Tuesday, 15 March 2011 15:30

VLF and ELF Electric and Magnetic Fields

Rate this item
(1 Vote)

Extremely low frequency (ELF) and very low frequency (VLF) electric and magnetic fields encompass the frequency range above static (> 0 Hz) fields up to 30 kHz. For this paper ELF is defined as being in the frequency range > 0 to 300 Hz and VLF in the range > 300 Hz to 30 kHz. In the frequency range > 0 to 30 kHz, the wavelengths vary from ∞(infinity) to 10 km and so the electric and magnetic fields act essentially independently of each other and must be treated separately. The electric field strength (E) is measured in volts per metre (V/m), the magnetic field strength (H) is measured in amperes per metre (A/m) and the magnetic flux density (B) in tesla (T).

Considerable debate about possible adverse health effects has been expressed by workers using equipment that operates in this frequency range. By far the most common frequency is 50/60 Hz, used for the generation, distribution and use of electric power. Concerns that exposure to 50/60 Hz magnetic fields may be associated with an increased cancer incidence have been fuelled by media reports, distribution of misinformation and ongoing scientific debate (Repacholi 1990; NRC 1996).

The purpose of this article is to provide an overview of the following topic areas:

  • sources, occupations and applications
  • dosimetry and measurement
  • interaction mechanisms and biological effects
  • human studies and effects on health
  • protective measures
  • occupational exposure standards.

 

Summary descriptions are provided to inform workers of the types and strengths of fields from major sources of ELF and VLF, biological effects, possible health consequences and current exposure limits. An outline of safety precautions and protective measures is also given. While many workers use visual display units (VDUs), only brief details are given in this article since they are covered in greater detail elsewhere in the Encyclopaedia.

Much of the material contained here can be found in greater detail in a number of recent reviews (WHO 1984, 1987, 1989, 1993; IRPA 1990; ILO 1993; NRPB 1992, 1993; IEEE 1991; Greene 1992; NRC 1996).

Sources of Occupational Exposure

Levels of occupational exposure vary considerably and are strongly dependent upon the particular application. Table 1 gives a summary of typical applications of frequencies in the range > 0 to 30 kHz.

Table 1. Applications of equipment operating in the range > 0 to 30 kHz

Frequency

Wavelength(km)

Typical applications

16.67, 50, 60 Hz

18,000–5,000

Power generation, transmissions and use, electrolytic processes, induction heating, arc and ladle furnaces, welding, transportation, etc., any industrial, commercial, medical or research use of electric power

0.3–3 kHz

1,000–100

Broadcast modulation, medical applications, electric furnaces, induction heating, hardening, soldering, melting, refining

3–30 kHz

100–10

Very long-range communications, radio navigation, broadcast modulation, medical applications, induction heating, hardening, soldering, melting, refining, VDUs

 

Power generation and distribution

The principal artificial sources of 50/60 Hz electric and magnetic fields are those involved in power generation and distribution, and any equipment using electric current. Most such equipment operates at the power frequencies of 50 Hz in most countries and 60 Hz in North America. Some electric train systems operate at 16.67 Hz.

High voltage (HV) transmission lines and substations have associated with them the strongest electric fields to which workers may be routinely exposed. Conductor height, geometrical configuration, lateral distance from the line, and the voltage of the transmission line are by far the most significant factors in considering the maximum electric field strength at ground level. At lateral distances of about twice the line height, the electric field strength decreases with distance in an approximately linear fashion (Zaffanella and Deno 1978). Inside buildings near HV transmission lines, the electric field strengths are typically lower than the unperturbed field by a factor of about 100,000, depending on the configuration of the building and the structural materials.

Magnetic field strengths from overhead transmission lines are usually relatively low compared to industrial applications involving high currents. Electrical utility employees working in substations or on the maintenance of live transmission lines form a special group exposed to larger fields (of 5 mT and higher in some cases). In the absence of ferromagnetic materials, the magnetic field lines form concentric circles around the conductor. Apart from the geometry of the power conductor, the maximum magnetic flux density is determined only by the magnitude of the current. The magnetic field beneath HV transmission lines is directed mainly transverse to the line axis. The maximum flux density at ground level may be under the centre line or under the outer conductors, depending on the phase relationship between the conductors. The maximum magnetic flux density at ground level for a typical double circuit 500 kV overhead transmission lines system is approximately 35 μT per kiloampere of current transmitted (Bernhardt and Matthes 1992). Typical values for the magnetic flux density up to 0.05 mT occur in workplaces near overhead lines, in substations and in power stations operating at frequencies of 16 2/3, 50, or 60 Hz (Krause 1986).

Industrial processes

Occupational exposure to magnetic fields comes predominantly from working near industrial equipment using high currents. Such devices include those used in welding, electroslag refining, heating (furnaces, induction heaters) and stirring.

