate of
mammary carcinomas in rats, there is not a high priority need at this time to initiate another
chronic experiment with electric fields. However, this same type of study is needed for ELF
magnetic fields. If these studies show that a carcinogenic response is induced in animals by
these ELF exposures, then whether RF fields modulated at the same ELF frequencies will
produce comparable effects is the next logical question, since modulated RF exposures are
common and some laboratory phenomena (Table 5-7) have the same effect with or without the
RF component.
For in vitro studies, several biological phenomena, having some relationship to possible
mechanisms of carcinogenesis, have been induced by EM fields. The discussion in Section
5.11 summarizes the large amount of missing information relative to the biological effects of
EM fields and forms the basis for this discussion. The overall goal of the research program
would be to select the most promising candidate mechanisms of cancer induction at ambient
electric and magnetic field strengths and frequencies and to experimentally investigate, in
laboratory in vitro tests and in whole animals, the way in which each process depends upon
several field exposure parameters, such as type of field (alternating electric and magnetic
fields, geomagnetic fields), field strength, and frequency and time patterns of exposure
(steady, intermittent, time of day). The leading research areas identified in this review are:
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Biological response to weak fields
If ambient 60-Hz magnetic fields [which have strengths on the order of 5 milligauss
(mG) or less] are really causing a cancer response, then tissue currents on the order
of 1CT4 microamperes per square centimeter (uA/cm2) must be able to induce some
kind of change in cellular metabolism. Of the processes reviewed in this document,
there are only three that occur at field strengths comparable to this: (1) calcium release
from chick brain tissue in response to crossed electric and magnetic fields; (2) the
change in melatonin secretion in rats induced by a small change in the orientation of
the static magnetic field; and (3) calcium release from chick brain tissue induced by
electric fields. Since the first phenomenon empirically exhibits frequency selectivity,
there is at least a theoretical possibility that weak currents of the correct frequency
could induce an effect even though they are within the range of thermal noise. There is
a need to establish a mechanism that would explain how magnetic fields could induce
such a calcium release from brain tissue. Ion cyclotron resonance and the quantum
beat models are two possibilities, and experiments are needed to test those hypothe-
ses. However, nuclear magnetic resonance has been suggested as another possibility,
and that has not been examined.
The effect of low-strength alternating magnetic fields on melatonin secretion has not
been measured, and the single observation that a very small change in magnetic field
orientation has induced an inhibition of synthetic activity needs to be verified. Of partic-
ular interest is the ELF frequency and intensity dependence of this inhibition. In addi-
tion, it would be of interest to ascertain whether modulated RF fields affect pineal
melatonin synthesis.
Chemical signalling pathways for controlling cell proliferation
Since the transduction of hormone and other chemical signals into the cell is a neces-
sary step in the hormonal control of cell proliferation, and since this transduction pro-
cess is defective in transformed cells, the influence of EM fields on signal transduction
has a potentially important role in the development of cancer. The experiments on or-
nithine decarboxylase (ODC) (Section 5.6), gene transcription (Section 5.3), and para-
thyroid hormone (Section 5.5) raise the possibility that electric and magnetic fields
interfere with the normal functioning of signal transduction pathways. The effects of
EM fields on one of the major pathways, the receptor-mediated activation of phos-
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phoinositide turnover, has not been explored but should be because this pathway is in-
volved in several phenomena related to cell proliferation. This pathway involves
diacylglycerol (DAG), which is a structural analogue of the tumor promoter TPA, both of
which activate protein kinase C (PKC), and, ultimately, ODC. It also involves inositol
trisphosphate (IPS), which is known to release calcium from intracellular stores and the
plasma membrane. Both DAG and IPS, through calcium release, activate PKC which
phosphorylates growth factor receptors and proto-oncogenes and is believed to play a
role in the control of cell proliferation. As our understanding of these pathways be-
comes more detailed, we will be able to postulate chemical synergisms and antago-
nisms with EM fields. Further study of parathyroid hormone as a mediator of bone
healing response to magnetic fields will lead to a better appreciation of the interaction
between hormones and EM fields in the control cellular proliferation.
In addition to the chemical events associated with the cell membrane, the influence of
EM fields on the dynamics of charged membrane-bound proteins needs to be studied.
There is a possibility that the alternating electric field at the membrane or currents in-
duced by these fields directly affect enzymatic reactions, such as ion transport reac-
tions, carried out by these proteins. There is also the possibility that the fields modify
the opening and closing of ion-conducting channels in the membrane, and they could
affect the stability of membrane receptors.
Gene expression
The influence of EM fields on the expression of genetic activity, both with respect to
transcription to mRNA's and in translation of genetic information into protein synthesis,
is needed. It is important to study how this process is connected to chemical signalling
pathways.
Cell transformation
The single experiment showing that modulated microwave radiation acts as an initiator
of the transformation of C3H10T1/2 cells to malignancy needs to be verified and re-
peated with ELF magnetic and electric fields. The interaction of EM-field exposure with
other factors known to influence transformation in this well-studied system may lead to
clues as to the mechanism of this transformation.
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Meiatonln Activity
Although it is well known that melatonin inhibits the growth of hormonally dependent tu-
mors and that electric field exposure inhibits the synthesis of melatonin by the pineal
gland, the effect of ELF fields on these end points has not been directly studied. In ad-
dition, the question of whether ELF magnetic fields inhibit melatonin secretion is espe-
cially important in view of the postulated human response to magnetic fields. This
mechanism becomes especially important to the induction of leukemias and lympho-
mas by EM fields in view of the successful treatment of clinical leukemia with melatonin
(Section 5.7.1).
Ion cyclotron resonance interaction
Several questions need to be answered about the ion cyclotron resonance phenome-
non:
- In artificial membranes impregnated with channel proteins of various ion
specificities, does the ion cyclotron resonance field open an ionic conduction
channel, as one experiment with cell suspensions suggests?
- Does the calcium release from brain tissue depend on an ion cyclotron resonance
process?
- Are other intracellular processes dependent on specific ions triggered by plasma
membrane ion gating induced by ion cyclotron field conditions? This process has
been implicated as a mechanism of diatom locomotion mediated by intracellular
calcium ions and hypothetical^ for rat behavioral patterns mediated by lithium, but
more examples are needed, perhaps with sensory cells and with cells in which
field-sensitive biochemical reactions are taking place.
In planning and executing this research, it is important to recognize that effects of fields on
the whole animal are likely to be unpredictable based on the results of laboratory in vitro
systems, so that there is a constant need to verify these effects in the whole animal before
being able to make valid inferences about effects in humans.
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7. SUMMARY AND CONCLUSIONS
7.1. INTRODUCTION
In this chapter each of the major chapters in the document are summarized; a final section
presents a discussion of the relationships among the individual chapters and the overall
conclusions.
7.2. MECHANISMS OF INTERACTION BETWEEN TISSUE AND ELECTROMAGNETIC
FIELDS
The basic processes by which energy from electromagnetic (EM) fields of radiofrequency
(RF) and extremely low frequency (ELF) frequencies is coupled to the body are described in
this section. The frequency dependence of the RF power absorbed by an organism is
dominated by the body size, so that mice, rats, and humans have different RF absorption
characteristics. For ELF fields and the lower RF frequencies near the source, the relationship
between the electric and magnetic fields is not fixed, as it is for RF fields, and they are
evaluated separately in this document. From the point of view of EM fields, the body is
composed of a solution of ions; it is an electrical conductor and the penetration of electric
fields into the body is very poor at ELF frequencies. Since the body is composed of
nonmagnetic materials, an external time-varying magnetic field permeates the body, inducing
ionic currents.
