The ultimate challenge in Mechanics from Feynmann
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The problem is best solved in plane polar coordinates. (For an analysis of motion in plane polar coordinates please refer to "Fundamentals of Mechanics" by I E Irodov) Velocity of B in the frame of A, (dr/dt)er + (r(d /dt)eth = [u - vcos ]er - (- vsin )eth(dr/dt) = u-vcos ------------------(1)And r(d /dt) = vsin ----------------(2)Dividing (1) by (2) and rearranging, (1/r)dr = (u/v)cosec d - cot d![]() d r (1/r)dr = pi/2 theta(u/v)cosec d - pi/2 thetacot d![]() ln(r/d) = ln[(cosec - cot )u/v/sin ]r/d = (1 - cos )u/v]/(sin )(u/v)+1Was quite an enjoyable problem ... can you tell me its source?? |
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/dt)
r (1/r)dr = pi/2







