• Acta Photonica Sinica
  • Vol. 49, Issue 8, 0812002 (2020)
Gao-fei GU, Jun ZHAO, Ming KONG*, Tian-tai GUO, and Dao-dang WANG
Author Affiliations
  • College of Metrology and Measurement Engineering, China Jiliang University, Hangzhou 310018, China
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    DOI: 10.3788/gzxb20204908.0812002 Cite this Article
    Gao-fei GU, Jun ZHAO, Ming KONG, Tian-tai GUO, Dao-dang WANG. Tomographic Three-dimensional Particle Position Measurement Based on Light Field Camera[J]. Acta Photonica Sinica, 2020, 49(8): 0812002 Copy Citation Text show less

    Abstract

    A light field camera is used to collect particle images, and the tomographic inversion algorithm is improved to obtain the three-dimensional spatial position of particles faster and more accurately. Based on imaging principle of the light field camera, a forward tracing model of light emitted by particles is established. On the basis of this model, a tomographic inversion model is constructed to reversely trace rays emitted from non-zero pixels and realize the mapping between non-zero pixels and spatial voxels. A descending dimension method is proposed to calculate the weighting matrix. The depth accuracy of MART algorithm is improved by combined with the similar triangle principle. According to the Gaussian Blob model, center position of voxel with the strongest intensity is taken as the three-dimensional position of particles. Experiments indicate that the improved MART algorithm can significantly reduce calculation time and memory size while meeting the accuracy requirement. The x-axis coordinate error is ±0.16 mm. The y-axis coordinate error is ±0.18 mm. The z-axis coordinate error is ±1.8 mm. It is more suitable for occasions that demand higher calculation speed and has better practical application value.
    $L = L\left( {x, y, x{\rm{'}}, y{\rm{'}}} \right) $ (1)

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    $\left[ {\begin{array}{*{20}{c}} {{x_1}}\\ {{y_1}}\\ {{\rm{tan}}{\theta _1}}\\ {{\rm{tan}}{\phi _1}} \end{array}} \right] = \left[ {\begin{array}{*{20}{c}} 1&0&{{s_{\rm{o}}}}&0\\ 0&1&0&{{s_{\rm{o}}}}\\ 0&0&1&0\\ 0&0&0&1 \end{array}} \right]\left[ {\begin{array}{*{20}{c}} {{x_0}}\\ {{y_0}}\\ {{\rm{tan}}{\theta _0}}\\ {{\rm{tan}}{\phi _0}} \end{array}} \right] $ (2)

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    $\left[ {\begin{array}{*{20}{c}} {{x_2}}\\ {{y_2}}\\ {{\rm{tan}}{\theta _2}}\\ {{\rm{tan}}{\phi _2}} \end{array}} \right] = \left[ {\begin{array}{*{20}{c}} 1&0&0&0\\ 0&1&0&0\\ { - 1/{f_{\rm{m}}}}&0&1&0\\ 0&{ - 1/{f_{\rm{m}}}}&0&1 \end{array}} \right]\left[ {\begin{array}{*{20}{c}} {{x_1}}\\ {{y_1}}\\ {{\rm{tan}}{\theta _1}}\\ {{\rm{tan}}{\phi _1}} \end{array}} \right] $ (3)

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    $\left[ {\begin{array}{*{20}{c}} {{x_3}}\\ {{y_3}}\\ {{\rm{tan}}\theta {}_3^{}}\\ {{\rm{tan}}{\phi _3}} \end{array}} \right] = \left[ {\begin{array}{*{20}{c}} 1&0&{{s_{\rm{i}}}}&0\\ 0&1&0&{{s_{\rm{i}}}}\\ 0&0&1&0\\ 0&0&0&1 \end{array}} \right]\left[ {\begin{array}{*{20}{c}} {{x_2}}\\ {{y_2}}\\ {{\rm{tan}}\theta _2^{}}\\ {{\rm{tan}}{\phi _2}} \end{array}} \right] $ (4)

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    $\left[ {\begin{array}{*{20}{c}} {{x_4}}\\ {{y_4}}\\ {{\rm{tan}}{\theta _4}}\\ {{\rm{tan}}{\phi _4}} \end{array}} \right] = \left[ {\begin{array}{*{20}{c}} 1&0&0&0\\ 0&1&0&0\\ { - 1/{f_{\rm{l}}}}&0&1&0\\ 0&{ - 1/{f_{\rm{l}}}}&0&1 \end{array}} \right]\left[ {\begin{array}{*{20}{c}} {{x_3}}\\ {{y_3}}\\ {{\rm{tan}}{\theta _3}}\\ {{\rm{tan}}{\phi _3}} \end{array}} \right] + \left[ {\begin{array}{*{20}{c}} 0\\ 0\\ {{s_x}/{f_{\rm{l}}}}\\ {{s_y}/{f_{\rm{l}}}} \end{array}} \right] $ (5)

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    $\left[ {\begin{array}{*{20}{c}} {x{}_5^{}}\\ {{y_5}}\\ {{\rm{tan}}{\theta _5}}\\ {{\rm{tan}}{\phi _5}} \end{array}} \right] = \left[ {\begin{array}{*{20}{c}} 1&0&{{f_{\rm{l}}}}&0\\ 0&1&0&{{f_{\rm{l}}}}\\ 0&0&1&0\\ 0&0&0&1 \end{array}} \right]\left[ {\begin{array}{*{20}{c}} {{x_4}}\\ {{y_4}}\\ {{\rm{tan}}{\theta _4}}\\ {{\rm{tan}}{\phi _4}} \end{array}} \right] $ (6)

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    $E\left( {x, y, z} \right) = A{\rm{exp}}\left[ { - \left( {\frac{{{{(x - {x_0})}^2}}}{{2\sigma _x^2}} + \frac{{{{(y - {y_0})}^2}}}{{2\sigma _y^2}} + \frac{{{{(z - {z_0})}^2}}}{{2\sigma _z^2}}} \right)} \right] $ (7)

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    $\mathop \sum \limits_{j \in {N_i}} {W_{i, j}}E\left( {{x_j}, {y_j}, {z_j}} \right) = I\left( {{x_i}, {y_i}} \right) $ (8)

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    $E{({x_j}, {y_j}, {z_j})^{k + 1}} = E{({x_j}, {y_j}, {z_j})^k}{\left( {\frac{{I\left( {{x_i}, {y_i}} \right)}}{{\mathop \sum\limits_{j \in {N_j}} {W_{i, j}}E{{({x_j}, {y_j}, {z_j})}^k}}}} \right)^{\mu {W_{i, j}}}} $ (9)

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    $W = \frac{1}{{\sqrt {2{\rm{\pi }}\sigma } }}{{\rm{e}}^{ - \frac{{{d^2}}}{{2{\sigma ^2}}}}} $ (10)

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    Gao-fei GU, Jun ZHAO, Ming KONG, Tian-tai GUO, Dao-dang WANG. Tomographic Three-dimensional Particle Position Measurement Based on Light Field Camera[J]. Acta Photonica Sinica, 2020, 49(8): 0812002
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