| Isaac Newton - Celestial mechanics - 1729 - 444 pages
...towards the horfe, and will obftrudt the progrefs of the one as much as it advances that of the other. If a body impinge upon another > and by its force change the motion of the other ; that body alfo (becaufe of the equality of {he mutual preflure,) will undergo an equal change* in its own motion,... | |
| Thomas Banks Strong - Double stars - 1906 - 282 pages
...of impact by Sir Christopher Wren's experiments before the Royal Society, which proved that, if one body impinge upon another, and by its force change the motion of the other, that first body also, because of the equality of the mutual pressure, will undergo an equal change in its... | |
| Thomas Banks Strong - Double stars - 1906 - 270 pages
...of impact by Sir Christopher Wren's experiments before the Royal Society, which proved that, if one body impinge upon another, and by its force change the motion of the other, that first body also, because of the equality of the mutual pressure, will undergo an equal change in its... | |
| Richard De Villamil - Mechanics, Analytic - 1928 - 240 pages
...relies on Newton's references to impact, let us turn to the Principia, where we read (Law III) : " If a body impinge upon another, and by its force change...also (because of the equality of the mutual pressure) — [equality of action and reaction] — will undergo an equal change in its motion [momentum]. .... | |
| Igor Hanzel - Philosophy - 1999 - 250 pages
...as "absolute force." This is readily seen from the commentary on the third law (1946, 14; 1687 [13]) If a body impinge upon another, and by its force change the motion of the other, that body also . . . will undergo an equal change, in its own motion, towards the contrary pan. So this law in fact... | |
| Jan Faye, Paul Needham, Uwe Scheffler, Max Urchs - Science - 2005 - 312 pages
...parts" (Newton, 1946, 13; Newton, 1999, 417). This is readily seen from the commentary on the third law "If a body impinge upon another, and by its force change the motion of the other, that body also [. . . ] will undergo an equal change, in its own motion, towards the contrary part" (Newton, 1946,... | |
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