CHAP. XI.

On the Rubbing of a piece of Iron on a Loadstone

in places midway between the poles, and upon

_the æquinoctial of a terrella_.

Select a piece of iron wire of three digits length, not touched by a

loadstone (but it will be better if its acquired verticity be rather weak

or have been damaged in some way); touch it and rub it on the æquator of a

terrella, exactly on the æquinoctial line in the direction of its length,

on the one end, or the ends only, or in all its parts; place the wire

touched in this * way on water in a cork fitted for it; it will swim about

doubtfully on the waves without any acquired verticity, and the verticity

previously implanted will be disturbed. If, however, it float by chance

toward the poles, it will be checked a little by the poles of the earth,

and will at length by the influence of the earth be indued with verticity.

* * * * *

{139} CHAP. XII.

In what way Verticity exists in any Iron that has

_been smelted though not excited by a lodestone_.

[Illustration]

Having thus far[211] demonstrated natural and inborn causes and powers

acquired by means of the stone, we will now examine the causes of magnetick

virtues in smelted iron that has not been excited by a stone. Loadstone and

iron furnish and exhibit to us wonderful subtilities. It has been

repeatedly shown above that iron not excited by a stone turns north and

south; further that it has verticity, that is, special and peculiar polar

distinctions, just as a loadstone, or iron which has been rubbed upon a

loadstone. This indeed seemed to us at first wonderful and incredible; the

metal of iron from the mine is smelted in the furnace; it runs out of the

furnace, and hardens into a great mass; this mass is divided in great

worksteads, and is drawn into iron bars, from which smiths again construct

many instruments and necessary pieces of iron-work. Thus the same mass is

variously worked up and transformed into very many similitudes. What is it,

then, which {140} preserves its verticity, and whence is it derived? So

take this first from the above[212] smithy. Let the blacksmith beat out

upon his anvil a glowing mass of iron of two or three ounces weight into an

iron spike of the length of a span of nine inches. Let the smith be

standing with his face to the north, his back to the south, so that * the

hot iron on being struck has a motion of extension to the north; and let

him so complete his work with one or two heatings of the iron (if that be

required); let him always, however, whilst he is striking the iron, direct

and beat out the same point of it toward the north, and let him lay down

that end toward the north. Let him in this way complete two, three, or more

pieces of iron, nay, a hundred or four hundred; it is demonstrable that all

those which are thus beaten out toward the north, and so placed whilst they

are cooling, turn round on their centres; and floating pieces of iron

(being transfixed, of course, through suitable corks) make a motion in the

water, the determined end being toward the north. In the same way also

pieces of iron acquire verticity from their direction whilst they are being

beaten out and hammered or drawn out, * as iron wires are accustomed to do

toward some point of the horizon between east and south or between south

and west, or in the opposite direction. Those, however, which are pointed

or drawn out rather toward the eastern or western point, conceive * hardly

any verticity or a very undecided one. That verticity is especially

acquired by being beaten out. But a somewhat inferior iron ore, in which no

magnetick powers are apparent, if put in a * fire (its position being

observed to be toward the poles of the world or of the earth) and heated

for eight or ten hours, then cooled away from the fire, in the same

position towards the poles, acquires a verticity in accordance with the

position of its heating and cooling. Let a rod of cast iron be heated

red-hot in a strong fire, in which it lies * meridionally (that is, along

the path of a meridian circle), and let be removed from the fire and

cooled, and let it return to its former temperature, remaining in the same

position as before; then from this it will turn out that, if the same ends

have been turned to the same poles of the earth, it will acquire verticity,

and the end which looked toward the North on water with a cork before the

heating, if it have been placed during the heating and cooling toward the

fourth, now turns round to the south. But if perchance sometimes the

rotation have been doubtful and somewhat feeble, let it be placed again in

the fire, and when it is taken out at a red heat, let it be perfectly

cooled toward the pole from which we desire the verticity, and the

verticity will be acquired. Let the same rod be heated * in the contrary

position, and let it be placed so at a red heat it is cool; for it is from

its position in cooling (by the operation of the verticity of the earth)

