Nuclear Physics: Radiation, Radioactivity & its
Applications
Nuclear Energy The Nucleus of an atom contains
Protons – Positively Charged Neutrons – no charge
Atomic Mass Number – denoted by the letter A, this number represents the total number of protons + neutrons in the nucleus, telling you what isotope of the element you have.
Atomic Number – denoted by the letter Z, this number represents the number of protons in the nucleus, telling you what element you have.
Nuclear Energy Atomic Symbol for
a given isotope of an element is generally given as noted to the right.
A prime example is an alpha particle or helium nucleus
XAZ
He42
Nuclear Reactions Two Types of Nuclear reactions
produce vast amounts of energy according to Einstein’s famous equation
E = mc2
Fission – the splitting of an atom into smaller parts
Fusion- the joining of two small nuclei to produce one larger nucleus
Nuclear Reactions Mass defect – is the amount of mass that is
converted to energy during fission or fusion.
Calculation of Mass defect is the difference between the actual mass of the atom and the known mass of each of its parts
The amount of energy that this mass is converted into is called the binding energy
Sample Problem
Calculate the mass defect and energy released in the creation of Carbon-13.
Solution Expected Mass: Protons = 6 (1.007276 u) = 6.043656 uNeutrons = 7(1.008665 u) = 7.060655 u 13.104311 uKnown Mass -13.003355 uMass Defect .100956 u
Energy Released = (931.5 MeV/u)(0.100956 u) = 94.04 MeV
Radioactivity Three types of Radioactivity
Alpha – α – is the nucleus of a helium atom Can be stopped by a sheet of paper, is harmful only if
ingested Beta – β – emission of an electron or positron
Can be stopped by a sheet of lead, is harmful to all living tissue
Gamma – γ – emission of a high energy photon Cannot be completely stopped. Very harmful to all
living tissue.
Nuclear Reactions
Alpha Decay
Beta Decay
Gamma Emission
HeRnRa 42
22286
22688
NN AZ
AZ *
eNC 147
146
Half Life The half life of a radioactive
material is the amount of time required for ½ of the sample to decay into another element or isotope.
Half lives are calculated according to the equation:
a = a0(½)x
Half Life a = amount of material left at any time a0 = amount of material that you begin with x = the number of half lives that have
passed since you have begun counting This type of decay is said to be
exponential since it can be described graphically as a hyperbola
Sample Problem
Carbon-14, a radioactive isotope of carbon, has a half life of 5730 years. If a 20 gram sample of carbon-14 is allowed to decay for 10,000 years, how much remains at the end of this period?
Solution
a = a0(½)x
a0 = 20 grams
x = 10,000 yrs/5730 yrs/half life = 1.75So a = 20 grams(½)1.75 = 5.95 grams
Detection of Radiation Counters
Geiger Counter – Radiation causes a gas to emit electrons causing a voltage which makes the counter “click”
Scintillation counter – uses a solid, liquid, or gas scintillator – a material which is excited by radiation to emit light. The light is captured and amplified by a Photomultiplier (PM) tube – which turns it into an electric signal.
Semi-conductor detector – uses a p-n junction diode which produces a short electric pulse when irradiated
Detection of Radiation Trackers
Photographic emulsion – the particle passing through the emulsion ionizes atoms in its path
Cloud chamber – a gas is cooled to a temperature slightly below its normal condensation temperature hence it condenses on any ionized molecule present this “tracks” the particle
Bubble chamber – a liquid is kept close to its boiling temperature and hence “bubbles” around any ionized particle – the bubbles are then left in the wake of the particle and photographed
Applications of Nuclear Processes
Energy can be released in a nuclear reaction by one of two processes: Fission – the splitting of a nucleus into
smaller nuclei Fusion – the joining of two smaller
nuclei into a larger nuclei
Fission Usually caused by neutron bombardment
of the nucleus, causing the nucleus to split Mass is converted into energy All current nuclear reactor technology uses
fission Fission is controlled by using a
moderator, a material which absorbs neutrons to keep the chain reaction under control
Fusion Fusion reactions take lighter nuclei,
often an isotope of hydrogen called deuterium and fuse them together to make a heavier nuclei, often helium
This must occur at high energy and is very difficult to produce under laboratory conditions
Currently no workable fusion reactor has been produced on earth
The sun and stars all produce energy due to nuclear fusion
Measurement of Radiation: Dosimetry
Since radiation can harm the body it is important to quantify the amount of radiation received, or the dose. The study of this is called dosimetry and is an important part of an emerging field known as Health Physics
Dosimetry is most often concerned with the number of rads or millirads of radiation received.
A rad is defined as the amount of radiation which deposits energy at a rate of 0.01 J/kg in any absorbing material
Things to Know Atomic number, Atomic mass number, atomic
symbols, atomic equations Mass defect, binding energy Types of Radiation
Alpha Beta Gamma
Detection of Radiation Nuclear Reactions
Fission Fusion
Dosimetry