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Let r be the distance of a particle from...

Let `r` be the distance of a particle from a fixed point to which it is attracted by an inverse square law force given by `F=k//r^2` (k=constant). Let m be the mass of the particle and L be its angular momentum with respect to the fixed point. Which of the following formulae is correct about the total energy of the system?

A

(a) `1/2m((dr)/(dt))^2-k/r+(L)/(2mr^2)=Constant`

B

(b) `1/2m((dr)/(dt))^2-k/r=Const ant`

C

(c) `1/2m((dr)/(dt))^2+k/r+(L^2)/(2mr^2)=Const ant`

D

(d) None

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To solve the problem, we need to derive the total energy of a particle under the influence of an inverse square law force, given by \( F = \frac{k}{r^2} \), where \( k \) is a constant, \( r \) is the distance from a fixed point, \( m \) is the mass of the particle, and \( L \) is its angular momentum. ### Step-by-Step Solution: 1. **Identify the Total Energy**: The total energy \( E \) of the system consists of kinetic energy \( K \) and potential energy \( U \): \[ E = K + U \] 2. **Calculate the Potential Energy**: The potential energy \( U \) associated with a conservative force can be found by integrating the force: \[ U(r) = -\int F \, dr = -\int \frac{k}{r^2} \, dr \] The integral of \( \frac{k}{r^2} \) is: \[ U(r) = -\left[-\frac{k}{r}\right] + C \] Assuming the potential energy at infinity is zero (\( U(\infty) = 0 \)), we have: \[ U(r) = -\frac{k}{r} \] 3. **Calculate the Kinetic Energy**: The kinetic energy \( K \) can be expressed in terms of the radial and angular components of velocity. The total velocity \( v \) can be expressed as: \[ v^2 = v_r^2 + v_\theta^2 \] where \( v_r \) is the radial component and \( v_\theta \) is the tangential component. The tangential component can be related to angular momentum \( L \): \[ v_\theta = \frac{L}{mr} \] Thus, the kinetic energy becomes: \[ K = \frac{1}{2} mv^2 = \frac{1}{2} m\left(v_r^2 + \left(\frac{L}{mr}\right)^2\right) \] Simplifying this, we get: \[ K = \frac{1}{2} mv_r^2 + \frac{L^2}{2mr^2} \] 4. **Combine Kinetic and Potential Energy**: Now, substituting the expressions for \( K \) and \( U \) into the total energy equation: \[ E = \frac{1}{2} mv_r^2 + \frac{L^2}{2mr^2} - \frac{k}{r} \] 5. **Final Expression for Total Energy**: The total energy can be expressed as: \[ E = \frac{L^2}{2mr^2} + \frac{1}{2} mv_r^2 - \frac{k}{r} \] ### Conclusion: The total energy of the system is given by: \[ E = \frac{L^2}{2mr^2} + \frac{1}{2} mv_r^2 - \frac{k}{r} \]

To solve the problem, we need to derive the total energy of a particle under the influence of an inverse square law force, given by \( F = \frac{k}{r^2} \), where \( k \) is a constant, \( r \) is the distance from a fixed point, \( m \) is the mass of the particle, and \( L \) is its angular momentum. ### Step-by-Step Solution: 1. **Identify the Total Energy**: The total energy \( E \) of the system consists of kinetic energy \( K \) and potential energy \( U \): \[ E = K + U ...
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