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In a projectile the statement are true o...

In a projectile the statement are true or false
`sin2alpha= (gR)/(u^(2))`
where the letters have the usual meanings.

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To determine whether the statement \( \sin 2\alpha = \frac{gR}{u^2} \) is true or false, we will analyze the projectile motion and derive the range formula step by step. ### Step 1: Understanding the Variables In the given statement: - \( R \) is the range of the projectile. - \( \alpha \) is the angle of projection. - \( u \) is the initial velocity. - \( g \) is the acceleration due to gravity. ### Step 2: Deriving the Range Formula The range \( R \) of a projectile launched at an angle \( \alpha \) with initial velocity \( u \) can be derived using the equations of motion. 1. **Vertical Motion**: The vertical component of the initial velocity is given by: \[ u_y = u \sin \alpha \] The time of flight \( T \) can be derived from the vertical motion. The vertical displacement is zero when the projectile returns to the same vertical level: \[ 0 = u_y T - \frac{1}{2} g T^2 \] This simplifies to: \[ T = \frac{2u \sin \alpha}{g} \] 2. **Horizontal Motion**: The horizontal component of the initial velocity is: \[ u_x = u \cos \alpha \] The range \( R \) is given by the horizontal distance traveled during the time of flight: \[ R = u_x T = (u \cos \alpha) \left(\frac{2u \sin \alpha}{g}\right) \] Substituting \( u_x \) and \( T \): \[ R = \frac{2u^2 \sin \alpha \cos \alpha}{g} \] 3. **Using the Double Angle Identity**: We can use the trigonometric identity \( \sin 2\alpha = 2 \sin \alpha \cos \alpha \): \[ R = \frac{u^2 \sin 2\alpha}{g} \] ### Step 3: Rearranging the Formula From the derived formula for range \( R \): \[ R = \frac{u^2 \sin 2\alpha}{g} \] We can rearrange this to express \( \sin 2\alpha \): \[ \sin 2\alpha = \frac{gR}{u^2} \] ### Conclusion The statement \( \sin 2\alpha = \frac{gR}{u^2} \) is **true**. ---
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