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A Comprehensive Review of the Research on Biological Effects of Pulsed Radiofrequency Radiation in Russia and the Former Soviet Union


Abstract and Figures

Pulsed radiofrequency (RF) radiation nowadays is among the most ubiquitous of environmental factors. Biological effects and health hazards of pulsed RF have been studied for decades, but there is still little consensus on whether the safety of pulsed RF should be given any special consideration compared to continuous wave (CW) emissions. While it is well known that pulsed fields can produce effects principally different from those of CW (e.g., an auditory effect, see Lin, 1990), potential implications of such effects for human safety and wellbeing continue to be debated.
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Andrei G. Pakhomov1,2 and Michael R. Murphy2
1McKessonHBOC BioServices, U.S. Army Medical Research Detachment of the Walter
Reed Army Institute of Research
2Directed Energy Bioeffects Division, Human Effectiveness Directorate, Air Force Research
Brooks Air Force Base, San Antonio, Texas, USA
Pulsed radiofrequency (RF) radiation nowadays is among the most ubiquitous of environmental
factors. Biological effects and health hazards of pulsed RF have been studied for decades, but there is still
little consensus on whether the safety of pulsed RF should be given any special consideration compared to
continuous wave (CW) emissions. While it is well known that pulsed fields can produce effects principally
different from those of CW (e.g., an auditory effect, see Lin, 1990), potential implications of such effects
for human safety and wellbeing continue to be debated.
A significant contribution to the field of bioelectromagnetics has been made by the research
performed in the former Soviet Union (FSU). Unfortunately, most of this research was published in
Russian; these publications are scarcely available in the West and have not ever been reviewed in English.
Even some key findings, which may affect the conceptual understanding of interaction mechanisms and
approaches to RF safety, seem to be not known in the West, and their replication in Western laboratories
has never been attempted.
The goal of the present paper is to fill in this void and deliver a comprehensive review of the FSU
research on biological effects and potential health hazards of pulsed RF radiations.
The principal source of information is a personal collection of scientific publications in Russian,
which was accumulated as a part of a 7-year effort of one of the authors (A.G.P.) to monitor and review the
Russian/FSU research in the area of electromagnetic biology. Currently, this collection includes over 1200
titles and is one of the largest of its kind.
Over 1000 of the collected studies were abstracted in English, and the abstracts are included in the
electronic EMF Database (produced and distributed by Information Ventures, Inc., PA, USA). This
Database (v. 3.2.4, 1999), which is the second major source of information for the current review, contains
about 26000 unique citations of studies on bioeffects of electromagnetic fields (from DC to mm-waves).
Out of them, there are about 3600 citations of studies performed in the FSU (and published in either
Russian or English); we estimate that this bibliography includes at least 80% of related studies performed
in the FSU and published in the open (unclassified) literature since 1975 (earlier papers are only scarcely
included in the Database). The EMF Database proved to be extremely convenient as a fast reference and
information search engine, while the scientific quality of studies usually had to be judged from the original
For the purpose of this review, the term "pulsed RF" applies to any pulsed, intermittent, or amplitude-
modulated electromagnetic emissions with carrier frequencies from units of megahertz up to 300 GHz. A
detailed search of the EMF Database revealed a total of 206 citations of pulsed RF studies performed in the
FSU. For convenience, they will be referred to below as "Russian" studies, disregarding the exact place of
origin (e.g., Russia or Ukraine) or the language of publication. A similar search for "non-Russian"
publications on the subject revealed 1342 citations. The percentage of pulsed RF publications out of the
total number in the Russian and non-Russian bibliographies was remarkably the same (6%).
These 206 citations were individually sorted to remove all meeting abstracts, review papers, and
papers on dosimetry, modeling, standards setting and enforcement; then we added appropriate Russian
papers not cited in the Database. The final outcome was 114 original experimental Russian studies on
pulsed RF bioeffects.
Of these studies, over 70% were performed in laboratory animals. Only a few studies (<4%)
employed pro- or eukaryotic cell cultures, whereas a lot of research was done in various isolated organ
preparations (about 20%). A relatively large number of studies (>35%) explored effects of chronic
It is generally accepted in Russian science that the nervous system is the most sensitive to
electromagnetic radiation. Indeed, studies of pulsed RF effects on nervous system function and structure
are by far the most numerous (>65%); electrophysiological and behavioral techniques are the most widely
used. In a striking contrast with the Western research, not a single study has explored possible carcinogenic
effects of pulsed RF; apparently, this possibility has never been a concern in Russian science.
Presumably nonthermal (or "RF-specific") bioeffects were found in 88 studies, which is more than
90% of all studies that searched for such effects. Among them, 34 studies compared bioeffects of various
modulation regimens and/or those of CW versus pulsed RF. In most cases (>80%), it was found that pulsed
RF effects indeed depend on modulation and/or are different from effects of CW irradiation at the
equivalent time-average intensity. These data indicated that pulsing may be an important (or even the most
important) factor that determines the biological effects of low-intensity RF emissions.
The most common question about Russian research in the bioelectromagnetic area is its scientific
quality. Indeed, noticed flaws include unclear or invalid experiment protocols (e.g., lack of a sham-exposed
control group); absence of good thermometry and dosimetry (in most animal studies, the specific
absorption rate (SAR) was neither measured nor calculated); inadequate statistical analysis; failure to take
into account specifics of biological experimentation with RF radiation (e.g., the use of metal recording
electrodes in electrophysiological studies with RF could cause serious artifacts); and failure to report if all
potential sources of the artifact were considered (e.g., the noise from a working RF transmitter can cause
behavioral responses that may be misinterpreted as an RF bioeffect). While many studies were flawed in
one way or another, or were poorly presented in publications, still many other Russian studies
demonstrated a high-quality research.
For any study on RF bioeffects, whether flawless or not, the most critical issue is independent
replication of findings. Until (or unless) proven wrong in replicative studies, the results of any reasonable-
quality research deserve attention and careful consideration. That is why we attempted to address in this
review all available Russian studies on pulsed RF bioeffects that meet at least the minimum scientific
quality criteria. The other studies, which failed to meet these criteria (as far as it could be judged from the
published material), were generally regarded as unacceptable. For example, all of the available Russian
epidemiological studies with pulsed RF reported adverse health effects of exposure (such as "asthenic
syndrome" or "radiofrequency disease"), but none of them showed reasonable evidence that these disorders
were in fact caused by the RF exposure; besides, these studies reported too little or even no data about the
exposure parameters. Because of the poor quality, none of the Russian epidemiological studies are
included in the present review.
Among the "acceptable" studies, more credit was given to those that (1) reported interesting and
potentially important findings, (2) presented data that were consistently reproduced over the years and
were reported in more than a single publication, and (3) focused on research topics that were independently
explored in different laboratories. The reviewed papers are arranged under the following categories: "In
Vitro and In Situ Studies", "Animal Studies: Acute Exposure", "Animal Studies: Chronic Exposure", and
"Bioeffects of Extremely High Power Pulses".
Kim and co-authors (1986) used fluorescent probes to reveal possible effect of pulsed microwaves
(800 MHz, 2 W/cm2, 50-μs pulses at 25-100 Hz) on the state of the cell membrane in erythrocyte ghosts.
The temperature of exposed samples was kept stable at 18-19 oC during 20-25 min of exposure. The
experiments established that fluorescence of probes that bind to the lipid-water boundary of the membrane
(2-toluidinonaphthalene-6-sulfonate, or 2,6-TNS, and 1-anilinonaphthalene-8-sulfonate, or 1,8-ANS)
depended on the modulation frequency. Fluorescence of 2,6-TNS was not different from control at 25-35
Hz, but exceeded it by 12-16% at 55-65 Hz, and by 6-9% at 80-100 Hz. With 1,8-ANS, the increase in
fluorescence intensity at 55 Hz was 16.9 ± 5.1%. (Hereinafter, shown average values represent the mean ±
standard error, unless stated otherwise.) Fluorescence increased to the maximum after 10-20 min of
exposure and then remained stable; the increase was more pronounced at higher concentrations of NaCl in
the medium (up to 300 mmol). In contrast, the fluorescence parameters of piren, a hydrophobic probe,
were not affected by irradiation. The authors supposed that the changes registered with fluorescent probes
were induced by mechanical oscillations generated by microwave pulses.
Pashovskina and Akoev (1996) studied the effect of pulsed 2375 MHz radiation on the ATPase
activity of rat actomyosin in vitro. Exposures for 1 min at either 40 or 200 mW/cm2 (50- to 310-Hz
modulation) heated the samples by less than 0.3 oC. ATPase activity was measured from accumulation of
the inorganic phosphate (IP). Two parallel control samples, prepared together with the exposed one and
from the same tissue homogenates, were used to establish the background IP contents at the time before
and after the exposure. With 40 mW/cm2 radiation, 130- and 300-Hz modulation suppressed the ATPase
activity to 50 ± 3% and 9.4 ± 2.7% of the control level, respectively (p<.05). In contrast, 270-Hz
modulation increased the ATPase activity almost 3-fold (p<.05). Most of other tested frequencies produced
weak or moderate (< 50%) activity changes. The dependence of the effects upon the modulation frequency
did not show any pattern or shape. Increasing the field intensity to 200 mW/cm2 entirely changed the
effectiveness of the same modulation frequencies. Exposure at 130 and 300 Hz then caused ATPase
activation (by 170.3 ± 3.3% and 61 ± 3.9%, respectively). The activation reached a maximum at 110-130
Hz modulation and decreased at higher and lower frequencies, forming a bell-shaped dependence. The
authors concluded that ATPase activity of actomyosin showed a complex dependence upon both the field
intensity and modulation, but were unable to explain this result.
Semin et al. (1995) studied the effect of weak RF on the stability of DNA secondary structure in vitro.
DNA was exposed in the presence of glycine and formaldehyde. Aminomethynol compounds, which form
in this medium, react with DNA bases at single-strand sites, which prevents recovery from damage to the
DNA secondary structure. The damage accumulates during the incubation, and its amount can be estimated
from the dynamics of thermal DNA denaturalization after RF or sham exposure. Samples were exposed for
30 min in an anechoic chamber at 18 oC by 10 different microwave frequencies simultaneously (4-to 8-
GHz range, 25-ms pulses, 1- to 6-Hz repetition rate, 0.4 to 0.7 mW/cm2 peak power, no heating). Parallel
control samples were sham exposed in a shielded area in the same chamber. The experiments established
that irradiation at 3 or 4 Hz and 0.6 mW/cm2 peak power clearly increased the accumulated damage to the
DNA secondary structure (P<0.00001). However, changing the pulse repetition rate to 1, 5, or 6 Hz, as
well as changing the peak power to 0.4 or 0.7 mW/cm2, eliminated the effect entirely. Thus, the effect
occurred only within narrow "windows" of the peak intensities and modulation frequencies.
