CHAP. VII.

Explanation of the diagram of the rotation of

_a magnetick needle_.

[Illustration]

Suppose A C D L to be the body of the earth or of a terrella, its centre M,

Æquator A D, Axis C L, A B the Horizon, which changes according to the

place. From the point F on a Horizon distant from the æquator A by the

length of C M, the semi-diameter of the earth or terrella, an arc is

described to H as the limit of the quadrants of declination; for {199} all

the quadrants of declination serving the parts from A to C begin from that

arc, and terminate at M, the centre of the earth. The semi-diameter of this

arc is a chord drawn from the æquator A to the pole C; and a line produced

along the horizon from A to B, equal to that chord, gives the beginning of

the arc of the limits of arcs of rotation and revolution, which is

continued as far as G. For just as a quadrant of a circle about the centre

of the earth (whose beginning is on the horizon, at a distance from the

æquator equal to the earth's semi-diameter) is the limit of all quadrants

of declination drawn from each several horizon to the centre; so a circle

about the centre from B, the beginning of the first arc of rotation, to G

is the limit of the arcs of rotation. The arcs of rotation and revolution

of the magnetick needle are intermediate between the arcs of rotation B L

and G L. The centre of the arc is the region itself or place in which the

observation is being made; the beginning of the arc is taken from the

circle which is the limit of rotations, and it stops at the opposite pole;

as, for example, from O to L, in a latitude of 45 degrees. Let any arc of

rotation be divided into 90 equal parts from the limit of the arcs of

rotation toward the pole; for whatever is the degree of latitude of the

place, the part of the arc of rotation which the magnetick pole on or near

the terrella or the earth faces in its rotation is to be numbered similarly

to this. The straight lines in the following larger diagram show this. The

magnetick rotation at the middle point in a latitude of 45 degrees is

directed toward the æquator, in which case also that arc is a quadrant of a

circle from the limit to the pole; but previous to this all the arcs of

rotation are greater than a quadrant, whilst after it they are smaller; in

the former the needle rotates more quickly, but in the succeeding positions

gradually more slowly. For each several region there is a special arc of

rotation, in which the limit to which the needle rotates is according to

the number of degrees of latitude of the place in question; so that a

straight line drawn from the place to the point on that arc marked with the

number of degrees of latitude shows the magnetick direction, and indicates

the degree of declination at the intersection of the quadrant of

declination which serves the given place. Take away the arc of the quadrant

of declination drawn from the centre to the line of direction; that which

is left is the arc of declination below the horizon. As, for example, in

the rotation of the versorium N, whose line respective proceeds to D, from

the quadrant of declination, S M, take away its arc R M; that which is left

is the arc of declination: how much, that is, the needle dips in the

latitude of 45 degrees.

* * * * *

{200} CHAP. VIII.

Diagram of the rotation of a magnetick needle,

_indicating magnetical declination in all latitudes, and_

from the rotation and declination, the

_latitude itself_.

In the more elaborate diagram a circle of rotations and a circle of

declinations are adjusted to the body of the earth or terrella, with a

first, a last, and a middle arc of rotation and declination. Now from each

fifth division of the arc which limits all the arcs of rotation (and which

are understood[238] as divided into 90 equal parts) arcs are drawn to the

pole, and from every fifth degree of the arc limiting the quadrants of

declination, quadrants are drawn to the centre; and at the same time a

spiral line is drawn, indicating (by the help of a movable quadrant) the

declination in every latitude. Straight lines showing the direction of the

needle are drawn from those degrees which are marked on the meridian of the

earth or a terrella to their proper arcs and the corresponding points on

those arcs.

To ascertain the elevation of the pole or the latitude of a place

anywhere

_in the world, by means of the following diagram, turned into

a magnetick instrument, without the help of the coelestial

bodies, sun, planets, or fixed stars, in fog

and darkness_.

[Illustration]

We may see how far from unproductive magnetick philosophy is, how

agreeable, how helpful, how divine! Sailors when tossed about on the waves

with continuous cloudy weather, and unable by means of the coelestial

luminaries to learn anything about the place or the region in which they

are, with a very slight effort and with a small instrument are comforted,

and learn the latitude of the place. With a declination instrument the

degree of declination of the magnetick needle below the horizon is

observed; that degree is noted on the inner arc of the quadrant, and the

quadrant is turned round about the centre of the instrument until that

degree on the quadrant touches the spiral line; then in the open space B at

the centre of the quadrant the latitude of the region on {201} the

circumference of the globe is discerned by means of the fiducial line A B.

Let the diagram be fixed on a suitable flat board, and let the centre of

the corner A of the quadrant be fastened to the centre of it, so that the

quadrant may rotate on that centre. But it must be understood that there is

also in certain places a variation in the declination on account of causes

already mentioned (though not a large one), which it will be an assistance

also to allow for on a likely estimate; and it will be especially helpful

to observe this variation in various places, as it seems to present greater

difficulty than the variation in direction; but it is easily learnt with a

declination instrument, when it dips more or less than the line in the

diagram.

[Illustration]

_To observe magnetick declination at sea_.

Set upon our variation instrument a declination instrument; a wooden disc

being placed between the round movable {202} compass and the declination

instrument: but first remove the versorium, lest the versorium should

interfere with the dipping needle. In this way (though the sea be rough)

the compass box will remain upright at the level of the horizon. The stand

of the declination instrument must be directed by means of the small

versorium at its base, which is set to the point respective of the

variation, on the great circle of which (commonly called the magnetick

meridian), the plane of the upright box is arranged; thus the declinatorium

(by its versatory nature) indicates the degree of declination.

In a declination instrument the magnetick needle, which

_in a meridional position dips, if turned

along a parallel hangs perpendicularly._

In a proper position a magnetick needle, while by its rotatory nature

conformed to the earth, dips to some certain degree below the horizon on an

oblique sphere. But when the plane of the instrument is moved out of the

plane of the meridian, the magnetick needle (which tends toward the pole)

no longer remains at the degree of its own declination, but inclines more

toward the centre; for the force of direction is stronger than that of

declination, and all power of declination is taken away, if the plane of

the instrument is on a parallel. For then the magnetick needle, because it

cannot maintain its due position on account of the axis being placed

transversely, faces down perpendicularly to the earth; and it remains only

on its own meridian, or on that which is commonly called the magnetick

meridian.

* * * * *

On the magnet, magnetick bodies also, and on the great magnet the earth a new physiology, demonstrated by many arguments & experiments · 第 93 / 110 题