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Question #43519
The Question
A satellite of mass is in a circular orbit of radius around the Earth (mass ). The thin atmosphere exerts a tangential drag force of magnitude on the satellite, where is its orbital speed and is a positive constant.
In Scenario A, the satellite's onboard engine provides a continuous tangential thrust to maintain the satellite in the exact same circular orbit of radius . Let be the mechanical power delivered by the engine.
In Scenario B, the engine is turned off, and the satellite's orbit slowly decays while remaining approximately circular. Let be the rate at which the gravitational potential energy of the satellite-Earth system decreases at the instant the orbital radius is .
What is the ratio ?
Options
- A.
- B.
- C.
- D.
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Correct Answer
Step-by-Step Solution
Explanation
How the Examiner Thinks
Variable_Constraint
Develop pure symbolic logic skills by mastering algebraic constraints without relying on numerical data.
Concepts Behind This Question
Geostationary Satellite Constraints|Power-Velocity Relationship|Integration
Why This Question Is Tricky
Common Mistakes
This question tests the application of the Work-Energy Theorem in orbital mechanics, specifically targeting the 'satellite paradox.' A common misconception is that the rate of loss of potential energy directly equals the power dissipated by drag (), which would incorrectly yield a ratio of 1.
However, because the orbit remains quasi-circular, the kinetic energy actually increases as the orbit decays ().
Since total energy is half the potential energy , the potential energy must decrease at twice the rate of the total energy loss to account for both the work done against drag and the simultaneous increase in kinetic energy.
Quick Facts About This Question
Question Information
| Subject | Physics |
| Chapter | Gravitation - Class 11 Part 1 |
| Concept | Geostationary Satellite Constraints |
| Difficulty | 8 |
| Cognitive Load | 7 |
| Target Solve Time | 160 sec |
| Access | Free |