Glossary of Radiation Terms

Total Page:16

File Type:pdf, Size:1020Kb

Glossary of Radiation Terms GLOSSARY – Nagasaki University Center for Frontier Life Sciences GLOSSARY OF expressed by the linear absorption RADIATION TERMS coefficient. ACCELERATOR (PARTICLE): A device that accelerates charged sub-atomic ABSOLUTE RISK: The rate of disease particles to very great energies. These among a population. particles may be used for basic physics research, radioisotope production or for ABSORBED DOSE, D: The fundamental direct medical irradiation of patients. dose quantity given by the mean energy imparted to matter of mass by ionizing ACTIVATION: Absorption, usually of radiation. The SI unit for absorbed dose is neutrons or charged particles (the minimum joule per kilogram (J kg-1) and its special energy to induce this effect is 10 MeV) by name is gray (Gy). 1 Gy = 1 J/kg = 100 nuclei thereby making them radioactive. rads. ACTIVE (RED) BONE MARROW: The ABSORBED DOSE, MEAN IN A TISSUE organ system bone marrow contains the OR ORGAN, DT: The absorbed dose DT, cell systems for the formation of blood cells averaged over the tissue or organ T, which starting from the pluripotent haematopietic is given by stem cells to the mature blood cells. ACTIVITY, A: Is the number of nuclear where εT is the mean total energy imparted transformations occurring in a given in a tissue or organ T, and mT is the mass quantity of material per unit time. The SI of that tissue or organ. unit for the transformation rate is the Becquerel (Bq), which is defined as one ABSORPTION: Transfer or deposition of disintegration per second. 1 Bq = 2.7 x some or all of the energy of radiation 10-11Ci. 1 Ci = 3.7 x 1010Bq. traversing matter. ACUTE RADIATION SYNDROME (ARS): ABSORPTION COEFFICIENT: Since the A serious illness caused by receiving a absorption of gamma or X-rays is dose greater than 75 rads of penetrating exponential in nature, these radiations radiation to the body in a short time (usually have no clear cut range. The fractional minutes). The earliest symptoms are decrease in the intensity of such a beam nausea, fatigue, vomiting, and diarrhea. per unit thickness of the absorber is 1 GLOSSARY – Nagasaki University Center for Frontier Life Sciences Hair loss, bleeding, swelling of the mouth ANNUAL LIMIT ON INTAKE (ALI): The and throat, and general loss of energy may activity of a radionuclide which, upon follow. If the exposure has been ingestion, results in an exposure equal to approximately 1,000 rads or more, death the annual maximum permissible dose. may occur within 2 – 4 weeks. APOPTOSIS: An active biochemical ADAPTIVE RESPONSE: A post-irradiation process of programmed cell death following cellular response which, typically, serves to radiation or other insults. increase the resistance of the cell to a subsequent radiation exposure. ATOM: A particle of matter indivisible by chemical means. It is the fundamental ALPHA PARTICLE: A positively charged building block of elements. highly energetic nuclear fragment, comprised of two neutrons and two protons ATOMIC ENERGY BASIC LOW: The (helium nucleus). Japanese Law established in 1955, which declares the use of atomic energy only for AMBIENT DOSE EQUIVALENT, H*(10): peaceful aim through democratic The dose equivalent at a point in a administration, autonomous radiation field that would be produced by accomplishment and results disclosure in the corresponding expanded and aligned the public. field in the ICRU sphere at a depth of 10 mm on the radius vector opposing the ATOMIC NUMBER: The number assigned direction of the aligned field. The unit of to each element on the basis of the number ambient dose equivalent is joule per of protons found in the element's nucleus. kilogram (J kg-1) and its special name is sievert (Sv). ATOMIC WEIGHT (ATOMIC MASS): Approximately the sum of the number of ANION: A negatively charged ion. protons and neutrons found in the nucleus of an atom. ANNIHILATION RADIATION: Positrons interact with negative electrons resulting in ATTENUATION: The reduction of the the disappearance of both particles and the intensity of a beam of gamma or x-rays as it release of two annihilation 511 keV passes through some material. Beam photons. energy can be lost by deposition (absorption) and/or by deflection (deflection 2 GLOSSARY – Nagasaki University Center for Frontier Life Sciences attenuation). The three primary defined as one nuclear disintegration per mechanisms by which energy is transferred second (dps). 