One more example of a "double window" was described by Gapeev et al. (1994). In this case, the
effect required a certain combination of the carrier and modulation frequencies, but did not show a window
dependence on the field intensity. The authors explored if the spontaneous locomotor activity of a
unicellular organism Paramecium caudatum could be affected by irradiation with CW and modulated
millimeter waves. Paramecia were placed in a thin layer of saline in a small round cuvette (7-mm
diameter). Hyperpolarization of cells by a 5-fold reduction of potassium content in the saline (to 0.2 mM)
made them constantly circle around in the cuvette for hours. A "motility index" (MI) was evaluated
automatically by an optic probe as the amount of light reflected from cells appearing in the field of vision
of a microscope during any 2-min interval. The MI increased with increasing average locomotion velocity,
and decreased when cells made more turns or when the number of active cells decreased. Radiation was
applied for 12 min after a 10-min stabilization period. Control samples were monitored for the same time
interval, but without irradiation.
In the first set of 30 experiments, cells were exposed at 42.2 GHz (CW) at power densities from units
of microwatts to tens of milliwatts per centimeter square. These exposures never affected the MI, even at
the highest intensities, which caused saline heating by 1-3 o
C. In the next 30 experiments, the carrier
frequency was modulated at 16, 8, 1, 0.5, 0.25, 0.1, or 0.05 Hz (0.1 to 20 mW/cm2, 0.5 duty ratio). No
effect was detected, except for the combination of 0.1 Hz modulation at 0.1 mW/cm2, which considerably
decreased the MI. More accurate study of the effect of various modulation rates revealed a clear resonant
dependence with a peak at 0.0956 Hz (Figure 1, A). At this modulation rate, the threshold field intensity
was near 0.02 mW/cm2. The maximum effect of about 20% MI reduction was achieved at 0.1 mW/cm2,
with no further increase at intensities of up to 50 mW/cm2 (Figure 1, C). Further experiments demonstrated
that the effect is induced only in a narrow window of carrier frequencies, with the peak at 42.25 GHz
(Figure 1, B).
Figure 1. Effects of pulsed millimeter-wave radiation on Paramecia motility index. A, the effect of modulation frequency
(abscissa, Hz) when the carrier frequency and power are kept constant at 42.2 GHz and 0.1 mW/cm2. B, the effect of carrier
frequency (abscissa, GHz) when the power and modulation are kept constant at 10 mW/cm2 and 0.0956 Hz. C, the effect of the
incident power density (abscissa, mW/cm2) at the resonance carrier and modulation frequencies (42.2 GHz and 0.0956 Hz).
Dashed line shows the temperature increase, oC. A single datapoint ("CW") illustrates the lack of motility changes for exposure
without modulation at 20 mW/cm2. Each datapoint is the mean of 5-10 experiments; the error bars are confidence intervals at
p<.05. See text for more detail. (Adopted from Gapeev et al., 1994).
This effect could not be explained by microwave heating, which reached only 0.1-0.2 o
C at 5
mW/cm2. Moreover, the effect could not be reproduced by heating with infrared radiation modulated at
0.0956 Hz. The authors suggested that the microwave-induced MI decrease could be caused by increasing
the intracellular Ca2+ level and resulting cell depolarization. However, they were unable to explain reasons
for the sharp resonant dependence of the effect upon both the modulation rate and radiation frequency.
A subsequent study by the same group of authors explored the effects of CW and modulated
millimeter waves on the respiratory burst in murine peritoneal neutrophils (Gapeev et al., 1997). Isolated
neutrophils were exposed in the far field for 20 min in the presence of a high concentration (7.5-10 μM) of
calcium ionophore A23187. After the exposure, a respiratory burst was activated by adding phorbol-12-
myristate-13-acetate (1 μM), and the production of reactive oxygen species (ROS) by neutrophils was
measured from luminol-dependent chemoluminescence. Experiments with CW irradiation at 50 μW/cm2 at
various fixed frequencies in the range 41.75-42.15 GHz revealed a 25% inhibition of ROS production at a
"resonance" frequency of 41.95 GHz; the half width of the resonance was about 100 MHz. At 41.95 GHz,
a 50% effect (half-maximum) was produced by intensities under 1 μW/cm2. The effect reached maximum
(about 24% inhibition) at 20 μW/cm2 and remained at this plateau level at higher intensities. Modulation of
41.95-GHz radiation at 1 Hz enhanced ROS production by about 10%, modulation rates of 0.1, 16, and 50
Hz inhibited ROS production by 16-20%, and the rates of 0.5, 2, 4 and 8 Hz had no effect. In the next
experiments, the modulation rate was kept constant at 1 Hz and the radiation frequency was varied. This
irradiation activated ROS production in the carrier frequency band of 41.95-42.05 GHz, and suppressed it
in the band of 41.8-41.9 GHz. The authors concluded that the microwave effect on ROS production is
nonthermal in nature, and is determined by specific combinations of the carrier frequency and modulation
rate. Tygranyan (1986) reported severe disturbances in isolated frog nerve and heart function if intense
enough microwave pulses coincided with the "active" state of the excitable membrane (e.g., were applied
during propagation of the compound action potential, CAP). In isolated frog sciatic nerve, these effects
included decrease of the CAP amplitude (by 90-95%) and velocity (by 35-40%) after some 30 min of
exposure. The same RF pulses delivered before, after, or asynchronously with CAP propagation produced
only a subtle thermal effect. The author supposed that microwave pulse energy is converted into a
mechanical pulse, which travels in a spiral between Schwann cell membranes of the nerve sheath. Due to a
phase synchronism effect, the traveling pulse triggers another mechanical pulse perpendicular to the nerve
surface, and the latter may be strong enough to damage the "active" nerve membrane. The author's
calculations based on dielectric and mechanical properties of nerve seemed to support this hypothesis.
The findings of Tygranyan motivated Pakhomov et al. (1991) to search for similar effects in giant
nerve fibers of the isolated ventral nerve cord of the earthworm Lumbricus terrestris. A length of about 2.5
mm of the cord was exposed in a small drop of Ringer's solution to 6.45-GHz CW or pulsed radiation, or
was sham exposed. Exposure duration was from 10 to 50 min at the peak SAR from 30 to 230 mW/g.
Action potentials, which were evoked by repetitive electrical stimulation and propagated along the nerve,
were recorded by two pairs of electrodes, positioned immediately before and after the exposure zone.
Therefore, comparison of these records provided an accurate measure indicating whether the nerve
conduction in the exposure zone was affected. Microwave pulses were synchronized with the action
potential crossing the exposure zone, or were delivered independently from the nerve stimulation (0.2- to
32-ms pulse width, 6- to 2000-Hz repetition rate). This study failed to produce any specific microwave
effect, regardless of RF pulse parameters or their phasing with the nerve firing. However, giant nerve fibers
of the earthworm ventral cord do not have a myelin sheath that was theoretically supposed to be essential
for Tygranyan's effect described above. The design of the exposure cell and the carrier frequency were also
different (6.45 GHz versus 800-915 MHz).
For the next study (Pakhomov et al., 1993), a microwave transmitter and irradiator were borrowed
from Tygranyan's laboratory, to replicate his exposure conditions with maximum care. The experiments
were performed in isolated frog sciatic nerve, which was continually stimulated at a rate of 50 twin
pulses/sec for 90 min. This high-rate stimulation caused gradual decline of the nerve function, i.e.,
increased the CAP latency and decreased its amplitude and tracing integral. Exposures or sham exposures
began 1 min after the onset of the high-rate stimulation and continued till the end of the experiment.
Microwave pulses (915 MHz, 5 to 70 W/g peak SAR, 0.5- or 3-ms width) were phased with CAP in
various ways, or were delivered asynchronously at a rate of 50 Hz. At the highest SAR, microwave heating
could reach 2.7 oC. Regardless of phasing, SAR, or pulse width, none of the exposure regimens caused
severe CAP suppression, therefore the results of Tygranyan (1986) failed to be independently confirmed.
At the same time, these experiments revealed a different microwave effect: The exposed nerves
displayed a faster decrease of the CAP amplitude and tracing integral during the course of the high-rate
stimulation. This effect was regarded as nonthermal or microwave-specific, since conventional heating of
the superfusing solution by 3 oC during sham irradiation caused the opposite changes. Within studied
limits, the magnitude of the effect showed no significant correlation with exposure parameters. In general,
this microwave-induced facilitation of the nerve vitality loss was similar to the effect reported earlier by
McRee and Wachtel (1980, 1982), but substantially weaker.
Two subsequent studies explored the dependence of this effect upon modulation (Pakhomov et al.,
1992; Pakhomov, 1993). The course of the high-rate stimulation and exposure was reduced to 20 min.
Microwave pulses of 1- to 1000-μs duration (915 MHz, 43-48 or 20-33 W/g peak SAR) were delivered at
duty cycles from 1/20 to 1/4000, and were not synchronized with nerve firing. These studies identified
effective and ineffective pulsing regimens. For instance, at 1/40 duty cycle and 43-48 W/g, 1- and 100-μs
pulses caused a statistically significant effect, while 10- or 1000-μs pulses did not, despite the fact that the
gross microwave heating by all these exposures was essentially the same.
Presumably a nonthermal effect of pulsed RF was observed in in situ frog heart by Grechko (1994).
This wide-scale study used 1680 male frogs to compare the effects of five different types of
electromagnetic fields on cardiotoxic effectiveness of a drug strophantine K. Injection of this drug caused a
characteristic heart arrest in systole in about 60 min. Irradiation by 3085 MHz, 1-μs pulses at 400 Hz, 0.3-
0.5 mW/cm2 for 30 min significantly increased the latency of the heart arrest (by 17-44%). In some cases,
the heart was even able to restore the activity, which never happened under sham exposure conditions. In
contrast, the same irradiation for 10 min at 2-3 mW/cm2 decreased the heart arrest latency by 10-25%.
Pakhomov et al. (1995b) attempted to replicate findings of Tinney and co-authors (1976) that
microwaves can cause beating rate changes in isolated heart by stimulation of neurotransmitter release
from autonomous nervous system intracardiac fiber terminals. CW exposure at 2-10 mW/g (960 MHz) was
reported to cause bradycardia in isolated turtle hearts. This effect could be blocked by a parasympathetic
blocker atropine, or enhanced by a sympathetic blocker propranolol. The replication experiments were
performed in isolated frog heart slices, using 915 MHz radiation; exposures continued for up to 40 min at
SAR levels from 0.1 to 52 mW/g (10- to 100-μs pulses at 16- to 2000-Hz repetition rates). Neither
irradiation alone nor in combination with atropine or propranolol caused bradycardia in the frog heart
slices. The only effect detected was a reversible beating rate increase when microwave heating exceeded
0.1 oC (when SAR exceeded 10 mW/g). One needs to note, however, that the studied drugs alone (i.e.,
without irradiation) caused marked beating rate changes in isolated turtle hearts (Tinney et al., 1976), but
not in the frog heart slices, even at much higher concentrations. This finding may reflect a principal
difference in physiological organization of these two heart preparations, which could be a reason for their
different sensitivity to microwave radiation.
