Week 10 - X-Ray Tubes (Part 2) Flashcards

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1
Q

X-Ray Tube Housing

A

The housing provides:

o Shielding from x-rays
 Usually achieved with lead shielding

o Insulation from high voltages
 To ensure tube housing does not become live

o Mechanical support for the tube

o Mounting for LBDs, cones & filters

o Access for high voltage cables

o Oil filled to provide additional insulation & cooling
 Could also be water

o Bellows allows for thermal expansion of the oil

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2
Q

Principal Parts of a Rotation Anode X-Ray Tube

A
  • Electrons created at filament –> accelerated to the target on the anode
  • Window allows for x-rays to exit
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3
Q

The Envelope

A
Borosilicate glass (like Pyrex) - heat resistant,
o	Or metal envelope for heavy duty tubes. 

Maintains the vacuum necessary for electron flow between cathode and anode.
o Any residual gas would:
 Impede projectile electrons moving from cathode to anode
 Produce secondary electrons and result in an avalanche of electrons reaching the anode.

o Tube window: approx. 5 cm square thin section to allow maximum transmission of x-rays

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4
Q

The Cathode

A
  • Negative electrode of the x-ray tube
  • Source of projectile elections
  • Size of the filament determines the size of the electron beam
    o Determining the spot size on the target
     Small Spot Size = Small filament
     Lower resolution / Larger spot size = larger filament
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5
Q

Cathode

A

Electrons are emitted from a heated filament by thermionic emission.
o The temperature must be >2200oC.

The filament is:
o A coil of wire approx. 2 mm in diameter by 10 to 20 mm long
o Heated by an electric current (Amps)
o Made of tungsten/thorium alloy

Tungsten is used because it:
o Has a high melting point (3410C),
o Does not vaporise easily
o Is mechanically strong.

The thorium (1%) improves thermionic emission

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6
Q

Dual Focus Tubes

A

Typical sizes:
o Small (fine), short filament focal spot size: 0.1 to 0.5 mm
 Can give high resolution

o	Large (broad), long filament focal spot size: 1.0 to 2.0 mm 
	Provides low resolution 

The two filaments can be side-by side or in-line.
o If in-line then a biangular anode is usually used.

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7
Q

Focussing Cup

A

Focuses the electron onto a small target area
o If generating a lot of electrons in a narrow region –> they will repel due to charge
o Therefore, some focus of the beam is lost
o Creates an electric field which refocuses the electron
 Overcomes the repulsion force between electrons

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8
Q

X-Ray Tube

A
  • Is controlled by the filament temperature which in turn is controlled by the filament current
  • Projectile electrons striking the target provide the tube current
  • Current applied to the filament is much higher

The filament current must be controlled very precisely
 Small changes result in a big change in tube current
• Can reduce image quality

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9
Q

Anode Cooling: Stationary and Rotating

A

Stationary
o Cooling is by conduction through a large mass of Cu.
 Cu is a good thermal conductor and has a high heat capacity.

Rotating
o Cooling is by radiation. The narrow Mo stem minimises heat conduction to the rotor and bearings.

o The rotating anode increases the target area
 Hence reduces anode temperatures and allows higher exposure factors.

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10
Q

The Anode: Stationary and Rotating

A

Stationary
o Low power applications, e.g., dental, mobile, therapy.

Rotating
o General purpose and heavy duty, i.e., high intensity and short exposure times.
o The rotor and stator behave like an electric induction motor.
o Stator: coils of wire carrying an alternating current
o Rotor: Solid Cu and Fe cylinder. Rotation speed is typically 3000 rpm.

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11
Q

Target Design

A
  • As it is rotating, electrons are dissipated across a greater target area
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12
Q

Tungsten Target

A
  • W is alloyed with rhenium to increase strength
  • Atomic Number: 74 (high-efficiency x-ray production and in high energy x-rays)
  • Thermal Conductivity:
    o Thermal conductivity nearly equal to that of copper
    o An efficient metal for dissipating the heat produced
  • High Melting Point
    o 3400 degrees celcius
    o Cu = 1100 degrees celcius
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13
Q

Line Focus

A

The line focus principle helps to increase the surface area over which the heat is generated.

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14
Q

Effective Focal Spot Length

A

Effective focal spot length = actual focal spot length x sin (theta)
o theta = target angle
o Helps to dissipate heat and maintain small focal spot size

  • Angle of target = alters size of the focal spot size
    o Larger focal spot size –> more heat is dissipated over a larger area
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15
Q

The Focal Spot Size is a Compromise

A
  • It needs to be small to give high spatial resolution (good detail) in the image, i.e. sharp edges to the shadows,
  • It needs to be large to spread the heat generated over a large area and keep the target temperature down.