Surveys on induction heaters used in industry, performed in Canada (Stuchly and Lecuyer 1985), in Poland (Aniolczyk 1981), in Australia (Repacholi, unpublished data) and in Sweden (Lövsund, Oberg and Nilsson 1982), show magnetic flux densities at operator locations ranging from 0.7 μT to 6 mT, depending on the frequency used and the distance from the machine. In their study of magnetic fields from industrial electro-steel and welding equipment, Lövsund, Oberg and Nilsson (1982) found that spot-welding machines (50 Hz, 15 to 106 kA) and ladle furnaces (50 Hz, 13 to 15 kA) produced fields up to 10 mT at distances up to 1 m. In Australia, an induction heating plant operating in the range 50 Hz to 10 kHz was found to give maximum fields of up to 2.5 mT (50 Hz induction furnaces) at positions where operators could stand. In addition maximum fields around induction heaters operating at other frequencies were 130 μT at 1.8 kHz, 25 μT at 2.8 kHz and in excess of 130 μT at 9.8 kHz.

Since the dimensions of coils producing the magnetic fields are often small there is seldom high exposure to the whole body, but rather local exposure mainly to the hands. Magnetic flux density to the hands of the operator may reach 25 mT (Lövsund and Mild 1978; Stuchly and Lecuyer 1985). In most cases the flux density is less than 1 mT. The electric field strength near the induction heater is usually low.

Workers in the electrochemical industry may be exposed to high electric and magnetic field strengths because of electrical furnaces or other devices using high currents. For instance, near induction furnaces and industrial electrolytic cells magnetic flux densities can be measured as high as 50 mT.

Visual display units

The use of visual display units (VDUs) or video display terminals (VDTs) as they are also called, grows at an ever increasing rate. VDT operators have expressed concerns about possible effects from emissions of low-level radiations. Magnetic fields (frequency 15 to 125 kHz) as high as 0.69 A/m (0.9 μT) have been measured under worst-case conditions close to the surface of the screen (Bureau of Radiological Health 1981). This result has been confirmed by many surveys (Roy et al. 1984; Repacholi 1985 IRPA 1988). Comprehensive reviews of measurements and surveys of VDTs by national agencies and individual experts concluded that there are no radiation emissions from VDTs that would have any consequences for health (Repacholi 1985; IRPA 1988; ILO 1993a). There is no need to perform routine radiation measurements since, even under worst-case or failure mode conditions, the emission levels are well below the limits of any international or national standards (IRPA 1988).

A comprehensive review of emissions, summary of the applicable scientific literature, standards and guidelines has been provided in the document (ILO 1993a).

Medical applications

Patients suffering from bone fractures that do not heal well or unite have been treated with pulsed magnetic fields (Bassett, Mitchell and Gaston 1982; Mitbreit and Manyachin 1984). Studies are also being conducted on the use of pulsed magnetic fields to enhance wound healing and tissue regeneration.

Various devices generating magnetic field pulses are used for bone growth stimulation. A typical example is the device that generates an average magnetic flux density of about 0.3 mT, a peak strength of about 2.5 mT, and induces peak electric field strengths in the bone in the range of 0.075 to 0.175 V/m (Bassett, Pawluk and Pilla 1974). Near the surface of the exposed limb, the device produces a peak magnetic flux density of the order of 1.0 mT causing peak ionic current densities of about 10 to 100 mA/m2 (1 to 10 μA/cm2) in tissue.

Measurement

Prior to the commencement of measurements of ELF or VLF fields, it is important to obtain as much information as possible about the characteristics of the source and the exposure situation. This information is required for the estimation of the expected field strengths and the selection of the most appropriate survey instrumentation (Tell 1983).

Information about the source should include:

  • frequencies present, including harmonics
  • power transmitted
  • polarization (orientation of E field)
  • modulation characteristics (peak and average values)
  • duty cycle, pulse width, and pulse repetition frequency
  • antenna characteristics, such as type, gain, beam width and scan rate.

 

Information about the exposure situation must include:

  • distance from the source
  • existence of any scattering objects. Scattering by plane surfaces can enhance the E field by a factor of 2. Even greater enhancement may result from curved surfaces, e.g., corner reflectors.

 

Results of surveys conducted in occupational settings are summarized in table 2.

Table 2. Occupational sources of exposure to magnetic fields

Source

Magnetic flux
densities (mT)

Distance (m)

VDTs

Up to 2.8 x 10–4

0.3

HV lines

Up to 0.4

under line

Power stations

Up to 0.27

1

Welding arcs (0–50 Hz)

0.1–5.8

0–0.8

Induction heaters (50–10 kHz)

0.9–65

0.1–1

50 Hz Ladle furnace

0.2–8

0.5–1

50 Hz Arc furnace

Up to 1

2

10 Hz Induction stirrer

0.2–0.3

2

50 Hz Electroslag welding

0.5–1.7

0.2–0.9

Therapeutic equipment

1–16

1

Source: Allen 1991; Bernhardt 1988; Krause 1986; Lövsund, Oberg and Nilsson 1982; Repacholi, unpublished data; Stuchly 1986; Stuchly and Lecuyer 1985, 1989.

