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Computed Tomography. Basic principles. V.G.Wimalasena Principal School of Radiography. Introduction. Computed tomography (CT) is a medical imaging method employing tomography . The word "tomography" is derived from the Greek tomos (slice) and graphein (to write).

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computed tomography

Computed Tomography

Basic principles

V.G.Wimalasena

Principal

School of Radiography

slide2

Introduction

  • Computed tomography (CT) is a medical imaging method employing tomography.
  • The word "tomography" is derived from the Greektomos (slice) and graphein (to write).
  • A large series of two-dimensional X-ray images (slices) of the inside of an object are taken around a single axis of rotation.
  • Digital geometry processing is used to generate three-dimensional images of the object from those slices.
slide3

History

  • The first commercially viable CT scanner was invented by Sir Godfrey Hounsfield in Hayes, United Kingdom at EMI Central Research Laboratories using X-rays. Hounsfield conceived his idea in 1967. and it was publicly announced in 1972.
  • Allan McLeod Cormack of Tufts University in Massachusetts independently invented a similar process, and both Hounsfield and Cormack shared the 1979 Nobel Prize in Medicine.
slide7

Label

  • gantry aperture (720mm diameter)
  • microphone
  • sagittal laser alignment light
  • patient guide lights
  • x-ray exposure indicator light
  • emergency stop buttons
  • gantry control panels
  • external laser alignment lights
  • patient couch
  • ECG gating monitor
slide9

Label

  • x-ray tube
  • filters, collimator, and reference detector
  • internal projector
  • x-ray tube heat exchanger (oil cooler)
  • high voltage generator (0-75kV)
  • direct drive gantry motor
  • rotation control unit
  • data acquisition system (DAS)
  • detectors
  • slip rings
slide10

Understanding Basic factors

  • Absorption :-stopping of x-rays with transfer of energy
  • Scatter:- deflection of x-rays
  • Incident Intensity :- No. of x-ray photons falling on an object
  • Transmitted Intensity:- No. of photons passing through

Scattered x-rays

Transmitted X-ray beam

Incident x-ray beam

slide11

Attenuation

The reduction of the beam intensity on passing through the material due to absorption plus scatter

The degree of attenuation is obtained by measuring and comparing the incident and transmitted intensities

More dense material

Less transmitted x-rays

More transmitted x-rays

Less dense material

slide12

Applications of X-ray attenuation & detection

  • Conventional X-ray (Radiography)
  • Conventional Tomography
  • Computed Tomography
slide13

Conventional X-Ray

  • Conventional x-ray produces a compression of a volume to a plane
  • The detector is the Silver halide crystal on a x-ray film
  • The degree of blackening represents the total attenuation through the path of x-ray photons
slide14

The higher the attenuation the lesser is the blackness

  • The structurewhich results more attenuation or more transmission predominates in the image
slide15

Conventional Tomography

  • The source and detector moves
  • Produces Images of coronal or sagittal sections (cuts) of areas of interest
  • Eliminates the superimposition of structures above and below
slide16

CT Scan

  • CT scan produces axial sections/cuts /Slices
  • The CT image is recorded through a SCAN.
  • Scan?
  • A scan is made up of multiple X-Ray attenuation measurements around an objects periphery

X-ray tube

Detector

slide17

Slice / Cut

  • The cross sectionalportion of the body which is scanned for the production of CT image is called a slice.
  • The slice has width and therefore volume.
  • The width is determined by the width of the x-ray beam

To be continued ….CTComplementary2

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