Section 2.8: Problem-Solving Strategies
This section introduces systematic strategies for solving gravitation and satellite-related problems efficiently.
List all given values and what is being asked. Draw diagrams for satellite orbits and forces if necessary.
Use Newton’s law of gravitation, centripetal force, orbital velocity, and energy conservation equations appropriately.
Check units, directions, and whether orbits are circular or elliptical. Use approximations if valid.
Substitute known values carefully. Solve algebraically before plugging numbers. Double-check arithmetic.
Check whether the answer is reasonable. Compare with known limits like Earth’s escape velocity, LEO/MEO/Geostationary ranges.
Example 1
A satellite of mass 500 kg orbits Earth at 500 km above the surface. Find its orbital speed and period.
Radius: r = 6371 + 500 = 6871 km = 6.871×10^6 m
Orbital speed: v = √(GM/r) ≈ √(6.674×10^-11 × 5.972×10^24 / 6.871×10^6) ≈ 7610 m/s
Orbital period: T = 2πr/v ≈ 2π×6.871×10^6 / 7610 ≈ 5670 s ≈ 1.58 h
Example 2
Determine the escape velocity from the surface of Mars (mass 6.42×10^23 kg, radius 3.39×10^6 m).
v_esc = √(2GM/R) = √(2 × 6.674×10^-11 × 6.42×10^23 / 3.39×10^6) ≈ 5.03 km/s
Practice Problems
- Calculate the orbital speed of a satellite 1000 km above Earth.
- Determine the period of a satellite in geostationary orbit.
- Compute escape velocity from the Moon (mass 7.35×10^22 kg, radius 1.74×10^6 m).
- Find the gravitational potential energy of a 200 kg satellite at 400 km above Earth.
- Calculate centripetal acceleration of a GPS satellite.
- Determine the speed required for a satellite to maintain a circular orbit around Earth at 2×10^7 m.
- Check reasonableness of orbital radius given a period of 90 minutes.
- Compare speeds of satellites in LEO vs MEO.
- Estimate orbital period of a satellite around Mars at 3×10^6 m above the surface.
- Explain why satellites in low Earth orbit experience faster orbital motion than geostationary satellites.