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Passage XI) The differential equation of...

Passage XI) The differential equation of a particle undergoing SHM is given by `a(d^(2)x)/(dt^(2))`+bx = 0. The particle starts from the extreme position.
The ratio of the maximum acceleration to the maximum velocity of the particle is

A

b/a

B

a/b

C

`sqrt(a/b)`

D

`sqrt(b/a)`

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The correct Answer is:
To solve the problem, we need to analyze the given differential equation of a particle undergoing Simple Harmonic Motion (SHM) and derive the required ratio of maximum acceleration to maximum velocity. ### Step-by-Step Solution: 1. **Understand the Differential Equation**: The differential equation given is: \[ a \frac{d^2x}{dt^2} + bx = 0 \] This represents the motion of a particle in SHM. 2. **Rearranging the Equation**: We can rearrange the equation to express the acceleration: \[ a \frac{d^2x}{dt^2} = -bx \] Dividing both sides by \(a\): \[ \frac{d^2x}{dt^2} = -\frac{b}{a} x \] 3. **Identifying the Angular Frequency**: The standard form of SHM is: \[ \frac{d^2x}{dt^2} = -\omega^2 x \] By comparing both equations, we can identify: \[ \omega^2 = \frac{b}{a} \] Therefore, the angular frequency \(\omega\) is: \[ \omega = \sqrt{\frac{b}{a}} \] 4. **Maximum Acceleration and Maximum Velocity**: - The maximum acceleration \(A_{max}\) in SHM is given by: \[ A_{max} = \omega^2 A \] - The maximum velocity \(V_{max}\) in SHM is given by: \[ V_{max} = \omega A \] 5. **Finding the Ratio**: We need to find the ratio of maximum acceleration to maximum velocity: \[ \frac{A_{max}}{V_{max}} = \frac{\omega^2 A}{\omega A} \] Simplifying this gives: \[ \frac{A_{max}}{V_{max}} = \frac{\omega^2}{\omega} = \omega \] 6. **Substituting the Value of \(\omega\)**: From our earlier calculation, we have: \[ \omega = \sqrt{\frac{b}{a}} \] Thus, the ratio of maximum acceleration to maximum velocity is: \[ \frac{A_{max}}{V_{max}} = \sqrt{\frac{b}{a}} \] ### Final Answer: The ratio of the maximum acceleration to the maximum velocity of the particle is: \[ \sqrt{\frac{b}{a}} \]
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