Instrumentation

An electric or magnetic field-measuring instrument consists of three basic parts: the probe, the leads and the monitor. To ensure appropriate measurements, the following instrumentation characteristics are required or are desirable:

  • The probe must respond only to the E field or the H field and not to both simultaneously.
  • The probe must not produce significant perturbation of the field.
  • The leads from the probe to the monitor must not disturb the field at the probe significantly, or couple energy from the field.
  • The frequency response of the probe must cover the range of frequencies required to be measured.
  • If used in the reactive near-field, the dimensions of the probe sensor should preferably be less than a quarter of a wavelength at the highest frequency present.
  • The instrument should indicate the root mean square (rms) value of the measured field parameter.
  • The response time of the instrument should be known. It is desirable to have a response time of about 1 second or less, so that intermittent fields are easily detected.
  • The probe should be responsive to all polarization components of the field. This may be accomplished either by inherent isotropic response, or by physical rotation of the probe through three orthogonal directions.
  • Good overload protection, battery operation, portability and rugged construction are other desirable characteristics.
  • Instruments provide an indication of one or more of the following parameters: average E field (V/m) or mean square E field (V2/m2); average H field (A/m) or mean square H field (A2/m2).

 

Surveys

Surveys are usually conducted to determine whether fields existing in the workplace are below limits set by national standards. Thus the person taking the measurements must be fully familiar with these standards.

All occupied and accessible locations should be surveyed. The operator of the equipment under test and the surveyor should be as far away as practicable from the test area. All objects normally present, which may reflect or absorb energy, must be in position. The surveyor should take precautions against radiofrequency (RF) burns and shock, particularly near high-power, low-frequency systems.

Interaction Mechanisms and Biological Effects

Interaction mechanisms

The only established mechanisms by which ELF and VLF fields interact with biological systems are:

  • Electric fields which induce a surface charge on an exposed body which results in currents (measured in mA/m2) inside the body, the magnitude of which is related to the surface charge density. Depending on the exposure conditions, size, shape and position of the exposed body in the field, the surface charge density can vary greatly, resulting in a variable and non-uniform distribution of currents inside the body.
  • Magnetic fields also act on humans by inducing electric fields and currents inside the body.
  • Electric charges induced in a conducting object (e.g., an automobile) exposed to ELF or VLF electric fields may cause current to pass through a person in contact with it.
  • Magnetic field coupling to a conductor (for example, a wire fence) causes electric currents (of the same frequency as the exposing field) to pass through the body of a person in contact with it.
  • Transient discharges (sparks) can occur when people and metal objects exposed to a strong electric field come into sufficiently close proximity.
  • Electric or magnetic fields may interfere with implanted medical devices (e.g., unipolar cardiac pacemakers) and cause malfunction of the device.

 

The first two interactions listed above are examples of direct coupling between persons and ELF or VLF fields. The last four interactions are examples of indirect coupling mechanisms because they can occur only when the exposed organism is in the vicinity of other bodies. These bodies can include other humans or animals and objects such as automobiles, fences or implanted devices.

While other mechanisms of interaction between biological tissues and ELF or VLF fields have been postulated or there is some evidence to support their existence (WHO 1993; NRPB 1993; NRC 1996), none has been shown to be responsible for any adverse consequence to health.

Health effects

The evidence suggests that most of the established effects of exposure to electric and magnetic fields in the frequency range > 0 to 30 kHz result from acute responses to surface charge and induced current density. People can perceive the effects of the oscillating surface charge induced on their bodies by ELF electric fields (but not by magnetic fields); these effects become annoying if sufficiently intense. A summary of the effects of currents passing through the human body (thresholds for perception, let-go or tetanus) are given in table 3.

Table 3. Effects of currents passing through the human body

Effect

Subject

Threshold current in mA

   

50 and 60 Hz

300 Hz

1000 Hz

10 kHz

30 kHz

Perception

Men

Women

Children

1.1

0.7

0.55

1.3

0.9

0.65

2.2

1.5

1.1

15

10

9

50

35

30

Let-go threshold shock

Men

Women

Children

9

6

4.5

11.7

7.8

5.9

16.2

10.8

8.1

55

37

27

126

84

63

Thoracic tetanization;
severe shock

Men

Women

Children

23

15

12

30

20

15

41

27

20.5

94

63

47

320

214

160

Source: Bernhardt 1988a.

