X-Ray Flashcards

1
Q

What is the energy range of X-radiation?

A

100 eV - 1 MeV

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2
Q

What are the components of an X-ray tube?

How does it work?

Draw it.

A

Components:

  • Vaccuum tube made of glass
  • anode and cathode

Function:

  1. tungsten filament (high Z, high melting point) of the cathode is heated by anode current I and emits e- by thermionic effect (no. of e- emitted depends on I)
  2. high voltage is applied btw the electrodes that accelerates e- towards the anode
  3. e- decelerated at anode, X-rays produced (if Ekin high enough also characteristic X-rays produced)
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3
Q

What is Bremsstrahlung?

How does its spectrum look like?
Draw the graph.

A

X-radiation generated by the deceleration of high speed (large Ekin) charged particles

  • has a smooth, continuous spectrum with a wavelenght minimum λmin
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4
Q

What does the Duane-Hunt law state?

Give the formula.

Explain it using a graph.

A

gives minimum wavelenght λmin of X-radiation produced by Bremsstrahlung

​ ⇒ higher accelerating U → Bremsstrahlung’s spectrum shifts towards lower λ, thus higher Ephoton

λmin = k/U

  • U = accelerating voltage
  • k = h*c/e = 1230 pm*kV
    • ​h = Planck’s constant
    • c = speed of light
    • e = charge of e-
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5
Q

The total power of Bremsstrahlung emitted by a X-ray tube depends on… ?

Refer to a formula.

A

integral of X-ray spectrum dependent on:

  • anode current I
  • accelerating voltage btw anode and cathode U
  • atomic number of the anode material Z

PX = cX U2 I Z

  • cX = X-ray constant = 1.1 * 10-9 V-1
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6
Q

How can the integral of the X-ray spectrum be changed?

A
  • increase I → P changes proportionally (intensity is increased because greater no. of e- hits anode)
  • increase U → P changes proportionally to U2 (cf. Duane-Hunt law)
  • increase Z → higher efficiency of conversion of Ee- to EX-ray
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7
Q

What is the precondition for characteristic X-radiation?

How does its spectrum look like?

Can it be changed and if so, how?

A

Ekin of the accelerated e- is high enough to eject an inner shell e- from the anode with high Z
→ empty orbital filled by an outer shell e-excess E emitted as X-radiation

  • line spectrum, position characteristic for the atom
  • position of lines is independent of U, only intensity (height of lines) can be changed by increasing I
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8
Q

What is the most important interaction type of X-radiation in diagnostics?

Explain it on molecular level.

Explain why contrast btw different tissues can be achieved w/r/t a formula.

A

mainly photoeffect → τM

  • photon of the X-radiation absorbed by an inner atomic e-, which is consequently ejected from the atom
  • τM strongly depends on Z → even small differences btw diff. tissues types lead to large attenuation effects

τM = C λ3Z3

⇒ also explains why high λ X-radiation used for elements with low Z (e.g. mammography)

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9
Q

What is another fairly important way of X-ray attenuation?

When is it especially important and why?

A

Compton scattering

important for atoms with low Z bc attenuation directly proportional to Z, not Z3 like in case of photoeffect attenuation

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10
Q

What is the minimum wavelenght λmin?

A

corresponds to the one-step process when the total Ekin of the e- is converted to one X-ray photon with E=hfmax (fmax because λmin)

Ekin e- = eU = U * I = hfmax = h c/λmin

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11
Q

Bragg diffraction

A

NOCH AUSSTEHEND

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12
Q

How was the Duane-Hunt law verified?

A
  • X-ray spectrum was measured at different U
  • different λmin could be observed → changing shape
  • plot λ vs. 1/v → good linear fit → Duane-Hunt constant k
  • calculation of Duane-Hunt constant
    λmin = k/U
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13
Q

How was the relation btw intensity of X-radiation and increasing current verified?

A
  • the spectrum was integrated at different anode currents
  • plot P vs. I → good linear fit → P proportional to increasing I
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14
Q

How was the Z-dependence of the τM verified?

A

NOCH AUSSTEHEND

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