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A projectile is thrown in the upward dir...

A projectile is thrown in the upward direction making an angle of `60^@` with the horizontal direction with a velocity of `150 ms^-1`. Then the time after which its inclination with the horizontal is `45^@` is

A

`15 (sqrt(3) - 1) s`

B

`15 (sqrt(3) + 1) s`

C

`7.5 (sqrt(3) - 1) s`

D

`7.5 (sqrt(3) + 1) s`

Text Solution

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The correct Answer is:
To solve the problem, we need to find the time after which the projectile's inclination with the horizontal is \( 45^\circ \). We start by breaking down the initial velocity into its horizontal and vertical components. ### Step 1: Break down the initial velocity The initial velocity \( u = 150 \, \text{m/s} \) is given at an angle of \( 60^\circ \) to the horizontal. We can find the horizontal and vertical components of the initial velocity using trigonometric functions. - Horizontal component \( u_x = u \cos(60^\circ) = 150 \cdot \frac{1}{2} = 75 \, \text{m/s} \) - Vertical component \( u_y = u \sin(60^\circ) = 150 \cdot \frac{\sqrt{3}}{2} = 75\sqrt{3} \, \text{m/s} \) ### Step 2: Determine the velocity at \( 45^\circ \) At the time when the projectile's inclination is \( 45^\circ \), the horizontal and vertical components of the velocity will be equal. Let \( v \) be the magnitude of the velocity at that time. From the geometry of the situation: - Horizontal component at \( 45^\circ \): \( v_x = v \cos(45^\circ) = \frac{v}{\sqrt{2}} \) - Vertical component at \( 45^\circ \): \( v_y = v \sin(45^\circ) = \frac{v}{\sqrt{2}} \) Since the horizontal component of the velocity remains constant: \[ \frac{v}{\sqrt{2}} = 75 \implies v = 75\sqrt{2} \, \text{m/s} \] ### Step 3: Find the vertical component of the velocity Using the relationship established, we can find the vertical component of the velocity at the time when the inclination is \( 45^\circ \): \[ v_y = \frac{v}{\sqrt{2}} = \frac{75\sqrt{2}}{\sqrt{2}} = 75 \, \text{m/s} \] ### Step 4: Apply the equations of motion Now, we can use the first equation of motion in the vertical direction to find the time \( t \): \[ v_y = u_y - g t \] Substituting the known values: \[ 75 = 75\sqrt{3} - g t \] Where \( g \) is the acceleration due to gravity, approximately \( 9.8 \, \text{m/s}^2 \). Rearranging gives: \[ g t = 75\sqrt{3} - 75 \] \[ t = \frac{75(\sqrt{3} - 1)}{g} \] ### Step 5: Substitute the value of \( g \) Using \( g \approx 9.8 \, \text{m/s}^2 \): \[ t = \frac{75(\sqrt{3} - 1)}{9.8} \] ### Final Result Calculating this gives the time after which the projectile's inclination with the horizontal is \( 45^\circ \).

To solve the problem, we need to find the time after which the projectile's inclination with the horizontal is \( 45^\circ \). We start by breaking down the initial velocity into its horizontal and vertical components. ### Step 1: Break down the initial velocity The initial velocity \( u = 150 \, \text{m/s} \) is given at an angle of \( 60^\circ \) to the horizontal. We can find the horizontal and vertical components of the initial velocity using trigonometric functions. - Horizontal component \( u_x = u \cos(60^\circ) = 150 \cdot \frac{1}{2} = 75 \, \text{m/s} \) - Vertical component \( u_y = u \sin(60^\circ) = 150 \cdot \frac{\sqrt{3}}{2} = 75\sqrt{3} \, \text{m/s} \) ...
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