Human nerve and muscle cells have been stimulated by the currents induced by exposure to magnetic fields of several mT and 1 to 1.5 kHz; threshold current densities are thought to be above 1 A/m2. Flickering visual sensations can be induced in the human eye by exposure to magnetic fields as low as about 5 to 10 mT (at 20 Hz) or electric currents directly applied to the head. Consideration of these responses and of the results of neurophysiological studies suggests that subtle central nervous system functions, such as reasoning or memory, may be affected by current densities above 10 mA/m2 (NRPB 1993). Threshold values are likely to remain constant up to about 1 kHz but rise with increasing frequency thereafter.

Several in vitro studies (WHO 1993; NRPB 1993) have reported metabolic changes, such as alterations in enzyme activity and protein metabolism and decreased lymphocyte cytotoxicity, in various cell lines exposed to ELF and VLF electric fields and currents applied directly to the cell culture. Most effects have been reported at current densities between about 10 and 1,000 mA/m2, although these responses are less clearly defined (Sienkiewicz, Saunder and Kowalczuk 1991). However, it is worth noting that the endogenous current densities generated by the electrical activity of nerves and muscles are typically as high as 1 mA/m2 and may reach up to 10 mA/m2 in the heart. These current densities will not adversely affect nerve, muscle and other tissues. Such biological effects will be avoided by restricting the induced current density to less than 10 mA/m2 at frequencies up to about 1 kHz.

Several possible areas of biological interaction which have many health implications and about which our knowledge is limited include: possible changes in night-time melatonin levels in the pineal gland and alterations in circadian rhythms induced in animals by exposure to ELF electric or magnetic fields, and possible effects of ELF magnetic fields on the processes of development and carcinogenesis. In addition, there is some evidence of biological responses to very weak electric and magnetic fields: these include the altered mobility of calcium ions in brain tissue, changes in neuronal firing patterns, and altered operand behaviour. Both amplitude and frequency “windows” have been reported which challenge the conventional assumption that the magnitude of a response increases with increasing dose. These effects are not well established and do not provide a basis for establishing restrictions on human exposure, although further investigations are warranted (Sienkievicz, Saunder and Kowalczuk 1991; WHO 1993; NRC 1996).

Table 4 gives the approximate ranges of induced current densities for various biological effects in humans.

Table 4. Approximate current density ranges for various biological effects

Effect

Current density (mA/m2)

Direct nerve and muscle stimulation

1,000–10,000

Modulation in central nervous system activity
Changes in cell metabolism in vitro

100–1,000

Changes in retinal function
Probable changes in central nervous system
Changes in cell metabolism in vitro


10–100

Endogenous current density

1–10

Source: Sienkiewicz et al. 1991.

Occupational Exposure Standards

Nearly all standards having limits in the range > 0-30 kHz have, as their rationale, the need to keep induced electric fields and currents to safe levels. Usually the induced current densities are restricted to less than 10 mA/m2. Table 5 gives a summary of some current occupational exposure limits.

Table 5. Occupational limits of exposure to electric and magnetic fields in the frequency range > 0 to 30 kHz (note that f is in Hz)

Country/Reference

Frequency range

Electric field (V/m)

Magnetic field (A/m)

International (IRPA 1990)

50/60 Hz

10,000

398

USA (IEEE 1991)

3–30 kHz

614

163

USA (ACGIH 1993)

1–100 Hz

100–4,000 Hz

4–30 kHz

25,000

2.5 x 106/f

625

60/f

60/f

60/f

Germany (1996)

50/60 Hz

10,000

1,600

UK (NRPB 1993)

1–24 Hz

24–600 Hz

600–1,000 Hz

1–30 kHz

25,000

6 x 105/f

1,000

1,000

64,000/f

64,000/f

64,000/f

64

 

Protective Measures

Occupational exposures that occur near high voltage transmission lines depend on the worker’s location either on the ground or at the conductor during live-line work at high potential. When working under live-line conditions, protective clothing may be used to reduce the electric field strength and current density in the body to values similar to those that would occur for work on the ground. Protective clothing does not weaken the influence of the magnetic field.

The responsibilities for the protection of workers and the general public against the potentially adverse effects of exposure to ELF or VLF electric and magnetic fields should be clearly assigned. It is recommended that the competent authorities consider the following steps:

  • development and adoption of exposure limits and the implementation of a compliance programme
  • development of technical standards to reduce the susceptibility to electromagnetic interference, for example, for pacemakers
  • development of standards defining zones with limited access around sources of strong electric and magnetic fields because of electromagnetic interference (e.g., for pacemakers and other implanted devices). The use of appropriate warning signs should be considered.
  • requirement of specific assignment of a person responsible for the safety of workers and the public at each site with high exposure potentials
  • development of standardized measurement procedures and survey techniques
  • requirements for the education of workers on the effects of exposure to ELF or VLF electric and magnetic fields and the measures and rules which are designed to protect them
  • drafting of guidelines or codes of practice for worker safety in ELF or VLF electric and magnetic fields. ILO (1993a) provides excellent guidance for such a code.

