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船舶磁场动态检测中磁场反演校正方法

周国华,夏帅,吴轲娜*,奉之翔,凌志   

  1. (海军工程大学 电气工程学院, 湖北武汉430033)
  • 收稿日期:2024-12-24 修回日期:2025-04-24
  • 通讯作者: *通信作者邮箱:kenawu@163.com
  • 基金资助:
    国家自然科学基金项目((52207020)

Magnetic Field Inversion Correction Method in Dynamic Detection of Ship’s Magnetic Field

ZHOU Guohua, XIA Shuai, WU Kena*, FENG Zhixiang, LING Zhi   

  1. (School of Electrical Engineering, Naval University of Engineering, Wuhan 430000, Hubei, China)
  • Received:2024-12-24 Revised:2025-04-24

摘要: 鉴于船舶磁场动态检测具有测量设备简单、隐蔽性好、建造成本低等优势,其已成为世界各国海军争相发展的一种船舶磁场检测方式,但磁场动态检测过程中姿态等航行动态因素变化会导致较大的磁场测量误差。本文基于船舶磁场动态检测的基本原理,建立船舶磁场动态检测数学模型,据此详细模拟分析了各动态因素对测量磁场的影响程度,并提出计及各动态因素影响的测量磁场反演校正方法,即通过动态测量多源数据构建船舶等效磁性反演校正模型,用lasso回归求解,继而通过反演等效磁性参数实现动态测量过程的磁场数据校正。算例结果表明,船舶在4个不同航行方向上的磁场动态检测中当航向、纵倾、横摇的动态变化幅值为2º、1º、1º,测磁噪声为20nT时,测量磁场的最大绝对误差为493nT、相对误差不小于5.32%。使用本方法进行校正后,在典型测量条件下航向、纵倾、横摇和测磁噪声为0.1º、0.01º、0.01º和5nT时,校正后磁场的最大绝对误差为22nT,相对误差不超过0.55%。物理缩比模型实验表明,船舶在4个不同航行方向上的磁场动态测量中当航向动态变化幅值为4º,校正前的最大绝对误差为374nT、相对误差不小于3.44%,校正后磁场的最大绝对误差为146nT、相对误差不超过2.35%。该方法对提高船舶磁场动态检测准确度精度及推广应用具有很好地工程指导意义。

关键词: 磁场动态检测, 等效磁性模型, 磁偶极子, 磁场校正

Abstract: As the dynamic detection of ship magnetic fields has the advantages of simple measuring equipment, high-level concealment and low construction cost, it has become a ship magnetic field detection method that is being actively developed by navies all over the world. Based on the basic principles of the dynamic detection of ship magnetic fields, this paper establishes a mathematical model for the dynamic detection of ship magnetic fields. Accordingly, it simulates and analyzes the influence degree of various dynamic factors on the measured magnetic field in detail, and proposes an inversion correction method for the measured magnetic field considering the influence of these dynamic factors. Specifically, an equivalent magnetic inversion correction model of the ship is constructed by using multi-source dynamic measurement data, which is solved by lasso regression. Subsequently, the magnetic field data in the dynamic measurement process is corrected by inverting the equivalent magnetic parameters. The experimental results demonstrate that during the dynamic magnetic field detection in four different navigation directions, the dynamic variation ranges for the ship's heading, trim, and roll are 2°, 1°, and 1°, respectively. When the magnetic measurement noise is 20 nT, the maximum absolute error in the measured magnetic field is 493 nT, with a relative error of no less than 5.32%. After applying the correction method proposed in this study, under typical measurement conditions where the heading, trim, roll, and magnetic measurement noise are 0.1°, 0.01°, 0.01°, and 5 nT, the maximum absolute error in the corrected magnetic field is reduced to 22 nT, with the relative error not exceeding 0.55%. Physical scale model experiments have shown that in the dynamic measurement of the magnetic field in four different sailing directions of a ship, when the amplitude of dynamic heading change is 4º, the maximum absolute error before correction is 374 nT, and the relative error is no less than 3.44%. After correction, the maximum absolute error of the magnetic field is 146 nT, and the relative error is no more than 2.35% . This method has great engineering guiding significance for improving the accuracy and application scope of the dynamic detection of ship magnetic fields.

Key words: magnetic field dynamic detection, equivalent magnetic model, magnetic dipole, magnetic field correction