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A particle is projected with a velocity ...

A particle is projected with a velocity `v` so that its range on a horizontal plane is twice the greatest height attained. If `g` is acceleration due to gravity, then its range is

A

`(4 v^2)/(5 g)`

B

`(4 g)/(5 v^2)`

C

`(4 v^3)/(5 g^2)`

D

`(4 v)/(5 g^2)`

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The correct Answer is:
To solve the problem, we need to find the range of a particle projected with an initial velocity \( v \) such that its range \( R \) is twice the greatest height \( H \) attained. ### Step-by-Step Solution: 1. **Identify the Relationship Between Range and Height**: We are given that the range \( R \) is twice the greatest height \( H \): \[ R = 2H \] 2. **Formulas for Range and Height**: The formulas for the range \( R \) and the maximum height \( H \) for a projectile launched at an angle \( \theta \) with an initial velocity \( v \) are: \[ R = \frac{v^2 \sin 2\theta}{g} \] \[ H = \frac{v^2 \sin^2 \theta}{2g} \] 3. **Substituting Height into the Range Equation**: From the relationship \( R = 2H \), we can substitute for \( H \): \[ R = 2 \left( \frac{v^2 \sin^2 \theta}{2g} \right) = \frac{v^2 \sin^2 \theta}{g} \] 4. **Equating the Two Expressions for Range**: Now we have two expressions for \( R \): \[ \frac{v^2 \sin 2\theta}{g} = \frac{v^2 \sin^2 \theta}{g} \] 5. **Simplifying the Equation**: We can cancel \( \frac{v^2}{g} \) from both sides (assuming \( v \neq 0 \)): \[ \sin 2\theta = \sin^2 \theta \] 6. **Using the Identity for Sine**: Recall that \( \sin 2\theta = 2 \sin \theta \cos \theta \): \[ 2 \sin \theta \cos \theta = \sin^2 \theta \] 7. **Rearranging the Equation**: Rearranging gives: \[ \sin^2 \theta - 2 \sin \theta \cos \theta = 0 \] Factoring out \( \sin \theta \): \[ \sin \theta (\sin \theta - 2 \cos \theta) = 0 \] 8. **Finding Possible Angles**: This gives us two cases: - \( \sin \theta = 0 \) (which is not valid for projectile motion) - \( \sin \theta = 2 \cos \theta \) or \( \tan \theta = 2 \) 9. **Finding the Range**: We can now express \( \sin \theta \) and \( \cos \theta \) in terms of \( \tan \theta \): Let \( \tan \theta = 2 \), then: \[ \sin \theta = \frac{2}{\sqrt{5}}, \quad \cos \theta = \frac{1}{\sqrt{5}} \] 10. **Substituting Back to Find Range**: Substitute \( \sin 2\theta = 2 \sin \theta \cos \theta \): \[ \sin 2\theta = 2 \left(\frac{2}{\sqrt{5}}\right) \left(\frac{1}{\sqrt{5}}\right) = \frac{4}{5} \] Now substitute into the range formula: \[ R = \frac{v^2 \cdot \frac{4}{5}}{g} = \frac{4v^2}{5g} \] ### Final Answer: Thus, the range \( R \) is: \[ R = \frac{4v^2}{5g} \]

To solve the problem, we need to find the range of a particle projected with an initial velocity \( v \) such that its range \( R \) is twice the greatest height \( H \) attained. ### Step-by-Step Solution: 1. **Identify the Relationship Between Range and Height**: We are given that the range \( R \) is twice the greatest height \( H \): \[ R = 2H ...
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