船船尾的磁场

E.C. Bullard , R.G. Mason
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引用次数: 38

摘要

船舶的磁化可分为永久磁化部分和感应磁化部分。如果感应部分是磁场分量的线性函数,而永久部分与磁场分量无关,则船舶对总力的扰动包含一个与磁航向无关的项,以及与航向的正弦和余弦成比例的项,并且是航向的两倍,正弦项小于余弦项的十分之一。随着船尾距离的变化类似于由于靠近船头的一根杆子和靠近船尾的一根杆子加上一条垂直偶极子线。这些结果通过实验得到了验证。“发现号”和“Sarsia”对磁场的干扰小于10 γ,距离船尾2个船长。据信,这一结果将适用于大多数船只。描述了一种确定主系数及其随距离变化的方法。
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The magnetic field astern of a ship

The magnetisation of a ship may be divided into a permanent and an induced part. If the induced part is a linear function of the field components and the permanent part is independent of them, the disturbance of the total force by the ship contains a term independent of magnetic heading and terms proportional to the sine and cosine of the heading and of twice the heading, the sine terms being less than a tenth of the cosine terms.

The variation with distance astern of the ship is similar to that due to a pole near the bow and one near the stern plus a line of vertical dipoles.

These results are verified by experiment. The disturbance of the field by Discovery II and by Sarsia is less than 10 γ at a distance of 2 ship's lengths astern. It is believed that this result will hold for most ships. A method for the determination of the principal coefficients and their variation with distance is described.

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