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A particle performs linear S.H.M. At a p...

A particle performs linear S.H.M. At a particular instant, velocity of the particle is `u` and acceleration is `alpha` while at another instant, velocity is `v` and acceleration `beta` `(0ltalphaltbeta)`. The distance between the two position is

A

`(u^(2)-v^(2))/(alpha+beta)`

B

`(u^(2)+v^(2))/(alpha+beta)`

C

`(u^(2)-v^(2))/(alpha-beta)`

D

`(u^(2)+v^(2))/(alpha-beta)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to determine the distance between two positions of a particle performing linear simple harmonic motion (SHM) given its velocities and accelerations at those positions. ### Step-by-Step Solution: 1. **Understanding SHM Relations**: - In SHM, the acceleration \( a \) at a position \( x \) is given by: \[ a = -\omega^2 x \] - The velocity \( v \) at a position \( x \) is given by: \[ v^2 = \omega^2 A^2 - x^2 \] where \( A \) is the amplitude and \( \omega \) is the angular frequency. 2. **Setting Up the Equations**: - For the first position \( x_1 \): - Velocity \( u \) and acceleration \( \alpha \): \[ \alpha = -\omega^2 x_1 \quad \text{(1)} \] \[ u^2 = \omega^2 A^2 - x_1^2 \quad \text{(2)} \] - For the second position \( x_2 \): - Velocity \( v \) and acceleration \( \beta \): \[ \beta = -\omega^2 x_2 \quad \text{(3)} \] \[ v^2 = \omega^2 A^2 - x_2^2 \quad \text{(4)} \] 3. **Relating Accelerations**: - From equations (1) and (3): \[ \alpha + \beta = -\omega^2 (x_1 + x_2) \] - Rearranging gives: \[ x_1 + x_2 = -\frac{\alpha + \beta}{\omega^2} \quad \text{(5)} \] 4. **Relating Velocities**: - Subtract equation (4) from equation (2): \[ u^2 - v^2 = (\omega^2 A^2 - x_1^2) - (\omega^2 A^2 - x_2^2) \] - Simplifying gives: \[ u^2 - v^2 = x_2^2 - x_1^2 \] - This can be factored as: \[ u^2 - v^2 = (x_2 - x_1)(x_2 + x_1) \quad \text{(6)} \] 5. **Substituting for \( x_1 + x_2 \)**: - From equation (5), substitute \( x_1 + x_2 \) into equation (6): \[ u^2 - v^2 = (x_2 - x_1)\left(-\frac{\alpha + \beta}{\omega^2}\right) \] - Rearranging gives: \[ x_2 - x_1 = \frac{u^2 - v^2}{-\frac{\alpha + \beta}{\omega^2}} = \frac{(u^2 - v^2) \omega^2}{\alpha + \beta} \] 6. **Final Result**: - The distance between the two positions \( x_2 - x_1 \) is: \[ x_2 - x_1 = \frac{u^2 - v^2}{\alpha + \beta} \] ### Conclusion: The distance between the two positions is given by: \[ \boxed{\frac{u^2 - v^2}{\alpha + \beta}} \]
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