Bartlett, W. H. C. (William Holms Chambers), 1804-1893 · New York : Barnes · leaf 78
tial ve-locity, and by Tthe time, we have for the measure of therectangle aT;and for the measure of the triangle, Eq. (7), ****; f . and if we denote by S the total length of path actuallydescribed by the body, we have value of thespace; S = aT + ±VlTa (10) and because the actual velocity at the… … graphical representation. § 69.—If we now suppose the constant force, instead uniformlyof increasing the initial velocity of the body, to diminish re ai e moit, the motion becomes uniformly retarded, and the linev0 v4 gives the law of the motion. By drawing v015 parallel to0t5, we see that the…
Mechanics · Acoustics · Optics
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