X-ray interaction with matter Flashcards

1
Q

basic production of radiographic image

A

source of X-rays - X-ray machine
- production of X-rays

object - teeth and jaws
- interaction of X-rays with matter

X-ray photons pass from tube, and some through patient to reach image receptor (IR)

Interaction with different tissues alters number of photons exiting patient

Variation in numbers of photons reaching IR produces radiographic appearance of different tissues

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2
Q

4 options for X-ray photons traversing image

A

pass through unaltered

change direction with no energy loss (scatter)

change direction losing energy (scatter and absorption)

be stopped, depositing all energy within tissue (absorption)

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3
Q

scatter

A

X-ray photons change direction with no energy loss

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4
Q

scatter and absorption

A

X-ray photons change direction and losing energy

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5
Q

absorption

A

x-ray photons be stopped, deposition all energy in tissue

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6
Q

effect on photon absorption on image

A

All photons reach film = black (e.g. air)

Partial attenuation = grey

Complete attenuation = white (e.g. amalgam)

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7
Q

structure of atoms

A

Central nucleus

  • Protons (positive charge)
  • Neutrons (no charge)

Orbiting electrons (negative charge)

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8
Q

atomic number Z

A

number of protons

Equivalent to no. electrons in neutral atom

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9
Q

atomic mass A

A

number of protons + number of neutrons

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10
Q

orbiting electrons

A

electrons orbit nucleus in “shells” K,L,M,….

maximum number of electrons in orbit greater in outer orbits (2 x n^2)

K shell electrons have highest binding energy (requires more energy to eject electron from shell)

outer shells have lower binding energies

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11
Q

2 principles of interactions of diagnostic X-rays in tissue

A

Photoelectric effect - Absorption

Compton effect – Scatter, and absorption

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12
Q

photoelectric effect

A

energy from X-ray photon is transferred to object

X-ray photon interacts with inner shell electron (usually K shell)

photon has energy just higher than the binding energy of electron

X-ray photon disappears

most of photon energy used to overcome binding energy of electron, remainder gives electron kinetic energy

electron is ejected (photoelectron)

Atom has “hole” in electron shell: +ve charge
- Not balanced

Ionised atom is unstable

Electron drops from outer shell, filling void

Difference in energy between 2 levels is emitted as light/heat (characteristic radiation)

Outer voids filled by “free” electrons

Results in complete absorption of photon energy: photon does not reach film

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13
Q

effect of photoelectric absorption

A

Results in complete absorption of photon, preventing any interaction with active component of image receptor:

image appears white if all photons involved,
grey if some photons not involved

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14
Q

photoelectric occurence proportional to

A

Atomic Number3 (Z^3)

1/photon energy3 (1/kV^3)

Density of material
- Noticeable differences between cubes
so Easy to differentiate materials

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15
Q

compton effect of X-ray interaction

A

X-ray photon interacts with loosely bound outer shell electron (not passing through, lower binding energy so lots of energy left in photon)

Photon energy considerably greater than electron binding energy

Electron is ejected taking some of photon energy as kinetic energy: recoil electron

Atom is then positively charged

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16
Q

what happens to excess energy in original photon in Compton effect?

A

Following collision, photon has lower energy (longer wavelength)

Called a scatter photon

Undergoes a change of direction
- Related to how much energy it has lost
Different to incoming energy direction (at least slightly different)

17
Q

following scatter effect (in compton effect)

A

Atomic stability is regained by capture of free electron as described before (see diagram in Photoelectric effect 2)

Recoil electron can interact with other atoms in tissue

Scatter photon, dependent on energy and position of bound electron involved, can be involved in more Compton or photoelectric interactions

18
Q

what happens to scattered photons

A

Scattered photons can travel in any direction

Direction of scatter is affected by energy of scatter photon:

  • high energy -> forward direction
  • backward direction
19
Q

probability of compton effect occurring

A

Proportional to density of material (electron density)
- Dense packed electrons – more likely to happen

Independent of atomic number

Not related to photon energy, although forward scatter more likely with high energy photons

20
Q

effect of compoton scattered photons

A

Scattered photons produced before the image receptor is reached, and scattered backwards, do not reach image receptor and do not contribute to the image

Scattered photons produced beyond image receptor, and scattered back towards it, may reach image receptor producing darkening:

  • As their path is randomly altered they do not contribute useful information to the image
  • Results in fogging of image, reducing contrast and image quality
21
Q

reduction of scatter - methods

A

Reduction of area irradiated (collimation), and therefore volume irradiated, will reduce the number of scattered photons produced as well as reducing patient dose

Lead foil within film packet prevents back scattered photons from oral tissues reaching film (in addition to absorbing some of the energy in the primary beam)
- Not used with digital receptors

22
Q

absorptions of photons more likely if: (3)

A

Object traversed has high atomic number

Object traversed is thicker

Photon energy is lower

23
Q

radiographic contrast

A

Difference in density of light and dark areas of radiograph

Image showing both light and dark areas with clear borders has high contrast

Contrast is greatest when difference in absorption by adjacent tissues is greatest
- E.g. amalgam and tooth (completely different material) clearer than caries and healthy tooth (same material but poorer state)

24
Q

effect of interaction on dose

A

Photoelectric absorption results in deposition of all photon energy within tissue:
- Increased patient dose but necessary for image quality

Compton scatter results in deposition of some photon energy within tissue:

  • Adds to patient dose but does not give useful information
  • May increase dose to operators/ people in the vicinity (stand far away should be find)
25
Q

photoelectric interaction effect on dose

A

results in deposition of all photon energy within tissue:

- Increased patient dose but necessary for image quality

26
Q

compton interaction effect on dose

A

deposition of some photon energy within tissue:

  • Adds to patient dose but does not give useful information
  • May increase dose to operators/ people in the vicinity (stand far away should be find)
27
Q

effect of low kVp on image quality and pt dose

A

Low tube potential difference (kVp) produces lower energy photons

Photoelectric interactions are increased

Contrast between different tissues increases BUT Dose absorbed by patient is increased

28
Q

effect of high kVp on image quality and pt dose

A

High tube kVp produces higher energy photons

Photoelectric interactions are reduced

Contrast is reduced but Dose absorbed by patient is reduced

No point reducing dose so much that image is of no diagnostic use
- Wasted dose

29
Q

how to choose kVp

A

compromise between diagnostic quality of the image and dose

Currently recommended that dental units have kVp 60-70kV

At GDH&S we currently use 70kV for all intra-orals.