Streaming Video | Ipod-friendly Download

Back to Notes

6.1.3.       Nuclear Theory & Radioactivity           <CJ chap 31  >

6.1.3.1. Discussion  ( sf )

6.1.3.1.1.     Nucleons are protons or neutrons – the particles that make up the nucleus of the atom

6.1.3.1.1.1. The neutron was discovered in 1932 by Chadwick with a mass slightly larger than the proton

6.1.3.1.1.2. The atomic number, Z =the number of protons, and A the mass number = the number of nucleons

6.1.3.1.1.2.1.     A nucleus is written as dsf where X is the chemical element corresponding to Z

6.1.3.1.1.2.2.     Isotopes are nuclei with the same number of protons but differing numbers of neutrons

6.1.3.1.1.2.3.     The nuclear forces felt by both the p and n are essentially identical

6.1.3.1.1.2.4.     The binding energy is the amount of energy needed to separate the nucleons

6.1.3.1.1.2.5.     The mass defect is the binding energy expressed in mass equivalence via E = mc2

6.1.3.1.1.2.6.     The binding energy per nucleon is greatest in mid-range of A (Fe) and less in Li and U

6.1.3.1.1.3. Nuclear reactions:

6.1.3.1.1.3.1.     Rutherford (1919) observed the first ‘transmutation of an element’ with a + N -> O + H

6.1.3.1.1.4. Radioactivity is the decay or disintegration of an unstable nucleus 

6.1.3.1.1.4.1.     a decay: The emission of an alpha particle or He nucleus (2p+2n) – easy to stop

6.1.3.1.1.4.1.1. Example of a decay     dfs  -> dfs  + dsf   + 4.3 MeV of energy

6.1.3.1.1.4.2.     b decay: The emission of an electron (or positron) via n -> p + e- + dsf - not hard to stop

6.1.3.1.1.4.2.1. Example of b decay     dsf  -> dsf  + dsf   

6.1.3.1.1.4.3.      

6.1.3.1.1.4.4.     g decay: The emission of a high energy photon releasing energy – needs lead to stop

6.1.3.1.1.4.5.     n decay: The emission of a neutron directly from the nucleus

6.1.3.1.1.4.6.     Half-life is the time required for half of a substance to undergo disintegration

6.1.3.1.1.4.7.     Radioactive dating: Carbon 14 has a half life of 5730 years

6.1.3.1.1.4.8.     The Becquerel (Bq) is the unit of radioactivity = 1 disintegration per sec

6.1.3.1.1.4.8.1. The Currie (Ci) is another unit of activity: 1 Ci = 3.70E10 Bq = 1 gr of pure radium

6.1.3.1.1.5. Biological Effects of Radiation

6.1.3.1.1.5.1.     Ionizing radiation (charges particles or g)  knocks electrons from atoms & damages cells

6.1.3.1.1.5.1.1. The SI unit of ionizing radiation is the Coulomb per kg or C/kg

6.1.3.1.1.5.1.2. The Roentgen (R) = 2.58E-4 C/kg is a more common historical unit

6.1.3.1.1.5.2.     Yet this measures only the ionization effect and not the effect on tissue for which we use:

6.1.3.1.1.5.2.1. Absorbed Dose = (Energy absorbed) / (Mass absorbing) unit = Grey (Gy)=J/kg

6.1.3.1.1.5.2.2. Radiation Absorbed Dose (RAD) = 0.01 Gy  is another common unit

6.1.3.1.1.5.3.     To compare the damage of absorbing different kinds of radiation we define:

6.1.3.1.1.5.3.1. Relative Biological Effectiveness (RBE) = (Dose of 200KeV X-rays Effect) / (Dose )

6.1.3.1.1.5.3.2. Then Biologically Equivalent Dose (rems) = Absorbed Dose (in rads) x RBE

6.1.3.1.1.5.3.2.1.     rem stands for roentgen equivalent man

6.1.3.1.1.5.3.2.2.     Humans receive an average dose of 360 mrem/yr from all sources

6.1.3.1.1.5.3.2.3.     (cosmic rays 28, earth 28, internal 39, Radon 200, Medical/dental 43,..

6.1.3.1.1.5.3.2.4.     The general population should not get more than 500 mrem / yr

6.1.3.1.1.5.3.2.5.     Workers should not get more than 5 rem / year (eg dental assistant) 

6.1.3.2. Mathematical

6.1.3.2.1.     The approximate radius of the nucleus is  r = 1.2E-15 A 1/3 

6.1.3.2.2.     Radioactive disintegration obeys N = N­0 e-lt  thus N/N­0 =1/2  =  e-lT1/2  

6.1.3.2.3.     Taking ln of both sides we get  ln ½ = ln (-lT1/2  ) thus T1/2  = ln2/ l thus relating  l to T1/2  

6.1.3.3. Advanced

6.1.3.3.1.     Radioactive decay obeys:  dN(t) = -l N0 dt with the solution: N = N­0 e-lt