1 Bq = 2.7 x 10-11Ci. 1 Ci = from the beam to the material through 3.7 x 1010Bq. which it passes are the photoelectric effect, the Compton effect and pair production. BETA PARTICLE: Negatively charged particle emitted from the nucleus of an ATTRIBUTABLE RISK: The estimated rate atom. It is just an energetic electron. of a disease (such as lung cancer) that could, in theory, prevented if all exposures BIAS: Factors that influence the outcome to a particular causative agent (such as of data collection, such as causing certain radon) were eliminated. measurements to have a greater chance of being included than others. AVERTED DOSE: The dose prevented or avoided by the application of a protective BINDING ENERGY: The minimum energy measure or set of protective measures, i.e., required to separate a nucleus into its the difference between the projected dose component neutrons and protons. if the protective measure(s) had not been applied and the expected residual dose. BIOASSAY: Any procedure used to determine the nature, activity, location, or BACKGROUND RADIATION: The retention of radionuclides in the body by in radiation to which a member of the vivo measurement or by in vitro analysis of population is exposed from natural sources, material excreted or otherwise removed such as terrestrial radiation due to naturally from the body. occurring radionuclides in the soil, cosmic radiation originating in outer space, and BOHR RADIUS: The size of a ground state naturally occurring radionuclides in the hydrogen atom as calculated by Niels Bohr human body. using a mix of classical physics and quantum mechanics. BEAM: A flow of electromagnetic or particulate radiation that is generally BRACHYTHERAPY: Radiation treatment unidirectional or is divergent from a of a patient using sealed or unsealed radioactive source but is confined to a sources of radiation placed within the small angle. patient’s body. BECQUEREL (Bq): The SI unit of activity BRANCHING: The occurrence of two or 3 GLOSSARY – Nagasaki University Center for Frontier Life Sciences more modes by which a radionuclide can undergo radioactive decay to the ultimate CASE-CONTROL STUDY: An stable state. An individual atom of a nuclide epidemiologic study in which people with exhibiting branching disintegrates by one disease and a similarly composed control mode only. The fraction disintegrating by a group are compared in terms of exposures particular mode is the branching fraction for to a putative causative agent. that mode. The branching ratio is the ratio of two specified branching fractions (also CHARACTERISTIC X-RAY: A collision of called multiple disintegration). the fast-moving electrons with the atom first causes a tightly bound inner-shell electron BREMSSTRAHLUNG: Secondary to be ejected from the atom; a loosely electromagnetic radiations produced by the bound outer-shell electron then falls into rapid deceleration of charged particles in the inner shell to fill the vacancy. In the strong electromagnetic fields. The process, a single photon (characteristic likelihood of emission is proportional to the X-ray) is emitted by the atom with an mass of the nucleus of the absorber. energy equal to the difference between the inner-shell and outer-shell vacancy states. BYSTANDER EFFECT: A response in unirradiated cells that is triggered by COHORT STUDY: An epidemiologic study signals received from irradiated in which groups of people (the cohort) are neighbouring cells. identified with respect to the presence or absence of exposure to a disease-causing CARRIER: A quantity of non-radioactive or agent, and in which the outcomes of non-labeled material of the same chemical disease rates are compared; also called a composition as its corresponding follow-up study. radioactive or labeled counterpart. COLLECTIVE DOSE: The estimated dose CARRIER-FREE: A preparation of for an area or region multiplied by the radioisotope to which no carrier has been estimated population in that area or region. added and for which precautions have been taken to minimize contamination with COMMITTED DOSE EQUIVALENT: The other isotopes. Material of high specific total dose equivalent averaged throughout activity is often loosely referred to as a tissue 50 years after body uptake of the "carrier-free" but is more correctly defined radionuclide. as "high isotopic abundance". 4 GLOSSARY – Nagasaki University Center for Frontier Life Sciences COMPTON EFFECT: Interactive effect of excess energy of unstable nucleus to one X-ray and gamma radiation with matter. of its own orbiting electrons. The Compton effect is the elastic scattering of a quantum with a free or quasi-free COSMIC RADIATION: Radiation produced electron from the electron sheath of an in outer space when heavy particles from atom. Part of the energy and the pulse of other galaxies (nuclei of all known natural the quantum is transferred to the electron, elements) bombard the earth. the rest remains with the scattered quantum. COULOMB (C): The quantity of electricity transported in one second by a current of CONFIDENCE LIMITS: An interval giving one ampere. the lowest and highest estimate of a parameter that is statistically compatible COUNTER: A general designation applied with the data. For a 95% confidence to radiation detection instruments or survey interval, there is a 95% chance that the meters that detect and measure radiation. interval contains the parameter. The signal that indicates an ionization event has been detected is called a count. CONTAMINATION, RADIOACTIVE: Unwanted deposition of radioactive COUNTER, SCINTILLATION: Scintillation material in or on any medium or surface.