 

Back

Read 13819 times Last modified on Wednesday, 27 July 2011 21:51

" DISCLAIMER: The ILO does not take responsibility for content presented on this web portal that is presented in any language other than English, which is the language used for the initial production and peer-review of original content. Certain statistics have not been updated since the production of the 4th edition of the Encyclopaedia (1998)."

Contents

Radiation: Non-Ionizng References

Allen, SG. 1991. Radiofrequency field measurements and hazard assessment. J Radiol Protect 11:49-62.

American Conference of Governmental Industrial Hygienists (ACGIH). 1992. Documentation for the Threshold Limit Values. Cincinnati, Ohio: ACGIH.

—. 1993. Threshold Limit Values for Chemical Substances and Physical Agents and Biological Exposure Indices. Cincinnati, Ohio: ACGIH.

—. 1994a. Annual Report of ACGIH Physical Agents Threshold Limit Values Committee. Cincinnati, Ohio: ACGIH.

—. 1994b. TLV’s, Threshold Limit Values and Biological Exposure Indices for 1994-1995. Cincinnati, Ohio: ACGIH.

—. 1995. 1995-1996 Threshhold Limit Values for Chemical Substances and Physical Agents and Biological Exposure Indices. Cincinnati, Ohio: ACGIH.

—. 1996. TLVs© and BEIs©. Threshold Limit Values for Chemical Substances and Physical Agents; Biological Exposure Indices. Cincinnati, Ohio: ACGIH.

American National Standards Institute (ANSI). 1993. Safe Use of Lasers. Standard No. Z-136.1. New York: ANSI.

Aniolczyk, R. 1981. Measurements of hygienic evaluation of electromagnetic fields in the environment of diathermy, welders, and induction heaters. Medycina Pracy 32:119-128.

Bassett, CAL, SN Mitchell, and SR Gaston. 1982. Pulsing electromagnetic field treatment in ununited fractures and failed artrodeses. J Am Med Assoc 247:623-628.

Bassett, CAL, RJ Pawluk, and AA Pilla. 1974. Augmentation of bone repair by inductively coupled electromagnetic fields. Science 184:575-577.

Berger, D, F Urbach, and RE Davies. 1968. The action spectrum of erythema induced by ultraviolet radiation. In Preliminary Report XIII. Congressus Internationalis Dermatologiae, Munchen, edited by W Jadassohn and CG Schirren. New York: Springer-Verlag.

Bernhardt, JH. 1988a. The establishment of frequency dependent limits for electric and magnetic fields and evaluation of indirect effects. Rad Envir Biophys 27:1.

Bernhardt, JH and R Matthes. 1992. ELF and RF electromagnetic sources. In Non-Ionizing Radiation Protection, edited by MW Greene. Vancouver: UBC Press.

Bini, M, A Checcucci, A Ignesti, L Millanta, R Olmi, N Rubino, and R Vanni. 1986. Exposure of workers to intense RF electric fields that leak from plastic sealers. J Microwave Power 21:33-40.

Buhr, E, E Sutter, and Dutch Health Council. 1989. Dynamic filters for protective devices. In Dosimetry of Laser Radiation in Medicine and Biology, edited by GJ Mueller and DH Sliney. Bellingham, Wash: SPIE.

Bureau of Radiological Health. 1981. An Evaluation of Radiation Emission from Video Display Terminals. Rockville, MD: Bureau of Radiological Health.

Cleuet, A and A Mayer. 1980. Risques liés à l’utilisation industrielle des lasers. In Institut National de Recherche et de Sécurité, Cahiers de Notes Documentaires, No. 99 Paris: Institut National de Recherche et de Sécurité.

Coblentz, WR, R Stair, and JM Hogue. 1931. The spectral erythemic relation of the skin to ultraviolet radiation. In Proceedings of the National Academy of Sciences of the United States of America Washington, DC: National Academy of Sciences.

Cole, CA, DF Forbes, and PD Davies. 1986. An action spectrum for UV photocarcinogenesis. Photochem Photobiol 43(3):275-284.

Commission Internationale de L’Eclairage (CIE). 1987. International Lighting Vocabulary. Vienna: CIE.

Cullen, AP, BR Chou, MG Hall, and SE Jany. 1984. Ultraviolet-B damages corneal endothelium. Am J Optom Phys Opt 61(7):473-478.

Duchene, A, J Lakey, and M Repacholi. 1991. IRPA Guidelines On Protection Against Non-Ionizing Radiation. New York: Pergamon.

