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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