Galilei, Galileo, De Motu Antiquiora

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406 which has preceded a natural motion: for even in the case of a natural motion which is preceded by a violent one, the mobile recedes as from a ratio of equality {2}, which is the ratio of rest. Now pay attention in order to understand this more clearly. {1}Let o be a mobile whose heaviness is 4: and let the line along which the violent motion takes place be oe. Thus it is manifest that in mobile o there can be impressed a force great enough to move {1} it as far as r; this force will necessarily be greater than 4, which is the heaviness of the mobile: again a force can be impressed which moves it only as far as t; again it will be greater than 4, and smaller than that which impelled it as far as r: again, a force can be impressed that is great enough to move the piece only as far as s; however it will be greater than 4, but smaller than that which impelled it as far as t: and so on, indefinitely, a force can always be impressed which will impel the mobile over any distance, however small; and yet this force will always be greater than 4. It remains, therefore, that that force is 4 which impels the mobile with a violent motion over no distance at all: from this it is evident that when mobile o recedes from the hand, it recedes with a force that is as great as 4; which then, since it is successively consumed by the heaviness, is the cause of the intensification of the motion. And what I have said will appear even more lucid if we consider that, when a heavy thing is at rest in the hand {1}, since by its heaviness it exerts pressure downward, it is necessary that it be impelled upward by something, namely the hand, with a force equal to it own heaviness, which exerts pressure downward: otherwise, unless it were hindered by another force, as great, impelling it upward, it would head downward, if the resistance were smaller; but upward, it it were greater. Therefore it is evident that, when it is abandoned by what sustains it, a heavy thing goes down with an impressed force equal to its proper heaviness; from which it follows, etc.

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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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