Design method and application of x-ray attenuator and ct device with attenuator designed by using the method
A design method and technology of attenuators, which are applied to measurement devices, instruments, scientific instruments, etc., can solve the problems of undiscovered patent publications, etc., and achieve the effects of reducing the dynamic counting range, improving the signal-to-noise ratio, and reducing the difficulty of selection.
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Embodiment 1
[0069] A kind of X-ray attenuator design method, the steps are as follows:
[0070] (1) According to the properties of the measured object, select an equivalent material close to the X-ray absorption coefficient of the measured object;
[0071] ⑵Establish the mapping relationship between the equivalent material thickness of the measured object and the attenuator thickness according to the equivalent material properties of the measured object, X-ray properties, filter properties and CT equipment parameters;
[0072] (3) According to the mapping relationship established in step (2) and the thickness distribution of X-rays passing through the equivalent material of the measured object in different directions, the thickness distribution of the attenuator is obtained;
[0073] (4) Process the attenuator according to the thickness distribution of the attenuator obtained in step (3).
[0074] Specifically, the steps can be as follows:
[0075] (1) Neglecting the influence of scatte...
Embodiment 2
[0101] A kind of X-ray attenuator design method, the steps are as follows:
[0102] Core CT scanning system such as figure 1 As shown, it consists of a ray source 2, a detector 4, a mechanical rotation system (not shown in the figure), an attenuator 1, and a control and computer (not shown in the figure). Neglecting the influence of scattering, the mathematical model of core CT is as follows:
[0103]
[0104] where x represents a point in a fixed coordinate system, μ s (E) represents the linear attenuation coefficient distribution of the equivalent material of core 3 to photons with energy E, μ a (E) represents the linear attenuation coefficient of the unit length of the attenuator to the photon of energy E, r is the thickness of the attenuator through which the ray reaches the detector unit, S(E) represents the normalized energy spectrum, where E min and E max represent the minimum and maximum values of photon energy, respectively, and I(t, r) represents the project...
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