Time period of satellite
T = 2π √((R+h)³ / (G M)) = 2π / ω. For low Earth orbit, T ≈ 84 min. Geostationary orbit: T = 24 h, altitude ≈ 35,786 km.
-- NCERT Class 11 Physics, Ch. 7, p. 13Time Period of a Satellite
The trap that costs marks here: treating the satellite's period T as linearly proportional to orbital radius. It is not. The correct relationship is T ∝ r^(3/2), and confusing the exponent turns a 45-second question into a lost mark.
A satellite in circular orbit at radius r from Earth's centre has its gravitational pull supplying the centripetal force. Setting GMm/r² = mv²/r gives the orbital velocity v = √(GM/r). The circumference of the orbit is 2πr, so the time period is:
T = 2πr / v = 2πr / √(GM/r) = 2π√(r³/GM)
Squaring: T² = (4π²/GM) r³
This is Kepler's third law applied to a circular orbit (NCERT Class 11 Physics Chapter 7, page 3). For a satellite at altitude h above Earth's surface, r = R + h, giving T = 2π√((R+h)³ / GM).
Key points:
Watch out: When a question says "orbital radius doubles," reach for the 3/2 power, not the linear scaling. The linear-scaling distractor appears repeatedly in NEET options.
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
The time period of a satellite orbiting Earth depends on which of the following?
What is the approximate time period of a satellite orbiting very close to Earth's surface? (Take R = 6400 km, g = 9.8 m/s²)
In the formula T² = (4π²/GM)r³ for a satellite's time period, the quantity 4π²/GM is:
A satellite orbits Earth with period T at orbital radius r. If another satellite orbits at radius 4r, what is its period?
Two satellites A and B orbit the same planet. Satellite A has an orbital radius 9 times that of satellite B. The ratio T_A / T_B is:
A geostationary satellite has a period of 24 hours. A satellite in a circular orbit at half the geostationary orbital radius would have a period of:
A planet has twice the mass and twice the radius of Earth. What is the ratio of the time period of a near-surface satellite on this planet to that on Earth?
A satellite orbits Earth at altitude h = R (where R is Earth's radius) with period T₁. Another satellite orbits at altitude h = 3R. What is the ratio T₂/T₁?
Given
- T_A = 8 years - r_B = 4 r_A
Required
Find T_B.
Concept
Kepler's third law relates the time period of orbiting bodies to their orbital radii when orbiting the same central mass: T² ∝ r³.
Formula
T₂/T₁ = (r₂/r₁)^(3/2) Source: NCERT Class 11 Physics Chapter 7, page 3.
Substitution
T_B / T_A = (4 r_A / r_A)^(3/2) = 4^(3/2)
Calculation
4^(3/2) = (4^1)(4^(1/2)) = 4 × 2 = 8 Note: The multiplier 4 (the radius ratio) is an exact integer from the problem statement — it does not limit significant figures. T_B = 8 × 8 years = 64 years
Final answer
**T_B = 64 years** The quantity 8 (years) is given exactly in the problem, and the ratio 4 is an exact integer, so the answer is exact: 64 years. No significant-figure truncation applies.
Common trap
A common mistake is to assume T ∝ r (linear), giving T_B = 4 × 8 = 32 years. This is wrong because Kepler's third law states T² ∝ r³ (i.e. T ∝ r^(3/2)), not T ∝ r. The linear-scaling distractor (32 years) is a high-frequency wrong option in NEET.
Similar NEET-style question
If a satellite orbiting Earth has period T at orbital radius r, what is the period of a satellite at orbital radius 9r around the same body? Answer: T_new = T × 9^(3/2) = 27T. ---
T = 2π √((R+h)³ / (G M)) = 2π / ω. For low Earth orbit, T ≈ 84 min. Geostationary orbit: T = 24 h, altitude ≈ 35,786 km.
-- NCERT Class 11 Physics, Ch. 7, p. 13Minimum speed for an object to escape gravity to infinity from radius R. Earth: ~11.2 km/s.
| Symbol | Quantity | SI Unit |
|---|---|---|
| v_e | escape velocity | m/s |
| M | planet mass | kg |
| R | planet radius | m |
| g | surface gravity | m/s^2 |
PE of two-body system; negative because gravity is attractive (work to separate them is positive).
| Symbol | Quantity | SI Unit |
|---|---|---|
| U | grav PE | J |
| M, m | two masses | kg |
| r | separation | m |
Gravitational acceleration decreases with altitude above Earth's surface.
| Symbol | Quantity | SI Unit |
|---|---|---|
| g_h | g at height h | m/s^2 |
| g | surface g | m/s^2 |
| R | Earth radius | m |
| h | altitude | m |
Inside Earth (uniform density), g decreases linearly with depth, vanishing at centre.
| Symbol | Quantity | SI Unit |
|---|---|---|
| g_d | g at depth | m/s^2 |
| g | surface g | m/s^2 |
| R | Earth radius | m |
| d | depth | m |
Square of orbital period proportional to cube of semi-major axis. Holds for elliptic orbits about a central mass.
| Symbol | Quantity | SI Unit |
|---|---|---|
| T | orbital period | s |
| a | semi-major axis | m |
| M | central mass | kg |
Speed of circular orbit at altitude h above body of mass M, radius R.
| Symbol | Quantity | SI Unit |
|---|---|---|
| v | orbital speed | m/s |
| M | central mass | kg |
| R+h | orbit radius | m |
Total energy = KE + PE = -KE (virial). Always negative for bound orbit; E -> 0 at infinity.
| Symbol | Quantity | SI Unit |
|---|---|---|
| E | total energy | J |
| M, m | central mass and satellite mass | kg |
| R+h | orbit radius | m |
Attractive force between any two masses. Inverse-square central force.
| Symbol | Quantity | SI Unit |
|---|---|---|
| F | force | N |
| G | grav constant = 6.674e-11 | N*m^2/kg^2 |
| m1, m2 | masses | kg |
| r | centre-to-centre distance | m |
These are the exact patterns that cause wrong answers in NEET. Each trap includes when it triggers and how to avoid it.
Category: Similar Terms
Student treats g(h) as linear in h. Actual: g(R/(R+h))² (inverse-square).
Question asks for g at significant altitude (e.g. R/2 above surface).
Use g_h = g (R/(R+h))². Linear approximation g(1 - 2h/R) only valid for h << R.
Category: Similar Terms
Student treats T proportional to a (linear) instead of a^(3/2).
Question gives change in semi-major axis and asks for new period.
T² ∝ a³, so T ∝ a^(3/2). Doubling a multiplies T by 2^(3/2) ≈ 2.83.
Root cause: formula misuse
Use g_h = g(R/(R+h))² (inverse-square). Linear approximation g(1-2h/R) is only valid for h << R. For h = R/2, the exact formula gives g_h = (2/3)² g = 4g/9, not g(1-1) = 0.
Root cause: formula misuse
T² ∝ a³, so T ∝ a^(3/2). Doubling a multiplies T by 2^(3/2) ≈ 2.83. Quadrupling a → 8× T.
forgets density not mass
Confuses planet mass with density given radius scaling
uses linear decrease with h
Treats g as linear in h instead of inverse-square
uses linear relation
Treats T proportional to a not a^(3/2)
forgets orbital KE component
Computes only PE change, ignoring orbital KE
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