Chapter 5 Flashcards

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1
Q

Define Fluence

A

Particles per unit area (in some predetermine amount of time)

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2
Q

Define Flux

A

Particles per unit time (in some predefined area)

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3
Q

Define HVL

A

Thickness of specified material to reduce fluence to half

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4
Q

Why is the first HVL usually smaller than subsequent?

Concrete How HVL e changes with energy?

Pb How HVL e Changes with energy?

A

the first layer filters a lot of low energy photons in the polyenergetic beam

Concrete TVL2 < TVL1 , high attenuation but big scatter just as water (increased low energy component of the beam has lower TVL) decrease TVL with depth.

Narrow Beam even in concrete TVL2 >TVL1 (beam hardening is the main effect not scatter).

For Pb, TVL 2> TVL1, in Pb Pair production is dominant.

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5
Q

Types of interactions

A

Compton, photoelectric, pair production (2-kinds) Raliegh, atomic interactions

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6
Q

What is the energy of a photoelectron

A

hv-Eb

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7
Q

Binding energy of a k shell photoelectron in Pb. What does is resonance?

A
  • Spikes are absorption edges and correspond to the binding energies of L and K shells (15 and 88 keV for Pb).
  • Resonance occurs when the photon has an energy that just equals the binding energuy of the L shell, significantly increasing the probability of photoelectric absorption
  • Beyond the L Shell resonance the probability of absorption decreases ~ 1/E3 until the next resonance at the K absorption edge.
  • Absorption edge of water is very low (~0.05 keV)
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8
Q

Where do jumps in photoelectric attenuation as a function of energy come from?

A

when a new shell becomes available the attenuation spikes then gradually decreases as the energy increases until the beam has enough energy to interact with the next level of shell

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9
Q

What is the dependence of compton scatter probability on Z?

How can you estimate the Shielding based on Compton for two different materials?

A
  • Compton tends to happen with essentially free electrons so it is more or less independent of Z
  • Compton effect depends almost exclusively on the electron density which is simply the number of electrons per grams * the physical density
  • The number of Electrons per gram is approximately the same for all materials except hydrogen
  • Linear attenuation properties can be estimated for two different materials based on the ratio of their difference in physical density (g/cm3) .
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10
Q

Given lead and water, which has the higher mass attenuation coefficient?

A

Lead is higher in pair production and photoelectric range about equal in the compton range

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11
Q

Compton equations: hv’ in terms of hv theta (e- angle) in terms of phi (photon angle) E (KE of e-) in terms of hv alpha in answer is hv/moc2

A
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12
Q

Two main neutron interactions

A

recoiling protons nuclear disintegration

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13
Q

Which absorbs more neutron energy - muscle or fat?

A

Fat - it has more hydrogen for interaction

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14
Q

Pair Production

A

If the energy of the photon is greater than 1.02 MeV, the photon may interact with matter through the mechanism of pair production. The photon interacts trongly with the electromagnetic field of an atomic nucleus and gives up all its energy in the process of creating a pair consisting of a negative electron (e-) and a positive electron (e+). The total kinetic energy available for the electron–positron pair is given by (hn - 1.02) MeV. The particles tend to be emitted in the forward direction relative to the incident photon.

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15
Q

Annihilation Radiation

A

The positron created as a result of pair production as an electron does, namely by ionization, excitation, and bremsstrahlung. Near the end of its range, the slowly moving positron combines with one of the free electrons in its vicinity to give rise to two annihilation photons, each having 0.51 MeV energy. Because momentum is conserved in the process, the two photons are ejected in opposite directions.

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16
Q

Photon beam attenuation is characterized by:

A

by attenuation coefficient μ: I(x) = I0e-mx

17
Q

HVL and attenuation coefficient are related by

A

HVL = 0.693/μ

18
Q

μ, μtr, and μen are parameters that respectively characterize

A

photon beam attenuation,

energy transfer,

energy absorption

as the beam traverses a medium

19
Q

Photon beams interact with matter through five major processes

A

coherent scattering, photoelectric effect, Compton effect, pair production, and photodisintegration

20
Q

Photoelectric probability varies as

A

Z3/E3

21
Q

Photodisintegration involves

A

a photon creating a nuclear reaction, In most cases it results in the emission of a neutron

22
Q

The total mass attenuation coefficient (μ/r)

A