U = -G M m / r (taking U → 0 as r → ∞). Negative sign reflects that gravity is attractive — work must be done against it to separate masses. For two-body system at separation r.
-- NCERT Class 11 Physics, Ch. 7, p. 8Grav Potential
Lesson
Gravitational potential is where sign errors silently cost you marks. The concept itself is straightforward, but NEET questions exploit the negative sign and the distinction between potential (a scalar field property) and potential energy (a system property).
Gravitational potential at a point is the work done per unit mass by an external agent in bringing a test mass from infinity to that point, against the gravitational field. For a point mass M at distance r (NCERT Class 11 Physics Chapter 7, page 8):
V = −GM/r
The negative sign is not a convention you can drop — it encodes that gravity is attractive. At infinity, V = 0 (the reference). As you approach the mass, V becomes more negative: the field does positive work on an inward-moving object, so an external agent does negative work.
Potential vs. potential energy. Gravitational potential V is a property of the field at a point (unit: J/kg). Gravitational potential energy U = mV = −GMm/r is a property of the two-body system (unit: J). Confusing the two — especially dropping the test mass m or misapplying the sign — is a common source of wrong answers.
Superposition. Gravitational potential is a scalar. For multiple masses, add potentials algebraically: V_total = V₁ + V₂ + … No vector resolution needed. This makes potential calculations simpler than force calculations in multi-body problems.
Key watch-out: When a question says "gravitational potential at the surface of Earth," the answer is V = −GM/R (negative). If you write +GM/R, you have the wrong sign and will pick a distractor. The magnitude alone is not the potential.
Practice MCQs
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
The SI unit of gravitational potential is:
The gravitational potential at a point infinitely far from an isolated mass M is:
Gravitational potential is a scalar quantity. When computing the net gravitational potential at a point due to multiple masses, you:
The gravitational potential at the surface of Earth is V. What is the gravitational potential energy of a body of mass m placed on the surface?
Two point masses, each of mass M, are placed a distance 2d apart. The gravitational potential at the midpoint of the line joining them is:
A particle is moved from the surface of a planet (radius R, mass M) to a height R above the surface. The change in gravitational potential is:
At the midpoint between two equal point masses, the gravitational field is zero but the gravitational potential is not zero. This is because:
A uniform sphere of mass M and radius R has gravitational potential V₁ at its surface and V₂ at a distance 3R from its centre. The ratio V₁/V₂ is:
Quick recall before you leave
Worked Example
- 1
Given
- Planet mass: M, radius: R (both exact problem-defined symbols) - Body mass: m - Initial position: surface (r₁ = R from centre) - Final position: height 2R above surface (r₂ = R + 2R = 3R from centre)
- 2
Required
Work done by external agent, W_ext
- 3
Concept
Work done by an external agent against gravity equals the change in gravitational potential energy of the system: W_ext = ΔU = U_final − U_initial. This uses the gravitational PE formula U = −GMm/r (NCERT Class 11 Physics Chapter 7, page 8).
- 4
Formula
U = −GMm/r W_ext = U_final − U_initial = (−GMm/r₂) − (−GMm/r₁)
- 5
Substitution
W_ext = (−GMm/(3R)) − (−GMm/R)
- 6
Calculation
W_ext = −GMm/(3R) + GMm/R W_ext = GMm/R × (−1/3 + 1) W_ext = GMm/R × (2/3) W_ext = 2GMm/(3R) Note: M, m, R are exact problem-defined quantities; the integers 2 and 3 are exact counting numbers. Neither constrains significant figures.
- 7
Final answer
W_ext = 2GMm/(3R) The work is positive, confirming that the external agent must do work against gravity to move the body outward.
- 8
Common trap
A common confusion is computing only the change in potential (ΔV) and forgetting to multiply by the body's mass m. ΔV = GM/(3R) − (−GM/R) would give a J/kg quantity, not the J required. Always use ΔU = mΔV for the actual work/energy. Another error: using the height (2R) as the final distance from the centre instead of the total distance (R + 2R = 3R). The formula U = −GMm/r requires the distance from the planet's centre, not from the surface.
- 9
Similar NEET-style question
A satellite of mass m is to be placed in orbit at height R above a planet of mass M, radius R. What minimum energy must be supplied to move it from the surface to that height? (Ignore orbital KE — only consider the change in gravitational PE.) ---
Before solving, remember these
Formulas
8 formulas — click to collapse
Escape velocity from a body's surface
Minimum 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 |
Valid when
- Launched from surface
- No air drag
- Body treated as point/sphere
Gravitational potential energy (point masses)
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 |
Valid when
- Reference U=0 at r=infinity
- Point or spherical masses
g variation with altitude
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 |
Valid when
- Static observer at altitude
- Earth treated as uniform sphere
g variation with depth
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 |
Valid when
- Earth treated as uniform density sphere
Kepler's third law
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 |
Valid when
- Two-body system with central mass M >> orbiting mass
- Bound orbit
Orbital velocity for circular orbit
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 |
Valid when
- Circular orbit
- M >> orbiting mass
Satellite total mechanical energy
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 |
Valid when
- Circular orbit
- Bound (E < 0)
Newton's law of gravitation
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 |
Valid when
- Point masses or spherically symmetric distributions
- r > sum of body radii (else use shell theorem)
Exam Traps & Common Mistakes
These are the exact patterns that cause wrong answers in NEET. Each trap includes when it triggers and how to avoid it.
4 items — click to collapse
Category: Similar Terms
Student treats g(h) as linear in h. Actual: g(R/(R+h))² (inverse-square).
When it triggers
Question asks for g at significant altitude (e.g. R/2 above surface).
How to avoid
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).
When it triggers
Question gives change in semi-major axis and asks for new period.
How to avoid
T² ∝ a³, so T ∝ a^(3/2). Doubling a multiplies T by 2^(3/2) ≈ 2.83.
Root cause: formula misuse
Correction
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
Correction
T² ∝ a³, so T ∝ a^(3/2). Doubling a multiplies T by 2^(3/2) ≈ 2.83. Quadrupling a → 8× T.
Past Year Questions
8 questions from NEET 2021, 2022, 2023, 2024, 2025. Answers verified against NTA official keys. — click to collapse
How NEET usually asks this
4 recurring patterns from past papers — click to collapse
Compare escape velocities for planets with different M, R. v_e ∝ sqrt(M/R). Common shape: 'planet has 4× radius and 2× density of Earth — find v_e'.
Common distractors
forgets density not mass
Confuses planet mass with density given radius scaling
Body weighs W on surface; find weight at height h above surface. Use g_h = g(R/(R+h))^2.
Common distractors
uses linear decrease with h
Treats g as linear in h instead of inverse-square
Given period T and semi-major axis a of one planet, find for another with different a. T^2 ∝ a^3.
Common distractors
uses linear relation
Treats T proportional to a not a^(3/2)
Energy required to launch satellite to altitude. Compute change in total mechanical energy.
Common distractors
forgets orbital KE component
Computes only PE change, ignoring orbital KE
Sources
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