Nuclear Physics
- Rutherford's Model of the Atom
- massive nucleus
- electrons around nucleus
- Before this model
- Henri Becquerel and Pierre and Marie Curie had observed emission from
atoms
- charges varied in magnitude and sign
- mass varied
- energy varied
- three types
- alpha (a) particles - most massive, positively charged, least
penetrating
- beta (b) particles - lighter, negatively charged, most common
- gamma (g) particles - no mass, no charge
- An atom would be a different element after the emission than before.
- process is occurring in nucleus
- Nucleus composed of protons and neutrons
- protons contribute to charge and mass
- neutrons contribute to mass, no charge
- Electrons???
- energies expected do not match energies observed
- magnetic moment does not match
- nuclear spin
- Rutherford proposed idea of neutral particle
- Chadwick - 1932
- Notation

- X
- A
- atomic mass (number of protons + neutrons)
- Z
- atomic number (number of protons), usually omitted
- N
- neutron number (number of neutrons), usually omitted
- isotope
- same atomic number, different atomic masses
- isotone
- isobar
- same atomic mass
- mirror isobars
- Z1 = N2, Z2 = N1

- dependence of chemical properties on N negligible
- atomic masses measured in atomic mass units (u)
- 1 u = 1/12 the mass of the neutral Carbon-12 atom
- 1 u = 1.66055 x 10-27 kg = 931.49 MeV/c2
- Nuclear Spin
- Stable Nuclei
- not all combinations possible
- A < 20 , roughly equal numbers of protons and neutrons
- nuclear energy levels
- filling energy levels
- even-even
- even-odd
- odd-odd
- A > 20, neutrons dominate
- Binding Energy
- mass of individual pieces is greater than the whole
- Au-197
- 79 hydrogen atoms (79 protons and 79 electrons) and 118 neutrons
- mass of the pieces
- mass of the whole
- mass difference
- 198.6406 - 196.966560 = 1.674085 u
- total binding energy
- Binding Energy/Nucleon
- More Examples
- Decay processes
- alpha decay

- atomic mass number decreases by four
- atomic number decreases by two
- occurs because nucleus is too large
- beta decay

- atomic mass number is unchanged
- atomic number increases by one
- occurs because nucleus has too many neutrons relative to protons
- positron emission

- atomic mass number is unchanged
- atomic number decreases by one
- occurs because nucleus has too many protons relative to neutrons
- electron capture

- atomic mass number is unchanged
- atomic number decreases by one
- occurs because nucleus has too many protons relative to neutrons
- gamma

- atomic mass number is unchanged
- atomic number is unchanged
- occurs because nucleus has excess energy
- statistical process
- cannot predict when one particular nucleus will decay
- activity is defined as the rate at which the nuclei decay or the number of decays per second

- the activity should be a positive quantity while the dN/dt will be negative so we add
the negative sign.
- 1 becquerel = 1 Bq = 1 decay/second
- 1 curie = 1 Ci = 3.7 x 1010 decays/second = 37 Gbq
- activity of 1 gram of radium -226
- We would expect the number of decays to be proportional to the number of radioactive nuclei
remaining

- lambda is the constant of proportionality and does not depend on time
- minus sign is needed because N decreases with increasing t
- use this expression to find the number of nuclei left as a function of time

- the number of radioactive nuclei will decrease with time and approaches zero as the
time gets very large.
- A useful time to use to describe the activity of a sample is the time when half of the
nuclei have decayed so that N = N0/2. We call this the half-life t1/2. The decay
constant is related to the half-life.