Recommended publications
  • Dead Time and Count Loss Determination for Radiation Detection Systems in High Count Rate Applications
    Scholars' Mine Doctoral Dissertations Student Theses and Dissertations Spring 2010 Dead time and count loss determination for radiation detection systems in high count rate applications Amol Patil Follow this and additional works at: https://scholarsmine.mst.edu/doctoral_dissertations Part of the Nuclear Engineering Commons Department: Nuclear Engineering and Radiation Science Recommended Citation Patil, Amol, "Dead time and count loss determination for radiation detection systems in high count rate applications" (2010). Doctoral Dissertations. 2148. https://scholarsmine.mst.edu/doctoral_dissertations/2148 This thesis is brought to you by Scholars' Mine, a service of the Missouri S&T Library and Learning Resources. This work is protected by U. S. Copyright Law. Unauthorized use including reproduction for redistribution requires the permission of the copyright holder. For more information, please contact [email protected]. DEAD TIME AND COUNT LOSS DETERMINATION FOR RADIATION DETECTION SYSTEMS IN HIGH COUNT RATE APPLICATIONS by AMOL PATIL A DISSERTATION Presented to the Faculty of the Graduate School of the MISSOURI UNIVERSITY OF SCIENCE AND TECHNOLOGY In Partial Fulfillment of the Requirements for the Degree DOCTOR OF PHILOSOPHY in NUCLEAR ENGINEERING 2010 Approved by Shoaib Usman, Advisor Arvind Kumar Gary E. Mueller Carlos H. Castano Bijaya J. Shrestha © 2010 AMOL PATIL All Rights Reserved iii PUBLICATION DISSERTATION OPTION This dissertation consists of the following two articles that have been, or will be submitted for publication as follows: Pages 4-40 are intended for submission to Journal of Radioanalytical and Nuclear Chemistry. Pages 41-62 have been published in Nuclear Technologies journal (February, 2009). iv ABSTRACT This research is focused on dead time and the subsequent count loss estimation in radiation detection systems.
    [Show full text]
  • How Do Radioactive Materials Move Through the Environment to People?
    5. How Do Radioactive Materials Move Through the Environment to People? aturally occurring radioactive materials Radionuclides can be removed from the air in Nare present in our environment and in several ways. Particles settle out of the our bodies. We are, therefore, continuously atmosphere if air currents cannot keep them exposed to radiation from radioactive atoms suspended. Rain or snow can also remove (radionuclides). Radionuclides released to them. the environment as a result of human When these particles are removed from the activities add to that exposure. atmosphere, they may land in water, on soil, or Radiation is energy emitted when a on the surfaces of living and non-living things. radionuclide decays. It can affect living tissue The particles may return to the atmosphere by only when the energy is absorbed in that resuspension, which occurs when wind or tissue. Radionuclides can be hazardous to some other natural or human activity living tissue when they are inside an organism generates clouds of dust containing radionu- where radiation released can be immediately clides. absorbed. They may also be hazardous when they are outside of the organism but close ➤ Water enough for some radiation to be absorbed by Radionuclides can come into contact with the tissue. water in several ways. They may be deposited Radionuclides move through the environ- from the air (as described above). They may ment and into the body through many also be released to the water from the ground different pathways. Understanding these through erosion, seepage, or human activities pathways makes it possible to take actions to such as mining or release of radioactive block or avoid exposure to radiation.