It was also reported that a caffeine antagonist, tetracaine, eliminated a nonthermal microwave effect in
isolated snail neurons (Arber and Lin, 1984). Therefore, Pakhomov et al. (1995b) inferred that caffeine
itself could enhance the microwave effect and tested this hypothesis in isolated frog heart slices. In contrast
to atropine and propranolol, superfusion of slices with 1 mM of caffeine strongly increased the average
heart power, which was calculated as a product of the beating rate and beats' amplitude. Exposure at 8-10
mW/g average SAR (1.5-ms pulses, 2.5-ms interpulse interval, 8 pulses/burst, 16 bursts/s, 915 MHz for 33
min) augmented the caffeine effect by about 15% (p<.02). Microwave heating was under 0.1 oC and could
not account for this exposure effect. Moreover, the same exposure without caffeine superfusion caused no
beating rate or amplitude changes.
Afrikanova and Grigoriev (1996) reported that pulsed, but not CW exposure increased the probability
of heart rate changes and heart arrest in isolated and in situ frog heart. The effect was observed at
intensities from 16 to 340 μW/cm2 at 9.3 GHz and modulation frequencies under 100 Hz (30% modulation
depth, 50% duty cycle). The maximum effect was produced by a 5-min exposure with modulation
frequency changing by 1-Hz steps from 6 to 10 Hz (1 min at each step). A longer exposure with this
modulation (10 or 19 min), as well as 5-min exposure using various other modulation patterns, produced
weaker or different effects.
Pulsed RF effects on individual neurons in isolated brain slices were explored in studies of Zakharova
and co-authors (1993, 1995, 1996). Spontaneous firing of cortical neurons was recorded by an extracellular
microelectrode before, during, and after a brief (4-5 min) 900-MHz exposure at 1.4 mW/g. The reactions
observed with 7-, 16-, 30-, and 60-Hz modulation (1/5 duty ratio) were a decrease of the firing rate and
desynchronization of firing of individual neurons. The probability of the firing rate inhibition and its
magnitude were the highest with 7- and 16-Hz modulation and the lowest with the 60-Hz modulation. For
instance, 16-Hz pulses inhibited the activity in 15 out of 17 tested neurons; the firing rate could fall by
24% on the 1st minute of irradiation, and by as much as 65% on the 4th min. The rate did not recover but
sometimes even decreased further after exposure. A far more intense conventional heating (by 0.33 oC/min,
as opposed to 0.02 oC/min under exposure) also inhibited the activity, but just in 7 out of 13 neurons, and
the firing rate did recover when the heating was over. The greater effectiveness of microwave treatment, its
dependence on modulation, as well as lack of the recovery after exposure, suggested a specific microwave
effect mechanism.
Philippova et al. (1988) reported an interesting effect of 900-MHz exposure on 3H-camphor binding in
isolated membrane fraction of rat olfactory epithelium. Under constant-temperature conditions, irradiation
markedly decreased specific 3H-camphor binding (down to 60-40% of the control), but did not affect its
nonspecific binding. The effect depended on SAR and duration of exposure, but not on modulation in the
studied range from 1 to 100 Hz. At 1 mW/g, the effect gradually increased and reached saturation after
some 10-20 min of exposure. For a 15-min exposure at various SARs, the effect gradually increased with
SAR and reached saturation at about 4 mW/g. The authors supposed that the observed decrease of ligand
binding resulted from microwave-induced release of specific camphor-binding protein from cell
membranes into solution.
The microwave effect on olfactory epithelium and neighboring respiratory epithelium was further
investigated in a histological study by Popov et al. (1996). Tissue samples were obtained from Wistar rats;
one sample from each animal served as a control, and the other one was exposed for 15 min at 15 W/kg to
0.9 GHz microwaves (16 Hz pulsed modulation, 50% duty ratio). Subsequent electron microscopy
revealed increased vacuolization of olfactory neurons in exposed samples, which indicated dying of these
cells. The most severe degenerative changes (swelling, appearance of vesicles and multilamellar structures)
developed in non-myelinated axons of olfactory neurons. Concurrently, support cells displayed pronounced
cytoplasmic vacuolization in apical parts of the cell body, which indicated that microwaves enhanced
mucus secretion. In the respiratory epithelium, the most remarkable effect was fusion of cilia into so-called
"giant cilia," which contained numerous basal bodies. These bodies formed axonemes with a typical
arrangement of microtubules. Giant cilia included 5-10 or more axonemes with basal bodies and numerous
vesicles (remains of fused membranes). As a rule, the cytoplasm of respiratory cells was strongly
vacuolated. Overall, the authors regarded these and other observed changes as a "direct and pronounced
degenerative effect of microwaves on neurons and other epithelial cells."
To complete this section on in vitro bioeffects, we will mention the studies that attempted to
demonstrate specific bioeffects of pulsed RF, but could find either no effects, or only the effects caused by
heating. Alexeev et al. (1987) could not find any but thermal effects on Ca2+ transmembrane current in
mollusk neurons (900 MHz, <10 min at 0.2-20 mW/g, 0.5- to 1,000-Hz modulation). Khitrov and
Kakushkina (1990) observed solely thermal effects of CW or pulsed exposure on K+ transport and oxygen
consumption in isolated rat liver tissue (2450 MHz, 0.1-5 W/g, 13-, 17-, 21-, or 25-Hz pulses at 1/1000
duty ratio). Khramov et al. (1991) could detect only thermal effects of microwaves on the electric activity
of a crayfish stretch receptor (37- to 78-GHz, 10 to 250 mW/cm2, from 20 sec to several hours, 0.01-1000
Hz modulation). In a study by Bolshakov and Alexeev (1992), pulsed but not CW radiation produced
bursting responses of snail neurons (900 MHz, 0.5 to 15 mW/g, 0.5 to 110 Hz); however, the authors
regarded this effect as possibly being an artifact from mechanical vibrations of the exposure chamber. In
experiments with isolated frog heart slices, Pakhomov et al. (1995a) tested over 400 modulation regimens
and concluded that changes in the beating rate and amplitude are entirely determined by the time-average
SAR and microwave heating (885 or 915 MHz, 1-μs to 10-ms pulses, 1/7 to 1/100,000 duty cycle, 100 to
3000 mW/g peak SAR for 2 min).
The possible impact of low-intensity pulsed microwaves on natural ecosystems was studied in a
laboratory model using a tick Hyalomma asiaticum (Korotkov et al., 1996). Exposure regimens tested in
this study differed in the microwave frequency, peak power, and modulation (see Table 1). Ticks were kept
at a room temperature of 21-23 oC in humidified chambers. Exposures were performed at different stages
of tick development (eggs, larvae, nymphs, imago); the number of specimens in each exposed group varied
from 20 (experiments with larvae) to as many as 3000 (experiments with eggs). Irradiation of eggs 5-6
days after they were laid did not affect the percent of appearing larvae (95-100% in any group). At the
same time, exposures significantly delayed larvae hatching. In the control group (S1), 50% of larvae
appeared in 11.9±1.0 days, while in the exposed groups this interval increased to 15.3±0.1 days (R2),
25.3±0.1 days (R3), and 32.2±0.7 days (R4); R5 and R6 were not tested in these experiments. Activation of
the larvae of S1- and R2-exposed groups occurred on the day of hatching, while R3 and R4 exposures
delayed it by 17.0±0.4 days and 23.9±0.5 days, respectively. Exposures R4 and R5 decreased the life span
of unfed larvae and nymphs by 20-30%, but this effect was not statistically significant.
Table. 1. Microwave exposure regimens* employed in the study by Korotkov et al., 1996.
Modulation Regimen Frequency,
GHz Peak power,
μW/cm2 Pulse width,
ms Pulse repetition
rate, Hz Burst duration,
ms Burst repetition
rate, Hz
S1 Sham - - - - -
R2 1-4 150 20 7 - -
R3 3 75 ** 1000 20 7
R4 3 150 ** 1000 20 7
R5 1-4 750 20 2 - -
R6 1 750 20 2 - -
* Exposure duration in all cases was 15 min (Grigoriev, 1999).
** Pulse width for regimens R3 and R4 is not specified in the paper.
Effects of R3-R6 exposure regimens were studied in replete larvae in winter and fall tick generations.
The larvae were exposed on the 10th day after feeding. The first nymphs appeared in 16-18 days after the
feeding in all the groups, but their survival, molting, and life span were adversely affected by exposures.
On the whole, irradiation by pulse bursts at 3 GHz (R3 and R4) was the most effective, and the effects
were more profound at the higher peak power (R4). On the contrary, the wide-band exposures (R2 and R5)
were the least effective, even at 750 μW/cm2 peak SAR. Active and fed ticks were less sensitive to
microwaves than hungry specimens or those in the diapause period. The authors concluded that low
intensity pulsed microwaves were a negative environmental factor for the tick H. asiaticum.
All other in vivo studies of acute bioeffects of pulsed RF were performed in warm-blooded laboratory
animals. The vast majority of these studies focused on changes in the nervous system and behavior; the
other ones dealt with general physiological changes (e.g., hormone production, blood composition, heart
rate), and just one study explored possible genetic damage from RF irradiation (Belokhvostov et al., 1995).
In this work, male albino rats (150-200 g) were exposed in an anechoic chamber to 1-μsec, 400-Hz
microwave pulses (3.085 GHz) at 5, 10, 20, or 46 mW/cm2. The exposure lasted for 24 min or 2 hours, and
the authors claimed that it caused no rise in the rectal temperature. The animals were decapitated 5 hours
after the exposure, and blood taken from 6-7 rats was pooled together and considered as one sample. Blood
cells were removed, and the samples were analyzed by DNA electrophoresis in polyacrylamide gel and by
polymerase chain reaction (PCR). Low-molecular-weight DNA fraction (175-185 nucleotide pairs) was
revealed in blood plasma in 38% of the samples from sham-exposed animals (6 samples out of 16). In
exposed groups, regardless of exposure duration and intensity, this fraction was found in 80 to 100% of
samples (e.g., 7 out of 8 samples after 24 min at 5 mW/cm2, see also Figure 2, A). The DNA fraction was
analyzed further by PCR to reveal complete and incomplete copies of so-called LINE elements (which are
a known marker of genetic transposition in various pathologic conditions). Complete copies of the LINE
element were not found in any control samples, but were present in 1 out of 7, 5 out of 7, and 1 out 7
samples after a 2-hour exposure at 5, 10, and 20 mW/cm2, respectively (i.e., 10 mW/cm2 was the most
effective). The amount of DNA was, on the average, 2.24 times higher after 10 mW/cm2 exposure than
after 20 mW/cm2 (n=3). Since the transposition of full copies of the LINE element is known to cause DNA
rearrangements within the genome, their release into blood plasma may indicate a possible adverse effect
of microwaves on genome stability.
