Chapter 2. Radiation 1.Radioactivity 2.Radiation interaction with Matter 3.Radiation Doses and hazard Assessment 2.1 Radioactivity 1) 2) 3) 4) 5) 6) Overview Types of Radioactive Decay Energetics of Radioactive Decay Characteristics of Radioactive Decay Decay Dynamics Naturally Occurring Radionuclides 1) Overview Radioactive Decays transmutations of nuclides Radioactivity means the emission of alpha () particles, beta () particles, or gamma photons () etc. from atomic nuclei. The term radioactivity was actually coined by Marie Curie Radioactive decay is a process by which the nuclei of a nuclide emit , or rays etc. In the radioactive process, the nuclide undergoes a transmutation, converting to another nuclide. 3 Conservation of charge Conservation of the number of nucleons Conservation of mass/energy (total energy) Conservation of linear momentum Conservation of angular momentum 2) Types of Radioactive Decay Apparatus similar to that used by Henri Becquerel to determine the magnetic deflection of radioactive decay products. The magnetic field is perpendicular to the direction of motion of the decay products. Radioactivity in Nature 222Rn is responsible for higher levels of background radiation in many parts of the world. Radon The uranium decay series. because it is a gas and can easily seep out of the earth into unfinished basements and then into the house 3) Energetics of Radioactive Decay The law of conservation of mass and energy covers all reactions. Sum of mass before reaction = Sum of mass after reaction + Q Q = Sum of mass before reaction - Sum of mass after reaction Energy in Radioactive Decay Interesting Items: Before decay Spectrum(能谱) of particles Energy in gamma decay Energy in beta decay Energy in alpha decay Recoiling nucleus a) Gamma Decay Energy Gamma, , rays are electromagnetic radiation emitted from atomic nuclei. The bundles of energy emitted are called photons. Excited nuclei are called isomers, and de-excitation is called isomeric transition (IT). Energy for photons hv=Ei-Ef Ei ____________ hv Ef ____________ Eothers _________ Nature of Gamma Transitions Types of Isomeric Transitions and their Ranges of Half-life Radiation Type Symbol J Partial half life t (s) Electric dipole Magnetic dipole Electric quadrupole Magnetic quadrupole Electric octupole Magnetic octupole Electric 24-pole Magnetic 24-pole 1 1 2 2 3 3 4 4 Yes No No Yes Yes No No Yes 5.7e-15 E–3 A–2/3 2.2e-14 E–3 6.7e-9 E–5 A–4/3 2.6e-8 E–5 A–2/3 1.2e-2 E–7 A–2 4.9e-2 E–7 A–4/3 3.4e4 E–9 A–8/3 1.3e5 E–9 A–2 E1 M1 E2 M2 E3 M3 E4 M4 Gamma Decay Energy and Spectrum Gamma transition of 7Li Various Gamma Transitions in 7Li ½+ 6.54 MeV M3 E3 M1 E1 M2 7/2+ 4.64 MeV ½ – 0.778 MeV 3/2– ground state a) Gamma Ray Spectrum of O18 2h+ Intensity 3.27 MeV 1.98 MeV 1.98 2+ 0+ 3.27 MeV 5.25 MeV E Intensities of the peaks are related to the population of the excited state as well as the half life of the transition. b) How is alpha energy evaluated and determined? What is a typical alpha spectrum An Ideal Alpha Spectrum and why? No. of MeV 8 10 211Po particle energy: | 98.9% 10.02 MeV | 0.5% 9.45 0.5% 8.55 Expeimentally? 207Pb | 7/ + 2 5/ + 2 1/ + 2 | | | – 0.5% 0.57 MeV – 0.5% 14 – 98.9% 0.90 MeV What is the initial kinetic energy of the alpha particle produced in the radioactive decay: The Qα value in mass units c) Beta Decay Spectra and Neutrino A Beta Decay Scheme P D Z Z+1 A Typical Beta Spectrum + +v – Intensity or # of ? E max Energy of Pauli: Neutrino with spin 1/2 is emitted simultaneously with beta, carrying the missing energy. 