problem10_p103

University Physics with Modern Physics with Mastering Physics (11th Edition)

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10.103: a) See Problem 10.92; . 3 2 1 2 1 r r mv T = r T d and b) are always antiparallel, so - = = - = 2 1 1 2 2 1 2 2 2 1 2 1 3 2 1 2 1 . 1 1 2 r r r r r r r mv r dr r mv dr T W c) so ), ( 2 1 1 2 r r v v = ' 1 2 ) ( 2 1 2 2 1 2 1 2 1 2 2 -
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Unformatted text preview: =-= ∆ r r mv v v m K which is the same as the work found in part (b)....
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