    [Show full text]
  • Radionuclides (Including Radon, Radium and Uranium)
    Radionuclides (including Radon, Radium and Uranium) Hazard Summary Uranium, radium, and radon are naturally occurring radionuclides found in the environment. No information is available on the acute (short-term) noncancer effects of the radionuclides in humans. Animal studies have reported inflammatory reactions in the nasal passages and kidney damage from acute inhalation exposure to uranium. Chronic (long-term) inhalation exposure to uranium and radon in humans has been linked to respiratory effects, such as chronic lung disease, while radium exposure has resulted in acute leukopenia, anemia, necrosis of the jaw, and other effects. Cancer is the major effect of concern from the radionuclides. Radium, via oral exposure, is known to cause bone, head, and nasal passage tumors in humans, and radon, via inhalation exposure, causes lung cancer in humans. Uranium may cause lung cancer and tumors of the lymphatic and hematopoietic tissues. EPA has not classified uranium, radon or radium for carcinogenicity. Please Note: The main sources of information for this fact sheet are EPA's Integrated Risk Information System (IRIS) (5), which contains information on oral chronic toxicity and the RfD for uranium, and the Agency for Toxic Substances and Disease Registry's (ATSDR's) Toxicological Profiles for Uranium, Radium, and Radon. (1) Uses Uranium is used in nuclear power plants and nuclear weapons. Very small amounts are used in photography for toning, in the leather and wood industries for stains and dyes, and in the silk and wood industries. (2) Radium is used as a radiation source for treating neoplastic diseases, as a radon source, in radiography of metals, and as a neutron source for research.
    [Show full text]
  • 6.2.43A Radiation-Dominated Model of the Universe
    6 BIG BANG COSMOLOGY – THE EVOLVING UNIVERSE 6.2.43A radiation-dominated model of the Universe R We have just seen that in the early Universe, the dominant energy density is that due to the radiation within the Universe. The Friedmann equation that was described in Chapter 5 (Box 5.4) can be solved for such conditions and the way in which the scale factor varies with time for such a model is shown in Figure 6.7. One important feature of such a model is that the scale factor varies in the following way: R(t) ∝ t1/2 (6.17) 0 t −4 Because the energy density of radiation is dominant for times when R(t)/R(t0) < 10 , all cosmological models which start at t = 0 with R(0) = 0, will go through a phase Figure 6.73The evolution of the that is well described by this radiation-dominated model. Thus we are in the rather scale factor with time in a remarkable position that regardless of which type of cosmological model best cosmological model in which the dominant contribution to the describes the Universe at the present, we can be reasonably confident that we energy density arises from the know how the scale factor varied with time in the first few tens of thousands of radiation within the Universe years of the big bang. (i.e. during the radiation-dominated However, the temperature of the background radiation varies with scale factor era). according to T(t) ∝ 1/R(t) (Equation 6.6). It follows that during the radiation- dominated era the temperature of the background radiation varies with time according to T(t) ∝ t −1/2 (6.18) This describes how temperature changes with time in an expanding universe where the energy density of radiation is the dominant component.
