I will be the depth on the incident radiation, dx would be the thickness of the material and μ is the material attenuation coefficient. μ primarily is made up of contributions through the photoelectric absorption impact as well as Compton scattering. If we take the integral on both sides we get hold ofRadiography - only one image is recorded for

Previously mentioned equation demonstrates us the SNR of the X-ray imaging system obviously is dependent upon the item, represented by e−twelve∫μ(x)dx and also on the amount of produced photons within the source N0. The SNR is proportional on the sq. root of the volume of emitted X-ray photons, hence growing the quantity of photons also enhanc

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