The human evidence, as described in the next section, suggests that magnetic fields,
rather than electric fields, are associated with cancer incidence, and mechanisms have been
sought to explain how weak currents induced by ELF magnetic fields could interact with cells
and body tissue in such a way as to induce a carcinogenic response. Three classes of
models for this interaction are reviewed. (1) The surface compartment model deals with the
movement of ions towards and away from the inner and outer surfaces of the plasma
membrane of the cell, and deals with ion-selective membrane channels, ionic pumps, and
membrane ion fluxes. The model describes the movement of ions in response to
perturbations of electric fields and magnetically induced currents around the cell. (2) The ion
cyclotron resonance hypothesis was developed in part to explain the frequency sensitivity of
calcium ion efflux studies of brain tissues. If the relationship among the frequency of
time-varying magnetic field, the strength of a parallel static magnetic field, and the ionic charge
to mass ratio of an ionic species is correct, then the ion will resonate, or synchronously follow
circular paths in a plane perpendicular to the field. In one experiment demonstrating this
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effect, conditions were set up for calcium cyclotron resonance, and the movement of benthic
diatoms was measured. The authors interpreted the experiment as showing that calcium ions
entered into the cell under these specific conditions and stimulated the motion of the cells,
whereas the cell is normally impermeable to calcium. This type of mechanism could be the
basis of an induced selective ion permeability of the plasma membrane and might ultimately
be capable of explaining both frequency selectivity of these effects and the sensitivity to small
induced currents. (3) Another class of models deals with cooperative motions of an ordered
array of lipid bilayer molecules and describes how a weak field affecting the motion of the
whole array could be transferred to just one site in the array. These theories have not yet
been tested in the context of ELF biological processes. At the present time, these basic
models of tissue interaction with EM fields cannot be linked to the biochemical or cellular
processes involved in the development of malignant growth.
7.3. HUMAN EVIDENCE
The effects of human exposure to EM fields from several sources have been reported. This
document discusses ELF fields separately from higher frequency exposure where possible.
Children with residential exposure are more appropriate subjects than adults for evaluating the
effects of ELF fields, since children have relatively little exposure to higher frequency fields and
occupational chemicals as a consequence of their normal activity patterns. Consequently,
studies of childhood cancer associated with residential exposure to 60-Hz power frequency
fields are discussed separately from occupational exposure to adults, which involves a mixture
of both ELF and RF fields.
7.3.1. Studies of Children
There have been seven case-control studies of cancer in children examining residential
exposure from power transmission and distribution systems. Two additional studies have
examined childhood cancer in relationship to father's occupation. Six of the seven residential
exposure studies showed positive associations with ELF field exposure; three were statistically
significant and the other three had odds ratios greater than one but not statistically significant.
Where different cancer sites were evaluated, leukemia, nervous system cancer, and, to a
lesser extent, lymphomas were found to be in excess in the five residential studies showing
positive associations. Electric fields were not found to be a critical factor thus far. Surrogates
of magnetic field exposure differed among the seven studies. Wire code configurations and
proximity to distribution lines were used in six of the seven studies, and measurements were
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taken in two of the seven studies. There is a reasonably good, but not perfect, correlation
between measured magnetic fields and wire code configurations. In two of the studies in
which magnetic field measurements were made, cases were observed in those exposed at or
above 2 to 3 milligauss (rnG) [0.2 to 0.3 microtesla (/
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7.3.2.2. Occupational Exposure to Extremely Low Frequency and Mixed
Frequency Fields
Twenty-eight reports dealing with cancer incidence or mortality in workers in electrical and
electronic occupations have been reviewed. These exposures have involved 50 or 60 Hz
power frequency fields as well as mixtures of higher frequency fields which are typically poorly
defined. The studies have been carried out in Europe, New Zealand, and the United States.
Many of them were re-examinations of previous studies or evaluations of vital records, cancer
registry, or occupational data bases, and thus the populations were not formed to test the
specific hypothesis of whether EM-field exposure is associated with increased cancer risk.
