 | Charles Bossut - 1803 - 580 ページ
...vertical line ; and that the whole weight of the body is to the weight of the quantity of fluid displaced, as the specific gravity of the fluid is to that of the floating body. This general theory he illustrates by various examples taken from the triangle, the... | |
 | Charles Hutton - 1807 - 464 ページ
...of the fluid as is equal to the immersed part ; and therefore the weights are the same. 285. Carol. 4. Hence the magnitude of the whole body, is to the...specific gravities, are reciprocally as their magnitudes. 286. Carol. 5. And because, when the weight of a body taken in a fluid, is subtracted from its weight... | |
 | John Ewing - 1809 - 672 ページ
...weighing them in different fluids. 11. The weight, which a body loses in a fluid, is to its whole weight, as the specific gravity of the fluid is to that of the body. Because the weight, which the body loses in the fluid, is the weight of the fluid equal in bulk with... | |
 | Charles Hutton - 1812 - 624 ページ
...of the fluid asis equal to the immersed part ; and therefore the weights are the same. 323. Carol. 4. Hence the magnitude of the whole body, is to the...are reciprocally as their magnitudes. ^ 324. Carol. S. And because when the weight of a body taken in a fluid, is subtracted from its weight out of the... | |
 | 1812 - 352 ページ
...as so much of the fluid as is equal to the immersed part, and therefore the weights are the same : hence, the magnitude of the whole body, is to the...equal weight, the densities or specific gravities, arc reciprocally as their magnitudes. After having considered hydrostatics, by which the weight and... | |
 | Charles Hutton - 1812 - 406 ページ
...opposite forces bx and abm becoming equal, then x = am, or 1: m: ; a : x, that is, the whole length is to the part immersed, as the specific gravity of the fluid is to that of the cylinder. And , if the latter be equal to half the former, which is nearly the case of fir timber,... | |
 | Charles Hutton - 1816 - 618 ページ
...the •fluid as is equal to the immersed part ; and therefore the weights are the same. 323. Carol. 4. Hence the magnitude of the whole body, is to the...gravities, are reciprocally as their magnitudes. 324. Coro'. 5. And because when the weight of a body taken in a fluid, is subtracted from its weight out... | |
 | Thomas Leybourn - 1817 - 454 ページ
...of hydrostatics, (see ror. 4, p. 220, vol. 2, Dr. Hutton's Course) the magnitude of the whole cone, is to the magnitude of the part immersed, as the specific gravity of the fluid to that of the body, or as 8 to 5 ; but the whole cone, and the part immersed being similar, their... | |
 | Charles Hutton - 1818 - 652 ページ
...the fluid as is equal to the immersed part ; and therefore the „ weights are the same. 323. Carol. 4. . Hence the magnitude of the whole body, is to...Carol. 5. And because when the weight of a body taken iu a fluid, is subtracted from its weight out of the fluid, the difference is the weight of an equal... | |
 | John Mason Good - 1819 - 800 ページ
...body is equal to the weight of a quantity of the fluid of the same bulk ns the part immersed. Hence, as the specific gravity of the fluid, is to that of the body, so is the whole magnitude of the body, to the magnitude of the part immersed. XIII. The specific gravities... | |
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Hence the magnitude of the whole body, is to the magnitude of the part immersed, as the specific gravity of the fluid, is to that of the body. 
