DECK 7 — BETA & GAMMA ATTENUATION

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32 Terms

1
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What is gamma-ray attenuation?

Gamma-ray attenuation is the reduction in photon intensity as gamma rays pass through matter.

2
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What equation describes gamma-ray attenuation?

The equation I = I0 · e^(−μx) describes gamma-ray attenuation.

3
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What is the linear attenuation coefficient μ?

The linear attenuation coefficient μ quantifies the probability of photon interaction per unit thickness.

4
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What is the mass attenuation coefficient μ/ρ?

The mass attenuation coefficient μ/ρ removes density dependence and allows material comparison.

5
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What does a larger attenuation coefficient indicate?

A larger coefficient indicates more interactions and stronger attenuation.

6
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What determines the attenuation coefficient for gamma rays?

Gamma energy and atomic number of the absorber determine the attenuation coefficient.

7
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What is a half-value layer (HVL)?

HVL is the thickness of material needed to reduce gamma intensity to one half.

8
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What is a tenth-value layer (TVL)?

TVL is the thickness needed to reduce gamma intensity to one tenth.

9
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How is HVL related to μ?

HVL = ln(2)/μ.

10
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How is TVL related to μ?

TVL = ln(10)/μ.

11
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Why does the HVL change with photon energy?

Photon interaction probabilities vary with energy, changing attenuation behavior.

12
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Why do high-Z materials attenuate gamma rays more effectively?

High-Z materials increase photoelectric and pair-production probabilities.

13
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Why does the photoelectric effect dominate at low gamma energies?

Photoelectric probability increases sharply as photon energy decreases.

14
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Why does Compton scattering dominate at intermediate energies?

Compton scattering has weak Z dependence and occurs across many materials.

15
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Why does pair production dominate at high gamma energies?

Pair production requires photon energies above 1.022 MeV and increases with energy.

16
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Why is buildup sometimes observed in gamma attenuation experiments?

Scattered photons may still reach the detector, increasing measured intensity.

17
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Why does gamma attenuation deviate from pure exponential at small distances?

Geometry, scattering, and source-detector alignment distort simple exponential behavior.

18
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What is beta attenuation?

Beta attenuation is the reduction of beta particle intensity through energy loss and scattering in matter.

19
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Why do beta particles not follow exponential attenuation?

Beta particles undergo continuous energy loss and scattering rather than discrete interactions.

20
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Why do beta particles have a maximum range?

Beta particles stop when they lose all kinetic energy through collisions.

21
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What determines the range of beta particles?

Initial energy, material density, and atomic number determine beta range.

22
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What is the continuous slowing down approximation (CSDA) range?

CSDA range is the average distance a beta particle travels before coming to rest.

23
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Why do beta particles produce bremsstrahlung in absorbers?

Beta particles decelerate in electric fields of nuclei and emit bremsstrahlung photons.

24
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Why should beta radiation be shielded with low-Z materials?

Low-Z materials reduce bremsstrahlung production compared to high-Z materials.

25
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Why does bremsstrahlung become significant for high-energy betas?

Higher beta energies cause stronger deceleration and more photon production.

26
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How is beta shielding different from gamma shielding?

Beta shielding uses low-Z materials to avoid bremsstrahlung, while gamma shielding uses high-Z materials.

27
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What effect does absorber thickness have on beta count rate?

Count rate decreases until beta particles are fully stopped, then levels off.

28
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Why might gamma background appear in a beta attenuation experiment?

Bremsstrahlung and source gamma emissions may be detected.

29
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How is the linear attenuation coefficient experimentally determined?

Plot ln(I) vs thickness and use the slope equal to −μ.

30
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Why is detector alignment important in attenuation experiments?

Misalignment changes geometric efficiency and distorts attenuation results.

31
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Why are narrow-beam conditions preferred for gamma attenuation measurements?

Narrow-beam geometry minimizes scattering contributions to the detector.

32
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Why does scattering complicate attenuation measurements?

Scattered photons may still reach the detector, causing non-exponential behavior.