Ct Imaging Flashcards

1
Q

are being used to create a gradient in the intensity of the X-ray beam

They are sometimes called “bow-tie” filters

They are mounted close to the X-ray tube.

The purpose of is to ⚫ reduce the dynamic range of the signal recorded by the CT

detector • Reduce the dose to the periphery of the patient

• Attempt to normalise the beam hardening of the beam - to aid with calibration

A

Beam shaping filters

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2
Q

CT scanner detectors

⚫___-__ detector elements along the detector arc •

A

800-1000

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3
Q

___-___detectors along z-axis

A

1-320

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4
Q

CT detectors are ___ in the axial plane (x-y plane), and ____ along the longitudinal axis (z-axis)

A

curved
rectangular

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5
Q

2 Detector type of CT & THEIR EFFICIENCY

A

Xenon gas filled-70%
Solid state- approaching 100%

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6
Q

Better detection efficiency

A

Solid state detector

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7
Q

Solid state detectors are generally
____

the photons interact with the detector and generate light.

A

scintillators

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8
Q

The light is converted into an electrical signal by ____

A

photodiodes

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9
Q

The septa and the strips of the anti scatter grid should be as __ as possible, since they reduce the effective area of the detector and thus reduce the detection of X-rays.

A

small

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10
Q

Detector sizes are the effective size at the ____

A

iso-centre

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11
Q

The minimum number of detector elements should be approximately ___to achieve a spatial resolution of d in the reconstructed image

A

2 FOV)/d

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12
Q

→___- detector elements are required to achieve aspatial resolution of 1 mm within a reconstructed image at a field of view of 400 mm

A

800

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13
Q

Spatial resolution can be improved by use of the ______ or_____

A

quarter detector shift
Dynamic focal spot

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14
Q

By shifting the detector elements by a distance of a quarter of the size of the detector elements, the theoretical achievable spatial

resolution becomes twice as good. It is generally implemented in detectors of all CT scanners.

A

Quarter detector shift

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15
Q

• Focal spot position on anode is rapidly oscillated during gantry rotation, doubling the number of projections

A

Dynamic or flying focal spot

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16
Q

With the current detector rows and/or quarter detector shift and/or flying focal spot a spatial resolution of ~___-___mm in the axial plane can be achieved

A

0.6-0.9

17
Q

4 active detector rows -19__

16 active detector rows-20__

64 active detector rows in- 20__
320 active detector rows - 20__

A

98
01
04
07

18
Q

A typical acquisition with a single detector row scanner covered ___.

A

5 mm

19
Q

In clinical practice the CT scanners with __active detector rows were primarily used to enhance longitudinal
could also be used for enhanced longitudinal coverage, for example by selecting a 4 x 2 = 8 mm, or even a 4x4 = 16 mm coverage.

Enhanced longitudinal coverage would allow for shorter scan times but without the benefit of improved longitudinal resolution.

A

4

20
Q

• These scanners provided excellent longitudinal spatial resolution high quality 3D reconstructions, and at the same time reduced scan times.

A

16 or 64

21
Q

The CT scanners with up to __ active detector rows generally cover a scan volume with a helical acquisition with multiple rotations.

A

64

22
Q

The __ detector row CT scanner covers 160 mm on one

rotation, for organs such as the brain or the heart within one rotation.

A

320

23
Q

An x ray tube (with a rotating __ anode) and high voltage generator are used for generating the x ray beam.
The beam is collimated to create the ‘dose slice’ (or’__’)

A

tungsten
cone

24
Q

In fast CT scanners with rotation times in the order of magnitude of __ seconds, rotating parts are exposed to
several tenths of g forces

A

0.35

25
Q

For multi-slice scanners where the longitudinal beam width
is no longer small the X-ray beam is often referred to as __

A

cone beam

26
Q

between detectors to
prevent photons crossing to
neighbouring detectors

A

septa

27
Q

Resolution in the reconstructed images depends on
• ___ - along the detector arc and the z-axis
• The ___

A

The size of detector elements
angular separation of the projection