Osiris, Volumen13Saint Catherine Press, 1958 |
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Página 309
... velocity that the body can acquire in falling , is to the velocity acquired in any given time , as the given force of gravity perpetually acting upon it , to the excess of this force over the force of resistance at the end of that time ...
... velocity that the body can acquire in falling , is to the velocity acquired in any given time , as the given force of gravity perpetually acting upon it , to the excess of this force over the force of resistance at the end of that time ...
Página 311
... velocity of the falling body to the maximum velocity that it can attain . Since therefore the moments LKNO and DTV of the areas ABKN and AVD are as the velocities , all the parts of these areas generated in the same times will be as the ...
... velocity of the falling body to the maximum velocity that it can attain . Since therefore the moments LKNO and DTV of the areas ABKN and AVD are as the velocities , all the parts of these areas generated in the same times will be as the ...
Página 326
... velocity is divided by 2 , as in II . The error of I may have arisen from taking the velocities as proportional to the centripetal forces directly , rather than to their square roots . Note 21. [ pp . 287/256 . . . . and that with a ...
... velocity is divided by 2 , as in II . The error of I may have arisen from taking the velocities as proportional to the centripetal forces directly , rather than to their square roots . Note 21. [ pp . 287/256 . . . . and that with a ...
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