Topic 4: x-rays Flashcards

1
Q

How is the number of e- released in an exposure determined?

A

By selected mA

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2
Q

How are the total number of X-rays produced in an exposure calculated?

A

mAs = mA x T
- mA = e- current
- T = time exposure in seconds

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3
Q

KE acquired by e- measured in?

A
  • Selected kV
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4
Q

3 types of interactions of e- + atoms

A

1) Incoming e- + outer shell e- of target atom
2) Incoming e- + inner shell e-
3) Incoming e- + nuclei

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5
Q

How far away is e- from surface of target when interactions occur?

A

0.5mm

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6
Q

Describe the interactions with tungsten atoms

A
  • Most e- are in the outer orbital = incoming e- need small amount of energy to interact
  • Small amount of energy = EM radiation = electrostatic repulsion BUT too small to produce X-rays
  • All energy released = heat
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7
Q

2 process X-ray produced in X-ray tube

A

1) Characteristic radiation
2) Bremsstrahlung

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8
Q

Describe characteristic radiation

A

1) Excitation: sufficient energy given to bound e- = raise to next orbital
2) Ionisation: binding energy of orbital e- is overcome + released from atom

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9
Q

Describe excitation

A
  • e- removal = temporary = returns to original position
  • Gives out photon = energy = gained by e- in raising itself to new shell
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10
Q

Describe ionisation

A
  • Released e- = delta ray = carries KE donated during interaction
  • Delta ray = goes to interact with other atoms until all KE lost
  • Ionization can only occur = if KE incoming e- =/> specific binding energy of orbital bound e-
  • Ionisation of K shell = leaves vacancy = e- from shell further from nucleus drops to K shell
  • Releases X-ray = value = difference in binding energies between shells
  • If L shell to K shell = K-alpha emission
  • If M shell to K shell = K-beta emission
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11
Q

3 variables of energy bands

A

1) Atom type = atomic number
2) Shell from which e- ejected
3) Shell from which replacement e- comes

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12
Q

Describe Bremsstrahlung

A
  • When electrically charged particle + large KE = deflected by second charged mass
  • Deflection = change in momentum for incoming e- = gives emission of photon of EM radiation
  • Loss of energy = incoming e- slow down
  • Amount of KE given to X-ray photon from incoming e- = determined by how close e- passes to nucleus
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