    [Show full text]
  • PE1128 Radiation Exposure in Medical Imaging
    Radiation Exposure in Medical Imaging This handout answers questions about radiation exposure and what Seattle Children’s Hospital is doing to keep your child safe. Medical imaging uses machines and techniques to provide valuable information about your child’s health. It plays an important role in helping your doctor make the correct diagnosis. Some of these machines use radiation to get these images. We are all exposed to small amounts of radiation in normal daily life from soil, rocks, air, water and even some of the foods we eat. This is called background radiation. The amount of background radiation that you are exposed to depends on where you live and varies throughout the country. The average person in the United States receives about 3 milli-Sieverts (mSv) per year from background radiation. A mSv is a unit of measurement for radiation, like an inch is a unit of length. Which medical MRI and ultrasound do not use ionizing (high-energy) radiation to make imaging exams images. MRI uses magnets and radio waves, and ultrasound uses sound waves. use radiation? Diagnostic An X-ray is a form of energy that can pass through your child’s bones and Radiography tissues to create an image. The image created is called a radiograph, sometimes referred to as an “X-ray.” X-rays are used to detect and diagnose conditions in the body. CT scan A CT (computed tomography) scan, sometimes called a “CAT scan,” uses X-rays, special equipment, and computers to make pictures that provide a multidimensional view of a body part.
    [Show full text]
  • Optimization of a Gas Flow Proportional Counter for Alpha Decay
    Optimization of a gas flow proportional counter for alpha decay measurements Elena Ceballos Romero Master Thesis Institut f¨urKernphysik Mathematisch-Naturwissenschaftliche Fakult¨at Westf¨alische Wilhelms-Universit¨atM¨unster Prof. Dr. Alfons Khoukaz October 2012 III I am among those who think that science has great beauty. A scientist in his laboratory is not only a technician: he is also a child placed before natural phenomena which impress him like a fairy tale. We should not allow it to be believed that all scientific progress can be reduced to mechanisms, machines, gearings, even though such machinery has its own beauty. -Marie Curie A magdalena, por ponerme en este camino. A mis padres, por siempre acompa~narmeen ´el. IV V I certify that I have independently written this thesis and no other sources than the mentioned ones have been used. Referent: Prof. Dr. Alfons Khoukaz Correferent: Dr. Mar´ıaVilla Alfageme VI Contents 1. Introduction 1 2. Introduction to natural radiations 5 2.1. Radioactivity . .5 2.1.1. Decay laws . .5 2.1.2. Activity . .7 2.2. Decays . .7 2.2.1. Alpha decay . .7 2.2.2. Beta decay . .9 2.2.3. Gamma decay . 11 3. Theoretical background: Gas-filled detectors 13 3.1. General properties . 13 3.1.1. Number of ion pairs formed . 14 3.1.2. Behaviour of charged particles in gases . 14 3.1.3. Operational modes of gas detectors . 15 3.2. Proportional counters: gas multiplication effect . 17 3.3. Gas flow detectors . 18 4. Experimental set-up 21 4.1. Detector . 21 4.1.1.
    [Show full text]
  • General Terms for Radiation Studies: Dose Reconstruction Epidemiology Risk Assessment 1999
    General Terms for Radiation Studies: Dose Reconstruction Epidemiology Risk Assessment 1999 Absorbed dose (A measure of potential damage to tissue): The Bias In epidemiology, this term does not refer to an opinion or amount of energy deposited by ionizing radiation in a unit mass point of view. Bias is the result of some systematic flaw in the of tissue. Expressed in units of joule per kilogram (J/kg), which design of a study, the collection of data, or in the analysis of is given the special name Agray@ (Gy). The traditional unit of data. Bias is not a chance occurrence. absorbed dose is the rad (100 rad equal 1 Gy). Biological plausibility When study results are credible and Alpha particle (ionizing radiation): A particle emitted from the believable in terms of current scientific biological knowledge. nucleus of some radioactive atoms when they decay. An alpha Birth defect An abnormality of structure, function or body particle is essentially a helium atom nucleus. It generally carries metabolism present at birth that may result in a physical and (or) more energy than gamma or beta radiation, and deposits that mental disability or is fatal. energy very quickly while passing through tissue. Alpha particles cannot penetrate the outer, dead layer of skin. Cancer A collective term for malignant tumors. (See “tumor,” Therefore, they do not cause damage to living tissue when and “malignant”). outside the body. When inhaled or ingested, however, alpha particles are especially damaging because they transfer relatively Carcinogen An agent or substance that can cause cancer. large amounts of ionizing energy to living cells.
    [Show full text]
  • What Is Electromagnetic Radiation?
