Intro to Radiation. Atom structure Types of radiation Properties of ionizing radiation Detection methods Dose reduction methods

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Radiation and Life Intro to Radiation Atom structure Types of radiation Properties of ionizing radiation Detection methods Dose reduction methods 1 Atom structure 2 Understanding Radiation Types of Ionizing Radiation 1. Alpha Radiation 2. Beta Radiation 3. Photon Radiation a. X-Ray Radiation b. Gamma Radiation 4. Neutron Radiation 1. Alpha Radiation, α A form of ionizing radiation that consists of 2 neutrons and 2 protons ejected from an atomic nucleus, or the nucleus of a Helium atom. Alphas therefore have large mass & charge, and as a result of this, alpha radiation is not very penetrating. Alphas are generally emitted during the decay of heavy naturally occurring radioisotopes such as uranium and radium (because of this, they are the major source of background radiation in the form of radon gas more on this later). 222 226 Radon-222, 86 Rn Radium-226, 88 Ra Decay to Daughter Emission of α Particle 4 α Particle, 2He + + 3 1

Understanding Radiation Types of Ionizing Radiation 2. Beta Radiation, β There are two forms of Beta Radiation, Beta Minus Decay and Beta Plus Decay. Beta Minus consists of high energy, high speed electrons that are emitted by certain radioactive nuclei, while Beta Plus emits positrons. Beta Minus Stems from an unstable nucleus with excess neutrons that undergoes decay in which a neutron is converted to a proton that stays in the nucleus, and an electron and an antineutrino which are emitted. neutron proton electron antineutrino β - Decay: 14 14 Nitrogen-14, Carbon-14, 7 6N C n+ Antineutrino ν - Electron 4 Understanding Radiation 2. Beta Radiation, β Types of Ionizing Radiation Beta Plus Also called Positron Decay, stems from an unstable nucleus with excess protons that undergoes decay in which a proton is converted to a neutron that stays in the nucleus, and a positron and a neutrino which are emitted. proton neutron positron neutrino β + Decay: 10 10 Carbon-10, Boron-10, 56B C Neutrino ν + n + Positron 5 Understanding Radiation Types of Ionizing Radiation 3. Photon Radiation There are two forms of Photon Radiation (emitted energy), X-Ray Radiation and Gamma Radiation. The two types of radiation are distinguished by their origin, with X-rays emitted by electrons outside the nucleus, and gamma rays emitted by the nucleus. Each is created by multiple means, however, only one method produces only gamma rays gamma decay. γ Decay: Gamma rays from radioactive gamma decay are produced when a nucleus emits an α or β particle and the daughter nucleus (or progeny the result of the reaction) is usually left in an excited state. In this case, the nucleus moves to a lower energy state by emitting a gamma ray. Emission of a gamma ray from an excited nuclear state typically requires only 10 12 seconds, and is thus nearly instantaneous. Gamma decay from excited states may also happen rapidly following certain nuclear reactions such as nuclear fission or nuclear fusion. Gamma decay is typically depicted by a Decay Scheme as seen below for Cobalt-60 to Nickel-60. Co 60 27 0.31 MeV β - (99.88%) 1.48 MeV β - (0.12%) 1.1732 MeV γ 60 28 1.3325 MeV γ Ni 99.88% of the time β - decay occurs in which 0.31 MeV of energy This is method emitted of depicting from the the excited decay Co-60 methods nucleus 0.12% that of take the place time is β Directly following this, - known decay as occurs a Decay in which Scheme, 1.48 MeV of a 1.1732 MeV γ-ray is emitted energy whereby is emitted the arrows from indicate the excited emitted Co-60 particles nucleus of type noted in the diagram. This allows for visual Lastly, representation a 1.3325 MeV of complex γ-ray is decay emitted reactions. bringing the nucleus to an electrically stable state as Nickel-60 6 2

