Chap. v.
How the Power dwells in the Loadstone.
T hat a loadstone attracts loadstone, iron and other magnetical bodies, has been shown above in the previous book, and also with what strength the magnetick coition is ordered; but now we must inquire how that vigour1 is disposed in a magnetick substance. And indeed an analogy must be inferred from a large loadstone. Any magnetick substance joins itself with a loadstone strongly, if the loadstone itself is strong; but more weakly, when it is somewhat imperfect or has been weakened by some flaw. A loadstone does not draw iron equally well with every part; or a magnetick substance does not approach every part of a loadstone alike; because a loadstone has its points, that is its true poles, in which an exceptional virtue2 excels. Parts nearer the pole are stronger, those far away more weak, and yet in all the power is in a certain way equal. The poles of a terrella are A, B; the æquinoctial is C, D. At A and B the alluring3 force seems greatest.
At C and D there is no force alluring magnetick ends to the body, for the forces tend toward both poles. But direction is powerful on the æquator. At C, D, the distances are equal from both poles; therefore iron which is at C, D, when it is allured4 in contrary ways, does not adhære with constancy; but it remains5 and is joined to the stone, if only it incline to the one or other side. At E there is a greater power of alluring than at F, because E is nearer the pole. This is not so because there is really greater virtue residing at the pole, but since all the parts are united in the whole, they direct their forces towards the pole. From the forces flowing from the plane of the æquinoctial towards the pole, the power increases. A fixed6 verticity exists at the pole, so long as the loadstone remains whole; if it is divided or broken, the verticity obtains other positions in the parts into which it is divided. For the verticity always changes in consequence of any change in the mass, and for this cause, if the terrella be divided from A to B, so that there are two stones, the poles will not be A, B, in the divided parts, but F, G, and H, I.
Although these stones now are in agreement with one another, so that F would not seek H, yet if A was previously7 the boreal pole163, F is now boreal, and H also boreal; for the verticity is not changed (as Baptista Porta incorrectly affirms in the fourth chapter of his seventh book); since, though F and H do not agree, so that the one would incline to the other, yet both turn to the same point of the horizon. If the hemisphere H I be divided into two quadrants, the one pole takes up its position in H, the other in I. The whole mass of the stone, as I have said, retains the site of its vertex constant; and any part of the stone, before it was cut out from the block164, might have been the pole or vertex. But concerning this more under Direction. It is important now to comprehend and to keep firmly in mind that the vertices are strong on account of the force of the whole, so that (the command being, as it were, divided by the æquinoctial) all the forces on one side tend towards the north; but those of an opposite way towards the south, so long as the parts are united, as in the following demonstration8.
For so, by an infinite number of curves from every point of the equator dividing the sphere into two equal parts, and from every point of the surface from the æquator towards the North, and from the æquator towards the Southern pole, the whole force tends asunder9 toward the poles. So the verticity is from the æquinoctial circle towards the pole in each direction. Such is the power reposed10 in the undivided stone. From A vigour is sent to B, from A, B, to C, from A, B, C, to D, and from them likewise to E. In like manner from G to H, and so forth11, as long as the whole is united. But if a piece A B be cut out (although it is near the æquator), yet it will be as strong in its magnetical actions as C D or D E, if torn away from the whole in equal quantity. For no part excels in special worth in the whole mass except by what is owing to the other adjoining parts by which an absolute and perfect whole is attained12.
Diagram of Magnetic Vigour transmitted from
the plane of the Æquator to the peripherery of
the terella or of the earth
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1 vigour | |
(=vigor)n.智力,体力,精力 | |
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2 virtue | |
n.德行,美德;贞操;优点;功效,效力 | |
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3 alluring | |
adj.吸引人的,迷人的 | |
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4 allured | |
诱引,吸引( allure的过去式和过去分词 ) | |
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5 remains | |
n.剩余物,残留物;遗体,遗迹 | |
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6 fixed | |
adj.固定的,不变的,准备好的;(计算机)固定的 | |
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7 previously | |
adv.以前,先前(地) | |
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8 demonstration | |
n.表明,示范,论证,示威 | |
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9 asunder | |
adj.分离的,化为碎片 | |
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10 reposed | |
v.将(手臂等)靠在某人(某物)上( repose的过去式和过去分词 ) | |
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11 forth | |
adv.向前;向外,往外 | |
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12 attained | |
(通常经过努力)实现( attain的过去式和过去分词 ); 达到; 获得; 达到(某年龄、水平、状况) | |
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13 periphery | |
n.(圆体的)外面;周围 | |
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14 eminence | |
n.卓越,显赫;高地,高处;名家 | |
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15 axis | |
n.轴,轴线,中心线;坐标轴,基准线 | |
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16 mighty | |
adj.强有力的;巨大的 | |
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17 intervals | |
n.[军事]间隔( interval的名词复数 );间隔时间;[数学]区间;(戏剧、电影或音乐会的)幕间休息 | |
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