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A body executing S.H.M.along a straight ...

A body executing S.H.M.along a straight line has a velocity of `3 ms^(-1)` when it is at a distance of 4m from its mean position and`4ms^(-1)` when it is at a distance of 3m from its mean position.Its angular frequency and amplitude are

A

`2 rad s^(-1) & 5m`

B

`1 rad s^(-1) & 10 m`

C

` 2 rad s^(-1)& 10 m`

D

` 1 rad s^(-1) & 5m`

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To solve the problem, we need to find the angular frequency (ω) and amplitude (A) of a body executing simple harmonic motion (SHM) given its velocities at specific displacements from the mean position. ### Step-by-Step Solution: 1. **Understand the relationship between velocity, angular frequency, amplitude, and displacement:** The velocity (v) of a body in SHM is given by the formula: \[ v = \omega \sqrt{A^2 - x^2} \] where: - \( v \) = velocity - \( \omega \) = angular frequency - \( A \) = amplitude - \( x \) = displacement from the mean position 2. **Set up the equations for the two given conditions:** We have two scenarios: - When \( x_1 = 4 \, m \), \( v_1 = 3 \, m/s \) - When \( x_2 = 3 \, m \), \( v_2 = 4 \, m/s \) From the formula, we can write: \[ v_1 = \omega \sqrt{A^2 - x_1^2} \quad \text{(1)} \] \[ v_2 = \omega \sqrt{A^2 - x_2^2} \quad \text{(2)} \] 3. **Substituting the known values into the equations:** From equation (1): \[ 3 = \omega \sqrt{A^2 - 4^2} \] \[ 3 = \omega \sqrt{A^2 - 16} \quad \text{(3)} \] From equation (2): \[ 4 = \omega \sqrt{A^2 - 3^2} \] \[ 4 = \omega \sqrt{A^2 - 9} \quad \text{(4)} \] 4. **Square both equations to eliminate the square root:** Squaring equation (3): \[ 9 = \omega^2 (A^2 - 16) \quad \text{(5)} \] Squaring equation (4): \[ 16 = \omega^2 (A^2 - 9) \quad \text{(6)} \] 5. **Rearranging equations (5) and (6):** From (5): \[ \omega^2 A^2 - 16\omega^2 = 9 \quad \Rightarrow \quad \omega^2 A^2 = 9 + 16\omega^2 \quad \text{(7)} \] From (6): \[ \omega^2 A^2 - 9\omega^2 = 16 \quad \Rightarrow \quad \omega^2 A^2 = 16 + 9\omega^2 \quad \text{(8)} \] 6. **Setting equations (7) and (8) equal to each other:** \[ 9 + 16\omega^2 = 16 + 9\omega^2 \] Rearranging gives: \[ 16\omega^2 - 9\omega^2 = 16 - 9 \] \[ 7\omega^2 = 7 \quad \Rightarrow \quad \omega^2 = 1 \quad \Rightarrow \quad \omega = 1 \, \text{rad/s} \] 7. **Substituting ω back to find A:** Using equation (3): \[ 3 = 1 \cdot \sqrt{A^2 - 16} \] \[ 3 = \sqrt{A^2 - 16} \] Squaring both sides: \[ 9 = A^2 - 16 \quad \Rightarrow \quad A^2 = 25 \quad \Rightarrow \quad A = 5 \, m \] ### Final Results: - Angular frequency \( \omega = 1 \, \text{rad/s} \) - Amplitude \( A = 5 \, m \)
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