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A ball is projected from a high tower wi...

A ball is projected from a high tower with speed 20 m/s at an angle `30^@` with horizontal x-axis. The x-coordinate of the ball at the instant when the velocity of the ball becomes perpendicular to the velocity of projection will be (take point of projection as origin):

A

`40sqrt(3)` m

B

40 m

C

`20sqrt(3)` m

D

20 m

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To solve the problem step by step, we will analyze the motion of the ball projected from a tower. The key points to consider are the initial velocity components, the equations of motion, and the condition for the velocity vector to be perpendicular to the initial velocity vector. ### Step 1: Determine the initial velocity components The ball is projected with a speed of 20 m/s at an angle of 30 degrees with the horizontal. We can break this initial velocity into its horizontal (Ux) and vertical (Uy) components using trigonometric functions. - \( U_x = U \cdot \cos(\theta) = 20 \cdot \cos(30^\circ) = 20 \cdot \frac{\sqrt{3}}{2} = 10\sqrt{3} \, \text{m/s} \) - \( U_y = U \cdot \sin(\theta) = 20 \cdot \sin(30^\circ) = 20 \cdot \frac{1}{2} = 10 \, \text{m/s} \) ### Step 2: Write the equations of motion Since there is no horizontal acceleration (Ax = 0) and the vertical acceleration is due to gravity (Ay = -g), we can write the equations of motion for the x and y coordinates. - Horizontal motion: \( x(t) = U_x \cdot t = 10\sqrt{3} \cdot t \) - Vertical motion: \( y(t) = U_y \cdot t - \frac{1}{2} g t^2 = 10t - \frac{1}{2} g t^2 \) ### Step 3: Determine the velocity components The velocity components at any time t can be expressed as: - \( V_x = U_x = 10\sqrt{3} \, \text{m/s} \) (constant) - \( V_y = U_y - g \cdot t = 10 - g \cdot t \) ### Step 4: Condition for perpendicularity The velocity vector becomes perpendicular to the initial velocity vector when their dot product is zero: \[ \vec{V} \cdot \vec{U} = 0 \] Substituting the components: \[ (10\sqrt{3}) \cdot (10\sqrt{3}) + (10 - g \cdot t) \cdot 10 = 0 \] This simplifies to: \[ 300 + 100 - 10g \cdot t = 0 \] \[ 400 = 10g \cdot t \] \[ t = \frac{400}{10g} = \frac{40}{g} \] ### Step 5: Calculate the time when the velocity is perpendicular Using \( g \approx 10 \, \text{m/s}^2 \): \[ t = \frac{40}{10} = 4 \, \text{s} \] ### Step 6: Calculate the x-coordinate at this time Now we can find the x-coordinate when \( t = 4 \, \text{s} \): \[ x(4) = U_x \cdot t = 10\sqrt{3} \cdot 4 = 40\sqrt{3} \, \text{m} \] ### Final Answer The x-coordinate of the ball at the instant when the velocity of the ball becomes perpendicular to the velocity of projection is \( 40\sqrt{3} \, \text{m} \). ---

To solve the problem step by step, we will analyze the motion of the ball projected from a tower. The key points to consider are the initial velocity components, the equations of motion, and the condition for the velocity vector to be perpendicular to the initial velocity vector. ### Step 1: Determine the initial velocity components The ball is projected with a speed of 20 m/s at an angle of 30 degrees with the horizontal. We can break this initial velocity into its horizontal (Ux) and vertical (Uy) components using trigonometric functions. - \( U_x = U \cdot \cos(\theta) = 20 \cdot \cos(30^\circ) = 20 \cdot \frac{\sqrt{3}}{2} = 10\sqrt{3} \, \text{m/s} \) - \( U_y = U \cdot \sin(\theta) = 20 \cdot \sin(30^\circ) = 20 \cdot \frac{1}{2} = 10 \, \text{m/s} \) ...
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