Elder, JA, PA Czerki, K Stuchly, K Hansson Mild, and AR Sheppard. 1989. Radiofrequency radiation. In Nonionizing Radiation Protection, edited by MJ Suess and DA Benwell-Morison. Geneva: WHO.

Eriksen, P. 1985. Time resolved optical spectra from MIG welding arc ignition. Am Ind Hyg Assoc J 46:101-104.

Everett, MA, RL Olsen, and RM Sayer. 1965. Ultraviolet erythema. Arch Dermatol 92:713-719.

Fitzpatrick, TB, MA Pathak, LC Harber, M Seiji, and A Kukita. 1974. Sunlight and Man, Normal and Abnormal Photobiologic Responses. Tokyo: Univ. of Tokyo Press.

Forbes, PD and PD Davies. 1982. Factors that influence photocarcinogenesis. Chap. 7 in Photoimmunology, edited by JAM Parrish, L Kripke, and WL Morison. New York: Plenum.

Freeman, RS, DW Owens, JM Knox, and HT Hudson. 1966. Relative energy requirements for an erythemal response of skin to monochromatic wavelengths of ultraviolet present in the solar spectrum. J Invest Dermatol 47:586-592.

Grandolfo, M and K Hansson Mild. 1989. Worldwide public and occupational radiofrequency and microwave protection. In Electromagnetic Biointeraction. Mechanisms, Safety Standards, Protection Guides, edited by G Franceschetti, OP Gandhi, and M Grandolfo. New York: Plenum.

Greene, MW. 1992. Non Ionizing Radiation. 2nd International Non Ionizing Radiation Workshop, 10-14 May, Vancouver.

Ham, WTJ. 1989. The photopathology and nature of the blue-light and near-UV retinal lesion produced by lasers and other optic sources. In Laser Applications in Medicine and Biology, edited by ML Wolbarsht. New York: Plenum.

Ham, WT, HA Mueller, JJ Ruffolo, D Guerry III, and RK Guerry. 1982. Action spectrum for retinal injury from near ultraviolet radiation in the aphakic monkey. Am J Ophthalmol 93(3):299-306.

Hansson Mild, K. 1980. Occupational exposure to radio-frequency electromagnetic fields. Proc IEEE 68:12-17.

Hausser, KW. 1928. Influence of wavelength in radiation biology. Strahlentherapie 28:25-44.

Institute of Electrical and Electronic Engineers (IEEE). 1990a. IEEE COMAR Position of RF and Microwaves. New York: IEEE.

—. 1990b. IEEE COMAR Position Statement On Health Aspects of Exposure to Electric and Magnetic Fields from RF Sealers and Dielectric Heaters. New York: IEEE.

—. 1991. IEEE Standard for Safety Levels With Respect to Human Exposure to Radiofrequency Electromagnetic Fields 3 KHz to 300 GHz. New York: IEEE.

International Commission on Non-Ionizing Radiation Protection (ICNIRP). 1994. Guidelines on Limits of Exposure to Static Magnetic Fields. Health Phys 66:100-106.

—. 1995. Guidelines for Human Exposure Limits for Laser Radiation.

ICNIRP statement. 1996. Health issues related to the use of hand-held radiotelephones and base transmitters. Health Physics, 70:587-593.

International Electrotechnical Commission (IEC). 1993. IEC Standard No. 825-1. Geneva: IEC.

International Labour Office (ILO). 1993a. Protection from Power Frequency Electric and Magnetic Fields. Occupational Safety and Health Series, No. 69. Geneva: ILO.

International Radiation Protection Association (IRPA). 1985. Guidelines for limits of human exposure to laser radiation. Health Phys 48(2):341-359.

—. 1988a. Change: Recommendations for minor updates to the IRPA 1985 guidelines on limits of exposure to laser radiation. Health Phys 54(5):573-573.

—. 1988b. Guidelines on limits of exposure to radiofrequency electromagnetic fields in the frequency range from 100 kHz to 300 GHz. Health Phys 54:115-123.

—. 1989. Proposed change to the IRPA 1985 guidelines limits of exposure to ultraviolet radiation. Health Phys 56(6):971-972.

International Radiation Protection Association (IRPA) and International Non-Ionizing Radiation Committee. 1990. Interim guidelines on limits of exposure to 50/60 Hz electric and magnetic fields. Health Phys 58(1):113-122.

Kolmodin-Hedman, B, K Hansson Mild, E Jönsson, MC Anderson, and A Eriksson. 1988. Health problems among operations of plastic welding machines and exposure to radiofrequency electromagnetic fields. Int Arch Occup Environ Health 60:243-247.

Krause, N. 1986. Exposure of people to static and time variable magnetic fields in technology, medicine, research and public life: Dosimetric aspects. In Biological Effects of Static and ELF-Magnetic Fields, edited by JH Bernhardt. Munchen: MMV Medizin Verlag.

