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A particle oscillating in simple harmon...

A particle oscillating in simple harmonic motion has amplitude 'a'. The distance from the mean position at which its velocity will be one half of the maximum velocity is

A

`(sqrt(3))/(2) a `

B

`sqrt(3) a`

C

`(2)/(sqrt(3))`a

D

`(1)/(sqrt(3))` a

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AI Generated Solution

The correct Answer is:
To solve the problem step by step, we can follow these instructions: ### Step 1: Understand the problem We need to find the distance \( x \) from the mean position where the velocity of a particle in simple harmonic motion (SHM) is half of its maximum velocity. ### Step 2: Write down the formulas The velocity \( V \) of a particle in SHM at a distance \( x \) from the mean position is given by: \[ V = \omega \sqrt{a^2 - x^2} \] where: - \( V \) is the velocity at position \( x \) - \( \omega \) is the angular frequency - \( a \) is the amplitude The maximum velocity \( V_{max} \) occurs at the mean position (when \( x = 0 \)): \[ V_{max} = a \omega \] ### Step 3: Set up the equation for half of the maximum velocity According to the problem, we need to find \( x \) when the velocity \( V \) is half of the maximum velocity: \[ V = \frac{1}{2} V_{max} = \frac{1}{2} (a \omega) = \frac{a \omega}{2} \] ### Step 4: Substitute into the velocity equation Now, substitute \( V = \frac{a \omega}{2} \) into the velocity equation: \[ \frac{a \omega}{2} = \omega \sqrt{a^2 - x^2} \] ### Step 5: Simplify the equation We can divide both sides by \( \omega \) (assuming \( \omega \neq 0 \)): \[ \frac{a}{2} = \sqrt{a^2 - x^2} \] ### Step 6: Square both sides to eliminate the square root Squaring both sides gives: \[ \left(\frac{a}{2}\right)^2 = a^2 - x^2 \] \[ \frac{a^2}{4} = a^2 - x^2 \] ### Step 7: Rearrange the equation Rearranging the equation, we get: \[ x^2 = a^2 - \frac{a^2}{4} \] \[ x^2 = a^2 \left(1 - \frac{1}{4}\right) \] \[ x^2 = a^2 \left(\frac{3}{4}\right) \] ### Step 8: Solve for \( x \) Taking the square root of both sides gives: \[ x = a \sqrt{\frac{3}{4}} = \frac{a \sqrt{3}}{2} \] ### Final Answer The distance from the mean position at which the velocity will be one half of the maximum velocity is: \[ x = \frac{a \sqrt{3}}{2} \] ---
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