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The maximum height reached by projectile...

The maximum height reached by projectile is `4 m`. The horizontal range is `12 m`. The velocity of projection in `m s^-1` is (g is acceleration due to gravity)

A

`5 sqrt(g//2)`

B

`3 sqrt(g//2)`

C

`(1)/(3) sqrt(g//2)`

D

`(1)/(5) sqrt(g//2)`

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The correct Answer is:
To find the velocity of projection for a projectile that reaches a maximum height of 4 m and has a horizontal range of 12 m, we can follow these steps: ### Step 1: Understand the Relationships The maximum height (H) and the horizontal range (R) of a projectile are related to the initial velocity (u) and the angle of projection (θ) through the following equations: 1. Maximum height: \[ H = \frac{u^2 \sin^2 \theta}{2g} \] 2. Range: \[ R = \frac{u^2 \sin 2\theta}{g} \] ### Step 2: Express \(\sin 2\theta\) Using the identity \(\sin 2\theta = 2 \sin \theta \cos \theta\), we can rewrite the range equation: \[ R = \frac{u^2 (2 \sin \theta \cos \theta)}{g} \] ### Step 3: Relate Height and Range From the maximum height equation, we can express \(u^2\): \[ u^2 = \frac{2gH}{\sin^2 \theta} \] Substituting this into the range equation gives: \[ R = \frac{(2gH/\sin^2 \theta)(2 \sin \theta \cos \theta)}{g} \] This simplifies to: \[ R = \frac{4H \cos \theta}{\sin \theta} \] Thus, we have: \[ R = 4H \cot \theta \] ### Step 4: Substitute Known Values Given \(H = 4 \, \text{m}\) and \(R = 12 \, \text{m}\), we can substitute these values: \[ 12 = 4 \times 4 \cot \theta \] This simplifies to: \[ 12 = 16 \cot \theta \] Thus, we find: \[ \cot \theta = \frac{12}{16} = \frac{3}{4} \] ### Step 5: Find \(\tan \theta\) Since \(\cot \theta = \frac{1}{\tan \theta}\), we have: \[ \tan \theta = \frac{4}{3} \] ### Step 6: Calculate \(\sin \theta\) and \(\cos \theta\) Using the relationship: \[ \tan \theta = \frac{\sin \theta}{\cos \theta} \] Let \(\sin \theta = 4k\) and \(\cos \theta = 3k\) for some \(k\). Then: \[ \sin^2 \theta + \cos^2 \theta = 1 \implies (4k)^2 + (3k)^2 = 1 \implies 16k^2 + 9k^2 = 1 \implies 25k^2 = 1 \implies k^2 = \frac{1}{25} \implies k = \frac{1}{5} \] Thus: \[ \sin \theta = \frac{4}{5}, \quad \cos \theta = \frac{3}{5} \] ### Step 7: Substitute Back to Find \(u\) Using the maximum height equation: \[ H = \frac{u^2 \sin^2 \theta}{2g} \implies 4 = \frac{u^2 \left(\frac{4}{5}\right)^2}{2g} \] This simplifies to: \[ 4 = \frac{u^2 \cdot \frac{16}{25}}{2g} \implies 4 \cdot 2g = \frac{16u^2}{25} \implies 8g = \frac{16u^2}{25} \] Multiplying both sides by 25: \[ 200g = 16u^2 \implies u^2 = \frac{200g}{16} = \frac{25g}{2} \] Thus: \[ u = \sqrt{\frac{25g}{2}} = \frac{5\sqrt{g}}{\sqrt{2}} \] ### Final Step: Express in Standard Form Thus, the velocity of projection \(u\) is: \[ u = \frac{5\sqrt{g}}{\sqrt{2}} \, \text{m/s} \]

To find the velocity of projection for a projectile that reaches a maximum height of 4 m and has a horizontal range of 12 m, we can follow these steps: ### Step 1: Understand the Relationships The maximum height (H) and the horizontal range (R) of a projectile are related to the initial velocity (u) and the angle of projection (θ) through the following equations: 1. Maximum height: \[ H = \frac{u^2 \sin^2 \theta}{2g} \] ...
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