A particle of mass $m$ is projected from the ground with an initial speed $u$ at an angle $\alpha$ with the…
- $\frac{\pi}{4}$
- $\frac{\pi}{4} + \alpha$
- $\frac{\pi}{2} - \alpha$
- $\frac{\pi}{2}$
Solution
\(v_{1}=\frac{u_{0} \cos \alpha}{2} \quad\) (by applying momentum conservation in horizontal direction)
\(\mathrm{v}_{2}=\frac{\mathrm{u}_{0} \cos \alpha}{2} \quad\) (by applying momentum conservation in vertical direction)
\(\theta=45^{\circ}\left(\mathrm{H}=\frac{\mathrm{u}_{0}^{2} \sin ^{2} \alpha}{2 \mathrm{~g}}\right)\)Asked in: JEE Advanced 2013 (Paper 1)
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