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A particle of mass m oscillates with a p...

A particle of mass m oscillates with a potential energy `U=U_(0)+alpha x^(2)`, where `U_(0)` and `alpha` are constants and x is the displacement of particle from equilibrium position. The time period of oscillation is

A

`2pi sqrt((m)/(alpha))`

B

`2pi sqrt((m)/(2 alpha))`

C

`pi sqrt((2m)/(alpha))`

D

`2pi sqrt((m)/(alpha^(2)))`

Text Solution

AI Generated Solution

The correct Answer is:
To find the time period of oscillation for a particle of mass \( m \) with a potential energy given by \( U = U_0 + \alpha x^2 \), we can follow these steps: ### Step 1: Understand the Potential Energy Function The potential energy function is given as: \[ U = U_0 + \alpha x^2 \] where \( U_0 \) is a constant, \( \alpha \) is a constant, and \( x \) is the displacement from the equilibrium position. ### Step 2: Determine the Force Acting on the Particle The force \( F \) acting on the particle can be derived from the potential energy using the formula: \[ F = -\frac{dU}{dx} \] Calculating the derivative of \( U \) with respect to \( x \): \[ \frac{dU}{dx} = \frac{d}{dx}(U_0 + \alpha x^2) = 0 + 2\alpha x = 2\alpha x \] Thus, the force becomes: \[ F = -2\alpha x \] ### Step 3: Relate the Force to Hooke's Law The force can be expressed in the form of Hooke's law: \[ F = -kx \] Comparing this with our expression for force, we identify: \[ k = 2\alpha \] ### Step 4: Calculate the Time Period of Oscillation The time period \( T \) of a simple harmonic oscillator is given by the formula: \[ T = 2\pi \sqrt{\frac{m}{k}} \] Substituting \( k = 2\alpha \) into the equation: \[ T = 2\pi \sqrt{\frac{m}{2\alpha}} \] ### Final Answer Thus, the time period of oscillation is: \[ T = 2\pi \sqrt{\frac{m}{2\alpha}} \] ---

To find the time period of oscillation for a particle of mass \( m \) with a potential energy given by \( U = U_0 + \alpha x^2 \), we can follow these steps: ### Step 1: Understand the Potential Energy Function The potential energy function is given as: \[ U = U_0 + \alpha x^2 \] where \( U_0 \) is a constant, \( \alpha \) is a constant, and \( x \) is the displacement from the equilibrium position. ...
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