Therefore:
o dual focus tubes
o angled anode
o rotating anode

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16
Q

Bi-Angular Anode Geometry

A
  • Bi-angular anodes are used when the two filaments are in-line
17
Q

Effective Focal Spot Varies Across the Image Plane

A
  • Spatial resolution varies across the imaging plane
18
Q

Heel Effect

A
  • Self-absorption of x-rays in the anode leads to reduced intensity at the anode end of the x-ray field and increased intensity at the cathode end.
    o Electrons undergoing Bremsstrahlung deeper into the target –> have more target to escape to
    o More x-rays at the cathode side of the x-ray tube than the anode side
    o Noise will vary across imaging plane
19
Q

Off-Focus (Extra Focal) X-Rays

A
  • Off-focus (extra-focal) x-rays degrade the contrast in the image by adding to the background ‘fog’.
  • Diaphragm can be used to collimate them out of the field
20
Q

X-Ray Quantity

A

Quantity refers to the amount (number) of x-rays produced during an exposure, but it is difficult to count x-rays
o Therefore, quantity is usually measured in terms of:
 Radiation exposure unit: roentgen, R (or milli-roentgen, mR) (These are old units and are usually found only in American textbooks.)
 Radiation dose SI units: gray (Gy) or sievert (Sv).

21
Q

X-Ray Quality

A

Quality refers to how penetrating a beam is and is closely related to the average x-ray photon energy of the beam.
o High quality → high average energy, hard x-rays, highly penetrating.
o Low quality → low average energy, soft x-rays, less penetrating.

Quality is expressed in terms of half-value layer (HVL) in units of mm of aluminium.
o HVL is a measure of how penetrating the beam is.

22
Q

Tube Current and Exposure Time

A
  • Intensity is proportional tube current
  • Intensity is proportional exposure time
  • Therefore: I is proportional mAs
23
Q

Tube Voltage

A

Ideally: I is proportional (kV)^2
o This is for the x-ray intensity at the anode surface.

o After being filtered through the tube window etc. it is more like:
 I is proportional (kV) 2.5 for high kV (60 to 100 kV)
 I is proportional (kV) 3.5 for low kV (20 to 40 kV) i.e. the exponent increases as kV decreases.

24
Q

Distance

A

X-ray quantity is inversely proportional to the square of the distance from the source

Inverse Square Law

25
Q

Filtration

A
  • Adding filtration reduces the x-ray intensity

- Inherent filtration = window

26
Q

Exposure from Changing Filtration

A

This graph shows X-ray beam intensity dependence on kVp and filtration for a single-phase full-wave rectified x-ray tube.
o Note the strong dependence of intensity on both kV and filtration.

27
Q

Tube Age

A

The intensity reduces with tube age due to:
o Grazing of the anode surface (no longer a smooth flat surface)
o Additional filtration due to the W film deposited on the inside of the envelope
 Due to vaporisation of the Tungsten

28
Q

Waveform

A

For other types of generators the values read from the graph should be multiplied by a constant, i.e.
o For three phase: × 1.3
o For constant potential: × 1.5

29
Q

Quality

A
  • Quality relates to the energy of the x-rays and therefore how penetrating an x-ray beams is.
  • It is measured in terms of half-value layer (HVL) in units of mm of aluminium.
  • HVL: the thickness of Al required to reduce the intensity of the beam to ½ of its initial intensity.
    (not to be confused with filtration, which is also expressed in mm of Al)
    o not to be confused with filtration, which is also expressed in mm of AI
30
Q

Factors Affecting X-Ray Quality and Quantity

A
  • Increase in mAs
    o Quality = none
    o Quantity = Increase
  • Increase in kVp
    o Quality = Increase
    o Quantity = Increase
  • Increase in Distance
    o Quality = None
    o Quantity = Reduce
  • Increase in Filtration
    o Quality = Increase
    o Quantity = Reduce
31
Q

Variation of Quality with kV

A
  • Quality increases with kV
32
Q

Filtration

A
  • Quality increases with added filtration because low energy x-rays are more likely absorbed than high energy ones, thus increasing the average x-ray photon energy.
  • Reduced patient dose by removing soft x-rays that would mainly be absorbed in the patient and not contribute to forming the image
  • An ideal quality beam would contain x-rays of only a single energy (mono-energetic beam)
  • Not possible to produce a mono-energetic beam with an x-ray tube
    o can be approximated with very heavy filtration, however this would reduce the quantity too much

By choosing filtration –> we can modify the penetration of the beam
o By doing so we reduce the number of x-rays but increase the mean energy