Understanding Radiation Types of Ionizing Radiation 3. Photon Radiation Continued Characteristic X-Rays: As specified previously there are multiple manners for producing x-rays, however, we will focus on one direct method similar to gamma decay for gamma ray emission: Characteristic X-Rays. In order to emit a characteristic x-ray, a high energy electron interacts with a bound electron in an atom ejecting it. The incident electron is scattered and the target electron is displaced from its shell. (In order to do this, the energy of the incident electron must exceed the binding energy of the target electron.) Once ejected the atom is left with a vacant energy level. This vacancy is then filled by an electron from a higher energy level within the atom emitting a characteristic x-ray photon. This x-ray photon in characteristic in that it has an energy that corresponds exactly to the difference in energy between the energy level that is vacant and the energy level from which an electron falls and is characteristic of the atom that had the vacancy and can therefore be used to identify the atom. Scattered Target e - Incident e - Target e - X-Ray Scattered Incident e - 7 Understanding Radiation 3. Photon Radiation Continued Types of Ionizing Radiation Some other important methods for producing photon radiation gamma and x-rays, include but are not limited to: Compton Scattering Photoelectric Effect Pair Production Bremsstrahlung Etc. 8 Understanding Radiation 4. Neutron Radiation Types of Ionizing Radiation Neutron radiation is a kind of ionizing radiation that consists of free neutrons. These Neutrons may be emitted from nuclear fusion or nuclear fission reactions as well as from any number of different nuclear reactions such as radioactive decay or particle interactions from particle accelerators, etc. Neutron radiation consists of the release of free neutrons from both stable molecules and isotopes. Once emitted, these free neutrons can then continue to react with nuclei of other stable molecules to form new isotopes of previously non-isotopic molecules, resulting in a chain reaction of nuclear radiation production. Neutron Reaction (n,α) Neutron becomes Alpha Particle + + 1 10 0 n 5 B 7 3 Li 4 α, ( He) 2 9 3

Alpha Hazards Made of Two protons and two neutrons Very large radiation therefore it is generally the least penetrating form of ionizing radiation Alpha particles can t penetrate the dead skin layer They are typically only an internal exposure hazard 10 Beta Hazards At least 70 KeV to penetrate the dead skin layer Average Beta energy is 1/3 of the max energy Range in air is about 12ft /MeV Can cause localized Skin exposures (hot particles) Can create Bremstrahllung radiation if shielded with high Z material 11 Gamma Hazards Travels at the speed of light (also called a photon) X-rays and gamma radiation are both photons Gammas originate in the nucleus X-rays originate from the energy transition of orbital electrons or as bremstrahlung (therefore they originate outside the nucleus) Very small radiation therefore it is generally the most penetrating form of ionizing radiation 12 4

Neutron Hazards Part of the atoms nucleus that is shed Neutral charge Interacts readily in hydrogenous materials Tissue is mostly hydrogen (by atomic abundance) 13 Radiation quantities and units Dose Dose equivalence Activity Rad, Grey Rem, Seiverts Curie, Becquerel 1Becquerel = 1 radioactive decay per second 1Curie = 3.7x10 10 decays per second 14 Half life (T ½) Time at which the radiation emitted from a source will be half of its initial radiation emitted Every isotope that emits radiation will have a half life Can range from microseconds to billions of years 15 5

100000 90000 Counting data over time 80000 70000 60000 Counts 50000 40000 30000 20000 10000 0 0 2 4 6 8 10 12 Time (minutes) 16 100000 90000 80000 70000 y = 100000e -0.3092x 60000 Counts 50000 40000 30000 20000 10000 0 0 2 4 6 8 10 12 Time (minutes) 17 100000 RUN Rise Counts 10000 y = 100000e -0.3092x Y intercept is 100000 Slope is rise/ run Rise / Run = 1 / -3.2 = -.3125 1000 0 2 4 6 8 10 12 Time (minutes) 18 6

Determine Half life from data A 0 e t Can equate to the exponential fit of the data 100000 e 0.3092 x Y intercept is the A 0 ln(2) 1 t 2 ln(2) 0.3092 1 t 2 t ln(2) 0.693 0.3092 0.3092 1 2 2.24min 19 Half life answers compared From data slope method T 1 / 2 = 2.21 min From data fit equation T 1 / 2 = 2.24 min Use the website to determine possible isotopes based on half life http://nucleardata.nuclear.lu.se/nucleardata/to i/perchart.htm 20 How do we detect radiation? Radiation detectors Geiger Mueller (GM) operates by collecting charge the of an ion pair (with gas multiplication) ionizing all the detector gas 21 7

