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The PE of a satellite is -U . Its KE is...

The PE of a satellite is -U . Its KE is

A

U

B

2U

C

`-U`

D

U/2

Text Solution

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The correct Answer is:
To find the kinetic energy (KE) of a satellite given that its potential energy (PE) is -U, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Potential Energy (PE) Formula**: The potential energy (PE) of a satellite in a gravitational field is given by the formula: \[ PE = -\frac{G M m}{r} \] where \( G \) is the gravitational constant, \( M \) is the mass of the planet, \( m \) is the mass of the satellite, and \( r \) is the distance from the center of the planet to the satellite. 2. **Set the Given PE**: According to the problem, the potential energy of the satellite is given as: \[ PE = -U \] Therefore, we can equate the two expressions: \[ -U = -\frac{G M m}{r} \] From this, we can derive: \[ U = \frac{G M m}{r} \quad \text{(Equation 1)} \] 3. **Determine the Velocity of the Satellite**: For a satellite in a circular orbit, the centripetal force required to keep it in orbit is provided by the gravitational force. The formula for the orbital velocity \( v \) of the satellite is: \[ v = \sqrt{\frac{G M}{r}} \] 4. **Calculate the Kinetic Energy (KE)**: The kinetic energy (KE) of the satellite can be expressed as: \[ KE = \frac{1}{2} m v^2 \] Substituting the expression for \( v \): \[ KE = \frac{1}{2} m \left(\sqrt{\frac{G M}{r}}\right)^2 \] Simplifying this gives: \[ KE = \frac{1}{2} m \frac{G M}{r} \] 5. **Relate KE to PE**: From Equation 1, we know that: \[ U = \frac{G M m}{r} \] Therefore, we can substitute this into the expression for KE: \[ KE = \frac{1}{2} \cdot U \] Thus, we find that: \[ KE = \frac{U}{2} \] ### Final Answer: The kinetic energy (KE) of the satellite is: \[ KE = \frac{U}{2} \]
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