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Computed Tomography

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Up to 500 mA instantaneously and must provide X-rays for 30 secs ... Projection data needs to be filtered before reconstruction ... – PowerPoint PPT presentation

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Title: Computed Tomography


1
Computed Tomography
  • FRCR Examination
  • Craig Moore
  • Clinical Scientist
  • Radiation Physics Service

2
Brief History of CT Scanning
3
First CT Scanner - 1972
  • 80 x 80 resolution
  • 4 min. per rotation
  • 8 grey levels
  • overnight reconstruction
  • dual slice.

4
Here and Now
  • 512 x 512 or 1024 x 1024 resolution
  • 0.4 sec. per rotation
  • 4096 grey levels
  • Reconstruction16 secs for 30 slices
  • 64 slices.

5
Basic Principles of CT ScanningWhy CT?
  • Conventional radiography suffers from the
    collapsing of 3D structures onto a 2D image
  • Although lower resolution than general
    radiography, it has extremely good low contrast
    resolution, enabling the detection of very small
    changes in tissue type
  • CT gives accurate diagnostic information about
    the distribution of structures inside the body

6
Collapse of 3D Data into 2D Plane
  • Planar imaging
  • 2D representation of 3D Distribution of Tissue
  • No depth information
  • Structures at different depths are superimposed
  • Loss of contrast

Object Contrast 41
X rays
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X-ray Tube
  • X-rays are produced by firing electrons at a
    metal target
  • Beam filtered (0.5 mm Cu and/or 1.3 mm Al
    filters) to optimise spectrum
  • Stops attenuation coefficients varying with depth
    via beam hardening

11
  • Compton scatter predominates over the kV range
    used
  • CT is very demanding of X-ray tubes
  • Up to 500 mA instantaneously and must provide
    X-rays for 30 secs
  • Large heat capacity and fast cooling rates
  • Up to 1.4 MHU/min
  • Tube rotation causes mechanical stresses (up to
    13 G)

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CT Numbers
  • Ideally the linear attenuation coefficient ?,
    calculated by the reconstruction algorithm would
    be absolutely correct
  • Coefficients can be regarded as correct in a
    relative fashion only
  • Relative accuracy of modern scanners lt 0.1
  • A CT number is a relative value of the
    attenuation coefficient

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Window Width and Level
  • The appearance of the image on the screen can be
    changed by altering the window width and level
  • Window width refers to the range of CT numbers
    selected for display
  • This range of CT numbers is centred at a
    particular level called the window level
  • e.g. if imaging bone window level should be 1000
  • Can spread a small range of CT numbers over a
    large range of grayscale values

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Window Level 593 Window Width 529 Good contrast
in lungs
Window Level 12 Window Width 400 Good soft
tissue contrast
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How do we get the picture?
  • Back Projection
  • Reverse the process of measurement of projection
    data to reconstruct image
  • Each projection if smeared back across the
    reconstructed image

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Back Projection
  • Back Project each planar image onto three
    dimensional image matrix

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Back Projection
  • Back Project each planar image onto three
    dimensional image matrix

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Back Projection
  • Back Project each planar image onto three
    dimensional image matrix

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Back Projection
  • Back Project each planar image onto three
    dimensional image matrix

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Back Projection
  • Back Project each planar image onto three
    dimensional image matrix

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Filtered Back Projection
  • Back projection produces blurred transaxial
    images
  • Projection data needs to be filtered before
    reconstruction
  • Different filters can be applied for different
    diagnostic procedures
  • Smoother filters for viewing soft tissue
  • Sharp filters for high resolution imaging
  • Back projection same as before

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Back Projection
  • More views better reconstruction
  • 1/r blurring, even with infinite number of views

29
Filtered Back Projection
  • Filter planar views prior to back projection
  • Correction of 1/r blurring requires Ramp Filter
  • Gives increasing weight to higher spatial
    frequencies
  • Amplifies Noise

30
Filtered Back Projection
  • In Practice
  • Use modifications of Ramp Filter
  • Compromise between Noise and Spatial Resolution

31
Problems with Filtered Back Projection
  • Back projection is mathematically correct, but
    real life images require Filtered Back Projection
  • Back Projection can introduce noise and streaking
    artefacts
  • Not good with attenuation correction
  • Filtered Back Projection can reduce noise and
    artefacts, but may degrade resolution

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Xenon v Solid State
  • Xenon Single detector chamber sub-divided
    by electrodes
  • Solid state Detector array made up of
    individual elements

41
Number of detectors and projections
  • Typically, for a 3rd generation scanner
  • 650 900 detectors
  • 1000 to 2000 projections per rotation

42
Gantry Rotation
  • Data transmission and power cables in old
    scanners meant start stop rotation
  • Change direction at end of rotation to rewind
  • Series of images acquired by rotating clockwise
    and anti-clockwise
  • Scan times as fast as 1 s

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Helical and Multi-Slice Scanning
46
Requirements for Helical Scanning
  • Slip rings
  • Continuous table feed through gantry

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Advantages of Helical Scanning
  • Speed
  • No need to pause between scans for table movement
  • Pitches greater than 1 allowed
  • Longer scan lengths within breath hold
  • Reduced patient movement artefacts

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Disadvantages of Helical Scanning
  • Broadening of Slice profile
  • Effective slice thickness increases poorer z
    axis resolution
  • Higher noise
  • Helical artefacts not seen in axial scanning

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Multi Slice CT
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Each element is 1.25 mm wide
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Beam width is varied
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Physical acquisition
Computer reconstruction
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Single slice
Multi slice
Single slice
Multi slice
3 rotations
One rotation
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Dose and Multi-Slice Scanners
  • Considerations similar to those of single slice
    scanners
  • Dose utilisation on z axis usually poorer than
    with single slice scanners
  • X ray beam width is generally broader than the
    total imaged width
  • Geometric efficiency down to 50 for very small
    slice thicknesses (sub mm)

65
Geometric Efficiency
Broader beam to negate the effect of penumbra
Extra beam/x geo eff
66
Dose and Helical CT
  • All helical scanning requires extra irradiation
    at the end of each run to obtain sufficient
    interpolation data to reconstruct the required
    volume
  • On multi-slice scanners this extra length can be
    quite long

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Helical multi-slice pitch
  • Pitch can be defined with respect to total beam
    collimation (x), or individual detector width (d)
  • In practice pitchx is useful when looking at
    patient dose, pitchd for image quality
  • Pitchx table travel/xray beam width
  • Pitchd table travel/detector width

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Helical Multi-Slice in the UK
  • Helical Multi-Slice scanning represent
    significant steps forward in CT
  • Better scanning of previous scans
  • Expansion of workload
  • Nearly all scanners sold in UK are multi-slice
  • Technology is still advancing
  • 32/40/64/256 slice scanners now available
  • More slices in the future?
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