How do we detect radiation? Scintillation counters operates by light production from radiation interaction in the detector and the photomultiplier or photodiode to convert the light to an electrical output 22 How do we detect radiation? Ion Chambers Large numbers of Charged particles interacting in the gas that creates a current that can be proportional to dose (dose to tissue if the detector wall material is the same Z as tissue) 23 How do we detect radiation? Proportional counters operates by gas multiplication to amplify charge from the original ion pair and measure low number of counts 24 8

How to keep doses As Low As Reasonably Achievable (ALARA) TIME- Decrease your time spent near a radiation source DISTANCE- Increase your distance from the radiation source SHIELDING- Increase shielding between yourself and the radiation source 25 TIME DOSE RATE: Dose in 60 min Dose in 30 min Dose in 15 min Dose in 1 min Dose in 1 sec 4000mrem/hr 4000 mrem 2000 mrem 1000 mrem 66 mrem 1 mrem 26 DOSE RATE: Dose rate @ 2m Dose rate @ 3m Dose rate @ 4m Dose rate @ 5m Dose rate @ 6m Distance 4000mrem/hr @1m DoseRate@1meter DoseRate@ x 2 x 1000 mrem/hr 444 mrem/hr 250 mrem/hr 160 mrem/hr 111 mrem/hr 27 9

Shielding 28 Sources of Radiation Exposures to the US population (NCRP 160) Dose Percent Source (mrem/year of total Background 311 50 Internal (inhalation of radon 228 37 and thoron) External (cosmic) 33 5 Computed Internal (ingestion) 29 5 Tomography Radon 21 & Thoron 3 24% External (terrestrial) 37% Medical 300 48 Nuclear Medicine 12% Computed tomography 147 24 Nuclear medicine 77 12 Other Background Fluoroscopy Fluoroscopy (Interventional) 43 7 13% (Interventional) Fluoroscopy and 7% 33 5 radiography (Conventional) Radiography, Fluoroscopy Consumer 13 2 Other (Conventional) 2% 5% Occupational 0.5 0.08 Industrial, security, medical 0.3 0.05 (education and research) TOTAL (6.2mSv) 620 29 Background Radiation Radon and Thoron Inhalation: 37% Background Radiation 30 10

Background Radiation Ingestion of Radionuclides: 5% Background Radiation Another source of background radiation is the ingestion of radionuclides found naturally in the foods that we eat. One of the most prominent sources of ingested radionulcides is Potassium-40 (K-40) found in numerous foods. However, nearly everything we eat has radionuclides as anything that comes from the ground naturally acquires these from the soil and similarly anything that survives from eating products from the soil acquires these as well. The concentration of the natural radioactivity in food is often in the range of 40 to 600 becquerel per kilogram of food. Examples of food products known to contain certain radionuclides can be seen below. The radioactivity from potassium alone may typically be 50 Bq/kg in 40K : milk, 420 Bq/kg in milk powder, 165 Bq/kg in potatoes, and 125 Bq/kg in beef. 31 Background Radiation Ingestion of Radionuclides: 5% Background Radiation Another source of background radiation is the ingestion of radionuclides found naturally in the foods that we eat. One of the most prominent sources of ingested radionulcides is Potassium-40 (K-40) found in numerous foods. However, nearly everything we eat has radionuclides as anything that comes from the ground naturally acquires these from the soil and similarly anything that survives from eating products from the soil acquires these as well. The concentration of the natural radioactivity in food is often in the range of 40 to 600 becquerel per kilogram of food. Examples of food products known to contain certain radionuclides can be seen below. Carbon-14 is present in the atmosphere, oceans, and all organic 14C : material. Carbon-14 occurs in the ratio of 6 picocuries (pci) of carbon-14 per gram of total carbon, and it is assimilated into tissues of all plants and animals. As such, Carbon-14 can be taken into the body by drinking water, eating food, or breathing air. Organics Water 32 Background Radiation Ingestion of Radionuclides: 5% Background Radiation Another source of background radiation is the ingestion of radionuclides found naturally in the foods that we eat. One of the most prominent sources of ingested radionulcides is Potassium-40 (K-40) found in numerous foods. However, nearly everything we eat has radionuclides as anything that comes from the ground naturally acquires these from the soil and similarly anything that survives from eating products from the soil acquires these as well. The concentration of the natural radioactivity in food is often in the range of 40 to 600 becquerel per kilogram of food. Examples of food products known to contain certain radionuclides can be seen below. 3 H : Hydrogen has three isotopes known as protium, H-1, with a single proton, deuterium, H-2, with one proton and one neutron and tritium, H-3, with one proton to two neutrons. The first of these are not radioactive, but tritium is with two neutrons that take it out of its stable state. Hydrogen s positive charge draws it to electrically negative polar Oxygen molecules to make water. However, in the case of tritium, heavy water is made due to the Hydrogen s extra neutron. Natural heavy water comprises less than 1% of water on earth and is made when cosmic rays interact with the atmosphere which is composed in part of Hydrogen. 33 11