    WHATHAT ISIS ELELECTRT R OMAGNETICOMAGNETIC RADIAADIATITIONON? MEET A PLANETARY SCIENTIST — Dr. Carlé Pieters, Brown University How are radio waves, visible light, and X-rays similar? They are all types of electromagnetic radiation. All three travel — radiate — What do you do? and are made or detected by electronic (or magnetic) sensors, like a T.V., a digital camera, or a dentist’s X-ray machine. Types of electromagnetic radiation with which we are most familiar include ultraviolet light (causing sunburn), infrared light (in remote controls), and microwaves (in ovens). Electromagnetic radiation is made of electromagnetic waves. It is classified by the distance from the crest of one wave to the crest of the next — the wavelength. These waves can be thousands of miles long, like radiowaves, or smaller than an atom, like gamma rays! Collectively, these wavelengths make a spectrum — the electromagnetic spectrum. The shorter the wavelength, the more energetic the electromagnetic radiation. Radio waves, including microwaves, have long wavelengths and relatively low energy levels. Visible light, ultraviolet rays, X-rays, and gamma rays have shorter wavelengths and correspondingly higher levels of energy. The wavelengths of ultraviolet light, X-rays, and gamma rays are short enough to interact with human tissue and even alter DNA. What have you investigated on the Moon? Radiation Cosmic and Ultraviolet Visible Infrared Type X-Rays Microwaves and Radio Waves Gamma Rays Light Light Light 0.01 10 400 700 1 million nanometers nanometers nanometers nanometers nanometers Relative Why should we return to the Moon? Size tip of atomic atom molecule bacterium butterflyastronaut buildings nucleus a pin (you!) WHATHAT ISIS REFLECTANCEEFLECTANCE SPECPECTRTROSCOPYOSCOPY? If someone wants to become a scientist, what should they do? Spectroscopy is the study of the electromagnetic radiation emitted, absorbed, or reflected by an object.
    [Show full text]
  • Radiation Glossary
    Radiation Glossary Activity The rate of disintegration (transformation) or decay of radioactive material. The units of activity are Curie (Ci) and the Becquerel (Bq). Agreement State Any state with which the U.S. Nuclear Regulatory Commission has entered into an effective agreement under subsection 274b. of the Atomic Energy Act of 1954, as amended. Under the agreement, the state regulates the use of by-product, source, and small quantities of special nuclear material within said state. Airborne Radioactive Material Radioactive material dispersed in the air in the form of dusts, fumes, particulates, mists, vapors, or gases. ALARA Acronym for "As Low As Reasonably Achievable". Making every reasonable effort to maintain exposures to ionizing radiation as far below the dose limits as practical, consistent with the purpose for which the licensed activity is undertaken. It takes into account the state of technology, the economics of improvements in relation to state of technology, the economics of improvements in relation to benefits to the public health and safety, societal and socioeconomic considerations, and in relation to utilization of radioactive materials and licensed materials in the public interest. Alpha Particle A positively charged particle ejected spontaneously from the nuclei of some radioactive elements. It is identical to a helium nucleus, with a mass number of 4 and a charge of +2. Annual Limit on Intake (ALI) Annual intake of a given radionuclide by "Reference Man" which would result in either a committed effective dose equivalent of 5 rems or a committed dose equivalent of 50 rems to an organ or tissue. Attenuation The process by which radiation is reduced in intensity when passing through some material.
