Acceleration due to gravity
The acceleration produced by gravitational force on a body in free fall near Earth's surface: g = G M / R² ≈ 9.8 m/s², where M and R are Earth's mass and radius.
-- NCERT Class 11 Physics, Ch. 7, p. 5Acceleration due to gravity is the acceleration a freely falling body experiences near a massive object. On Earth's surface, g ≈ 9.8 m/s² and connects to Newton's law of gravitation: equating F = GMm/R² with mg gives g = GM/R² (NCERT Class 11 Physics Chapter 7, page 5).
The trap that costs marks: when a question gives altitude as a fraction of R — say h = R — students reach for the linear approximation g(1 − 2h/R) and get nonsensical answers. That approximation is only valid when h ≪ R. The exact formula is:
g_h = g (R / (R + h))²
For h = R, the exact result is g/4, while the linear formula gives g(1 − 2) = −g — physically meaningless. NEET has tested this in 2024 and 2025.
Variation with depth follows a different law. Assuming uniform density:
g_d = g (1 − d/R)
This IS genuinely linear — g decreases uniformly and reaches zero at Earth's centre. The common confusion is mixing up which formula is linear and which is inverse-square: altitude is inverse-square, depth is linear.
Why this matters for you: g-variation questions appear roughly every 2–3 years. They carry medium negative-marking risk because the linear-vs-inverse-square trap generates plausible-looking wrong options. If you can write down the correct formula within 5 seconds of reading the stem, the question is free marks.
Watch-out: problems sometimes give height as a multiple of R (h = R/2, h = 2R) precisely to punish the linear approximation. Always check whether h is comparable to R before choosing your formula.
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 on Earth's surface is related to the universal gravitational constant by which expression?
At what location does the acceleration due to gravity become zero, assuming Earth has uniform density?
The variation of g with depth below Earth's surface (uniform density) is:
A body weighs 720 N on Earth's surface. What is its weight at a height equal to half the radius of Earth (h = R/2) above the surface?
At what height above Earth's surface does the acceleration due to gravity reduce to 25% of its surface value? (Express answer in terms of Earth's radius R.)
A mine shaft reaches a depth of R/4 below Earth's surface (R = Earth's radius, uniform density assumed). The acceleration due to gravity at the bottom of the shaft is:
A body weighs W on Earth's surface. It is taken to a height h = R above the surface. Separately, the same body is taken to a depth d below the surface where it has the same weight as at height h. Find d in terms of R. (Assume uniform density.)
The ratio of g at a depth of R/2 to g at a height of R/2 above the surface is: (Assume uniform density.)
Pattern: Weight at altitude — direct application of g_h = g(R/(R+h))² (observed in NEET 2024 and 2025).
Given
A body weighs 800 N on the surface of Earth. Earth's radius R is given. Find the body's weight at a height h = R above the surface.
Required
Weight at height h = R above the surface.
Concept
Acceleration due to gravity decreases with altitude. Since h = R is NOT small compared to R, the exact inverse-square formula must be used. The linear approximation g(1 − 2h/R) is invalid here.
Formula
g_h = g × (R / (R + h))²
Substitution
g_h = g × (R / (R + R))² g_h = g × (R / 2R)² g_h = g × (1/2)²
Calculation
g_h = g × 1/4 = g/4 Weight at height R = 800 × (1/4) = 200 N. **Note on exact values:** The integers 800, 1, 2, and 4 are exact (counting/problem-defined values) and do not limit significant figures.
Final answer
**Weight at height h = R is 200 N** (one-quarter of surface weight).
Common trap
Using the linear approximation: g(1 − 2R/R) = g(1 − 2) = −g. This gives a negative, physically meaningless result. The linear formula is only valid when h ≪ R. For h = R, you MUST use the exact formula g(R/(R+h))².
Similar NEET-style question
A satellite orbits at height h = 3R above Earth's surface. What fraction of surface gravity does it experience? *Approach:* g_h = g(R/(R+3R))² = g(1/4)² = g/16. The satellite experiences 1/16 of surface gravity. ---
The acceleration produced by gravitational force on a body in free fall near Earth's surface: g = G M / R² ≈ 9.8 m/s², where M and R are Earth's mass and radius.
-- NCERT Class 11 Physics, Ch. 7, p. 5Minimum 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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