Most of them used death certificates as a source of occupational information; this information
furnishes only a very crude indicator of actual exposure to EM fields. Many of these are
proportional mortality studies, which are less informative than studies of cohort and
case-control designs because their results are affected by extraneous causes of death.
In these studies three types of cancer predominate: (1) hematopoietic system, especially
leukemia and specifically acute myeloid leukemia; (2) nervous system cancer, including brain
tumors; and (3) malignant melanoma of the skin. These cancer sites are found consistently
across different geographic regions, age groups, industries, occupational classifications, and
study designs. Given this diversity of studies, in addition to the likelihood that across broad
job categories the exposures to various chemicals is not uniform, it is difficult to identify any
single agent or group of confounding exposures that could explain the consistent finding of
these same cancer sites.
7.3.2.3, Radiofrequency Exposure
Reports that focused primarily on exposures to RF radiation have shown mixed results, but
most of the studies were difficult to interpret. Two early reports concerning microwave
exposure of U.S. embassy personnel in Moscow and radar exposure of U.S. Navy personnel
showed only a slight tendency for increased cancer risk at all sites, and somewhat higher
odds ratios for hematopoietic system cancers. A study of personnel in a World War II radar
research and development laboratory found no convincing evidence of increased cancer
incidence, but errors of exposure misclassification are likely. A series of reports of ham radio
operators found a statistically elevated incidence of acute myeloid leukemia and other
neoplasms of the lymphoid system, but no clear dose-response trend was seen with longer
exposure, where the degree of exposure was inferred by FCC operator license class. One
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report of military exposure to radar found increasing rates of hematopoietic cancer of specific
sites, but a lack of detail limits the ability to interpret the results.
7.3.3. Summary of Human Evidence
The strongest evidence that there is a causal relationship between certain forms of cancer,
namely leukemia, cancer of the nervous system, and, to a lesser extent, lymphoma and
exposure to magnetic fields comes from the childhood cancer studies. Several studies have
consistently found modestly elevated risks (some statistically significant) of these three
site-specific cancers in children. In two of the studies in which magnetic field measurements
were made, cases were observed in those exposed above 2 to 3 mG (0.2 to 0.3/*T) but not in
children exposed below that level. This is supported by the fact that children have relatively
few confounding influences that could explain the association. In fact, the few potential
confounders and biases that might have had an effect on the results were examined by one of
the authors in some detail and found not to be a serious problem. No other agents have been
identified to explain this association. However, there are contradictory results within these
same studies, and dose-response relationships could not be substantiated. Furthermore,
there is little information on personal exposure and duration of residency in the EM fields.
Additional, but weaker evidence that there is an elevated risk of leukemia, cancer of the
nervous system, and perhaps other sites comes from occupational studies of EM-field
exposure. Although many of these studies have found an excess risk of these forms of cancer
with employment in certain jobs that have a high potential for exposure to EM fields, few or no
measurements have actually been taken in those occupations. Furthermore, information
about occupation has come generally from sources that could be characterized as sketchy
The likelihood that misclassification or information bias is present in these studies is high.
However, exposure misclassification, if random, tends to bias relative risks toward the null.
Despite these weaknesses, the occupational studies tend to support the results of the
childhood studies, since the excess relative risks occur at the same sites.
The studies of residential adult exposures to EM fields provide little evidence of a risk of
leukemia, mainly due to a lack of statistical power and/or probably little exposure to levels of
EM fields that have been found to be associated with cancer in children. These studies cannot
be interpreted as evidence either for or against a causal association between cancer and
EM-field exposures. On the other hand, the case-control study of cancer in Colorado
residents does support an association of central nervous system cancer and lymphoma if
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proximity to high-current electrical wiring configurations is assumed to be an adequate
surrogate for exposure.
The studies of adults exposed to RF radiation produced mixed results, primarily because ol
limited sample size, inadequate length of follow-up, imprecise exposure data, and lack of
information on potential confounders. These problems prevent conclusions to be made about
causal relationships with RF exposure. However, the statistically significant excess risks of
leukemia in amateur radio operators requires further examination.
