Without loss of generality, we only need to look at the equation for the x-position, since we

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Without loss of generality, we only need to look at the equation for the x-position, since we know that centripetal acceleration points towards the center of the circle. Thus, when θ = 0, the second derivative of x with respect to time must be the centripetal acceleration.

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Without loss of generality, we only need to look at the equation for the x-position, since we

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The first derivative of x with respect to time t is dxdt Rsin... View the full answer

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