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Handbook of Magnetic Compass Adjustment - Maritime Safety ...

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CHAPTER II<br />

MAGNETISM<br />

201. The magnetic compass. The principle <strong>of</strong> the present day magnetic compass is in no way different from that <strong>of</strong> the<br />

compass used by the ancients. It consists <strong>of</strong> a magnetized needle, or array <strong>of</strong> needles, pivoted so that rotation is in a<br />

horizontal plane. The superiority <strong>of</strong> the present day compass results from a better knowledge <strong>of</strong> the laws <strong>of</strong> magnetism,<br />

which govern the behavior <strong>of</strong> the compass, and from greater precision in construction.<br />

202. Magnetism. Any piece <strong>of</strong> metal on becoming magnetized, that is, acquiring the property <strong>of</strong> attracting small particles <strong>of</strong><br />

iron or steel, will assume regions <strong>of</strong> concentrated magnetism, called poles. Any such magnet will have at least two poles, <strong>of</strong><br />

unlike polarity. <strong>Magnetic</strong> lines <strong>of</strong> force (flux) connect one pole <strong>of</strong> such a magnet with the other pole as indicated in figure<br />

202. The number <strong>of</strong> such lines per unit area represents the intensity <strong>of</strong> the magnetic field in that area. If two such magnetic<br />

bars or magnets are placed side by side, the like poles will repel each other and the unlike poles will attract each other.<br />

Figure 202 – Lines <strong>of</strong> magnetic force about a magnet<br />

203. Magnetism is in general <strong>of</strong> two types, permanent and induced. A bar having permanent magnetism will retain its<br />

magnetism when it is removed from the magnetizing field. A bar having induced magnetism will lose its magnetism when<br />

removed from the magnetizing field. Whether or not a bar will retain its magnetism on removal from the magnetizing field<br />

will depend on the strength <strong>of</strong> that field, the degree <strong>of</strong> hardness <strong>of</strong> the iron (retentivity), and also upon the amount <strong>of</strong> physical<br />

stress applied to the bar while in the magnetizing field. The harder the iron the more permanent will be the magnetism<br />

acquired.<br />

204. Terrestrial magnetism. The accepted theory <strong>of</strong> terrestrial magnetism considers the earth as a huge magnet surrounded<br />

by lines <strong>of</strong> magnetic force that connect its two magnetic poles. These magnetic poles are near, but not coincidental, with the<br />

geographic poles <strong>of</strong> the earth. Since the north-seeking end <strong>of</strong> a compass needle is conventionally called a red pole, north pole,<br />

or positive pole, it must therefore be attracted to a pole <strong>of</strong> opposite polarity, or to a blue pole, south pole, or negative pole.<br />

The magnetic pole near the north geographic pole is therefore a blue pole, south pole, or negative pole; and the magnetic pole<br />

near the south geographic pole is a red pole, north pole, or positive pole.<br />

205. Figure 205 illustrates the earth and its surrounding magnetic field. The flux lines enter the surface <strong>of</strong> the earth at<br />

different angles to the horizontal, at different magnetic latitudes. This angle is called the angle <strong>of</strong> magnetic dip, θ, and<br />

increases from zero, at the magnetic equator, to 90° at the magnetic poles. The total magnetic field is generally considered as<br />

having two components, namely H, the horizontal component, and Z, the vertical component. These components change as<br />

the angle θ changes such that H is maximum at the magnetic equator and decreases in the direction <strong>of</strong> either pole; Z is zero at<br />

the magnetic equator and increases in the direction <strong>of</strong> either pole.<br />

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