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A sphere of mass m is tied to end of a s...

A sphere of mass m is tied to end of a string of length l and rotated through the other end along a horizontal circular path with speed v . The work done in full horizontal circle is

A

0

B

`((mv^(2))/(l)).2pil`

C

`mg.2pi l`

D

`((mv^(2))/(l)).(l)`

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AI Generated Solution

The correct Answer is:
To solve the problem of the work done when a sphere of mass \( m \) is tied to a string of length \( l \) and rotated in a horizontal circular path with speed \( v \), we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Forces Acting on the Sphere:** - The sphere experiences two main forces: the tension \( T \) in the string acting upwards and the gravitational force \( mg \) acting downwards. - In the horizontal circular motion, the net force acting towards the center of the circle is provided by the horizontal component of the tension. 2. **Analyzing the Circular Motion:** - The sphere moves in a horizontal circle, so the tension in the string must provide the necessary centripetal force required for circular motion. - The centripetal force \( F_c \) can be expressed as: \[ F_c = \frac{mv^2}{r} \] - Here, \( r \) is the radius of the circular path, which is equal to the length of the string \( l \) in this case. 3. **Setting Up the Equation for Tension:** - The vertical forces must balance since the sphere does not move vertically. Therefore, we can write: \[ T - mg = 0 \quad \Rightarrow \quad T = mg \] 4. **Finding the Work Done:** - Work done \( W \) is defined as the dot product of force and displacement: \[ W = \vec{F} \cdot \vec{d} \] - In this scenario, the tension \( T \) acts perpendicular to the displacement of the sphere as it rotates. Since the angle \( \theta \) between the tension force and the displacement is \( 90^\circ \): \[ W = T \cdot d \cdot \cos(90^\circ) \] - Since \( \cos(90^\circ) = 0 \), the work done is: \[ W = T \cdot d \cdot 0 = 0 \] 5. **Conclusion:** - The work done in completing a full horizontal circle is zero because the force (tension) is always perpendicular to the displacement of the sphere. ### Final Answer: The work done in a full horizontal circle is \( \boxed{0} \).
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