radiation detection & gamma surveys lec 7&8 Flashcards
specific activity
amount of activity to a gram of material
Radioactive material with long half-lives have low specific activity.
why are neutrons hard to detect
no charge
can cause damage to the lattice
more charge=
more friction so shorter range
attenuations
When an energetic charged particle passes through matter it will rapidly slow down and lose its energy by interacting with the atoms of the material (detector or body)
Shielding
neutrons need something hydrous
gamma (concrete or lead)
higher atomic number
larger u in general
Photoelectric effect (gamma interaction)
electron comes in, kicks out a electron, complete absorbion, no scattering, has to be higher than the binding energy so enough energy to kick it out
emits charteristic energy
0.03MeV
Compton scattering (gamma interaction)
interaction happening in the electron cloud
electron has bit more energy, nocks electron and scatters, gamma energy continues and can hit another one, lots of low energy event
annoying for shielding or counting
pair production (gamma interaction)
positron annihilation
high energy comes along (<1.02MeV), interacts with nucleus creating electron/positron pair
Both the electron and the positron lose energy via ionization until an
annihilation event takes place yielding two photons of 0.51 MeV moving in
opposite directions.
types of detectors -gas detectors
geiger counters -alpha beta gamma
just tells you something is there (clicks)
cheap, easy, sensitive, no specific
uses light gas (he), need very thin window for alpha (diff windows-diff rad)
rad comes in causes collisions /ionizations and clicks (chain reaction)
types of detectors- solid state detectors
scintillator
flash of light when interacts with something (electromagnetic rad)
will detect alpha gamma and beta (w a thin window)
bigger flash of light-more rad
500 pounds
scintillation detection 6 steps
- Inside a scintillator:
1. Excitation due to absorption of radiation
2. Emission of light photons from de-excitation
3. Transit of light to photocathode inside photomultiplier tube - Inside a photomultiplier tube:
4. Production of photoelectrons in photocathode
5. Multiplication of photoelectrons - At the back-end of the scintillator and photomultiplier tubes:
6. Conversion of electronic detector output to useful information
solid state detectors- semiconductors
moving electrons to the hole
little fluctuation in output for a given energy of rad, fast, higher spectral resolution, sensitive to vibration
expensive, need to be cooled
gamma surveying
geophysics technique
gamma spectrometers
solid state and scintillate for surveys
aerial- can be unmaned
gamma spectrometers
can identify specific radionuclides
measurement are usually slow and expensive
typically laboratory based