In contrast to complete LINE elements, partial copies of the LINE sequence (with 3'-end fragment and
the middle portion of the sequence) were present in all samples taken from the exposed animals. For some
sequence clones, the amount of DNA was proportional to the intensity of irradiation. For example, for the
clone 43 (the sequence is given in the original article), the amount of DNA increased as 1.0/1.85/1.92/2.98
in the series sham/5/10/20 mW/cm2 (Fig. 2, B). The increased presence of the partial LINE copies does not
indicate any pathological processes, but may be a useful index for biological dosimetry of microwave
Microwave exposure of the head of rabbits for 1 min at 0.2 mW/cm2 (6 GHz, 50-Hz pulses at 1/2 duty
cycle) changed the spontaneous firing rate of individual neurons in the sensomotor cortex (Lukianova et
al., 1995). The firing rate was recorded extracellularly with glass microelectrodes (5- to 20- Mohm
resistance). The microelectrode holder and micromanipulator were affixed to the animal's skull. These
devices were custom made of plastic, to prevent any artifacts arising from metal objects introduced into the
microwave field. For the same reason, plastic tubes filled with saline were used instead of metal wires to
connect the microelectrode holder with an amplifier. The activity of 53 neurons was analyzed in 67 3-min
experiments; each experiment was a continual activity recording for 1 min before, 1 min during, and 1 min
after irradiation. The data were compared to those recorded from 54 neurons in control experiments with
sham irradiation. During the exposure or sham exposure, the firing rate of an individual neuron could
either increase or decrease, or showed no statistically significant changes. In the control experiments, the
firing rate decreased in 8.2% of neurons and increased in 13.07%. In the experiments with irradiation,
these numbers changed to 49.5% and 6.4%, respectively (p<.05). Thus, the most characteristic effect of
exposure was suppression of the neuron firing. This suppression developed with an average latency of 12
sec after the onset of exposure. Other parameters studied, such as spike amplitude or firing pattern, were
not affected by microwaves.
Figure 2. A, Presence of a low-weight (175-185 nucleotide pairs) DNA fraction in blood plasma of rats after pulsed RF
exposure. 1: sham exposure, 2: 20 mW/cm2 for 2 hours, M: molecular weight marker. Values to the right show the number of
nucleotide pairs in marker DNA. B, Revealing of the 3'-end fragment of the LINE DNA element (clone 43) by 25 cycles of PCR
amplification. 1: sham exposure, 2: 5 mW/cm2, 3: 10 mW/cm2, and 4: 20 mW/cm2. See text for more detail. (Adopted from
Belokhvostov et al., 1995).
Similar experimental techniques and protocol were employed by Moiseeva (1996) and by Lukianova
and Moiseeva (1998) to study the effect of 1.5 GHz microwaves. These two papers described effects of two
different pulsing regimens in an experiment with 22 rabbits. For both the regimens, the pulse width was 0.4
ms and the peak power was 0.3 mW/cm2. These pulses were either continually delivered at a 1000-Hz
repetition rate, or were arranged in 16-ms bursts (0.12 bursts/sec, 1000 pulses/sec within bursts). The data
were collected from a total of 240 neurons in the sensomotor cortex and 220 neurons in the occipito-
parietal cortex. Lack of statistically significant firing rate changes was the predominant response to sham
exposure, while microwave irradiation markedly increased the percentage of neurons that either decreased
or increased their firing rate (Table 2). Overall, about 60% of neurons reacted to microwaves. Both tested
irradiation regimens caused a practically identical response. As a rule, exposure suppressed the activity in
neurons with initially high firing rate, and facilitated the activity in neurons with initially low firing rate.
The magnitude of changes also was higher under microwave exposure. For exposure with repetitive
microwave pulses, for example, the pre-exposure firing rate in the sensomotor cortex was 6.1 ± 0.89
pulses/sec; it increased to 11.2 ± 0.64 pulses/sec under irradiation (p<.05), and returned to 9.2 ± 0.58
pulses/sec after the irradiation. The respective numbers for sham exposure were 5.2 ± 1.32, 6.94 ± 1.5, and
7.8 ± 1.09 pulses/sec (the changes are not statistically significant). The average latency of the response was
10 ± 3 sec for firing activation, and 9 ± 2 sec for firing suppression.
Table 2. Changes in "spontaneous" firing rate of neurons in rabbit cerebral cortex caused by a 1-min sham
or microwave exposure. (Adopted from Moiseeva, 1996, and Lukianova and Moiseeva, 1998).
Type of response, % of the total number of neurons
Significant changes in the firing rate
Area of the
cortex Exposure
regimen Number of
Rate increase Rate decrease
Lack of
Sham 72 2.7 11.1 86.2
Pulses1 105 27.6* 32.4* 40.0*
Bursts2 63 24.2* 31.0* 44.8*
Sham 73 5.5 11.0 83.5
Pulses1 84 25.0* 29.8* 45.2*
Bursts2 63 23.2* 30.5* 46.3*
1 1.5 GHz, 0.3 mW/cm2 peak power, 0.4-ms pulses, 1000 pulses/sec.
2 1.5 GHz, 0.3 mW/cm2 peak power, 0.4-ms pulses, 1000 pulses/sec within 16-ms bursts, 0.12 bursts/sec.
* The percentage of neurons is significantly different from sham control (p<.01, χ2 test)
Pulsed RF effects on brain receptors have been continually studied for more than 10 years (Akoev et
al., 1985, Kuznetsov et al., 1991, Kolomytkin et al., 1994, Iurinskaia et al., 1996). A brief exposure of rats
to 800, 880, or 915 MHz microwaves increased radiolabelled agonist binding to glutamate receptors,
decreased binding to gamma-aminobutyric acid (GABA) receptors, and decreased acetylcholinesterase
activity in brain. These effects required 16-Hz modulation, at either 85% or 32% duty ratio; CW irradiation
or other modulation frequencies (3 to 30 Hz) caused no statistically significant changes. Interestingly, brief
(1- and 5-min) exposures often produced greater effects than prolonged exposures (15-60 min). For a 5-
min exposure with 16-Hz modulation, the threshold field intensity was between 10 and 50 μW/cm2. The
magnitude of the effects gradually increased or remained almost unchanged for the field intensities from
0.1 to 1 mW/cm2.
These findings can be illustrated in more detail by the paper of Iurinskaia et al. (1996). Four separate
series of experiments were performed in male Wistar rats (150-200-g body weight). Animals were kept in
normal vivarium conditions, and were made accustomed to experimental manipulations, environment, and
handling for 7-10 days prior to experiments. All experiments were performed at the same time of day. The
animals were exposed in groups of 3 in a plastic cage, from an open end of a waveguide. Control animals
were treated in exactly the same manner and were subjected to a sham exposure. Rats were decapitated
immediately after irradiation, and the brain was extracted and processed to evaluate the specific binding of
radiolabelled agonists (3H-glutamate and 3H-muscimol) to glutamate and GABA receptors. In the first set
of experiments, the authors studied the dependence of binding on the incident power density (from 0.01 to
1 mW/cm2), when other exposure parameters were kept constant (915 MHz, 16 Hz modulation for 5 min).
Microwaves increased binding of 3H-glutamate and decreased binding of 3H-muscimol. At 10 μW/cm2,
these indices changed to 120 ± 12% and 88 ± 12%, respectively (sham control was taken as 100%). At
higher power densities, both effects gradually became more substantial (over 200% and 70-80%,
respectively) and statistically significant (Figure 3, A).
The next series of experiments was focused on determining the role of modulation in the induction of
these effects. Animals were exposed for 5 min at 1 mW/cm2 (800 MHz for experiments with 3H-muscimol
and 915 MHz for experiments with 3H-glutamate), modulated at 0, 2.5, 3, 5, 7, 16, or 30 Hz (32% duty
ratio). Neither CW nor modulated regimens produced a statistically significant change in 3H-muscimol
binding, except for 16-Hz modulation which decreased binding to 70 ± 5%. Maximum increase in the 3H-
glutamate binding (to 200-220%) also occurred at 16-Hz modulation (Figure 3, B).
In the third set of experiments, the exposure duration was varied from 1 to 60 min, keeping the other
parameters constant (800 or 915 MHz, 16 Hz modulation, 1 mW/cm2). Maximum decrease in the 3H-
muscimol binding (to 45-50%) occurred after a 1-min exposure, and the effect gradually weakened for
longer exposures. For 3H-glutamate binding, the maximum effect of 200-220% was observed after a 5-min
exposure; after 1-min exposure, it was 130 ± 6%. The ability to produce the effects with very low
intensities of radiation, as well as dependencies on modulation and exposure duration indicated a
nonthermal mechanism of the effects.
Figure 3. Changes in the binding activity of glutamate and GABA receptors in the rat brain after exposure to modulated 915-
MHz microwaves. A, the effect of a 5-min exposure with 16-Hz modulation on binding of radiolabelled muscimol (Mu) and
glutamate (Glu) at different incident power densities (abscissa, μW/cm2). B, the effect of a 5-min, 1 mW/cm2 exposure on
glutamate binding at different modulation frequencies (Hz). The data shown are the mean ± s.e., in % to sham-exposed controls.
See text for more detail. (Adopted from Iurinskaia et al., 1996).
In the forth set of experiments, the authors studied microwave effects on the concentration
dependences of the change in binding characteristics. Irradiation only slightly affected the dissociation
constant of muscimol, but decreased the number of binding sites from 17.4 ± 0.8 to 10 ± 2 pmol per mg of
protein. In contrast, irradiation did not change the number of binding sites for glutamate, but decreased its
dissociation constant from 277 ± 15 nM (control) to 103 ± 10 nM.
Summarizing their experimental results, the authors noted that the dynamics of the changes they
observed in the state of brain receptor systems is similar to the effects produced by an electric shock, pain,
or immobilization stress. They hypothesized that electromagnetic radiation works as a stressing factor, with
adaptation developing under a prolonged exposure.
A series of studies performed under the leadership of K. V. Sudakov explored neurophysiological and
behavioral effects of the lower RF frequencies (30 to 40 MHz, 30 to 300 V/m, 2- to 50-Hz sinusoidal
modulation). The experiments were performed in rats and rabbits, and exposures lasted from 2-5 min to
45-90 min. These exposures inhibited the autonomous nervous system response to stimulation of the
hypothalamus (Kashtanov and Sudakov, 1981); alleviated stress response to immobilization and electrical
stimulation of the skin (Gorbunova et al., 1981); induced spreading epileptiform activity in the brain,
followed by EEG suppression; induced the appearance of slow waves and even catalepsy in some animals
(Sudakov and Antimonii, 1977); suppressed defensive behavior and motor activity, and inhibited
extinction of the conditioned response (Sudakov, 1976, 1998). Depending on the modulation frequency,
the exposure had a biphasic effect on the self-stimulatory behavior in rats (activation followed by
suppression at 2-Hz modulation, or no effect followed by suppression at 7-Hz modulation), or even
suppressed the self-stimulation practically from the onset of exposure at 50-Hz modulation (Antimonii et
al., 1976).
However, these interesting findings should be taken with caution. One reason is that, in many cases,
the authors used regular metal electrodes for brain stimulation and recording of the electric activity. The
use of such electrodes during the electromagnetic field exposure could cause field distortion and various
artifacts (e.g., demodulation of the field and direct stimulation of biological structures by electric current at
the modulation frequency). Without independent replication in artifact-free conditions, it is not possible to
judge if these findings were in fact the effect of the field, or were just a result of the flawed experiment
Konovalov and Andreeva (1989) studied microwave effects on apomorphine-induced motor
stereotypy in rabbits and rats. In rabbits, a 30-min exposure of the head (880 MHz, 8 mW/cm2, 16- or 30-
Hz pulses or CW) decreased the number of "simultaneous hits" by hind limbs by 15-25%, but this
difference was not statistically significant. The authors noted, however, that in 3 animals (out of 34) 16-Hz
pulses decreased the number of "simultaneous hits" 3-4 times, while the other exposure regimens had only
a subtle effect. In rats, a 1 mg/kg dose of apomorphine caused them to circle around the cage in the left or
right direction. A single 60-min whole-body exposure with 16-Hz pulses suppressed this behavior by 21%
(p<.05 compared with sham exposed controls); a series of 5 exposures for 60 min/day suppressed it by
40% (p<.01).
