Variation of g with altitude
At height h above Earth's surface: g_h = g (R/(R+h))² ≈ g(1 - 2h/R) for h << R. Decreases with altitude.
-- NCERT Class 11 Physics, Ch. 7, p. 6The trap that costs marks: You see "find g at height h = R above the surface" and instinctively write g_h = g(1 − 2h/R). That gives g(1 − 2) = −g — a negative acceleration due to gravity. The answer is obviously wrong, but under exam pressure, students pick the distractor built from exactly this mistake. This trap has appeared in NEET 2024 and 2025.
The actual formula. Gravitational acceleration at altitude h above a spherical Earth of radius R is:
g_h = g × (R / (R + h))²
This is an inverse-square dependence on the distance from Earth's centre, not a linear decrease from the surface. The derivation is direct: at the surface, g = GM/R²; at height h, the distance from the centre is (R + h), so g_h = GM/(R + h)² = g × R²/(R + h)² (NCERT Class 11 Physics Chapter 7, page 6).
When does the approximation work? The linear form g_h ≈ g(1 − 2h/R) is a binomial expansion valid only when h ≪ R. For a satellite 200 km above Earth (R ≈ 6400 km), h/R ≈ 0.03 — the approximation is fine. For h = R/2, h = R, or h = 2R, it fails badly.
Quick checkpoint: at h = R, the exact formula gives g_h = g(R/2R)² = g/4. The linear approximation gives g(1 − 2) = −g. If your answer is negative, you used the wrong formula.
Watch-out for NEET stems: Questions often state height as a fraction of R (e.g., "at a height equal to half the radius"). Convert to h = R/2 and substitute into the exact formula. Do not default to the approximation unless the problem explicitly states h ≪ R.
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
The acceleration due to gravity at a height h above the Earth's surface is given by which expression? (R = radius of Earth, g = surface gravity)
The approximate formula g_h ≈ g(1 − 2h/R) for variation of g with altitude is valid under which condition?
At what altitude above the Earth's surface does the acceleration due to gravity become zero, according to g_h = g(R/(R + h))²?
A body weighs 63 N on the surface of the Earth. What is its weight at a height equal to half the radius of the Earth above the surface?
The acceleration due to gravity at a height of 3200 km above the Earth's surface is (take R = 6400 km, g = 9.8 m/s²):
At what height above the Earth's surface does the acceleration due to gravity reduce to 1/9 of its surface value? (R = radius of Earth)
A body weighs W on the surface of the Earth. At what height above the surface will its weight become W/16? Express your answer in terms of R (radius of Earth).
The ratio of acceleration due to gravity at a height R above the Earth's surface to that at a depth R/2 below the Earth's surface is: (R = radius of Earth, assume uniform density)
Given
A body weighs 900 N on the surface of the Earth. Find its weight at a height equal to the radius of the Earth (h = R) above the surface. Take R = 6400 km.
Required
Weight at height h = R.
Concept
Gravitational acceleration decreases with altitude as an inverse-square function of the distance from Earth's centre (NCERT Class 11 Physics Chapter 7, page 6). Weight is proportional to local g.
Formula
g_h = g × (R / (R + h))² W_h = W × (R / (R + h))²
Substitution
h = R, so (R + h) = 2R. W_h = 900 × (R / 2R)² W_h = 900 × (1/2)²
Calculation
W_h = 900 × 1/4 = 225 N Note: the factor 4 in the denominator is an exact counting integer (2² = 4) and does not affect significant-figure count.
Final answer
W_h = 225 N The exact constant 4 (from 2² in the denominator) and the integer ratio R/2R = 1/2 do not limit significant figures. The precision is governed by the given weight (900 N, which we treat as exact for this problem since it is a clean given value).
Common trap
Using the linear approximation g(1 − 2h/R) here gives g(1 − 2) = −g, implying negative weight. This is the high-frequency trap for this topic — the approximation requires h ≪ R, and h = R violates that condition completely.
Similar NEET-style question
A satellite orbits at a height equal to 3 times the radius of the Earth. What fraction of the surface gravity does it experience? (Answer: g_h = g(R/4R)² = g/16.) ---
At height h above Earth's surface: g_h = g (R/(R+h))² ≈ g(1 - 2h/R) for h << R. Decreases with altitude.
-- NCERT Class 11 Physics, Ch. 7, p. 6Minimum 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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