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A particle moves under a hypothetical force so that its velocity vector is v=
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whata hard bout that?
acceleration is the derivative of velocity with respect to time
assuming k is a constant
\[a = < k \frac{d}{dt} ( tcos(t)) , k \frac{d}{dt} ( tsin(t) ) > \]
k can be factored out of the vector, and it will just provide a scalar multiple
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\[a = k < ( \cos(t) -tsin(t)) , (\sin(t) + tcos(t)) > \]
by product rules
wow you are such a genius. I admire you all
?
bt i need the radial accn, not the total accn....
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at time t=0
yeh i dnt have clue on that :|
radial is apparently equal to centripetal= v^2 / r
but i dont have a clue
hey i got it neway ..thnx
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\[\vec{a}_n=<-kt\sin{t},kt\cos{t}>\]
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