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A thin of length L is bent to form a sem...

A thin of length `L` is bent to form a semicircle. The mass of rod is M. What will be the gravitational potential at the centre of the circle ?

A

`-(GM)/(L)`

B

`-(GM)/(2piL)`

C

`-(piGM)/(2L)`

D

`-(piGM)/(L)`

Text Solution

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The correct Answer is:
To find the gravitational potential at the center of a semicircular rod of length \( L \) and mass \( M \), we can follow these steps: ### Step 1: Relate the length of the rod to the radius of the semicircle The length \( L \) of the rod is equal to the circumference of the semicircle. The circumference \( C \) of a full circle is given by \( C = 2\pi r \). Therefore, for a semicircle, the length can be expressed as: \[ L = \pi r \] From this equation, we can solve for the radius \( r \): \[ r = \frac{L}{\pi} \] ### Step 2: Use the formula for gravitational potential The gravitational potential \( V \) at a distance \( r \) from a mass \( M \) is given by the formula: \[ V = -\frac{GM}{r} \] where \( G \) is the universal gravitational constant. ### Step 3: Substitute the radius into the gravitational potential formula Now that we have \( r \) in terms of \( L \), we can substitute \( r = \frac{L}{\pi} \) into the gravitational potential formula: \[ V = -\frac{GM}{\frac{L}{\pi}} = -\frac{GM\pi}{L} \] ### Step 4: Final expression for gravitational potential Thus, the gravitational potential at the center of the semicircle is: \[ V = -\frac{GM\pi}{L} \] ### Summary The gravitational potential at the center of the semicircle formed by the rod of length \( L \) and mass \( M \) is given by: \[ V = -\frac{GM\pi}{L} \]

To find the gravitational potential at the center of a semicircular rod of length \( L \) and mass \( M \), we can follow these steps: ### Step 1: Relate the length of the rod to the radius of the semicircle The length \( L \) of the rod is equal to the circumference of the semicircle. The circumference \( C \) of a full circle is given by \( C = 2\pi r \). Therefore, for a semicircle, the length can be expressed as: \[ L = \pi r \] From this equation, we can solve for the radius \( r \): ...
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