Please clarify my doubt

A shooter aims at a point located on a wall at a distance 5root3 m from him. The gun is at the same level of the point. The bullet would exactly hit the target. But when he fires, with a speed of 10m/s, suddenly gravity disappears. The height above the point where the bullet hits the wall is A) root3 m B) 5/root3 C) 5m D) 5root3 m

Note by Sri Chaitanya
2 years, 10 months ago

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Comments

The shooter accounts for gravity when aiming. Assume that g=10m/s2g = 10 \, m/s^2 . The shooter first has to determine the appropriate firing angle. The shooting location and the target are at the same vertical position.

Accounting for gravity, the bullet flight time is:

tf=2vsinθgt_f = \frac{2 v \, sin\theta }{g}

The horizontal travel distance is:

xf=vcosθtf=2v2sinθcosθgx_f = v \, cos \theta \, t_f = \frac{2 v^2 \, sin\theta \, cos \theta }{g}

Setting this equal to the known horizontal distance to the wall:

2v2sinθcosθg=dsinθcosθ=gd2v2=10×532×102=34\frac{2 v^2 \, sin\theta \, cos \theta }{g} = d \\ sin\theta \, cos \theta = \frac{g d}{2 v^2} = \frac{10 \times \, 5 \sqrt{3}}{2 \times 10^2} = \frac{\sqrt{3}}{4}

This yields two possible launch angles:

θ=π3orπ6\theta = \frac{\pi}{3} \, \text{or} \, \frac{\pi}{6}

Now we will compute a general formula for the final vertical displacement, assuming gravity disappears right at launch. The total flight time in this case is:

tf=dvcosθt_f = \frac{d}{v \, cos\theta}

The final vertical displacement is:

yf=vsinθtf=dvsinθvcosθ=dtanθy_f = v \, sin\theta \, t_f = \frac{d \, v \, sin\theta}{v \, cos\theta} = d \, tan \theta

For θ=π3\theta = \frac{\pi}{3}:

yf=dtan(π3)=533=15y_f = d \, tan \Big (\frac{\pi}{3} \Big ) = 5 \, \sqrt{3} \, \sqrt{3} = 15

For θ=π6\theta = \frac{\pi}{6}:

yf=dtan(π6)=5313=5y_f = d \, tan \Big (\frac{\pi}{6} \Big ) = 5 \, \sqrt{3} \, \frac{1}{\sqrt{3}} = 5

Steven Chase - 2 years, 10 months ago
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