Applying work energy theorem to unifrom circular motion

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Vriska
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Homework Statement


attempt to derive the equation of centripetal acceleration using work energy theorem

Homework Equations



work done = Change in kinetic energy

The Attempt at a Solution



consider diametrically opposed points occurring in uniform circular motion - displacement = 2*R and let force be denoted by F

By work energy theorem ; F*2R = 1/2mv^2 - (-1/2mv^2)
F = mv^2/2R

...
So close...
Where did I go wrong
 
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In uniform circular motion, the force and displacement are always at right angles--no work is done.