A satellite is held in orbit by a \( 2000-\mathrm{N} \) gravitational force. Each time the satellite completes an orbit of circumference 80000 km , the work done on it by gravity is: 1) \( 1.6^{\prime} 10^{8} \mathrm{~J} \). 2) \( 1.6^{\cdot} 10^{11} \mathrm{~J} \). 3) \( 6.4^{\prime} 10^{11} \mathrm{~J} \). 4) 0 . 5) None of the above.
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The Deep Dive
When a satellite orbits the Earth, the gravitational force acts as a centripetal force, maintaining the satellite's circular motion. However, since the direction of the gravitational force is always directed towards the center of the Earth and the satellite is moving tangentially, the gravitational force does no work on the satellite as it travels along its orbit. Consequently, the work done by gravity over one complete orbit is 0 Joules. In practical scenarios like satellite maintenance, engineers need to consider the satellite's orbital decay and potential adjustments. By utilizing rocket thrusters, satellites can effectively counteract gravitational pull and maintain their designated orbit, ensuring functionality for longer periods. It's a fascinating balance of physics and real-world application!
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