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A particle moves in a circular orbit ...

A particle moves in a circular orbit under the action of a central attractive force which is inversely proportional to the distance 'r' . The speed of the particle is

A

proportional to ` r^(2)`

B

Independent of `r`

C

proportional to r

D

proportional to 1/r

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The correct Answer is:
To solve the problem, we need to analyze the motion of a particle in a circular orbit under the influence of a central attractive force that is inversely proportional to the distance \( r \). ### Step-by-Step Solution: 1. **Identify the Forces Acting on the Particle:** The particle is moving in a circular orbit due to a central attractive force. This force can be expressed as: \[ F = \frac{k}{r} \] where \( k \) is a constant. 2. **Use Centripetal Force Equation:** For an object moving in a circular path, the required centripetal force \( F_c \) is given by: \[ F_c = \frac{mv^2}{r} \] where \( m \) is the mass of the particle and \( v \) is its speed. 3. **Set the Attractive Force Equal to the Centripetal Force:** Since the attractive force provides the necessary centripetal force, we can set these two forces equal to each other: \[ \frac{mv^2}{r} = \frac{k}{r} \] 4. **Simplify the Equation:** We can multiply both sides by \( r \) (assuming \( r \neq 0 \)): \[ mv^2 = k \] 5. **Solve for Speed \( v \):** Rearranging the equation gives us: \[ v^2 = \frac{k}{m} \] Taking the square root of both sides, we find: \[ v = \sqrt{\frac{k}{m}} \] 6. **Conclusion:** The speed of the particle \( v \) is independent of the radius \( r \) and depends only on the constant \( k \) and the mass \( m \). ### Final Answer: The speed of the particle is given by: \[ v = \sqrt{\frac{k}{m}} \]

To solve the problem, we need to analyze the motion of a particle in a circular orbit under the influence of a central attractive force that is inversely proportional to the distance \( r \). ### Step-by-Step Solution: 1. **Identify the Forces Acting on the Particle:** The particle is moving in a circular orbit due to a central attractive force. This force can be expressed as: \[ F = \frac{k}{r} ...
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