7.4. ANIMAL EVIDENCE
7.4.1. Extremely Low Frequency Fields
No lifetime animal carcinogen bioassay studies of ELF fields have been reported in the
literature. Several studies currently in progress are designed to observe the induction of a
carcinogenic response to chronic magnetic field exposures.
7.4.2. Radiofrequency Radiation
Two chronic studies in mice have used unmodulated RF radiation at 800 megahertz (MHz)
and 2450 MHz, respectively. Two studies in rats have used pulse modulated 2450 MHz of low
power density and pulsed RF of all frequencies from 0 to about 20 MHz of high power density,
respectively. One mouse study used pulsed RF radiation of 9270 MHz.
7.4.2.1. Unmodulated Radiofrequency Radiation
For unmodulated RF radiation one of the mouse studies (Szmigeilski et al., 1982) shows
that the radiation enhances the growth rate of spontaneous mammary tumors and in a
separate experiment enhances the growth rate of skin tumors initiated by a chemical
carcinogen, benzo[a]pyrene. In a shorter test (3 months), the same authors showed that the
radiation also enhances the growth rate of transplanted lung carcinoma cells, an effect
attributed to the lowering of cell-mediated immunity. Unfortunately, histopathology was not
reported in the other mouse study (Spalding et al., 1971), so conclusions about
carcinogenicity from that study are difficult to make.
The special nature of the response indicates that unmodulated RF radiation might be a
promoter or cocarcinogen, since the growth rate of spontaneous breast tumors, BaP-induced
skin tumors, and transplanted lung sarcoma cells is enhanced by the radiation. There is a
remote possibility that body heating could have contributed to this response, since the
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absorbed RF power is estimated to be at least one-half of the basal metabolic rate of the
animals.
7.4.2.2. Modulated Radiofrequency Radiation
For modulated RF radiation of relatively low power density [i.e., excluding the high power
electromagnetic pulse (BMP) experiment of Baum et al. (1976)], the mouse experiment
(Prausnitz and Susskind, 1962) showed a reversible pattern of lymphoma and leukemia which,
in serial sacrifices, occurred toward the end of the 14-month exposure period but was not
present in animals after a 5-month recovery period. However, the short 4.5-minute daily
exposure was intense enough to raise the body core temperature by 3° C, raising the
possibility that thermal effects were a contributing factor in the response. The rat study (Guy
et al., 1985) showed the induction of benign adrenal medulla pheochromocytomas and a
statistically significant increase in carcinomas of all organ and tissue sites. There was also a
statistically significant increase in glandular organ carcinomas which was unaccompanied by
an increase in the incidence of benign tumors of these sites. Such an increase of tumors of all
types in the aggregate without increase of tumors at any one of the sites is regarded as only
minimal evidence of a carcinogenic response.
7.5. SUPPORTING EVIDENCE OF CARCINOGENICITY
Section 5.11. presents a summary of the effects of EM fields on a variety of basic biological
phenomena relevant in some way to mechanisms of carcinogenesis; that information is not
repeated here. ELF fields of relatively high intensity [producing induced body currents on the
order of 10 microamperes per square centimeter (^A/cm2)] have enhanced DNA synthesis,
altered the transcription of DNA into mRNA, altered the molecular weight distribution during
protein synthesis, delayed the mitotic cell cycle, induced chromosome aberrations, blocked
the action of parathyroid hormone at the site of its plasma membrane receptor, induced
enzymes normally active during cell proliferation, inhibited differentiation and stimulated the
growth of carcinoma cell lines, inhibited the cytotoxicity of T-lymphocytes (which indicates an
impairment of the immune system) in vitro but not in vivo, inhibited the synthesis of melatonin
(a hormone that suppresses the growth of several types of tumors), and caused alterations in
the binding of calcium to brain tissues. The large variety of exposure conditions and the lack
of detail on the geometry of the biological samples in these studies precludes a systematic
evaluation of the actual induced currents and field strengths at the tissue and cellular levels
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that are causing these effects. In addition, the lack of reproducible results between
laboratories limits the interpretation of much of this literature.
