| Denison Olmsted - Physics - 1838 - 376 pages
...through which a body would fall by gravity in the time (t), and complete the parallelogram PMOL; then O will be the place of the body at the end of the time ((); and in the same manner the other Fig. 19. points of the curve POQ might be determined. Now since PN is described with a uniform velocity,... | |
| Denison Olmsted - Physics - 1844 - 618 pages
...through which a body would fall by gravity in the time t, and complete the parallelogram PMOL; then O will be the place of the body at the end of the time t; and in the same manner the other points of the curve POQ might be determined. Now since PN is described... | |
| Denison Olmsted - Physics - 1844 - 610 pages
...through which a body would fall by gravity in the time t,and complete the parallelogram PMOL ; then O will be the place of the body at the end of the time t ; and in the same manner the other points of the curve POQ might be determined. Now since PN is described... | |
| Denison Olmsted - Philosophy - 1854 - 620 pages
...gravity through the space PV. Complete the parallelogram PNVQ ; then for the same reason as in Art. 41, the body at the end of that given time would be found...will be the place of the body at the end of the time t ; and in the same manner the other points of the curve POQ might be determined. Now since PN is described... | |
| William Smyth - Calculus - 1859 - 244 pages
...it is evident, will be convex to the given plane, and will be in the plane of the axes AX, AY. Let M be the place of the body at the end of the time t ; let AP = x, PM = y, and a = the distance of the point of projection of the body from the given... | |
| Samuel Newth - Mechanics, Analytic - 1864 - 392 pages
...= the space due to the action of gravity in the time t. Then, by the second law of motion, P will A be the place of the body at the end of the time t. Let y and x be the co-ordinates of P, referred to AT and the vertical line through A as axes. Then... | |
| Isaac Todhunter - Mechanics - 1867 - 368 pages
...t, under the action of gravity. Complete the parallelogram A TPM. Then P, the corner opposite to A, will be the place of the body at the end of the time t. For, by the Second Law of Motion, gravity will communicate the same vertical velocity to the body... | |
| Isaac Todhunter - Mechanics - 1867 - 372 pages
...<, under the action of gravity. Complete the parallelogram ATPM. Then P, the corner opposite to A, will be the place of the body at the end of the time I. For, by the Second Law of Motion, gravity will communicate the same vertical velocity to the body... | |
| Samuel Newth - Mechanics, Analytic - 1869 - 390 pages
...-J-^2 .. the space duo to the action of gravity in the time t. Then, by the second law of motion, P will be the place of the body at the end of the time t. Let y and x be the co-ordinates of P, referred to AT and the vertical line through A as axes. Then... | |
| Isaac Todhunter - Philosophy - 1877 - 452 pages
...described parallel to AT and AM respectively will be the same as if each alone had been described. Thus P will be the place of the body at the end of the assigned time. 295. It is obvious that by the method just given wo may determine the position which... | |
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