16 c) The mass of the neutrino is negligibly small. d) Positron Decay Energy Positron Emission – + 18 2.1 Radioactivity 1) 2) 3) 4) 5) 6) Overview Types of Radioactive Decay Energetics of Radioactive Decay Characteristics of Radioactive Decay Decay Dynamics Naturally Occurring Radionuclides 4) Characteristics of Radioactive Decay 137mBa decay data, activity or decay rate A decay constant Radioactivity or decay rate A is the rate of disintegration of nuclei. Initially (at t = 0), we have No nuclei, and at time t, we have N nuclei. This rate is proportional to N, and the proportional constant is called decay constant . the number of decays or transmutations per unit of time dN A = – ––––– = N dt ln N = ln No – t Integration gives Also A = Ao e – t or Stochastic process N = No e – t specific activity normalized to the mass or volume of the sample Many safety limits and regulations are based on the specific activity concept Radioactive Decay Kinetics -exponential Variation of N as a function of time t No N N = No e Also A = Ao e - t - t t Number of radioactive nuclei decrease exponentially with time as indicated by the graph here. As a result, the radioactivity vary in the same manner. Note N =A No = Ao Radioactive Decays 23 Condition? Half-life and its measurement Variation of N as a function of time t Ln(N or A) No N N = No e - t Also A = Ao e - t ln N1 – ln N2 = ––––––––––– t1 – t2 t t½ * = ln 2 Be able to apply these equations! N = No e– t A = Ao e – t Half life is not affected by chemical and physical state of matter. t ln N = ln No – t ln A = ln Ao – t Determine half life, 24 t½ Decay Probability for a Finite Time Interval does not decay does decay As the time interval becomes very small, i.e., t —>Δt « 1, p(t)dt, probability a radionuclide, which exists at time t = 0, decays in the time interval between t and t + dt the probability distribution function for when a radionuclide decays. Decay by competing Processes Ln A t λ is the overall decay constant The probability fi that the nuclide will decay by the ith mode is What is the probability 64Cu decays by positron Emission? The decay constants for the three decay modes of this radioisotope are λ β+ = 0.009497 h-1, λ β- = 0.02129 h-1, and λ EC = 0.02380 h-1. The overall decay constant is The probability that an atom of 64Cu eventually decays by positron emission is 2.1 Radioactivity 1) 2) 3) 4) 5) 6) Overview Types of Radioactive Decay Energetics of Radioactive Decay Characteristics of Radioactive Decay Decay Dynamics Naturally Occurring Radionuclides a) Decay with Production Q(t) is the rate at which the radionuclide of interest is being created the special case that Q(t) = Q0 (a constant production rate) N(t) -> Ne = Q0/λ t -> the equilibrium condition b) Three Component Decay Chains Daughter Decays Faster than the Parent λI < λ2, transient equilibrium: daughter's decay rate is limited by the decay rate of the parent. λI << λ2, The activity of the daughter approaches that of the parent. This extreme case is known as secular equilibrium(久期平衡). 6.1 Cosmogenic Radionuclides The most prominent of the cosmogenic radionuclides are tritium 3H and 14C. 14N(n,T)12C and 16O(n,T)14N 14N(n,p)14C 6.2 Singly Occurring Primordial (原生)Radionuclides The solar system was formed about 5 billion years ago. These radionuclides are seen to all have half-lives greater than the age of the solar system. Of these radionuclides, the most significant are 40K and 87Rb since they are inherently part of our body tissue. Families of Radioactive Decay Series Radioactive Decay Series of 238U 238U92 234Th90 + 42 234Th90 234Pa91 234Pa91 (t1/2 4.5e9 y) + – + (t1/2 24.1 d) 234U92 + – + 234U92 (t1/2 6.7 h) . . . (continue) . . . Only alpha decay changes the mass number by 4. 206Pb82 There are 4 families of decay series. 4n, 4n+1, 4n+2, 4n+3, Each naturally occurring radioactive n being an integer. nuclide with Z > 83 is a member of one of three long decay chains, Radioactivity - 238U radioactive decay series The Decay Path of 4n + 2 or 238U Family 234 230 226 222 218 210 Po 210 206 Pb 206 Tl 206 214 Bi 210 Hg Po 214 Pb Bi 214 210 Tl Pb At 218 Po Rn U 238 234 Pa 234 Th Th Ra decay Major route Minor route decay U Radioactivity - 239Np radioactive decay series The Decay Paths of the 4n + 1 or 237Np93 Family Series 233 (1.6e5 y) 229 221 213 209 Bi83 209 Po84 Pb82 209 Np93 (2e6 y) 233 Pa91 Th90 (7300 y; minor path) 225 (10 d) Ac89 U92 237 225 Fr87 217 At85 (1 min) 213 83 Bi Ra88 81 Tl Radioactive Decays 36 2.1 Radioactivity 1) 2) 3) 4) 5) 6) Overview Types of Radioactive Decay Energetics of Radioactive Decay Characteristics of Radioactive Decay Decay Dynamics Naturally Occurring Radionuclides