Grigoriev and Stepanov (1998) studied delayed effects of pulsed RF exposure on imprinting behavior
in chicks. Eggs were exposed on the 16th day of incubation, for 5 min at 40 μW/cm2 (10 GHz, 1-, 2-, 3-, 7-
, 9-, or 10-Hz modulation). Two days after hatching, chicks were given a choice of two flashing light
stimuli. The flashing rate of one light was the same as the modulation rate in the previous RF exposure of
the egg; the flashing rate of the other light was offset by 8 Hz. It was found that chicks exposed in eggs to
9- or 10-Hz RF pulses showed preferences to the light flashes of the same frequency. Sham-exposed chicks
and those exposed at other RF pulsing rates did not show a preference to either light stimulus.
A single 50-min microwave exposure at very low average intensity (15 μW/cm2, 6 GHz, 2-Hz pulses)
produced no statistically significant changes in the physiological condition of adult rabbits (Rynskov et al.,
1995). The condition of microwave- and sham-exposed animals was evaluated immediately after the
exposure and also on the next day. The tests employed in this study were electrocardiogram,
electroencephalogram, compound myogram of musculus gastrocnemius, pneumogram, and blood contents
of cortisol, testosterone, insulin, and thyroxin.
Lukianova and co-authors (1995) compared formation of conditioned avoidance reflexes to light,
sound, pulsed microwaves (6 GHz, 50-Hz pulses, 200 μW/cm2 average and 400 μW/cm2 peak power), and
1000-Oe constant magnetic field. Rabbits were taught to respond to only one type of the conditioning
stimuli (3 animals per group), and 4 other animals were subjected to "sham stimuli". Exposures and sham
exposures were performed 6 times every other day, up to the total of 400 treatments for each animal. In 20
sec after the onset of the conditioning stimulation, the rear left extremity was stimulated with electric
current, causing a flexor reaction. Withdrawal of the leg within this 20-sec interval prevented the electric
stimulation and was regarded as a conditioned reflex response. Consolidation of the conditioned reflex was
observed in all but one exposed animal and in none of the sham-treated controls. Consolidation took
noticeably more time in the case of magnetic field exposures (243-245 combinations of stimuli) than with
exposures to microwaves, sound, or light (139-154, 98-134, and 114-184 combinations, respectively). The
maximum reflex percentage per 50 combinations established for the above groups was 40-60%, 30-60%,
60-78%, and 70-80%, respectively. The average latency of the reflex to the magnetic field (8.5 ± 0.12 sec)
and to microwaves (7.76 ± 0.35 sec) significantly exceeded the corresponding numbers for sound (4.9 ±
0.09 sec) and light (4.47 ± 1.17 sec).
Navakatikian (1992) has described a behavioral technique sensitive enough to detect the effect of
acute pulsed RF exposure at 10 μW/cm2 (or 2.7 μW/g). The author employed a well-known shuttle-box
method of studying the conditioned reflex of active avoidance, but scrupulously refined the shuttle box
design and optimized the schedules of animal training and testing. Particular attention was given to
selection of uniform experimental and control groups and to statistical analysis of the animals' performance
data. An experiment with microwave exposure illustrated all the detail of how to use this behavioral
method and how to process the raw data.
Adult male rats (280- to 360-g body weight) were trained to respond to a sound stimulus by relocating
from one compartment of the shuttle box into another, in order to avoid punishment by electrical
stimulation. The optimum training schedule consisted of three training series, each with 75 combinations
of stimuli. One additional, so-called "testing" series (identical to the previous training series) was
performed immediately after a 30-min sham or microwave exposure (3000-MHz, 10 μW/cm2, 400-Hz
pulse repetition rate, 2-μsec pulse width, 4 pulses per burst, one burst every 3.75 sec). The difference in
each animal's performance in the testing series and in the last training series was taken as an individual
change (IC) index. The IC values were averaged over groups of 11 exposed and 11 control rats. For the
latency of the reflex response, the average IC was -0.11 ± 0.06 sec for the sham-treated group, and +0.17 ±
0.09 sec in the exposed group (p<.05). The author noted that, for an acute exposure, the minimum
microwave intensity that was reported in literature to change conditioned reflexes is 1000 μW/cm2. The
method described in this paper has therefore been proven to be sensitive enough to establish an effect of
acute microwave exposure at an intensity two orders of magnitude less than previously reported.
However, the significance of this demonstration should not be overestimated. The reason is, that with
the employed pulsing regimen, the incident energy density per pulse reached 9 μJ/cm2, which clearly
exceeds the established threshold of 1.5-3 μJ/cm2 for auditory perception of RF pulses by rats (Chou et al.,
1985). Therefore, it is not surprising that a sensitive behavioral technique could reveal some effect of a 30-
min RF auditory stimulation. On the other hand, the author has reported elsewhere (Navakatikian, 1993)
that the described method reliably detects the effect of 2450 MHz CW exposure at 0.1 mW/cm2 (27 μW/g);
this finding suggests that the microwave effect does not necessarily involve just auditory or thermal
A substantial number of studies have explored behavioral and physiological effects of exposure
conditions that imitated actual occupational or residential exposures from various military and civilian
radar systems. The employed modulation schemes could be rather complex, such as regular bursts of
pulses from rotating antennas or field modulation by Morse code.
Potential health effects of a coastal radar were explored by Tomashevskaia and Solenyi (1986). Field
measurements established that population within 0.1-1-km distance from the coastal radar can be exposed
to intermittent bursts of 400- or 800-Hz microwave pulses (3- or 10-cm wavelength) at levels from 10 to
80 μW/cm2; the intermittence was produced by antenna rotation at 16 rpm. White mongrel rats (130 -140 g
body weight) were exposed to intermittent 10-cm (2750 MHz) pulsed microwaves for 16 hours a day at
100, 500, or 2500 μW/cm2 over a 4-month period; control animals were sham exposed. This microwave
treatment significantly decreased the animals' motor activity (100 and 500 μW/cm2), increased
electrodermal sensitivity (500 and 2500 μW/cm2), decreased the glycogen content in liver and brain (all
intensities), decreased cytochrome oxidase activity in brain mitochondria (2500 μW/cm2), and changed
some immune indices (500 and 2500 μW/cm2). Mathematical analysis of the collected data has predicted
the "no-effect field intensity" to be at 10 μW/cm2, which was therefore recommended as a maximum
permissible irradiation level for residential areas.
The authors continued with studying the effects of a civil aviation radar system (Tomashevskaia and
Dumanskii, 1988). Adult white rats were exposed to 400-Hz microwave pulses for 16 hours/day for 4
months using various carrier frequencies, intermittence regimens, and field intensities: (1) 2750 MHz, 50,
100, or 500 μW/cm2, 40-μsec bursts, 1 burst per 20 sec, (2) 1310 MHz, 20 or 100 μW/cm2, 28-μsec bursts,
1 burst per 10 sec, and (3) 850 MHz, 20, 100, or 500 μW/cm2, 67-μsec bursts, 1 burst per 6 sec. The
experiments established that exposures at 20 and 50 μW/cm2 produced no statistically significant effects
compared to sham-exposed controls. Exposures at 100 and 500 μW/cm2 could cause statistically
significant changes in the activity of several marker enzymes (cholinesterase, cytochrome oxidase,
succinate dehydrogenase, and ceruloplasmin); the magnitude of changes in different tissues varied
depending on the particular irradiation regimen.
Navakatikian and co-authors (1991) exposed rats to 3000-MHz pulsed radiation for 2 months, 12
hours/day during the nighttime. Bursts of 20, 4, or 2 pulses (2-μsec pulse width, 400-Hz repetition rate)
were emitted every 20, 3.75, or 2.07 sec, respectively, simulating antenna rotation speeds of 3, 16, and 29
rpm. The average energy output was virtually the same for all the pulsing regimens (60, 64, and 58
pulses/min). The incident power density levels studied were 0.1, 0.5, and 2.5 mW/cm2. Exposure effects
evaluated were the animals' exploratory activity (measured as an amount of movement in a special maze)
and conditioned avoidance reflex in a shuttle box test. Most of the exposure regimens slightly stimulated
the locomotor activity (except 20-pulse bursts at 0.5 and 2.5 mW/cm2). Performance in the shuttle-box
after exposures was characterized by decreased latency of responses and increased number of correct
responses. Overall, the changes were interpreted as a prolonged and moderately expressed activation of the
central nervous system.
Bioeffects of the above-mentioned exposure regimens were explored further and compared to the
effects of 2450 MHz, 0.01-1 mW/cm2 CW irradiation (Navakatikian and Tomashevskaya, 1994). In
particular, it was found that 2-month CW exposure caused suppression of the central nervous system, in
contrast to weak activation under pulsed irradiation. Histological examination of the thyroid gland revealed
functional activation of the zona fasciculata after pulsed microwave exposure. Pulsed microwaves
consistently and reproducibly decreased blood levels of insulin and testosterone, while CW exposure had
no effect. The authors have speculated that inhibition of behavior was a direct effect of irradiation on the
nervous system, whereas activation might be mediated by hormonal changes.
Another study has replicated the exposure conditions of meteorological radar personnel (Navakatikian
et al., 1991). Adult female rats were subjected to simultaneous irradiation from 9375- and 1765-MHz
sources for 12 hours daily, 30 min each hour. The average incident power levels for 9375 MHz were 0.12,
0.24, and 0.36 mW/cm2; for 1765 MHz, the power output was set 24 times less, so the integral intensities
used were 0.125, 0.25, and 0.375 mW/cm2. Modulation pulse width and repetition rate were 1.1 μs, 475
Hz for 1765 MHz, and 2 μs, 300 Hz for 9375 MHz. For 9375-MHz microwaves only, the pulses were
assembled into 20-msec bursts and delivered at a rate of 1 burst every 10 sec. Behavioral endpoints after 1,
2, 3, and 4 months of everyday exposure were compared with those in a sham-exposed group. The
exploratory activity in animals was slightly but statistically significantly suppressed after 1-month
exposure at 0.375 mW/cm2 and after 2-months exposure at 0.125 mW/cm2. Conditioned reflex
performance in a shuttle box was suppressed after 2 months of exposure at 0.25 mW/cm2. After 3 and 4
months of exposure, all behavioral parameters were the same as in the control group. Overall, behavioral
effects observed in this study were regarded as "weak and unstable".
In a study by Grigoriev et al. (1995), adult rabbits were exposed to 1.5-GHz pulsed microwaves for 30
min a day for 1 month, excluding weekends and holidays (16-ms pulse width, 0.3 mW/cm2 peak power,
0.12-Hz pulse repetition rate). Exposures were performed in an anechoic chamber, one animal at a time.
