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A stone is projected with speed of 50 ms...

A stone is projected with speed of `50 ms^(-1)` at an angle of `60^(@)` with the horizontal. The speed of the stone at highest point of trajectory is

A

`75 ms^(-1)`

B

`25ms^(-1)`

C

`50 ms^(-1)`

D

cannot find

Text Solution

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The correct Answer is:
To solve the problem of finding the speed of a stone at the highest point of its trajectory when projected with a speed of 50 m/s at an angle of 60 degrees with the horizontal, we can follow these steps: ### Step-by-Step Solution: 1. **Identify the Initial Velocity Components**: The initial velocity \( u \) can be broken down into horizontal and vertical components using trigonometric functions: - Horizontal component \( V_x = u \cos \theta \) - Vertical component \( V_y = u \sin \theta \) Given: - \( u = 50 \, \text{m/s} \) - \( \theta = 60^\circ \) Calculate: \[ V_x = 50 \cos(60^\circ) = 50 \times \frac{1}{2} = 25 \, \text{m/s} \] \[ V_y = 50 \sin(60^\circ) = 50 \times \frac{\sqrt{3}}{2} \approx 43.3 \, \text{m/s} \] 2. **Understand the Motion at the Highest Point**: At the highest point of the trajectory, the vertical component of the velocity \( V_y \) becomes zero due to the effect of gravity. However, the horizontal component \( V_x \) remains constant throughout the motion because there are no horizontal forces acting on the stone. 3. **Determine the Speed at the Highest Point**: At the highest point, the speed of the stone will only be due to the horizontal component: \[ V_{\text{highest point}} = V_x = 25 \, \text{m/s} \] 4. **Conclusion**: Therefore, the speed of the stone at the highest point of its trajectory is \( 25 \, \text{m/s} \). ### Final Answer: The speed of the stone at the highest point of trajectory is **25 m/s**. ---

To solve the problem of finding the speed of a stone at the highest point of its trajectory when projected with a speed of 50 m/s at an angle of 60 degrees with the horizontal, we can follow these steps: ### Step-by-Step Solution: 1. **Identify the Initial Velocity Components**: The initial velocity \( u \) can be broken down into horizontal and vertical components using trigonometric functions: - Horizontal component \( V_x = u \cos \theta \) - Vertical component \( V_y = u \sin \theta \) ...
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