A particle moves so that its position vector ˜r at time t is = ˜r ˜a coswt +˜bsinwt, where w is a constant and ˜a and ˜b are constant vectors. Show that (a) ˜ ˜ r × r˙ is independent of t, ˜
(a)
"=\\cos^2\\omega t+\\sin^2\\omega t=1"
(b)
"\\dfrac{d\\vec v}{dt}=-\\omega^2\\vec a\\cos\\omega t-\\omega^2\\vec b\\sin \\omega t"
The acceleration is everywhere towards the origin and proportional to "\\vec r."
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