Background Radiation Ingestion of Radionuclides: 5% Background Radiation Another source of background radiation is the ingestion of radionuclides found naturally in the foods that we eat. One of the most prominent sources of ingested radionulcides is Potassium-40 (K-40) found in numerous foods. However, nearly everything we eat has radionuclides as anything that comes from the ground naturally acquires these from the soil and similarly anything that survives from eating products from the soil acquires these as well. The concentration of the natural radioactivity in food is often in the range of 40 to 600 becquerel per kilogram of food. Examples of food products known to contain certain radionuclides can be seen below. 210 Po : Food ingestion also represents the major source of naturally occurring Po-210 intake at 77%, while 5% is taken in via water and 1% from the air. Additionally, 17% is added by cigarettes. Po-210 is a daughter of Pb-210 and enters the food chain via plant uptake from soil and water and particle deposition from the decay of Rn-222 in the atmosphere as we already learned about, with greater preference on the latter deposited during rainfall. Po-210 is mostly found in leafy vegetables and grains. 34 Background Radiation Ingestion of Radionuclides: 5% Background Radiation Another source of background radiation is the ingestion of radionuclides found naturally in the foods that we eat. One of the most prominent sources of ingested radionulcides is Potassium-40 (K-40) found in numerous foods. However, nearly everything we eat has radionuclides as anything that comes from the ground naturally acquires these from the soil and similarly anything that survives from eating products from the soil acquires these as well. The concentration of the natural radioactivity in food is often in the range of 40 to 600 becquerel per kilogram of food. Examples of food products known to contain certain radionuclides can be seen below. Similar to Po-210, Ra-226 is part of the Radium decay series and is released 226Ra : into the atmosphere and deposited in and on vegetation via soil and water uptake and precipitation. Radium is chemically similar to calcium and, when Ingested, a small fraction is transferred across the small intestine and most is deposited in bone, which contains 70-95% of the total ingested body radium. 35 Background Radiation Cosmic Radiation: 5% Background Radiation Another source of background radiation is Cosmic Radiation. This form of radiation is delivered via cosmic rays, or energetic charged subatomic particles that originate from outer space and produce secondary charged particles that can penetrate the Earth s atmosphere and surface. Most cosmic radiation is composed of familiar stable subatomic particles that normally occur on Earth, such as protons, atomic nuclei, or electrons and photons, as well as some positrons. Such radiation is primarily comprised of low energy photons that are remnants from the creation of the universe and from active stars, such as the Sun. This radiation is of more consequence at higher altitudes. Therefore, cosmic radiation has a heightened effect, delivering more dose when flying on a plane or living in the mountains versus at sea level. 36 12

