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水体MTF的推导

何大华 许东阳 方珍

何大华, 许东阳, 方珍. 水体MTF的推导[J]. 中国光学(中英文). doi: 10.37188/CO.2026-0010
引用本文: 何大华, 许东阳, 方珍. 水体MTF的推导[J]. 中国光学(中英文). doi: 10.37188/CO.2026-0010
HE Da-hua, XU Dong-yang, FANG Zhen. Derivation of water MTF[J]. Chinese Optics. doi: 10.37188/CO.2026-0010
Citation: HE Da-hua, XU Dong-yang, FANG Zhen. Derivation of water MTF[J]. Chinese Optics. doi: 10.37188/CO.2026-0010

水体MTF的推导

cstr: 32171.14.CO.2026-0010
基金项目: 船舶重工装备预研联合基金(No. 6141B042006)
详细信息
    作者简介:

    何大华(1973—),男,湖北武汉人,博士,高级工程师,主要从事水下光电成像及图像处理方面的研究。E-mail:470444534@qq.com

  • 中图分类号: P733.3

Derivation of water MTF

Funds: Supported by China Shipbuilding Industry Corporation Joint fund for Equipment Pre-Research (No. 6141B042006)
More Information
  • 摘要:

    水体对光线的多次散射会形成水下光场,水下光场的存在使水下光电成像质量显著恶化,为了对水下光电图像质量退化进行定量分析,需要研究水下光场分布,建立严格的水下图像传输模型。假定水体体散射函数为球形对称,首先计算出理想点光源的水下光场分布,然后通过沿路径的亮度积分得到水体点扩展函数,最后借助于球谐函数与球面卷积等数学工具推导出球面空间中的水体调制传递函数。在已知水体固有光学参数的条件下,给出了水体调制传递函数以及对比度极限因子的图象。该算法模型解决了球形体散射函数条件下的水体调制传递函数推导问题,为解决非球形体散射函数及动态光场条件下水体调制传递函数的推导问题奠定了基础。

     

  • 图 1  理想水下光电成像模型

    Figure 1.  Ideal underwater optoelectronic imaging model

    图 2  点光源形成的水下光场(c=0.1/m, b=0.05/m)

    Figure 2.  Underwater light field formed by point light source (c=0.1/m, b=0.05/m)

    图 3  水体PSF求解原理图

    Figure 3.  Schematic diagram for solving water PSF

    图 4  在2AL处的水体PSF(c=0.1/m, b=0.05/m)

    Figure 4.  Water PSF at 2AL(c=0.1/m, b=0.05/m)

    图 5  水体MTF求解流程图

    Figure 5.  Flow chart for solving water MTF

    图 6  在2AL处的水体MTF曲线(c=0.1/m, b=0.05/m)

    Figure 6.  Water MTF at 2AL(c=0.1/m, b=0.05/m)

    图 7  不同水体的对比度极限因子曲线(红色曲线:c=0.1/m, b=0.03/m;黑色曲线:c=0.1/m, b=0.05/m;绿色曲线: c=0.1/m, b=0.07/m)

    Figure 7.  Limit of MTF of different types of water (Red: c=0.1/m, b=0.03/m; Black: c=0.1/m, b=0.05/m; Green: c=0.1/m, b=0.07/m)

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出版历程
  • 收稿日期:  2026-01-24
  • 录用日期:  2026-03-31
  • 网络出版日期:  2026-04-21

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