Philosophical MagazineTaylor & Francis, 1803 - Physics |
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Page 55
... motion must be greater than the force which op- poses its motion , otherwise it could not overcome it ; and hence , if there were no other objection than this , it is evi- dent that the friction could not be very accurately obtained ...
... motion must be greater than the force which op- poses its motion , otherwise it could not overcome it ; and hence , if there were no other objection than this , it is evi- dent that the friction could not be very accurately obtained ...
Page 115
center at the beginning of the motion , we shall have the whole rotatory motion ; hence , therefore , v + a -- a2 x as2 ra TS a2 2 F x = √√ a - 2 Fz , consequently z = - - 2 v x rs + a x ra ra2 2 Fx as2 motion becomes uniform . the ...
center at the beginning of the motion , we shall have the whole rotatory motion ; hence , therefore , v + a -- a2 x as2 ra TS a2 2 F x = √√ a - 2 Fz , consequently z = - - 2 v x rs + a x ra ra2 2 Fx as2 motion becomes uniform . the ...
Page 116
... motion being then de- stroyed , and the rotatory motion still continuing in the direction gef , will cause the body to return with an ac- celerative velocity until the friction ceases by the body's beginning to roll , after which it ...
... motion being then de- stroyed , and the rotatory motion still continuing in the direction gef , will cause the body to return with an ac- celerative velocity until the friction ceases by the body's beginning to roll , after which it ...
Contents
Account of a Journey to the Summit of the Peak | 31 |
On Mr ARTHUR WOOLFs improved Apparatus | 40 |
On the Motion of Bodies affected by Friction | 47 |
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