Galilei, Galileo, De Motu Antiquiora

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261 through more subtle media: which is certainly false; for many are the mobiles which are moved with a natural motion faster in thicker media than in more subtle ones, as, for example, in water than in air. For if we take as an example a very thin inflated bladder, it will in air go down slowly with a natural motion; but if it is let go from deep in water, it will fly very swiftly upward, again with a natural {1} motion. But at this point I know that someone may retort that the bladder in air certainly is moved and is carried fast downward; but in water, not only it does not go down more swiftly, but it does not even go down. To this I would reply, on the contrary, that the bladder in water is carried upward very swiftly, but then in air it is not moved. But, in order not to prolong the dispute, I say that in more subtle media it is not every motion that comes about faster, but only motion downward; and motion upward is swifter in thicker media. And it is certainly reasonable that this happens: for it is necessary that where motion downward takes place with difficulty, motion upward takes place with ease. Consequently, having abandoned his opinion, in order that we may bring forth the true cause of the slowness and the swiftness of motion, care must be taken that swiftness is not separated from motion: for he who assumes motion, necessarily assumes swiftness; and slowness is nothing other than lesser swiftness. Consequently, swiftness comes from the same thing as does motion: and so, since motion comes from heaviness and lightness, it is necessary that slowness or swiftness come from the same thing; from a greater heaviness of the mobile comes a greater swiftness of that motion which happens because of the heaviness of the mobile, that is, motion downward; and from a lesser heaviness, a slowness of that same motion; and, on the other hand, from a greater lightness of the mobile will emanate a greater swiftness of that motion which happens because of the lightness of the mobile, namely motion upward. It is consequently manifest how diversity in swiftness and in slowness of motion comes about in different mobiles in motion in the same medium: for if the motion is downward, what is heavier will be moved more swiftly than what is less heavy: but if the motion is upward, what is lighter will be moved faster. But whether two mobiles carried in the same medium observe the same ratio in the swiftness of their motions as there is between their heavinesses, as Aristotle believed, will be examined below. {1} Next, concerning the swiftness and slowness of the same mobile in different media, it happens, similarly, that a mobile is moved more swiftly [262] downward in that medium in which it is heavier, than in another in which it is less heavy; and it goes up more swiftly in that medium in which it is lighter, than in another in which it is less light. {1} Hence it is manifest that, if we find in what media the same mobile will be heavier, the media will have been found in which it will go down more swiftly; but if, on the other hand, we demonstrate how much heavier the same mobile is in this medium than in that one, it will also have been demonstrated how much more swiftly it will be moved downward in this medium than in that one: and, by examining the light in converse fashion, when we find in which medium the same mobile will be lighter, a medium will have been found in which the mobile will go up more swiftly; but if we discover by how much the same mobile is lighter in this medium than in that one, it will then have been discovered how much more swiftly the mobile will go up in this medium than in that one. But, in order that all these things may be grasped with more exactitude in the case of any particular motion, treating first of all those motions that are made by different mobiles in the same medium, we will show what ratio their motions observe with one another, with respect to slowness and swiftness; next, inquiring about motions that are made by the same mobile in different media, we will similarly demonstrate what ratio they observe in motions of this sort.

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Searching "tower" (fulltextMorph)
1. Page 16, Sentence 4:How ridiculous this opinion is, is clearer than daylight: for who will ever believe that if, for example, two lead balls were released from the sphere of the Moon, one being a hundred times larger than the other, if the larger took an hour to come to Earth, the smaller would use in its motion a space of time of a hundred hours? or, if from a high tower {1}, two stones, one being double the size of the other, were thrown at the same moment, that, when the smaller was at mid-tower, the larger would already have reached the ground?
2. Page 24, Sentence 18:For if one takes two different mobiles, which have such properties that one is carried twice as swiftly as the other, and then releases them from the top of a tower, it will certainly not hit the ground faster, twice as swiftly: what is more, if one makes the observation, the one which is lighter at the beginning of the motion will precede the heavier and will be faster.
3. Page 68, Sentence 9:But this way of thinking is not only false, but ridiculous: for, if it were true, it would follow that a stone going down from a very high tower would be moved more slowly at mid-tower, than if the same stone were falling to the ground from a very low place, and for this reason the mobile [falling from a greater height] would also make a lesser impact.
4. Page 76, Sentence 3:There is a fourth well-known argument concerning a large stone going down from a tower, which will not be sufficiently blocked by a pebble impelled upward by force, so as to permit the pebble to be at rest for any time: hence surely the pebble will not be at rest at the ultimate point of its upward motion, and Aristotle notwithstanding, it will make use of the ultimate point for the two limits, namely of upward motion and of downward motion; and the ultimate instant is taken twice, namely, for the end of one time and for the beginning of the other.
5. Page 79, Sentence 4:Now in the case of heavier things, since a great amount of contrary force must be consumed in their descent, a greater time will be required for it to be consumed; in which time, since they are carried swiftly, they will descend a great distance: since we cannot avail ourselves of such great distances from which to release heavy things, it is not astonishing if the stone, released from merely the height of a tower, will seem to accelerate all the way to the ground; for this short distance and short time of motion are not sufficient to destroy the whole contrary force.
6. Page 84, Sentence 6:Yet experience shows the contrary: for it is true that wood at the beginning of its motion is carried more speedily than lead; but a little later the motion of lead is so accelerated that it leaves the wood behind, and, if they are released from a high tower, the lead gets ahead of it by a large distance: and I have often put this to the test. {1}
7. Page 134, Sentence 6:But if we go up a very high tower, on the top of which there is a bathtub, the same thing will happen to us when in it as if we were to go into the sea: for we will not be weighed down by the water, even though the latter, having air underneath it, is outside its proper place.
8. Page 150, Sentence 12:For if a stone goes down from a high tower, its swiftness seems always to be increased: yet this happens because the stone, in comparison /// with the medium through which it is carried, namely air, is very heavy; and since it goes away with an amount of impressed force as great as its heaviness, it assuredly goes away with a great impressed force, which the motion from the height of a tower is not sufficient to consume, so that the swiftness is always intensified all through the height of a single tower.

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