Radiofrequency fields modulated at the same ELF frequencies that cause some of the
effects noted above also result in the same responses, indicating that the ELF component may
be responsible for these effects. Unmodulated RF radiation has not caused any of the effects
noted above except for chromosome aberrations. None of the EM fields have caused gene
mutations, sister chromatid exchanges, or DNA damage (as measured by DNA breaks, DNA
repair, or differential killing of repair defective organisms) in a large number of studies.
Only three ELF effects have been induced at field strengths comparable to the low
environmental exposures at which human cancer has putatively been caused: (1) the calcium
efflux from brain tissue preparations using 16-Hz electric and magnetic fields that were
perpendicular to each other, (2) calcium efflux from chick brain tissue after exposure of the
developing embryo to electric fields, and (3) the inhibition of melatonin synthesis by the pineal
gland when a static magnetic field of approximately the strength of the earth's magnetic field is
changed through a small angle of rotation. The results of the first experiment are one of
several phenomena that show a complex dependence on frequency, intensity, and orientation
with respect to the earth's magnetic fields.
In view of all of the laboratory studies referred to in this section, there is reason to believe
that the findings of carcinogenicity in humans are biologically plausible. However, the
explanation of which of the biological processes is involved and the way in which these
processes causally relate to each other and to the induction of malignant tumors is not
understood. Most of the effects have been observed at field strengths that are many times
higher than the ambient fields which are the putative cause of the childhood cancers in
residential situations; as a consequence, many of the candidate mechanisms actually may not
be involved in the response to low environmental fields. The same issue of low-dose
extrapolation arises in the evaluation of chemical agents.
7.6. INTEGRATED DISCUSSION OF SEPARATE CHAPTERS
The occurrence of cancer in humans exposed to low frequency electric and magnetic
fields has been observed under several different conditions in different populations.
Residential exposure of children, but not adults, has been associated with leukemia,
lymphoma, and brain cancer, and the same sites occur in multiple studies of children. The EM
fields involved in these associations have been magnetic fields rather than electric fields, and
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their frequency is made up of primarily 60-Hz components but with inevitable high-frequency
components introduced by electric motors and the switching of currents on and off. These
effects have been observed jn children exposed to magnetic fields at or above 2 to 3 mG (O.2
to 0.3 fiJ). The types of EM-field exposures in the occupational studies are variable according
to job category, with some jobs involving pulsed and modulated RF fields as well as 60-Hz
power frequency components. It is not possible to rule out the involvement of electric fields in
these studies. Exposure to electric fields is extremely variable under ambient conditions and is
difficult to define.
There is some, but not well-established, evidence that higher frequency components have
different effects than 60-Hz components. Electrical switchyard workers exposed to spark
discharges just before blood samples are taken have chromosome aberrations, whereas
similar workers with no such exposure do not. Chromosome aberrations have been induced
by unmodulated RF fields as well as by ELF fields. A recent preliminary report of an
epidemiologic study of telephone workers shows a different effect (rare breast tumors in
males) in people working in the "central office," where switching equipment is typically
concentrated, than in cable splicers (leukemia) who presumably are exposed to predominantly
60-Hz power frequencies. Both electric and magnetic fields are more effective in inducing
currents in the body if their frequency is higher, so that if induced currents are responsible for
these effects, then the higher frequency components are expected to be more effective. If it is
true that, as two studies indicate, the father's occupation in electrical jobs is a factor in the
development of leukemia in their children, then the question is raised whether the effect could
be transmitted via heritable genetic damage in sperm. This speculative hypothesis needs to
be investigated.
