Download presentation
Published byDominic Price Modified over 9 years ago
1
Chapter 1 Structure of matter Chapter 2 Nuclear transformation
2
The nucleus A the mass number (Nproton+ Nneutron)
Z the atomic number (Nproton ) isotope same Nproton, different Nneutron isotone same Nneutron, different Nproton isobar same (Nneutron+ Nproton), different Nproton isomer same Nproton, same Nproton, different nuclear energy state
3
Charts of isotopes Z=N Isotone Isotope Isobar
4
Atomic mass and energy units
1 amu = mass of =1.6610-27 kg 1 eV =1 V1.602 10-19 C =1.602 10-19 J Einstein’s principle of equivalence of mass and energy
5
Decay constant ()
6
Activity 1 Ci =3.71010 disintegrations/sec =3.71010 dps =3.71010 Bq
7
The half-life (T1/2) & the mean life (T)
8
Radioactive equilibrium
9
Transient equilibrium
T1>T2 (1<2) Transient equilibrium time activity
10
Secular equilibrium T1>>T2 (1<<2) A2 = A1 activity
time activity
11
particle decay Q = the disintegration energy
= the difference in mass between the parent nucleus and product nuclei E 510 MeV (discrete energy)
12
Negatron(-) emission
An excessive number of neutrons or a high neutron-to-proton (n/p) ratio anti-neutrino Q = the difference in mass between and the sum of the masses of and the particles emitted.
13
Positron(+) emission
A deficit of neutrons or a low n/p ratio neutrino Annihilation 0.511 MeV photon + positron free electron
14
The -ray spectrum The average energy of the particles is approximately Emax/3.
15
Electron capture The unstable nuclei with neutron deficiency may increase their n/p ratio by EC. An alternative process to the positron decay K capture characteristic x-rays (L or M capture) Auger electrons
16
Characteristic radiation
An empty hole in a shell is filled by electron from outer shell with an emission of characteristic radiation. discrete energy h=EK - EL hole K L M
17
Auger Electrons The absorption of characteristic x-rays by orbital electrons and reemission of the energy in the form of monoenergetic electrons discrete energy E=h-EM=EK – EL-EM K L M hole
18
Nuclear reactions (1) The , p reaction The , n reaction
Threshold energy AX (, p) A+3Y The , n reaction Proton bombardment Deuteron bombardment
19
Nuclear reactions (2) Neutron bombardment Photon disintegration
Neutron, no electric charge effective in penetrating the nuclei and producing nuclear reactions n, reaction Photon disintegration Fission Chain reaction Fusion
20
Activation of nuclides
The yield of a nuclear reaction The number of bombarding particles The number of target nuclei The probability of the occurrence Cross-section 1 barn = cm2 The growth of activity Saturation activity
21
Thank you for your attention!
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.