Neutron Protection Flashcards
What are the sources of neutrons?
Radionuclides, accelerators (produced by ion beams or photonuclear reactions), nuclear reactions (prompt fission nuetrons, delayed neutrons, photoneutrons, gamma radiation), and nuclear fuel reprocessing plants.
Describe the properties of Beryllium.
Large nucleus; small atom
Close packed crystal structure
Can be formed into high purity metal components
Almost transparent to x-rays
High cross section for high energy alphas or protons
Neutrons discovered by irradiating Be with alphas
e.g. Be-9 + He-4 = C-12 + n-1
Be-9 binding energy per neucleon: 6.46 MeV
What is the binding energy per nucleon of Beryllium, and why does this mean it is useful for neutron production?
6.46 MeV
Beryllium is used as has a low binding energy, so is easy to release neutrons from nucleus as less energy required to overcome binding energy. So high energy alphas or protons produce high energy neutrons.
Describe the main principles of neutron therapy.
Cyclotron-produced protons (26-66 MeV) onto Be target (more common).
Deuterium (12.5-14 MeV) onto Tritium target (less common).
Therapeutic beams are mixture of x-rays and neutrons
What is photodisintegration?
A photon passes through an electron cloud and interacts with a nucleus. This produces a neutron (photoneutron) or possible a proton or alpha particle, and an ionising recoil nucleus with a changed mass number and/or atomic number.
I.e: Photon hits a nucleus, if energy>B.E = recoil nucleus (with changed mass/atomic number) + photoneutron (or maybe proton/alpha).
What is the threshold photon energy to produce a photo-neutron?
10 MeV
What is the threshold photon energy to produce an alpha or proton from photodisintegration?
Much higher than 10 MeV.
What is the mass energy conservation equation?
hv + m(0)c^2 = m(1)c^2 + k(1) + m(n)c^2 + k(n)
where:
hv is energy of incoming LINAC photon
m0c2 is the initial mass-related energy of the nucleus
m1c2 is the final mass-related energy of the nucleus
mnc2 is the final mass-related energy of the neutron
k1 and kn are final kinetic energies of nucleus and neutron
What are the consequences of neutrons in a linac bunker?
Contribute to patient dose
Contribute to a radiation hazard at the maze
Present an additional radiation hazard at the treatment as a result of activated products.
What are the 4 types of neutrons and at what energy ranges do they occur?
Thermal neutrons (<0.4 keV) Intermediate neutrons (0.4-200 keV) Fast neutrons (200 keV - 10 MeV) Relativistic neutrons (>10 MeV)
Describe thermal neutrons.
Energy distribution same as atoms and molecules of surrounding medium
Maxwellian distribution of velocities
(Epithermal neutrons: 0.4 eV – 100 eV)
Most common interaction with matter is neutron capture but other reactions may also occur
Describe intermediate neutrons.
Produced as result of elastic scattering of fast neutrons in materials with low atomic number e.g. carbon or hydrogen or in the human body
Interact with matter by elastic scattering
Describe fast neutrons.
Interact with light nuclei primarily through elastic scattering
Although inelastic scattering predominates with higher energies
fast-neutron monitoring instruments become insensitive and inaccurate below 200 keV
Describe relativistic neutrons.
Inelastic scattering more important than elastic
elastic cross-section negligible for high atomic number materials
main form of non-elastic collision ejection of protons or neutrons from target nucleus
At very high energies energy appearing as gamma radiation negligible c.f. energy transferred to cascade protons, neutrons and other nuclei.
What are the 5 interactions of neutrons with matter?
Elastic scattering: (n,n) Inelastic scattering: (n,n'), (n,nγ) Capture: (n,γ) Non-elastic reactions: (n,n), (n,p), (n,d), (n,α), (n,t), (n,αp), etc. Fission: (n,f)
Describe elastic scattering for neutrons.
Neutron shares initial kinetic energy with the target nucleus
Target nucleus suffers only recoil and is not left in an excited state
Total kinetic energy in system remains constant.
Momentum is conserved.
Describe inelastic scattering for neutrons.
only possible with fast neutrons
Total energy of scattered neutron and recoil nucleus < incident neutron
nucleus left in excited state
In (n,nγ) process, excitation energy released by nucleus via emission of prompt gamma ray
In (n,n’) process, nucleus remains in a metastable state