Although there are several candidate EM field-induced biological phenomena (discussed in
Chapter 5) that could explain how a cancer response is caused in the whole organism by
these fields, none of these or any combination of them has been verified experimentally, either
in laboratory animals or in humans. Without understanding which combination of these is
relevant to the carcinogenic process, it is not possible to hypothesize what aspect of EM-field
exposure is responsible for biological effects; i.e., frequency, average peak field strength,
duration, time of day, whole-body average versus local critical site, electric versus magnetic
fields, orientation with respect to the earth's static magnetic field. The choice of which aspect
of the fields is the most relevant could be based on either knowledge of the correct
mechanism of action or on empirical epidemiology correlations, but, given the current lack of
information, neither method can serve as a basis for a dose-response analysis.
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There are several indications that EM fields might contribute to the induction of cancer via
indirect mechanisms, in contrast to a direct mutagenic action of DMA as is the case with
nitrosamines, polycyclic aromatic hydrocarbons, or other DNA-alkylating agents.
First, EM fields have not caused gene mutations in any of the large number of experiments
carried out with both ELF and RF fields (Section 5.1.3).
Second, there is no indication from the animal studies that RF fields cause a de novo
induction of tumors (Section 4.1.2.7). On the contrary, the mouse experiments by Szmigielski
et al. (1982) (see Section 4.4) indicate that unmodulated RF radiation acts as a growth
stimulator for pre-existing tumors. The same growth-stimulating or promotion characteristics
of RF fields could explain the induction of glandular tumors in the Guy et al. (1985) lifetime rat
study of modulated RF radiation (Section 4.1.2.7), since many of the glandular tumors in that
study had a naturally high spontaneous incidence.
A third factor indicating that there may be multiple causes of carcinogenic action is that
120-Hz pulse-modulated 2450 MHz radiation can act as an initiator of phorbol ester-promoted
cell transformation in mouse embryo cell cultures (Section 5.3.3).
Finally, there are possible cancer induction mechanisms mediated by the central nervous
system causing neuroendocrine influence on cellular proliferation (Section 5.7.5). These
mechanisms involve possible extremely sensitive detection of magnetic fields by the retina
(Section 5.10.4) with resulting neural control of pineal melatonin activity, which in turn
modulates estrogen and prolactin levels in the blood supply to the breast, prostate, and other
hormonally sensitive tissues (Section 5.7.1). Other speculative chains of events could be
fabricated from the existing information in this document; this one is mentioned here only as
an example that there are many possible explanations, but no verified ones.
In view of these indications, it is likely that if EM fields do contribute to the induction of
cancer, the causal relationship will probably turn out to be dependent on many chemical
factors and physiological conditions that are currently poorly understood.
There are two issues in the hazard evaluation of chemical carcinogens that are analogous
to issues for EM fields. It may be helpful to explore whether the assumptions and conventions
developed for chemicals are applicable to the EM fields problem.
One analogy is that EM fields are mixtures consisting of several frequencies, intensities,
and combinations of electric and magnetic fields that (for ELF frequencies) occur in arbitrary
proportions. One approach to the assessment of chemical mixtures is to identify hazardous
components of the mixture apd, assuming additivity of components, consider the risk of the
mixture to be proportional to the risk of the hazardous components. If this concept were
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applied to the EM fields problem, then magnetic fields from 60-Hz power usage in the home
would be the only "hazardous component" identified, although there is some indication that
occupational exposures of adults to mixed fields may cause the same effect. Laboratory
studies under relatively controlled conditions of exposure have not been able to test the
additivity assumption for EM-field components or for chemical components except for a few
rare cases, but one feels more comfortable with the latter. With chemical agents, the basic
phenomenon is ultimately some chemical reaction, which is expected to have additive
properties at low enough concentrations, or at least to be monotonic in the sense that more
chemical produces a greater effect. With EM fields, however, the ultimate causative interaction
between fields and biological systems is unknown, and there is certainly no additivity with RF
and ELF fields, or with ELF electric and ELF magnetic fields. The consequence of not being
able to add the risks for different exposures is that the effects for each combination must be
investigated and assessed separately.