During the exposure, animals were placed into a special Perspex cage (40 x 40 x 40 cm) with a built-in
piezoelectric probe for recording motor activity. The authors performed two identical series of
experiments. In each series, 5 animals were exposed and 5 were sham-exposed. Sham exposures were done
in the same chamber in a random sequence with microwave exposures. In both series, the motor activity of
the sham-exposed animals was maximum in the first 2 days, reflecting an orientation-exploratory reaction.
The later period (until the 15th day) was characterized by extensive fluctuations of motor activity, which
was interpreted as development of adaptation. After 2 weeks of treatment, motor activity stabilized at a
significantly lower level, showing that adaptation is completed. In exposed animals, this decrease of motor
activity was not significant, and this effect was observed in both series of experiments. For example, in the
control group of the second series, the number of movements recorded during 30 min of sham exposure
decreased from 117 ± 13 (the first 2 weeks' average) to 64 ± 7.8 (the second 2 weeks' average, p<.05). The
respective numbers for microwave-exposed animals were 120 ± 11 and 105 ± 13 (p>.05). This irradiation
effect was regarded as inhibition of the adaptive reaction, or disadaptation. The 30-min dynamics of motor
activity did not show any difference between exposed and control animals, but one type of movements
(rapid moving of paws up and down) significantly increased in the exposed animals in the second 2 weeks
of the experiment. This type of activity pointed to an enhancement of excitatory processes in the central
nervous system, increased anxiety and distress.
Physiological effects of fields generated by ship radio transmitters (13 MHz, 250 or 500 V/m,
modulated by Morse code) were reported in a series of studies by Minkina et al. (1985) and Nikitina et al.
(1989a,b). Male albino rats (160-180 g body weight) were exposed to the field for 2 hours a day, 5 times a
week, over a 2- or 6-week period. The authors did not supply information as to whether or not these
exposures affected the body temperature of the animals. After the course of exposures, animals were
decapitated and various tissues were taken for morphological and histological examination.
In the first of these studies, 2 weeks of exposure at 500 V/m slightly activated the neurosecretory
function of supraoptic and paraventricular nuclei in hypothalamus. These alterations disappeared after 6
weeks of exposure, but, by this time, the mass of the adrenals was considerably decreased. Irradiation at
250 V/m for 30 days reduced the blood plasma level of corticosterone, with no other effect on adrenals or
hypothalamus. Changes observed in the thyroid gland morphology indicated activation of its function by
500 V/m exposure and suppression by 250 V/m exposure. Out of studied tissues and organs, spermaries
proved to be the most sensitive to irradiation. Disorders of spermatogenesis, hemorrhagia, degenerative
and dystrophic changes increased with longer course and higher intensity of exposures.
The second study (Nikitina et al., 1989a) was primarily focused on cytogenetic effects of exposure
(500 V/m for 10 days). Chromosome aberration frequency significantly increased in bone marrow cells (to
10-11% versus 5-6% in sham exposed controls, p<.05), but not in corneal cells. At the same time, the
mitotic index in corneal cells fell from 1.01% to 0.66% (p<.05). The ascorbic acid concentration in the
hypophysis and adrenal cortex increased from 264 ± 17 mg% and 403 ± 15 mg% in control animals to 361
± 27 mg% and 478 ± 24 mg%, respectively. The size of the adrenal cortex cells decreased. In thyroid
gland, the growth of colloid accumulation in follicular cavities was observed. The follicular area filled with
colloid increased from 10.8 ± 2.8% to 29.7 ± 6.1% after irradiation. Irradiation disrupted spermatogenesis
and reduced the mitotic activity of spermatic epithelium. The observed morphological changes indicated
suppression of adrenocorticotropic hormone secretion and of the adrenal cortex and thyroid gland function.
The production of luteotropic and follicle-stimulating hormones apparently was not affected.
In the third study (Nikitina et al., 1989b), the authors suggested that individual features of the animals,
namely, "the type of organization of their nervous function", might play a role in their sensitivity to
radiofrequency exposure. As in the previous studies, the experiments were performed in male albino rats.
Based on the animals' characteristic behavior in an open-field test, they were assigned to groups with "low-
entropy" (LE) and "high-entropy" (HE) organization of the nervous function. After 60 days of exposure at
500 V/m, the authors evaluated the condition of the animals by 30 various indices (morphology of thyroid,
adrenals, hypophysis; blood level of testosterone, luteinizing and follicle-stimulating hormones, etc.) and
the condition of their progeny on the 20th day of embryo development by 13 other indices (body mass and
length, organ pathology, ossification rate, etc.). Examination of the sham-exposed group revealed 7 indices
that were significantly different in the LE and HE animals; in the exposed group, there were 17 such
indices. The authors provided three examples that were characteristic for these differences. The
morphological changes in the thyroid gland evidenced for its activation in both LE and HE exposed
animals; however, in the LE specimens this actually was manifested as an increment in the epithelial cells
height, and in the HE specimens it was an increment in the cell nucleus area. Exposure significantly
diminished body mass in the exposed LE animals (by about 10% compared with LE controls), but did not
change it in HE animals. There was no difference in the rate of ossification in the progeny of the control
HE and LE animals, while the EMF treatment decreased this index in the offsprings of the LE specimens
and increased it in the offsprings of the HE specimens. Thus, the experimental results revealed
considerable differences in the EMF sensitivity between the LE and HE animals. It was recommended to
consider such individual differences in future behavioral studies and in the development of safety
Perhaps the most pronounced and unambiguously adverse effects of low-intensity microwave
radiation were reported by Lokhmatova (1994). Effects of a 4-month exposure for 2 hours/day (3-GHz,
0.25 mW/cm2) on reproductive organs were studied in 22 adult male rats. While the transmitter operated in
a CW mode, an intermittent irradiation regimen was achieved by rotating the transmitter horn antenna at 22
rpm. A similar group of 22 animals underwent the same course of sham exposures. Morphological and
histochemical analyses of the testes and epididymides were performed right after the end of the exposures
and also 4 months later. The experiments revealed explicit morphofunctional disorders in RF-exposed
animals. The number of normal seminiferous tubules decreased to 28.2 ± 5.3% (compared with 47.1 ±
5.3% in the controls), while the number of the tubules with dying cells increased to 27.2 ± 4.4% (14.7 ±
3.3% in the controls, p<.05). The number of Leydig cells markedly decreased, and some of them showed
pyknotic and destructive alterations. RF exposures increased alkaline phosphatase activity in the vicinity of
basal membranes and in the spermatic channel walls, and increased levels of NADH and succinate
dehydrogenases. Most of these disorders showed only a subtle or no trend to recovery in 4 months after the
end of exposures. The author concluded that the changes evoked by the prolonged microwave exposure are
likely to result in stable impairments of production and balance of steroid hormones and premature loss of
reproductive function.
Nowadays, EHPP technologies and applications are among the fastest growing areas, but very little is
known about EHPP bioeffects and health hazards. The overall number of biological studies with RF pulses
of 1-100 kW/g does not exceed 2-3 dozen (including meeting abstracts), and only a few isolated studies
have explored still higher peak field intensities. Russian EHPP studies employed the most advanced pulsed
power sources (which are still not available for biologists in the West), but the quality of reported
biological research often is questionable.
Tambiev et al. (1989) studied the effect of 10-ns wide, 200 kW/cm2 RF pulses (3-cm wavelength, 1
pulse per 6 min) on the growth rate and photosynthetic oxygen evolution in blue-green alga Spirulina
platensis and unicellular green algae Platymonas viridis. It was found that exposure to 10-15 pulses
stimulated cell culture growth and oxygen evolution. For example, by the 30th day after a single exposure,
the biomass of S. platensis cultures increased by 52% in comparison with sham-exposed controls, and that
of P. viridis increased by 17%. Maximum stimulatory effect (by up to 115%) was achieved when a
treatment by 10-15 EHPP was performed immediately after a 30-min exposure to 2.2 mW/cm2, 7.1-mm
wavelength CW radiation (this mm-wave irradiation alone enhanced the growth by about 50%). The same
combined treatment caused the most pronounced enhancement of the photosynthetic oxygen evolution
(about 1.5 times). Further experiments demonstrated that a greater number of EHPP (20-25) had the
opposite effect, i.e., suppressed the alga growth.
Deviatkov et al. (1994, 1998) studied the effects of 10-ns EHPP (3-cm wavelength, 100-MW peak
output power) on malignant neoplasm development in vivo and in vitro. Exposure of Wistar rats for 9 days,
43 pulses/day, prior to inoculation with Walker carcinoma, decelerated the neoplasm growth rate 1.5 times
and increased the life expectancy by 25-30%. In vitro exposure of Walker carcinoma cell suspensions (80
kV/cm, 6 pulses/min for 5 to 30 min) increased the number of degenerating cells and those in a stage of
lysis. Further experiments studied combined effects of EHPP and an anti-tumor drug endoksan on alveolar
hepatic cancer RS-1 in rats. The drug treatment and exposures (6 pulses/min, 30 min/day for 7 days) began
when the tumor volume reached 3-4 cm3. By the 55th day after tumor inoculation, the tumor volume was
84.7 cm3 in controls, 14 cm3 in the endoksan-treated group, and 8.9 cm3 in the group treated by endoksan
and EHPP. A similar experiment with Lewis lung carcinoma found that EHPP treatment (6 pulses/min, 30
min/day for 4 days and then for 5 days more, after a 1-day interval) suppressed metastases, from 3.0 points
(untreated controls) to 2.3 ± 0.4 (EHPP only) or 0.6 ± 0.2 (EHPP + endoksan); endoksan only decreased
this index to 1.4 ± 0.4. For a health risk assessment, 58 animals were exposed to EHPP (from 130 to 720
pulses in 5 sessions) and compared with 64 control animals. Periodic examinations (3-4 times a month)
over a period of 1-1.5 years have not revealed any modifications in behavioral responses or in the general
state of health of the animals. Autopsy of animals in one year after the exposure did not reveal any
pathological modifications in the liver, kidneys, adrenals, thymus, spleen, or other organs. We have to
note, however, that lack of sufficient detail on the experimental data, protocols, dosimetry, and statistics in
this study makes it difficult to evaluate the validity of reported findings.
An interesting EHPP study has been recently reported from the Institute of High Current Electronics
in Tomsk, Russia (Bolshakov et al., 1999). The study was designed to check out several likely mechanisms
of EHPP biological action, namely (1) membrane electroporation by high instant voltages of the electric
field, (2) direct influence of the intense electric filed on macromolecular charged complexes, such as
unfolded DNA sites and cytoskeleton fibers, and (3) changes in the rate of biochemical reactions, diffusion
of substances and cell migration due to temperature gradients caused by EHPP absorption. These
mechanisms were tested in experiments with (1) growth rate of Escherichia coli culture, (2) proliferation
and growth of simple eukaryotic organisms (fungus Fusarium), and (3) ontogenetic development of
Drosophila flies. All exposures employed a relativistic microwave generator with 200-MW output, 10-ns
pulse duration, and 3-cm wavelength. The incident E-field in the exposure zone (about 25-cm diameter)
was 1.5 MV/m, which corresponds to the incident power density of 300 kW/cm2.
