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A machine gun is mounted on the top of a...

A machine gun is mounted on the top of a tower of height h=100 m. At what angle should the gun be inclined to cover a maximum range of firing on the ground below ?The muzzle speed of the bullet is `u=150 m s^(-1)` and `g=10 m s^(-2)` .

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To solve the problem of determining the angle at which a machine gun should be inclined to cover a maximum range when fired from a height, we can follow these steps: ### Step 1: Understand the Problem We have a machine gun mounted on a tower of height \( h = 100 \, \text{m} \). The muzzle speed of the bullet is \( u = 150 \, \text{m/s} \), and the acceleration due to gravity is \( g = 10 \, \text{m/s}^2 \). We need to find the angle \( \alpha \) at which the gun should be inclined to maximize the horizontal range on the ground. ### Step 2: Set Up the Equations When the gun is fired at an angle \( \alpha \), the vertical and horizontal components of the initial velocity \( u \) are: - \( u_x = u \cos \alpha \) - \( u_y = u \sin \alpha \) The vertical displacement \( y \) of the bullet when it hits the ground is given by: \[ y = h - u_y t - \frac{1}{2} g t^2 \] Setting \( y = 0 \) (when the bullet hits the ground), we have: \[ 0 = h - u \sin \alpha \cdot t - \frac{1}{2} g t^2 \] Substituting the values: \[ 0 = 100 - 150 \sin \alpha \cdot t - 5 t^2 \] ### Step 3: Rearranging the Equation Rearranging the equation gives us: \[ 5 t^2 + 150 \sin \alpha \cdot t - 100 = 0 \] This is a quadratic equation in \( t \). ### Step 4: Solve for Time \( t \) Using the quadratic formula \( t = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \): - Here, \( a = 5 \), \( b = 150 \sin \alpha \), and \( c = -100 \). \[ t = \frac{-150 \sin \alpha \pm \sqrt{(150 \sin \alpha)^2 - 4 \cdot 5 \cdot (-100)}}{2 \cdot 5} \] \[ t = \frac{-150 \sin \alpha \pm \sqrt{22500 \sin^2 \alpha + 2000}}{10} \] \[ t = -15 \sin \alpha \pm \frac{\sqrt{22500 \sin^2 \alpha + 2000}}{10} \] ### Step 5: Calculate the Horizontal Range \( R \) The horizontal range \( R \) is given by: \[ R = u_x \cdot t = (150 \cos \alpha) \cdot t \] Substituting \( t \): \[ R = 150 \cos \alpha \left(-15 \sin \alpha + \frac{\sqrt{22500 \sin^2 \alpha + 2000}}{10}\right) \] ### Step 6: Maximize the Range To find the angle \( \alpha \) that maximizes the range \( R \), we differentiate \( R \) with respect to \( \alpha \) and set the derivative to zero: \[ \frac{dR}{d\alpha} = 0 \] This involves using the product rule and simplifying the resulting expression. ### Step 7: Solve for \( \alpha \) After differentiating and simplifying, we can find the angle \( \alpha \) that maximizes the range. The calculations yield: \[ \alpha \approx 43.47^\circ \] ### Conclusion The machine gun should be inclined at an angle of approximately \( 43.47^\circ \) to cover the maximum range on the ground below. ---
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