Another analogy is the similarity between the "biologically effective dose" for chemical
agents and the critical electrical measure of tissue "dose" which causes the effect for EM fields.
For chemical agents the relationship between "administered dose" and "effective dose" has
been studied occasionally, but only rarely. In the absence of this information, the default
position for chemical agents has been to assume a linear relationship. Then there are several
unresolved questions in determining whether the biological effect is proportional to the
"effective dose." These questions arise when, as is usually the case, the mechanism of action
is not known. Here again the linearity assumption is made in the absence of knowledge, and
the overall default position is that the adverse effect is proportional to the administered dose of
the chemical agent. For EM fields, the "tissue doses" could be calculated, typically with great
difficulty and uncertainty, but the same type of questions need to be answered about which of
these dose metrics are relevant for EM-field exposure. As with chemical agents, the choice of
a candidate mechanism of action dictates which tissue dose metric is appropriate, and there
could be several mechanisms for each of the administered agents. For EM fields, the default
linearity assumption may not be appropriate, basically because there are frequency and
intensity "windows" of activity for more than one EM field-induced biological effect, and such
"window" interactions cannot be ruled out as contributory to cancer causation. On the other
hand, ambient human exposure involves a wide range of static magnetic fields, frequencies,
intensities, and intermittent exposures, so that narrow windows of response may not be the
dominant practical exposure consideration, and a higher average field may simply increase the
probability that a "windowed" condition will occur.
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In conclusion, several studies showing leukemia, lymphoma, and cancer of the nervous
system in children exposed to magnetic fields from residential 60-Hz electrical power
distribution systems, supported by similar findings in adults in several occupational studies
also involving electrical power frequency exposures, show a consistent pattern of response
that suggests a causal link. Frequency components higher than 60 Hz cannot be ruled out as
contributing factors. Evidence from a large number of biological test systems shows that
these fields induce biological effects that are consistent with several possible mechanisms of
carcinogenesis. However, none of these processes has been experimentally linked to the
induction of tumors, either in animals or humans, by EM fields. The particular aspects of
exposure to the EM fields that cause these events are not known.
in evaluating the potential for carcinogenicity of chemical agents, the U.S. Environmental
Protection Agency has developed an approach that attempts to integrate all of the available
information into a summary classification of the overall weight of evidence that the agent is
carcinogenic in humans. At this time such a characterization regarding the link between
cancer and exposure to EM fields is not appropriate because the basic nature of the
interaction between EM fields and biological processes leading to cancer is not understood.
For example, if induced electrical currents were the causative factor, then exposure to electric
as well as magnetic fields would be important and the effect would be more severe as the
frequency increases. But if the direct magnetic field interaction were the critical factor, then the
ambient static magnetic field as well as the alternating magnetic field would be critical and the
effect may be confined to specific frequencies, resulting in an extremely complicated
dose-response relationship. In addition, if they were shown to be causative agents, these
fields probably exert their effects via other chemical and environmental factors rather than
directly causing events known to be causally related to the carcinogenic process, having the
direct property of causing cancer, as with genotoxic chemical agents.
Because of these uncertainties, it would be inappropriate to classify the carcinogenicity of
EM fields in the same way as the agency does for chemical carcinogens. As additional studies
with more definitive exposure assessment become completed, a better understanding of the
nature of the hazard will be gained. With our current understanding we can identify 60 Hz
magnetic fields from power lines and perhaps other sources in the home as a possible, but not
proven, cause of cancer in people. The absence of key information summarized above makes
it difficult to make quantitative estimates of risk. Such quantitative estimates are necessary
before judgments about the degree of safety or hazard of a given exposure can be made.
This situation indicates the need to continue to evaluate the information from ongoing studies
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and to further evaluate the mechanisms of carcinogenic action and the characteristics of
exposure that lead to these effects.
ti- U.S. GOVERNMENT PRINTING OFFCE: 1990-548-187/2050^
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