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Two bodies are projected from the same point with equal velocities in such a directions that they strike on the same point on a plane whose inclination is `beta`. If `alpha` is the angle of projection of the first , the ration of there times of flight is

A

`sin ( alpha - beta) : cos alpha`

B

`cos alpha : sin ( alpha - beta)`

C

`sin alpha + beta : cos alpha`

D

`cos alpha : sin ( alpha + beta)`

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The correct Answer is:
To solve the problem, we need to determine the ratio of the times of flight of two bodies projected from the same point with equal velocities, striking the same point on an inclined plane. Let's break it down step by step. ### Step 1: Understand the Problem We have two bodies projected from the same point with equal velocities \( u \). The first body is projected at an angle \( \alpha \) with respect to the horizontal, and the second body is projected at an angle \( \alpha' \) (which we will determine) such that both bodies hit the same point on a plane inclined at an angle \( \beta \). ### Step 2: Write the Range Formula The range \( R \) of a projectile on an inclined plane is given by the formula: \[ R = \frac{u^2}{g \cos^2 \beta} \left( \sin(2\theta - \beta) \right) \] where \( \theta \) is the angle of projection. ### Step 3: Write the Range for Both Bodies For the first body (angle \( \alpha \)): \[ R_1 = \frac{u^2}{g \cos^2 \beta} \left( \sin(2\alpha - \beta) \right) \] For the second body (angle \( \alpha' \)): \[ R_2 = \frac{u^2}{g \cos^2 \beta} \left( \sin(2\alpha' - \beta) \right) \] ### Step 4: Set the Ranges Equal Since both bodies strike the same point, we have: \[ R_1 = R_2 \] This gives us: \[ \sin(2\alpha - \beta) = \sin(2\alpha' - \beta) \] ### Step 5: Use the Sine Function Property The equality of the sine functions implies: \[ 2\alpha - \beta = 2\alpha' - \beta \quad \text{or} \quad 2\alpha - \beta = \pi - (2\alpha' - \beta) \] From the first equation: \[ 2\alpha = 2\alpha' \implies \alpha = \alpha' \] This is trivial and does not help us find \( \alpha' \). From the second equation: \[ 2\alpha - \beta = \pi - 2\alpha' + \beta \] Rearranging gives: \[ 2\alpha + 2\alpha' = \pi + 2\beta \implies \alpha' = \frac{\pi}{2} - \alpha - \beta \] ### Step 6: Calculate Time of Flight The time of flight \( T \) for a projectile is given by: \[ T = \frac{u \sin(\theta)}{g} \] For the first body: \[ T_1 = \frac{u \sin(\alpha)}{g} \] For the second body: \[ T_2 = \frac{u \sin(\alpha')}{g} \] ### Step 7: Find the Ratio of Times of Flight Now, we find the ratio \( \frac{T_1}{T_2} \): \[ \frac{T_1}{T_2} = \frac{\sin(\alpha)}{\sin(\alpha')} \] Substituting \( \alpha' = \frac{\pi}{2} - \alpha - \beta \): \[ \sin(\alpha') = \sin\left(\frac{\pi}{2} - \alpha - \beta\right) = \cos(\alpha + \beta) \] Thus, the ratio becomes: \[ \frac{T_1}{T_2} = \frac{\sin(\alpha)}{\cos(\alpha + \beta)} \] ### Final Answer The ratio of the times of flight of the two bodies is: \[ \frac{T_1}{T_2} = \frac{\sin(\alpha - \beta)}{\cos(\alpha)} \]
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