that verticity is put into the iron, and it turns round to parts contrary

to its former verticity. So {141} the end which formerly looked toward the

north now turns to the south. In accordance with these reasonings and in

these ways the boreal pole of the earth gives to the end of a piece of iron

turned toward it a southern verticity, and that end is attracted by that

pole. * And here it must be observed that this happens to iron not only

when it is cooled in the plane of the horizon, but also at any angle to it

almost up to the perpendicular toward the centre of the earth. So the

heated iron conceives vigour and verticity from the earth more quickly in

the course of its return to its normal state, and in its recovery, as it

were (in the course of which it is transformed), than by its mere position

alone. This is effected better and more * perfectly in winter and in colder

air, when the metal returns more certainly to its natural temperature, than

in summer and in warm regions. Let us see also what position alone and a

direction toward the poles of the earth can effect by itself without fire

and heat. Iron rods which have been placed and fixed for a long time,

twenty * or more years, from south to north (as they not infrequently are

fixed in buildings and across windows), those rods, I say, by that long

lapse of time acquire verticity and turn round, whether hanging in the air,

or floating (being placed on cork), to the pole toward which they were

pointing, and magnetically attract and repel a balanced iron magnetick; for

the long continued position of the body toward the poles is of much avail.

This fact (although conspicuous by manifest experiments) is confirmed by an

incident related in an Italian letter[213] at the end of a book of Maestro

Filippo Costa, of Mantua, _Sopra le Compositioni degli Antidoti_ written in

Italian, which translated runs thus: "A druggist of Mantua showed me a

piece of iron entirely changed into a magnet, drawing another piece of iron

in such a way that it could be compared with a loadstone. Now this piece of

iron, when it had for a long time held up a brick ornament on the top of

the tower of the church of St. Augustine at Rimini, had been at length bent

by the force of the winds, and remained so for a period of ten years. When

the monks wished to bend it back to its former shape, and had handed it

over to a blacksmith, a surgeon named Maestro Giulio Caesare discovered

that it was like a magnet and attracted iron." This was caused by the

turning of its extremities toward the poles for so long a time. And so what

has been laid down before about change of verticity should be borne in

mind; how in fact the poles of iron spikes are altered, when a loadstone is

placed against them only with its pole and points toward them, even at a

rather long distance. Clearly it is in the same way that that large magnet

also (to wit, the earth itself) affects a piece of iron and changes its

verticity. For, although the iron may not touch the pole of the earth, nor

any magnetick part of the earth, yet verticity is acquired and changed; not

because the poles of the earth and the point itself which is 39° distant

{142} from our city of London, changes the verticity at a distance of so

many miles; but because the whole magnetick earth, that which projects to a

considerable height, and to which the iron is near, and that which is

situated between us and the pole, and the vigour existing within the orbe

of its magnetick virtue (the nature of the whole conspiring thereto),

produces the verticity. For the magnetick effluence of the earth rules

everywhere within the orbe of its virtue, and transforms bodies; but those

things which are more similar to it, and specially connected with it by

nature, it rules and controls; as loadstone and iron. Wherefore in very

many matters of business and actions it is clearly not superstitious and

idle to observe the positions and conditions of lands, the points of the

horizon and the places of the stars. For as when a babe is brought forth

into the light from its mother's womb, and acquires respiration and certain

animal activities, then the planets and celestial bodies[214], according to

their position in the universe, and according to that configuration which

they have with regard to the horizon and the earth, instil peculiar and

individual qualities into the newly born; so that piece of iron, whilst it

is being formed and lengthened out, is affected by the common cause (to

wit, the earth); whilst it is returning also from its heated condition to

its former temperature, it is imbued with a special verticity in accord

with its position. Rather long pieces of iron sometimes have the same

verticity * at each end; wherefore they have motions which are less certain

and well ordered on account of their length and of the aforesaid processes,

exactly as when an iron wire four feet long is rubbed at each end upon the

same pole of a loadstone.

* * * * *

On the magnet, magnetick bodies also, and on the great magnet the earth a new physiology, demonstrated by many arguments & experiments · 第 66 / 110 题