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Page 24
Table 3.1 Technological Improvements in the First 20 Years of Computed Tomography
| Scan Parameter
| Typical Values, 1972
| Typical Values, 1994
| | Matrix size
| 80 x 80
| 1024 x 1024
| | Spatial resolution
| 3 line pairs/cm
| 15 line pairs/cm
| | Contrast resolution
| 5 mm/5 HU/50 mGy
| 3 mm/3 HU/30 mGy
| | Scan time
| 5 min
| < 1 sec
| | Data size per scan
| 50 kByte
| 2 MByte
| | X-ray power
| 2 kW
| 40 kW
| | Definitions: mGy = milligrays, where a gray is the SI unit for radiation dose. HU = Hounsfield units; the contrast scale used in CT is defined by zero attenuation (air) = -1000 HU and attenuation coefficient of water = 0 HU (see equation 3.3).
| |
three-dimensional representation of anatomical structures.
3.1.2 Principle of Operation
The attenuation of monochromatic x-rays in homogeneous objects is governed by

where I is the x-ray intensity behind the object, I 0 is the x-ray intensity without the object, x is the length of the x-ray path through the object, and a is the linear attenuation coefficient of the material for the x-ray energy employed.
For inhomogeneous objects like the human body, the attenuation of x-rays consequently can be described by

This model is explored further in section 14.1.1.
In CT scanners the x-ray attenuation according to equation 3.2 is measured along a variety of lines within a plane perpendicular to the long axis of the patient with the goal of reconstructing a map of the attenuation coefficients a for this plane. The resulting attenuation coefficients are usually expressed with reference to water:
