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Starting from the origin a body oscillat...

Starting from the origin a body oscillates simple harmonically with a period of 2s . After time `(1)/(x)` second willthe kinetic energy be `75%` of its total energy , then value of x is

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To solve the problem, we will follow these steps: ### Step 1: Understand the relationship between kinetic energy and total energy in simple harmonic motion (SHM). In SHM, the total mechanical energy (E) is given by: \[ E = \frac{1}{2} m \omega^2 A^2 \] where \( \omega \) is the angular frequency and \( A \) is the amplitude. The kinetic energy (K.E) at a displacement \( x \) is given by: \[ K.E = \frac{1}{2} m \omega^2 (A^2 - x^2) \] ### Step 2: Set up the equation for kinetic energy being 75% of total energy. We know that at time \( \frac{1}{x} \) seconds, the kinetic energy is 75% of the total energy. Therefore, we can write: \[ K.E = 0.75 E \] Substituting the expressions for kinetic energy and total energy, we get: \[ \frac{1}{2} m \omega^2 (A^2 - x^2) = 0.75 \left(\frac{1}{2} m \omega^2 A^2\right) \] ### Step 3: Simplify the equation. Cancelling \( \frac{1}{2} m \omega^2 \) from both sides, we have: \[ A^2 - x^2 = 0.75 A^2 \] ### Step 4: Rearranging the equation. Rearranging gives: \[ A^2 - 0.75 A^2 = x^2 \] \[ 0.25 A^2 = x^2 \] ### Step 5: Solve for \( x \). Taking the square root of both sides, we find: \[ x = \sqrt{0.25} A = \frac{A}{2} \] ### Step 6: Find the value of \( x \). Since the question asks for \( x \) in terms of the time period, we need to relate it back to the time period. The angular frequency \( \omega \) is given by: \[ \omega = \frac{2\pi}{T} \] where \( T = 2 \) seconds. Thus, \[ \omega = \frac{2\pi}{2} = \pi \text{ rad/s} \] The displacement \( x \) after a time \( t \) is given by: \[ x = A \sin(\omega t) \] Given that \( t = \frac{1}{x} \), we can substitute this into our equation for \( x \): \[ x = A \sin\left(\pi \cdot \frac{1}{x}\right) \] ### Conclusion From the previous steps, we found that: \[ x = \frac{A}{2} \] Thus, the value of \( x \) is \( 2 \).
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