Orbital Velocity, Time Period, Geostationary Orbit and Kepler's Laws
Gravitation: Orbital Velocity, Time Period, Geostationary Orbit and Kepler's Laws
Orbital Velocity, Time Period, Geostationary Orbit and Kepler's Laws
Orbital Velocity, Time Period, Geostationary Orbit and Kepler's Laws
What you'll learn
- Orbital velocity: v_o = √(GM/r) — speed for circular orbit at radius r.
- Time period: T = 2πr/v_o = 2π√(r³/GM) — Kepler's third law built in.
- Kepler's three laws: elliptical orbits, equal areas, T² ∝ r³.
- Geostationary orbit: r ≈ 42,400 km from Earth's centre; T = 24 h; used for communication satellites.
- Total energy of orbiting satellite: E = −GMm/(2r) (half of potential energy).
Key concepts
Level 1 — Foundations
Verbal: A satellite in circular orbit has gravity providing centripetal force — just fast enough that it keeps missing the Earth as it falls.
Orbital velocity derivation: GMm/r² = mv²/r → v_o = √(GM/r). Note: v_o decreases as r increases — higher orbits are slower.
Time period: T = 2πr/v_o = 2πr/√(GM/r) = 2π√(r³/GM).
Kepler's Third Law: T² ∝ r³ (for all planets/satellites around same central body). Precise form: T² = (4π²/GM) r³.
Kepler's First Law: Planets move in ellipses with Sun at one focus.
Kepler's Second Law: Line joining planet to Sun sweeps equal areas in equal time intervals (angular momentum conservation).
Geostationary satellite: T = 24 h, orbit in equatorial plane, appears stationary from Earth. r_geo ≈ 42,400 km from Earth's centre (≈ 36,000 km above surface).
Level 2 — JEE / NEET depth
Orbital speed vs escape speed: v_e = √2 × v_o at same radius.
Energy of satellite in circular orbit:
- KE = ½mv_o² = GMm/(2r)
- PE = −GMm/r
- Total E = KE + PE = GMm/(2r) − GMm/r = −GMm/(2r)
- Binding energy = +GMm/(2r) (energy needed to remove satellite from orbit).
When orbit radius increases: Speed decreases (v ∝ 1/√r), PE increases (less negative), KE decreases, but total E increases (less negative). Adding energy to satellite raises orbit and slows it down (counterintuitive).
Ratio method for two orbits: T₁²/T₂² = r₁³/r₂³ (very useful for JEE without computing GM).
Kepler 3rd law extended: For any body around same M: T²/r³ = 4π²/GM = constant.
Geostationary orbit calculation: T = 2π√(r³/GM), T = 24×3600 s, GM_earth = 4×10¹⁴. r³ = GMt²/(4π²) → r ≈ 4.24×10⁷ m = 42,400 km.
Polar orbit: Low Earth orbit, T ≈ 90 min, covers all latitudes — used for remote sensing and weather satellites.
Worked example
Orbital velocity and time period at two heights
Find orbital velocity and time period for satellites at:
(a) Just above Earth surface (r = R = 6.4×10⁶ m, g = 9.8 m/s²)
(b) r = 4R from Earth's centre.
G M_earth = g R² = 9.8 × (6.4×10⁶)² = 9.8 × 4.096×10¹³ = 4.014×10¹⁴ m³/s²
Part (a) — r = R:
v_o = √(GM/R) = √(4.014×10¹⁴ / 6.4×10⁶) = √(6.28×10⁷) ≈ 7920 m/s ≈ 7.9 km/s
T = 2π√(R³/GM) = 2π√(R/g) = 2π√(6.4×10⁶/9.8)
= 2π × √(6.53×10⁵) = 2π × 808 ≈ 5077 s ≈ 84.6 min
Part (b) — r = 4R:
v_o = √(GM/4R) = v_o(surface) / √4 = 7920/2 = 3960 m/s ≈ 4 km/s
T = 2π√((4R)³/GM) = 2π√(64R³/GM) = T_surface × √64 = 84.6 × 8 ≈ 677 min ≈ 11.3 h
(Or use T²∝r³: T₂ = T₁ × (r₂/r₁)^(3/2) = 84.6 × 4^(3/2) = 84.6 × 8 ≈ 677 min ✓)
Kepler's law ratio problem
Mars orbits Sun at mean radius 1.52 AU. Earth's period = 1 year.
Find Mars's orbital period.
Step 1 — Kepler's third law (same central body = Sun):
T_Mars² / T_Earth² = r_Mars³ / r_Earth³
Step 2 — Ratio:
T_Mars² = T_Earth² × (1.52)³ = 1² × 3.512 = 3.512 yr²
Step 3 — Period:
T_Mars = √3.512 ≈ 1.874 years ≈ 687 days ✓ (actual: 687 days)
Common mistakes
| Mistake | Why it happens | Fix |
|---|---|---|
| v_o increases with height | Confusing with escape speed | v_o = √(GM/r) — decreases with r; higher orbit → slower |
| T ∝ r (linear) | Forgetting exponent | Kepler: T² ∝ r³, so T ∝ r^(3/2) |
| Total satellite energy is positive | Forgetting negative sign | Bound orbit: E = −GMm/(2r) — negative means bound |
| Geostationary orbit height ≈ 36,000 km above surface | Confusing height and radius | r_geo = 42,400 km from centre; height above surface = 36,000 km |
Quick check
- What is the orbital velocity of a satellite at height h = R above Earth's surface?
- State Kepler's three laws in one sentence each.
- A satellite's orbital radius doubles. By what factor does its period change?
- Why does a geostationary satellite always appear fixed over one location?
- Stretch: A satellite has total energy −5×10⁹ J. Find its KE and PE. Is it in orbit or escaping?
NCERT Chapter 8 link: Orbital mechanics unites Newton's gravitation with Kepler's empirical laws — Kepler derived patterns, Newton explained them. Use T²∝r³ as a ratio shortcut instead of substituting GM. Remember: total energy of satellite = −(KE), so raising orbit requires adding energy.
Exam connections: JEE tests: orbital speed at given height; T using Kepler ratio; geostationary orbit height; energy of satellite (which is PE/2 in magnitude); comparison of orbital and escape speeds. Classic: satellite moved to higher orbit — speed decreases but energy increases (less negative).
Study strategy: Derive v_o and T from scratch (gravitational force = centripetal force) at least once to understand the physics. Then use ratio methods for speed problems. Always distinguish r (from Earth's centre) from h (height above surface): r = R + h.
Interactive Exploration Suggestions (Drishti Live Worlds)
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AI Mentor Prompts (Socratic, Board-Adaptive)
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Key Takeaways (TL;DR)
- What you'll learn
- Key concepts
- Worked example
- Common mistakes
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