The growth of E. coli culture was measured from changes in its optical density. Two identical
thermostabilized (± 1 oC) vials with the bacterial culture were simultaneously placed in an anechoic
chamber, but one of the vials (control) was shielded from microwave radiation. Exposures for 5 or 15 min
at various EHPP repetition rates (up to 100 Hz) caused no significant changes in the cell growth rate. This
result was interpreted as lack of cell electroporation by the EHPP pulses.
Proliferation rate of the Fusarium fungus was measured by micrometry, from the diameter of cell
colonies and the length of hyphae. Exposure regimens were the same as in experiments with E. coli; in
addition, some samples were exposed in cycles (5 min exposure, 5 min pause) for a total of 1 hour at the
EHPP repetition rate of 6 Hz. All tested exposure regimens substantially decelerated the growth of hyphae,
on the average from 0.338 ± 0.055 mm/hour (control) to 0.242 ± 0.033 mm/hour. This deceleration was
equivalent to the effect of conventional heating by 20-25 oC; however, heating of samples during
microwave exposure was less than 1 oC.
For experiments with Drosophila eggs, larvae, and pupa, each group included at least 300 specimens.
Each group was exposed or sham exposed just a single time, at different stages of ontogenesis. The
exposure duration was 5 min or 60 min (12 cycles of 5-min exposure with 5-min intervals); the EHPP
repetition rate was 6, 10, 16, or 22 Hz. All tested exposure parameters typically caused a 2- to 10-fold
increase of cases of interrupted specimen development. Exposures of 1-hour-old embryos could cause
developmental abnormalities (morphoses) in 6 to 9% of specimens (versus zero cases in parallel controls),
increased imago lethality, and caused infertility in survivors. Additional experiments with imago flies
established that 5 to 12% of flies died during a 1-min exposure at EHPP repetition rates of 16, 50, and 100
Hz. At the rates of 6 and 10 Hz, no flies died, but their first generation progeny became almost entirely
nonviable (34% had morphoses, 38% died on the first day, and 100% were unable to lay eggs). Since the
average heating by microwave exposures was negligible, the observed effects point to certain specific
mechanisms of EHPP biological action.
We conclude that Russian/FSU studies constitute an important source of information on pulsed RF
bioeffects. Particular emphasis in these studies was given to RF-induced changes in the nervous system
function, while such issues as RF-induced carcinogenesis apparently have not been a concern and were not
studied at all.
While many (perhaps, most) of the studies were flawed, a number of good-quality studies have
convincingly demonstrated significant bioeffects of pulsed microwaves. Modulation often was the factor
that determined the biological response to irradiation, and reactions to pulsed and CW emissions at equal
time-averaged intensities in many cases were substantially different. These results showed that bioeffects
of pulsed RF may involve some specific mechanisms of interaction, which are not understood yet.
Most reported bioeffects of low-intensity pulsed microwaves were just subtle functional changes,
which did not exceed the limits of normal physiological variation and could only be detected by sensitive
physiological tests. However, some studies did report clearly pathogenic effects, and an independent
confirmation of these findings would be of principle importance for understanding of the health hazards
from RF exposure and development of safety standards. These studies deserve careful consideration and
their replication in the West and/or with participation of Western scientists should be given a high priority.
The work was supported in part by the U.S. Army Medical Research and Materiel Command and the
U.S. Air Force Research Laboratory (HEDR and AFOSR) under U.S. Army contract DAMD17-94-C-4069
awarded to McKessonHBOC BioServices. The views expressed are those of the authors and should not be
construed as reflecting the official policy or position of the Department of the Army, Department of the Air
Force, or the United States Government.
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... In addition, pulsed microwaves reportedly may alter blood-brain barrier permeability, disrupt long-term potentiation and result in DNA strand breaks (11). Pakhomov and Murphy (12) reviewed an extensive body of microwave experiments performed in Russia and the former Union of Soviet Socialist Republics. In these works, animal brains were found to be considerably more sensitive to pulsed microwaves than to continuous wave microwaves; they concluded that microwave heating did not, at least primarily, cause this injury effect. ...
... Microwave exposure alters blood brain barrier permeability to cause DNA damage (11,12). Blood brain injury also is known to occur in blast injury but is much better described (28)(29)(30). ...
... Energies involved in this injury compare to those found in low level blast effects ranging from ∼47 kPa to levels < 100 kPa resulting in nanoscale injuries in the absence of gross or microscopic organ damage (18). Long term studies of single or pulsed microwave injuries resulting in chronic glial or astrocytic effects have not been done, while limited data on blood brain barrier effects imply endothelial vacuolization in the olfactory region (11,12). High explosive blasts have long been known to generate wide wavelength microwaves likely with differing effects than the short-wave high frequency microwaves here considered (32). ...
Full-text available
Pulsed microwaves above specific energy thresholds have been reported to cause brain injury in animal models. The actual physical mechanism causing brain damage is unexplained while the clinical reality of these injuries remains controversial. Here we propose mechanisms by which pulsed microwaves may injure brain tissue by transduction of microwave energy into damaging acoustic phonons in brain water. We have shown that low intensity explosive blast waves likely initiate phonon excitations in brain tissues. Brain injury in this instance occurs at nanoscale subcellular levels as predicted by physical consideration of phonon interactions in brain water content. The phonon mechanism may also explain similarities between primary non-impact blast-induced mild Traumatic Brain Injury (mTBI) and recent clinical and imaging findings of unexplained brain injuries observed in US embassy personnel possibly due to directed radiofrequency radiation. We describe experiments to elucidate mechanisms, RF frequencies and power levels by which pulsed microwaves potentially injure brain tissue. Pathological documentation of nanoscale brain blast injury has been supported experimentally using transmission electron microscopy (TEM) demonstrating nanoscale cellular damage in the absence of gross or light microscopic findings. Similar studies are required to better define pulsed microwave brain injury. Based upon existing findings, clinical diagnosis of both low intensity blast and microwave-induced brain injury likely will require diffusion tensor imaging (DTI), a specialized water based magnetic resonance imaging (MRI) technique.
... Several in vitro and in vivo studies have shown that the response to radiations from the different modulation modes can be remarkably different. This subject has been extensively reviewed by Pakhomov et al. (1998), Belyaev et al. (2000, Pakhomov and Murphy (2000), and Hyland (2001). ...
... A number of experimental data have shown that both beneficial and adverse health effects can be induced by MWs dependent on conditions of exposure (Pakhomov and Murphy 2000;Kundi et al. 2004). It is particularly interesting to note that MWs at very low power densities could either inhibit or stimulate the same functions depending on conditions of exposure (Pakhomov et al. 1998). ...
... In all of these experimental systems and clinical applications, acceleration of extracellular matrix synthesis and tissue healing was observed. In [49], it was confirmed in experiments that the stimulating effect of modulation at frequencies less than 100 Hz during microwave irradiation on the development of pathological effects. A recent study by Global Quantech [51] confirms that irradiation with low-intensity EMR causes inhibition of tumor growth and suppression of the viability of cancer cells by more than 1.5 times due to molecular structuring of the aqueous medium of a living organism; ...
From the standpoint of fundamental physical optics, clinical images and medical cases of a number of human viral diseases are considered under the influence of the environment on a sick organism, namely: Solar-geomagnetic disturbances and modern anthropogenic background. Microwave emission of the terrestrial ionosphere disturbed by flares on the Sun and during periods of magnetic storms was determined to be the agent of such an impact, and the anthropogenic influence is associated with the continuously increasing radiation of the microwave flux during the development of mobile cellular communications. Separately, new experimental results on the effect of weightlessness on the mitosis of cancer cells, including those created artificially are being studied. A unified interpretation of these results within the framework of supramolecular physics of the generation of supramolecular structures (water-containing associates) in a living organism is presented.
... Exposure limits based on time-averaged SAR dosimetry or power density, without consideration of the impact of amplitude or frequency modulations, do not adequately address potential health effects of real-world exposures to RFR. There is ample evidence that various effects of RFR exposure depend on carrier wave modulations, frequency, or pulsing [43,107,108]. In contrast to ICNIRP/FCC, the IARC monograph on RFR carcinogenicity noted that RFR effects may be influenced by such exposure characteristics as duration of exposure, carrier frequency, type of modulation, polarization, exposure intermittence, and background electromagnetic fields [44]. ...
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In the late-1990s, the FCC and ICNIRP adopted radiofrequency radiation (RFR) exposure limits to protect the public and workers from adverse effects of RFR. These limits were based on results from behavioral studies conducted in the 1980s involving 40–60-minute exposures in 5 monkeys and 8 rats, and then applying arbitrary safety factors to an apparent threshold specific absorption rate (SAR) of 4 W/kg. The limits were also based on two major assumptions: any biological effects were due to excessive tissue heating and no effects would occur below the putative threshold SAR, as well as twelve assumptions that were not specified by either the FCC or ICNIRP. In this paper, we show how the past 25 years of extensive research on RFR demonstrates that the assumptions underlying the FCC’s and ICNIRP’s exposure limits are invalid and continue to present a public health harm. Adverse effects observed at exposures below the assumed threshold SAR include non-thermal induction of reactive oxygen species, DNA damage, cardiomyopathy, carcinogenicity, sperm damage, and neurological effects, including electromagnetic hypersensitivity. Also, multiple human studies have found statistically significant associations between RFR exposure and increased brain and thyroid cancer risk. Yet, in 2020, and in light of the body of evidence reviewed in this article, the FCC and ICNIRP reaffirmed the same limits that were established in the 1990s. Consequently, these exposure limits, which are based on false suppositions, do not adequately protect workers, children, hypersensitive individuals, and the general population from short-term or long-term RFR exposures. Thus, urgently needed are health protective exposure limits for humans and the environment. These limits must be based on scientific evidence rather than on erroneous assumptions, especially given the increasing worldwide exposures of people and the environment to RFR, including novel forms of radiation from 5G telecommunications for which there are no adequate health effects studies.
... Pulsed radio-frequency radiation such as WCR exhibits substantially different bioeffects, both qualitatively and quantitatively (generally more pronounced) compared to continuous waves at similar time-averaged power densities [33][34][35][36]. The specific interaction mechanisms are not well understood. ...
