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Example 4.3 A Bulls-Eye Every Time In a popular lecture demonstration, a projectile is fired at a target in such a way that

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We have no acceleration due to gravity in horizontal translation of the projectile hence, time taken by projectile to cover distance d is simply

t=\frac{d}{v_{i_x}}\Rightarrow \frac{d}{v_i\cos \theta}

Using normal kinematic equations and applying the above obtained expression for time we have

\\ h=v_i\sin \theta . t-\frac{1}{2}gt^2 \\ h=v_i \sin \theta. \left (\frac{d}{v_i\cos \theta} \right )-\frac{1}{2}g.\left (\frac{d}{v_i\cos \theta} \right )^2 \\ h=d\tan \theta -\frac{1}{2}g. \left (\frac{d}{v_i\cos \theta} \right )^2

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