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A particle of mass m moves on the x-axis...

A particle of mass m moves on the x-axis under the influence of a force of attraction towards the origin O given by `F=-(k)/(x^(2))hat(i)`. If the particle starts from rest at x = a. The speed of it will attain to reach at distance x from the origin O will be

A

`sqrt((2k)/(m))[(x-a)/(ax)]^(1//2`

B

`sqrt((2k)/(m))[(a+x)/(ax)]^(1//2`

C

`sqrt((k)/(m))[(ax)/(x-a)]`

D

`sqrt((m)/(2k))[(a-x)/(ax)]^(1//2)`

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The correct Answer is:
To solve the problem of a particle of mass \( m \) moving under the influence of a force given by \( F = -\frac{k}{x^2} \hat{i} \), we will apply the work-energy principle. The particle starts from rest at \( x = a \) and we want to find its speed when it reaches a distance \( x \) from the origin. ### Step-by-Step Solution: 1. **Identify the Force and Potential Energy**: The force acting on the particle is given by: \[ F = -\frac{k}{x^2} \hat{i} \] This is a central force directed towards the origin. The potential energy \( U(x) \) associated with this force can be found by integrating the force: \[ U(x) = -\int F \, dx = -\int -\frac{k}{x^2} \, dx = \frac{k}{x} + C \] We can choose the constant \( C = 0 \) for simplicity, so: \[ U(x) = \frac{k}{x} \] 2. **Calculate the Initial and Final Potential Energy**: At the initial position \( x = a \): \[ U(a) = \frac{k}{a} \] At the position \( x \): \[ U(x) = \frac{k}{x} \] 3. **Apply the Conservation of Energy**: The total mechanical energy at the initial position (where the particle starts from rest) is purely potential: \[ E_{initial} = U(a) = \frac{k}{a} \] At position \( x \), the total energy is the sum of kinetic energy \( K \) and potential energy \( U(x) \): \[ E_{final} = K + U(x) = \frac{1}{2} mv^2 + \frac{k}{x} \] By conservation of energy, we set the initial energy equal to the final energy: \[ \frac{k}{a} = \frac{1}{2} mv^2 + \frac{k}{x} \] 4. **Rearranging the Equation**: Rearranging the equation to solve for \( v^2 \): \[ \frac{1}{2} mv^2 = \frac{k}{a} - \frac{k}{x} \] \[ \frac{1}{2} mv^2 = k \left( \frac{1}{a} - \frac{1}{x} \right) \] \[ v^2 = \frac{2k}{m} \left( \frac{1}{a} - \frac{1}{x} \right) \] 5. **Finding the Speed**: Taking the square root to find the speed \( v \): \[ v = \sqrt{\frac{2k}{m} \left( \frac{1}{a} - \frac{1}{x} \right)} \] ### Final Answer: The speed of the particle when it reaches a distance \( x \) from the origin is given by: \[ v = \sqrt{\frac{2k}{m} \left( \frac{1}{a} - \frac{1}{x} \right)} \]

To solve the problem of a particle of mass \( m \) moving under the influence of a force given by \( F = -\frac{k}{x^2} \hat{i} \), we will apply the work-energy principle. The particle starts from rest at \( x = a \) and we want to find its speed when it reaches a distance \( x \) from the origin. ### Step-by-Step Solution: 1. **Identify the Force and Potential Energy**: The force acting on the particle is given by: \[ F = -\frac{k}{x^2} \hat{i} ...
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