Simultaneous reconstruction method for spherical particle optical constant and particle system particle size distribution based on forward scattering multi-angle measurement
A technology of optical constants and spherical particles, applied in the field of physical parameter measurement of spherical particles, can solve the problems of inaccurate measurement results and inability to obtain measurement results at the same time
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specific Embodiment approach 1
[0038] Specific implementation mode one: the following combination figure 1 Describe this embodiment, the simultaneous reconstruction method of spherical particle optical constant and particle size distribution based on forward scattering multi-angle measurement described in this embodiment, it includes the following steps:
[0039] Step 1: Fill the particles to be tested with the same concentration into a thickness of L 1 The first sample container is inside and the thickness is L 2 in the second sample container, so that the sample particles to be tested in the two sample containers are in a suspended state;
[0040] Step 2: Use the wavelength as λ 1 The continuous laser light vertically irradiates the left side surface of the first sample container along the thickness direction of the first sample container, and is incident on the sample particle system to be measured in the first sample container, and then along the right side of the first sample container Surface trans...
specific Embodiment approach 2
[0061] Specific implementation mode 2: This implementation mode further explains the implementation mode 1, and the inverse problem in step 4 and step 7 is realized by leapfrog algorithm.
specific Embodiment approach 3
[0062] Specific implementation mode three: this implementation mode further explains implementation mode one or two, and the specific method for obtaining the radiation intensity field in the calculation domain in step five is:
[0063]Calculated using the following radiative transfer equation:
[0064] ∂ I ( x , θ ) ∂ x = - ( κ a + κ s ) I ( x , θ ) + κ s 2 ∫ 0 π I ( x , ...
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