radiation detection & gamma surveys lec 7&8 Flashcards

1
Q

specific activity

A

amount of activity to a gram of material
Radioactive material with long half-lives have low specific activity.

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2
Q

why are neutrons hard to detect

A

no charge
can cause damage to the lattice

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3
Q

more charge=

A

more friction so shorter range

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4
Q

attenuations

A

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)

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5
Q

Shielding

A

neutrons need something hydrous
gamma (concrete or lead)

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6
Q

higher atomic number

A

larger u in general

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7
Q

Photoelectric effect (gamma interaction)

A

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

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8
Q

Compton scattering (gamma interaction)

A

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

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9
Q

pair production (gamma interaction)

A

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.

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10
Q

types of detectors -gas detectors

A

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)

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11
Q

types of detectors- solid state detectors
scintillator

A

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

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12
Q

scintillation detection 6 steps

A
  • 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
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13
Q

solid state detectors- semiconductors

A

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

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14
Q

gamma surveying

A

geophysics technique
gamma spectrometers
solid state and scintillate for surveys
aerial- can be unmaned

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15
Q

gamma spectrometers

A

can identify specific radionuclides
measurement are usually slow and expensive
typically laboratory based

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16
Q

radiometric survey measures the spatail distribution of three radioactive elements

A

potassium, thorium, uranium
use thing further down the decay chain- daughter emits gamma
energy of gamma rays characteristic of element

17
Q

gamma rays stopped by

A

water and other molecules -hence rad map only detects near surface sources
wet soil hinders survey

18
Q

gamma ray spectra U

A

gammas lower down in the chain
have to assume its in secular equilibrium- takes the longest half life to refill all the decay chain

19
Q

secular equilibrium

A

activity of any of the isotopes present is the same as that of the initial parent
1:1 ratio

20
Q

survey methodology
flight line direction

A

flight direction should be perpendicular to geological structure of interest
in mountain terrain -follow contours of the ground
fallout monitoring- line should be perpendicular to the winds which were blowing at the time

21
Q

survey methodology
flight line spacing

A

determined by budget
1km line spacing typical
wide line spacing first- then closer line spacing in contaminated areas

22
Q

calibrations and processing
equipment dead time

A

time it takes detector to process
if 10% of time not collecting, times it by 1.1 to bring back the dead time

23
Q

calibrations and processing
cosmic background rad

A

the higher the survey the more background
need to take it away from the values measured
no terrestrial gamma rays have energies above 3 MeV so we bin all of them
flights carried out over the sea when on-shore breeze so radon contribution to all channels in negligible

24
Q

calibrations and processing
radon background

A

sticks to everything

25
Q

calibrations and processing
survey altitude

A

radiation dispersal
higher lose radiation -drops of exponentially

26
Q

calibrations and processing
radioelement concentrations

A

fully corrected count rate data can be used to estimate the concentrations in
the ground of each of the three radioelements, K, U and Th
Concentration of element=count rate/source sensitivity

27
Q

gamma surveying all the corrections

A

dead time, background, stripping, attenuation correction
all standardized one meter above surface

28
Q

Non-collimated mapping is useful for

A

improved coverage. With a collimated mapper you will be more sensitive to a smaller area of ground and might suffer large physical gaps in your data
and lower count rates.

29
Q

background dose rad for Bristol

A

0.2-0.3 uSv/hr

30
Q

Explain why it is inappropriate to model the Fukushima fallout zone as a point source of radiation for the purposes of mapping. Does the inverse-square law still apply?

A

Blanketed with radioactive material so acts as a wide planar (rather than point) source. A planar source can be thought of as many point sources contributing simultaneously. Inverse square law may provide a rough estimation but no longer really valid – as the detector moves away it samples contributions from more sources.

31
Q

attenuation length -length to stop radiation

A

bigger AL =more shielding and takes longer to stop
pb = high mass, long linear attenuation length (good blocker)
polyethylenes = low mass, short linear attenuation length

32
Q

Thermoluminescent dosimeter / film badge good for

A

Monitoring exposure of personnel during routine work in a nuclear power station

33
Q

pulse mode- semiconductors

A
34
Q

current mode- semi conductors

A

No saturation, no preamplifier and no upper count rate

35
Q

Measurements for radon gas are often carried out during house surveys. Why might this isotope be
present in areas containing granite? Which areas of a house might you expect to find it accumulate?

A

Granites contain uranium, decaying to radon. Volatile radon gas can escape the rock into basements which generally show the highest levels. Radon denser than air so accumulates in depressions.