Step 1: For a satellite in a stable circular orbit, the gravitational force provides the centripetal force.
The total mechanical energy \( E_{\text{total}} \) of the satellite is:
\( E_{\text{total}} = -\frac{G M m}{2r} \), where:
- \( G \) is the gravitational constant
- \( M \) is the mass of Earth
- \( m \) is the mass of the satellite
- \( r \) is the orbital radius
Step 2: The kinetic energy of the satellite in orbit is:
\( E = \frac{G M m}{2r} \)
Step 3: To escape Earth, the satellite must have zero total mechanical energy:
That means it must gain enough kinetic energy to cancel out the negative potential energy:
So, required kinetic energy for escape = \( \frac{G M m}{r} \)
Step 4: Compare this with orbital kinetic energy:
Orbital kinetic energy = \( \frac{G M m}{2r} = E \)
Escape kinetic energy = \( \frac{G M m}{r} = 2E \)
Final Answer: \( 2E \)