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Background and aim: Coronavirus disease (COVID-19) public health policy has focused on the severe acute respiratory syndrome coronavirus 2 (SARS-CoV-2) virus and its effects on human health while environmental factors have been largely ignored. In considering the epidemiological triad (agent-host-environment) applicable to all disease, we investigated a possible environmental factor in the COVID-19 pandemic: ambient radiofrequency radiation from wireless communication systems including microwaves and millimeter waves. SARS-CoV-2, the virus that caused the COVID-19 pandemic, surfaced in Wuhan, China shortly after the implementation of city-wide (fifth generation [5G] of wireless communications radiation [WCR]), and rapidly spread globally, initially demonstrating a statistical correlation to international communities with recently established 5G networks. In this study, we examined the peer-reviewed scientific literature on the detrimental bioeffects of WCR and identified several mechanisms by which WCR may have contributed to the COVID-19 pandemic as a toxic environmental cofactor. By crossing boundaries between the disciplines of biophysics and pathophysiology, we present evidence that WCR may: (1) cause morphologic changes in erythrocytes including echinocyte and rouleaux formation that can contribute to hypercoagulation; (2) impair microcirculation and reduce erythrocyte and hemoglobin levels exacerbating hypoxia; (3) amplify immune system dysfunction, including immunosuppression, autoimmunity, and hyperinflammation; (4) increase cellular oxidative stress and the production of free radicals resulting in vascular injury and organ damage; (5) increase intracellular Ca2+ essential for viral entry, replication, and release, in addition to promoting pro-inflammatory pathways; and (6) worsen heart arrhythmias and cardiac disorders. Relevance for patients: In short, WCR has become a ubiquitous environmental stressor that we propose may have contributed to adverse health outcomes of patients infected with SARS-CoV-2 and increased the severity of the COVID-19 pandemic. Therefore, we recommend that all people, particularly those suffering from SARS-CoV-2 infection, reduce their exposure to WCR as much as reasonably achievable until further research better clarifies the systemic health effects associated with chronic WCR exposure.
... Millimeter wave energy, with the very small wavelengths associated with such high-frequency radiation, couples maximally with human skin tissue. Because of this efficient skin coupling, beneficial/therapeutic effects have been known for decades, especially in former Soviet Union countries, from short-term MMW exposures, while longer exposures have produced potentially adverse effects [258,269,281,282]. ...
Ambient levels of electromagnetic fields (EMF) have risen sharply in the last 80 years, creating a novel energetic exposure that previously did not exist. Most recent decades have seen exponential increases in nearly all environments, including rural/remote areas and lower atmospheric regions. Because of unique physiologies, some species of flora and fauna are sensitive to exogenous EMF in ways that may surpass human reactivity. There is limited, but comprehensive, baseline data in the U.S. from the 1980s against which to compare significant new surveys from different countries. This now provides broader and more precise data on potential transient and chronic exposures to wildlife and habitats. Biological effects have been seen broadly across all taxa and frequencies at vanishingly low intensities comparable to today’s ambient exposures. Broad wildlife effects have been seen on orientation and migration, food finding, reproduction, mating, nest and den building, territorial maintenance and defense, and longevity and survivorship. Cyto- and geno-toxic effects have been observed. The above issues are explored in three consecutive parts: Part 1 questions today’s ambient EMF capabilities to adversely affect wildlife, with more urgency regarding 5G technologies. Part 2 explores natural and man-made fields, animal magnetoreception mechanisms, and pertinent studies to all wildlife kingdoms. Part 3 examines current exposure standards, applicable laws, and future directions. It is time to recognize ambient EMF as a novel form of pollution and develop rules at regulatory agencies that designate air as ‘habitat’ so EMF can be regulated like other pollutants. Wildlife loss is often unseen and undocumented until tipping points are reached. Long-term chronic low-level EMF exposure standards, which do not now exist, should be set accordingly for wildlife, and environmental laws should be strictly enforced.
... At the moment, 5G communications, which use extremely high frequency MW or millimeter waves (MMW, wavelength 1-10 mm), is planned to be introduced in many countries. It follows from multiple studies that MMW can affect biological systems and human health, both positively and negatively, under specific conditions of exposure at very low intensities below the ICNIRP guidelines (107)(108)(109). Various biological and health effects have been described, which commonly depend on multiple physical and physiological parameters. ...
... The literature on the NT MW effects is very broad. There are four lines of evidence for the NT MW effects: (1) altered cellular responses in laboratory in vitro studies and results of chronic exposures in vivo studies (Cook et al., 2006;Grigoriev et al., 2003;Huss et al., 2007;Lai, 2005), (2) results of medical application of NT MW in the former Soviet Union countries (Betskii et al., 2000;Devyatkov et al., 1994;Pakhomov and Murphy, 2000;Sit'ko, 1989), (3) hypersensitivity to electromagnetic fields (EMFs) (Hagstrom et al., 2013;Havas and Marrongelle, 2013), and (4) epidemiological studies suggesting increased cancer risks for mobile phone users (Hardell et al., 2013a,b). It should be noted that along with detrimental effects, beneficial effects of NT MW have also been reported (Arendash et al., 2010;Dragicevic et al., 2011) supporting long-standing notion that interplay of physical MW parameters and biological parameters of the exposed object defines the value of the NT MW effect (Sit'ko, 1989). ...
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Under some occupational conditions, workers are inevitably exposed to high-intensity radiofrequency (RF) fields. In this study, we investigated the effects of one-month exposure to a 220 MHz pulsed modulated RF field at the power density of 50 W/m2 on the sperm quality in male adult rats. The sperm quality was evaluated by measuring the number, abnormality and survival rate of sperm cells. The morphology of testis was examined by hematoxylin–eosin (HE) staining. The levels of secreting factors by Sertoli cells (SCs) and Leydig cells (LCs) were determined by enzyme linked immunosorbent assay (ELISA). The level of cleaved caspase 3 in the testis was detected by immunofluorescence staining. Finally, the expression levels of the apoptosis-related protein (caspase 3, BAX and BCL2) in the testis were assessed by Western blotting. Compared with the sham group, the sperm quality in the RF group decreased significantly. The levels of secreting factors of SCs and the morphology of the testis showed an obvious change after RF exposure. The level of the secreting factor of LCs decreased significantly after RF exposure. The levels of cleaved caspase 3, caspase 3, and the BAX/BCL2 ratio in the testis increased markedly after RF exposure. These data collectively suggested that under the present experimental conditions, 220 MHz pulsed modulated RF exposure could impair sperm quality in rats, and the disruption of the secreting function of LCs and increased apoptosis of testis cells induced by the RF field might be accounted for by this damaging effect.
Isolated frog sciatic nerves were exposed to high-peak-power microwave pulses (915 MHz) with the help of a stripline slot irradiator. The nerves were stimulated using twin pulses separated by a 6-ms interval at a repetition rate of 50 pairdsec. Microwave pulses (0.5 ms or 3 ms width, peak specific absorption rate 33-72 and 6-13 kW/kg) were either synchronized with stimuli in various manners or were asynchronous (50 p.p.s.). Nerve heating during exposure was within 1.5-2.7°C. The exposed nerves underwent faster decrease of compound action potential (CAP) amplitude and tracing integral; the effect was microwave-specific since the equivalent conventional heating of nerve produced the opposite changes. The magnitude of the effect had little, if any, correlation with the intensity of the microwave pulses and their phasing with the nerve action potential. CAP onset and peak velocities as well as nerve refractivity were not affected by microwave exposure.
Dependence of the microwave effect on modulation parameters (pulse width, duty ratio, and peak intensity) was studied in an isolated frog auricle preparation. The rate and amplitude of spontaneous auricle twitches were measured during and after a 2 min exposure to 915 or 885 MHz microwaves and were compared to preexposure values. The studied ranges of modulation parameters were: pulse width, 10⁻⁶--10⁻² s; duty ratio, 7:100000, and peak specific absorption rate, 100--3,000 W/kg. Combinations of the parameters were chosen by chance, and about 400 various exposure regimes were tested. The experiments established that no regime was effective unless the average microwave power was high enough to induce preparation heating (0.1--0.4 C). The twitch rate instantly increased, and the amplitude decreased, as the temperature rose; similar changes could be induced by equivalent conventional heating. the data provide evidence that the effect of short-term microwave exposure on the isolated heart pacemaker and contractile functions depends on pulse modulation just as much as modulation determines the average absorbed power. These functions demonstrated no specific dependence on exposure parameters such as frequency or power windows.
Functioning of the giant axon of the isolated earthworm ventral nerve cord was examined during exposure to 6.45 GHz microwaves. We used continuous wave and pulsed irradiation, either synchronized with stimuli or asynchronous, lasting for 10–50 min at specific absorption rate from 30 to 230 W/kg. Action potential (AP) conduction velocity and the capability of nerve fiber to answer long-lasting high-frequency stimulation served as indices of microwave effect. Under some experimental conditions the nerve appeared to have extreme sensitivity to subtle temperature changes, induced by irradiation, but no non-thermal microwave effects were detected.
Proceeding from P.K. Anokhin's theory of the functional systems, the paper considers the action of a modulated electromagnetic field (MEMF) on different stages of the central architectonics of purposeful behaviour of rats: afferent synthesis, decisions making, acceptor of the action results. The action of MEMF was studied in different experimental situations: choice of an alimentary or defensive reaction to one conditioned stimulus in different situations; extinction of conditioned alimentary reactions; elaboration and extinction of alimentary conditioned reactions in animals group contacts; choice of the side of reinforcement in a T-shaped maze, and, lastly, self-stimulation reactions. The experiments have shown that MEMF has a selective effect on the animals' emotional reactions. Greater disturbances are observed in the mechanisms of the animals' appraisal of the action of situational and trigger stimuli or surrounding individuals of their species and, hence, of decisions making and anticipation of future results of the action, the acceptor of the action results.
The effect of electromagnetic field with various modulation frequencies (2, 7, and 50 hertz) on the reaction of selfstimulation was studied in rats. The frequency of 2 hertz proved to cause a primary increase in the incidence of the selstimulation reaction, followed by its depression; the frequency 7 hertz at first failed to alter the selfstimulation intensity and then led to the gradual reduction of the incidence of the selfstimulation reaction; the frequency of 50 hertz depressed the selfstimulation reaction practically from the very beginning. The changes in the selfstimulation reaction were independent of the localization of the stimulating electrodes, but were determined by the frequency of the EMF modulation.
Microelectrode and voltage-clamp techniques were modified to record spontaneous electrical activity and ionic currents of Lymnea stagnalis neurons during exposure to a 900-MHz field in a waveguide-based apparatus. The field was pulse-modulated at repetition rates ranging from 0.5 to 110 pps, or it was applied as a continuous wave (CW). When subjected to pulsed waves (PW), rapid, burst-like changes in the firing rate of neurons occurred at SARs of a few W/kg. If the burst-like irregularity was present in the firing rate under control conditions, irradiation enhanced its probability of occurrence. The effect was dependent on modulation, but not on modulation frequency, and it had a threshold SAR near 0.5 W/kg. CW radiation had no effect on the firing rate pattern at the same SAR. Mediator-induced, current activation of acetyl-choline, dopamine, serotonin, or gamma-aminobutyric-acid receptors of the neuronal soma was not altered during CW or PW exposures and, hence, could not have been responsible for the bursting effect.
The effect of 800 mHz microwaves of 0, 3, 5, 7, 16, and 30 Hz modulation on GABA receptor concentration in rat brain cortex has been investigated. Irradiation of the whole body at a modulation frequency of 16 Hz readily decreases the GABA receptor concentration. Irradiation at other modulation frequencies is ineffective. Irradiation of the whole body modulated at 16 Hz with various exposure times (5, 15 and 60 min) has revealed the highest effect at 5 min, while at a longer exposure the effect decreases.