Background Radiation Cosmic Radiation: 5% Background Radiation 37 Background Radiation Cosmic Radiation: 5% Background Radiation In flight there are two principal sources of natural radiation to consider: - Galactic Cosmic Rays (GCR) which are always present - Solar Energetic Particle (SEP), or Solar Cosmic Ray (SCR) events which occur sporadically Dose Equivalent Rate (mrem/h) Solar Minimum (10/86) Solar Maximum (7/89) 35 degrees Altitude 70 degrees 35 degrees 70 degrees North Latitude (x1000 ft) North Latitude North Latitude North Latitude 0 0. 401 0.412 0.374 0.38 10 1.99 2.07 1.73 1.81 20 9.85 11.4 8.75 9.53 30 32.5 40.6 28.5 32.4 40 67.8 90.2 58.8 69.9 50 97.1 138 83.6 103 60 111 171 94.9 123 70 114 192 96.8 133 80 112 206 94.4 138 GCR provides an inescapable radiation background which varies over the solar cycle of about 11 years. GCR are maximum when solar activity is minimum and vice-versa. The resulting dose equivalent at aircraft also varies quite strongly with altitude and latitude. The following table provides estimates of the radiation dose equivalent at the times of a recent solar minimum (10/86) and solar maximum (7/89) for representative high and low latitude (values obtained by use of the CARI-6 program developed by the Civil Aeromedical Institute of the Federal Aviation Administration). (NOAA.gov) 38 Background Radiation Terrestrial Radiation: 3% Background Radiation The last main source of background radiation is Terrestrial Radiation. This radiation arises as a result of naturally occurring radioactive materials in the Earth such as Uranium, Radium, Radon and Thoron, serving as a source of external exposure. 39 13

Background Radiation Summarization of Background Radiation 40 Risk Benefit Analysis Balance between the risk of use (exposure) and the benefit of its use RISK One is exposed to 800-1300mrem BENEFIT Allows for diagnosis and lifesaving of the patient 41 Risk in Perspective Health risk Days of life lost Smoking 1 pack of cigarettes a day 2370 20% overweight 985 Average US alcohol consumption 130 Home Accidents 95 Dose of 5000 mrem/hr 32 Dose of 500 mrem/hr 3 42 14

Medical uses of Radiation Xrays Observe broken bones contrast material for x-ray, Barium enema (not radioactive barium, angiogram for cardiology viewing) Mammogram to view breast tissue looking for tumors Computerized Tomography (CT) exam Xrays with computer processing to get 2-d slices of the body 43 Medical uses of Radiation Nuclear Medicine -Injecting or ingesting radioactive material short lived (biological or radioactive) material as Check organ function, blood flow, respiration PET (Positron emission tomography) scan Imaging 44 Medical uses of Radiation Radiation oncology Brachytherapy seed treatments of all kinds of cancer Linear accelerator and Intensity modulated Radiation therapy (high energy x-rays and electron beams) Gamma stereotactic surgery (gamma knife) for treatment of muscle issues (face tics), reduce tumors, blood vessel defects, epilepsy and Parkinson s disease. 45 15

Industrial uses of Radiation Power generation- use of fissionable material to heat water and spin a turbine generator that will produce power 46 Industrial uses of Radiation Industrial radiography- Iridium 192 to take images of welds, pipes, etc. Industrial Radiography 47 Industrial uses of Radiation Guaging devices- measure thickness of metals, determine content of an item (XRF)gamma and neutron emitters 48 16

Industrial uses of Radiation Well logging- gamma or neutron source sent in a well to determine viability for certain valuable mineral mining 49 Industrial uses of Radiation X-rays for security + inspection Dual energy x-ray image Z backscatter x-ray image http://www.as-e.com/popups/zback_animation_wmv.asp 50 Industrial uses of Radiation Food irradiation kills bacteria that cause food to rot quicker USDA Product Wheat 1963 Potatoes 1964 Seasonings 1983 Pork 1986 Fruit and 1986 vegetables Herbs + spices 1986 enzymes 1986 Papaya 1987 Poultry 1992 Red Meat 1999 Eggs 2000 Approved 51 17

Industrial uses of Radiation Sterilization- hospital equipment, mail potentially containing biological compounds 52 Industrial uses of Radiation Static eliminating devices (po-210 alpha) to ionize the air 53 Radiation Exposure per Activity Flight from NY to LA 2.5 mrem/trip Full Mouth X-Ray 9 mrem/scan Chest X-Ray 10 mrem/scan Ct Scan 800-1300 mrem/scan Radon Gas 200 mrem/yr Smoking 1300 mrem/yr 54 18

Radiation Exposure (non Rad workers) Medical personnel 70 mrem/yr Grand central station workers 120 mrem/yr Nuclear power plant 160 mrem/yr Airline flight crew 1000 mrem/yr 55 Household uses of Radiation Smoke detector (0.001 mrem/year NUREG 1717) Thoriated lenses (thorium impregnated) believed to capture light better Thorium lantern Old radium dial watches Fiesta ware dinnerware Old Glassware 56 19