Lövsund, P and KH Mild. 1978. Low Frequency Electromagnetic Field Near Some Induction Heaters. Stockholm: Stockholm Board of Occupational Health and Safety.

Lövsund, P, PA Oberg, and SEG Nilsson. 1982. ELF magnetic fields in electrosteel and welding industries. Radio Sci 17(5S):355-385.

Luckiesh, ML, L Holladay, and AH Taylor. 1930. Reaction of untanned human skin to ultraviolet radiation. J Optic Soc Am 20:423-432.

McKinlay, AF and B Diffey. 1987. A reference action spectrum for ultraviolet induced erythema in human skin. In Human Exposure to Ultraviolet Radiation: Risks and Regulations, edited by WF Passchier and BFM Bosnjakovic. New York: Excerpta medica Division, Elsevier Science Publishers.

McKinlay, A, JB Andersen, JH Bernhardt, M Grandolfo, K-A Hossmann, FE van Leeuwen, K Hansson Mild, AJ Swerdlow, L Verschaeve and B Veyret. Proposal for a research programme by a European Commission Expert Group. Possible health effects related to the use of radiotelephones. Unpublished report.

Mitbriet, IM and VD Manyachin. 1984. Influence of magnetic fields on the repair of bone. Moscow, Nauka, 292-296.

National Council on Radiation Protection and Measurements (NCRP). 1981. Radiofrequency Electromagnetic Fields. Properties, Quantities and Units, Biophysical Interaction, and Measurements. Bethesda, MD: NCRP.

—. 1986. Biological Effects and Exposure Criteria for Radiofrequency Electromagnetic Fields. Report No. 86. Bethesda, MD: NCRP.

National Radiological Protection Board (NRPB). 1992. Electromagnetic Fields and the Risk of Cancer. Vol. 3(1). Chilton, UK: NRPB.

—. 1993. Restrictions On Human Exposure to Static and Time-Varying Electromagnetic Fields and Radiations. Didcot, UK: NRPB.

National Research Council (NRC). 1996. Possible health effects of exposure to residential electric and magnetic fields. Washington: NAS Press. 314.

Olsen, EG and A Ringvold. 1982. Human corneal endothelium and ultraviolet radiation. Acta Ophthalmol 60:54-56.

Parrish, JA, KF Jaenicke, and RR Anderson. 1982. Erythema and melanogenesis: Action spectra of normal human skin. Photochem Photobiol 36(2):187-191.

Passchier, WF and BFM Bosnjakovic. 1987. Human Exposure to Ultraviolet Radiation: Risks and Regulations. New York: Excerpta Medica Division, Elsevier Science Publishers.

Pitts, DG. 1974. The human ultraviolet action spectrum. Am J Optom Phys Opt 51(12):946-960.

Pitts, DG and TJ Tredici. 1971. The effects of ultraviolet on the eye. Am Ind Hyg Assoc J 32(4):235-246.

Pitts, DG, AP Cullen, and PD Hacker. 1977a. Ocular effects of ultraviolet radiation from 295 to 365nm. Invest Ophthalmol Vis Sci 16(10):932-939.

—. 1977b. Ultraviolet Effects from 295 to 400nm in the Rabbit Eye. Cincinnati, Ohio: National Institute for Occupational Safety and Health (NIOSH).

Polk, C and E Postow. 1986. CRC Handbook of Biological Effects of Electromagnetic Fields. Boca Raton: CRC Press.

Repacholi, MH. 1985. Video display terminals -should operators be concerned? Austalas Phys Eng Sci Med 8(2):51-61.

—. 1990. Cancer from exposure to 50760 Hz electric and magnetic fields: A major scientific debate. Austalas Phys Eng Sci Med 13(1):4-17.

Repacholi, M, A Basten, V Gebski, D Noonan, J Finnic and AW Harris. 1997. Lymphomas in E-Pim1 transgenic mice exposed to pulsed 900 MHz electromagnetic fields. Radiation research, 147:631-640.

Riley, MV, S Susan, MI Peters, and CA Schwartz. 1987. The effects of UVB irradiation on the corneal endothelium. Curr Eye Res 6(8):1021-1033.

Ringvold, A. 1980a. Cornea and ultraviolet radiation. Acta Ophthalmol 58:63-68.

—. 1980b. Aqueous humour and ultraviolet radiation. Acta Ophthalmol 58:69-82.

—. 1983. Damage of the corneal epithelium caused by ultraviolet radiation. Acta Ophthalmol 61:898-907.

Ringvold, A and M Davanger. 1985. Changes in the rabbit corneal stroma caused by UV radiation. Acta Ophthalmol 63:601-606.

Ringvold, A, M Davanger, and EG Olsen. 1982. Changes of the corneal endothelium after ultraviolet radiation. Acta Ophthalmol 60:41-53.