    [Show full text]
  • UV Radiation (PDF)
    United States Air and Radiation EPA 430-F-10-025 Environmental Protection 6205J June 2010 Agency www.epa.gov/ozone/strathome.html UV Radiation This fact sheet explains the types of ultraviolet radiation and the various factors that can affect the levels reaching the Earth’s surface. The sun emits energy over a broad spectrum of wavelengths: visible light that you see, infrared radiation that you feel as heat, and ultraviolet (UV) radiation that you can’t see or feel. UV radiation has a shorter wavelength and higher energy than visible light. It affects human health both positively and negatively. Short exposure to UVB radiation generates vitamin D, but can also lead to sunburn depending on an individual’s skin type. Fortunately for life on Earth, our atmosphere’s stratospheric ozone layer shields us from most UV radiation. What does get through the ozone layer, however, can cause the following problems, particularly for people who spend unprotected time outdoors: ● Skin cancer ● Suppression of the immune system ● Cataracts ● Premature aging of the skin Did You Since the benefits of sunlight cannot be separated from its damaging effects, it is important to understand the risks of overexposure, and take simple precautions to protect yourself. Know? Types of UV Radiation Ultraviolet (UV) radiation, from the Scientists classify UV radiation into three types or bands—UVA, UVB, and UVC. The ozone sun and from layer absorbs some, but not all, of these types of UV radiation: ● tanning beds, is UVA: Wavelength: 320-400 nm. Not absorbed by the ozone layer. classified as a ● UVB: Wavelength: 290-320 nm.
    [Show full text]
  • Radiation Fields Using a Tepc*
    XA00XC014 EUROPEAN LABORATORY FOR PARTICLE PHYSICS CERN/TIS-RP/95-14/CF A STUDY OF BUILD-UP EFFECTS IN HIGH-ENERGY RADIATION FIELDS USING A TEPC* M. Hofert1), A. Aroua2), A. V. Sannikov3) and G. R. Stevenson1) !) CERN, European Laboratory for Particle Physics, CH 1211 Geneva 23, Switzerland 2) IAR, Institute for Applied Radiophysics, CH 1015 Lausanne, Switzerland 3) IHEP, Institute for High-Energy Physics, RU 142284 Protvino, Russia * Supported by EU Research Contract FI3P-CT92-0026 Abstract A dose of 2 mSv close to the body surface of a pregnant woman is considered by ICRP to assure a dose limit of 1 mSv to the foetus. Such an assumption depends on the energy spectrum and composition of the external radiation field and it was tested in radiation fields containing high-energy particles similar to those found around high-energy particle accelerators and in air-craft. Measurements of dose and dose equivalent were performed as a function of wall thickness using a tissue-equivalent proportional counter (TEPC) in radiation fields at the CERN-EU Reference Radiation Facility. Results are presented both with respect to integral quantities and event size spectra. The decrease in dose and dose equivalent at a depth equivalent to that of the foetus was typically 10% in a high-energy stray radiation field and in the case of Pu- Be source neutrons amounted to only 30%. It is concluded that it would be prudent under such exposure conditions to limit the dose of a pregnant woman to 1 mSv in order to assure that the dose to the foetus remains below the same limit.
    [Show full text]
  • Gamma-Ray Interactions with Matter
    2 Gamma-Ray Interactions with Matter G. Nelson and D. ReWy 2.1 INTRODUCTION A knowledge of gamma-ray interactions is important to the nondestructive assayist in order to understand gamma-ray detection and attenuation. A gamma ray must interact with a detector in order to be “seen.” Although the major isotopes of uranium and plutonium emit gamma rays at fixed energies and rates, the gamma-ray intensity measured outside a sample is always attenuated because of gamma-ray interactions with the sample. This attenuation must be carefully considered when using gamma-ray NDA instruments. This chapter discusses the exponential attenuation of gamma rays in bulk mater- ials and describes the major gamma-ray interactions, gamma-ray shielding, filtering, and collimation. The treatment given here is necessarily brief. For a more detailed discussion, see Refs. 1 and 2. 2.2 EXPONENTIAL A~ATION Gamma rays were first identified in 1900 by Becquerel and VMard as a component of the radiation from uranium and radium that had much higher penetrability than alpha and beta particles. In 1909, Soddy and Russell found that gamma-ray attenuation followed an exponential law and that the ratio of the attenuation coefficient to the density of the attenuating material was nearly constant for all materials. 2.2.1 The Fundamental Law of Gamma-Ray Attenuation Figure 2.1 illustrates a simple attenuation experiment. When gamma radiation of intensity IO is incident on an absorber of thickness L, the emerging intensity (I) transmitted by the absorber is given by the exponential expression (2-i) 27 28 G.
    [Show full text]