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The equation of a projectile is y = sqrt...

The equation of a projectile is `y = sqrt(3)x - ((gx^2)/2)` the horizontal range is

A

`(2g)/ sqrt(3)`

B

`(2sqrt(3))/g`

C

`g/(2 sqrt(3))`

D

`(sqrt(3)g)/2`

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The correct Answer is:
To find the horizontal range of the projectile given the equation \( y = \sqrt{3}x - \frac{g x^2}{2} \), we can follow these steps: ### Step 1: Identify the form of the projectile equation The standard equation of the trajectory of a projectile is given by: \[ y = x \tan \theta - \frac{g x^2}{2u^2 \cos^2 \theta} \] where \( \theta \) is the angle of projection, \( u \) is the initial velocity, and \( g \) is the acceleration due to gravity. ### Step 2: Compare the given equation with the standard form From the given equation: \[ y = \sqrt{3}x - \frac{g x^2}{2} \] we can identify that: - \( \tan \theta = \sqrt{3} \) - The coefficient of \( x^2 \) gives us \( \frac{g}{2u^2 \cos^2 \theta} = \frac{g}{2} \) ### Step 3: Determine the angle of projection From \( \tan \theta = \sqrt{3} \), we find: \[ \theta = 60^\circ \] ### Step 4: Calculate \( u \) using the cosine of the angle Using \( \cos 60^\circ = \frac{1}{2} \): \[ \frac{g}{2u^2 \cos^2 60^\circ} = \frac{g}{2} \] Substituting \( \cos^2 60^\circ = \left(\frac{1}{2}\right)^2 = \frac{1}{4} \): \[ \frac{g}{2u^2 \cdot \frac{1}{4}} = \frac{g}{2} \] This simplifies to: \[ \frac{g \cdot 4}{2u^2} = \frac{g}{2} \] Cross-multiplying gives: \[ 4g = gu^2 \] Dividing both sides by \( g \) (assuming \( g \neq 0 \)): \[ u^2 = 4 \implies u = 2 \text{ m/s} \] ### Step 5: Calculate the horizontal range The formula for the horizontal range \( R \) of a projectile is given by: \[ R = \frac{u^2 \sin 2\theta}{g} \] Calculating \( \sin 2\theta \) where \( \theta = 60^\circ \): \[ \sin 120^\circ = \sin(180^\circ - 60^\circ) = \sin 60^\circ = \frac{\sqrt{3}}{2} \] Now substituting the values: \[ R = \frac{(2)^2 \cdot \frac{\sqrt{3}}{2}}{g} = \frac{4 \cdot \frac{\sqrt{3}}{2}}{g} = \frac{2\sqrt{3}}{g} \] ### Final Answer The horizontal range of the projectile is: \[ R = \frac{2\sqrt{3}}{g} \] ---
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