Roberts, NJ and SM Michaelson. 1985. Epidemiological studies of human exposure to radiofrequency radiation: A critical review. Int Arch Occup Environ Health 56:169-178.

Roy, CR, KH Joyner, HP Gies, and MJ Bangay. 1984. Measurement of electromagnetic radiation emitted from visual display terminals (VDTs). Rad Prot Austral 2(1):26-30.

Scotto, J, TR Fears, and GB Gori. 1980. Measurements of Ultraviolet Radiations in the United States and Comparisons With Skin Cancer Data. Washington, DC: US Government Printing Office.

Sienkiewicz, ZJ, RD Saunder, and CI Kowalczuk. 1991. Biological Effects of Exposure to Non-Ionizing Electromagnetic Fields and Radiation. 11 Extremely Low Frequency Electric and Magnetic Fields. Didcot, UK: National Radiation Protection Board.

Silverman, C. 1990. Epidemiological studies of cancer and electromagnetic fields. In Chap. 17 in Biological Effects and Medical Applications of Electromagnetic Energy, edited by OP Gandhi. Engelwood Cliffs, NJ: Prentice Hall.

Sliney, DH. 1972. The merits of an envelope action spectrum for ultraviolet radiation exposure criteria. Am Ind Hyg Assoc J 33:644-653.

—. 1986. Physical factors in cataractogenesis: Ambient ultraviolet radiation and temperature. Invest Ophthalmol Vis Sci 27(5):781-790.

—. 1987. Estimating the solar ultraviolet radiation exposure to an intraocular lens implant. J Cataract Refract Surg 13(5):296-301.

—. 1992. A safety manager’s guide to the new welding filters. Welding J 71(9):45-47.
Sliney, DH and ML Wolbarsht. 1980. Safety With Lasers and Other Optical Sources. New York: Plenum.

Stenson, S. 1982. Ocular findings in xeroderma pigmentosum: Report of two cases. Ann Ophthalmol 14(6):580-585.

Sterenborg, HJCM and JC van der Leun. 1987. Action spectra for tumourigenesis by ultraviolet radiation. In Human Exposure to Ultraviolet Radiation: Risks and Regulations, edited by WF Passchier and BFM Bosnjakovic. New York: Excerpta Medica Division, Elsevier Science Publishers.

Stuchly, MA. 1986. Human exposure to static and time-varying magnetic fields. Health Phys 51(2):215-225.

Stuchly, MA and DW Lecuyer. 1985. Induction heating and operator exposure to electromagnetic fields. Health Phys 49:693-700.

—. 1989. Exposure to electromagnetic fields in arc welding. Health Phys 56:297-302.

Szmigielski, S, M Bielec, S Lipski, and G Sokolska. 1988. Immunologic and cancer related aspects of exposure to low-level microwave and radiofrequency fields. In Modern Bioelectricity, edited by AA Mario. New York: Marcel Dekker.

Taylor, HR, SK West, FS Rosenthal, B Munoz, HS Newland, H Abbey, and EA Emmett. 1988. Effect of ultraviolet radiation on cataract formation. New Engl J Med 319:1429-1433.

Tell, RA. 1983. Instrumentation for measurement of electromagnetic fields: Equipment, calibrations, and selected applications. In Biological Effects and Dosimetry of Nonionizing Radiation, Radiofrequency and Microwave Energies, edited by M Grandolfo, SM Michaelson, and A Rindi. New York: Plenum.

Urbach, F. 1969. The Biologic Effects of Ultraviolet Radiation. New York: Pergamon.

World Health Organization (WHO). 1981. Radiofrequency and microwaves. Environmental Health Criteria, No.16. Geneva: WHO.

—. 1982. Lasers and Optical Radiation. Environmental Health Criteria, No. 23. Geneva: WHO.

—. 1987. Magnetic Fields. Environmental Health Criteria, No.69. Geneva: WHO.

—. 1989. Non-Ionization Radiation Protection. Copenhagen: WHO Regional Office for Europe.

—. 1993. Electromagnetic Fields 300 Hz to 300 GHz. Environmental Health Criteria, No. 137. Geneva: WHO.

—. 1994. Ultraviolet Radiation. Environmental Health Criteria, No. 160. Geneva: WHO.

World Health Organization (WHO), United Nations Environmental Programme (UNEP), and International Radiation Protection Association (IRPA). 1984. Extremely Low Frequency (ELF). Environmental Health Criteria, No. 35. Geneva: WHO.

Zaffanella, LE and DW DeNo. 1978. Electrostatic and Electromagnetic Effects of Ultra-High-Voltage Transmission Lines. Palo Alto, Calif: Electric Power Research Institute.

Zuclich, JA and JS Connolly. 1976. Ocular damage induced by near-ultraviolet laser radiation. Invest Ophthalmol Vis Sci 15(9):760-764.