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PhysicsHigh Weightage β˜…β˜…β˜…β˜…Class 11

Gravitation

Kepler's laws, universal gravitation, escape velocity, and orbital mechanics β€” tied together by one inverse-square law. Expect 3–4 EAPCET questions.

3–4Questions in EAPCET
~3%Paper Weightage
8Core Formulas
4Mistake Traps

Concept Core

From Newton's law to satellites β€” the universe in one chapter.

Newton's Law of Universal Gravitation

Every mass attracts every other mass with force:

F = GMm/rΒ²   (G = 6.674Γ—10⁻¹¹ NΒ·mΒ²/kgΒ²)

Force is along the line joining the two masses. It is attractive, conservative, and central. It obeys Newton's 3rd law β€” both masses experience equal, opposite forces.

Acceleration Due to Gravity

At Earth's surface: g = GM/RΒ² β‰ˆ 9.8 m/sΒ²

Variation with height h above surface:

g_h = g(1 βˆ’ 2h/R)   (h << R)

Variation with depth d below surface:

g_d = g(1 βˆ’ d/R)

At centre: g = 0. g decreases both above and below surface.

Gravitational Potential Energy

PE of mass m at distance r from Earth's centre:

U = βˆ’GMm/r   (negative, zero at infinity)

At surface: U = βˆ’GMm/R = βˆ’mgR

The negative sign means work must be done against gravity to move mass away from Earth.

Escape Velocity

Minimum speed to escape Earth's gravity entirely (reach r = ∞ with zero KE):

v_e = √(2GM/R) = √(2gR) β‰ˆ 11.2 km/s

Independent of mass of the escaping object. No angle dependence β€” same in any direction.

Orbital Velocity & Satellites

For circular orbit at radius r from Earth's centre:

v_o = √(GM/r) = √(gR²/r)

At surface (r=R): v_o = √(gR) β‰ˆ 7.9 km/s. Note: v_e = √2 Γ— v_o

Time period: T = 2Ο€r/v_o = 2Ο€βˆš(rΒ³/GM)

Kepler's Three Laws

1st Law (Ellipse): Planets move in ellipses with the Sun at one focus.

2nd Law (Equal Areas): Line from Sun to planet sweeps equal areas in equal times. β†’ Planet moves fastest at perihelion (closest), slowest at aphelion (farthest).

3rd Law (TΒ² ∝ rΒ³): TΒ² = 4π²rΒ³/GM. The ratio TΒ²/rΒ³ is constant for all planets around the same star.

Formula Vault

Every gravitation formula for EAPCET.

Newton's Gravity
F = GMm/rΒ²
G = 6.674Γ—10⁻¹¹ NΒ·mΒ²/kgΒ²
g at Surface
g = GM/RΒ²
g β‰ˆ 9.8 m/sΒ² at Earth's surface
g at Height h
g_h = g(1βˆ’2h/R)
Valid for h << R
g at Depth d
g_d = g(1βˆ’d/R)
g=0 at Earth's centre
Gravitational PE
U = βˆ’GMm/r
Negative; zero at infinity
Escape Velocity
v_e = √(2gR) = √(2GM/R)
β‰ˆ11.2 km/s from Earth
Orbital Velocity
v_o = √(GM/r) = √(gR²/r)
v_e = √2 Γ— v_o at surface
Orbital Period
T = 2Ο€βˆš(rΒ³/GM)
Kepler's 3rd: T²∝r³
Kepler's 3rd Law
TΒ²/rΒ³ = 4π²/GM = const
Same for all planets of a star
Binding Energy
BE = GMm/2r
Energy to remove satellite from orbit

Worked Examples

5 problems β€” gravity variation, escape velocity, satellites, and Kepler.

EasyFind g at height h = R above Earth's surfaceβ–Ύ
Find the value of g at height h = R (one Earth radius above surface). g at surface = 9.8 m/sΒ².
1
At height h, exact formula: g_h = gΓ—RΒ²/(R+h)Β²
2
h = R: g_h = gΓ—RΒ²/(2R)Β² = g/4 = 9.8/4 = 2.45 m/sΒ²
βœ“  g at height R = g/4 = 2.45 m/sΒ²
EasyEscape velocity of a planet with half Earth's radius and same massβ–Ύ
A planet has mass = M (Earth's mass) and radius = R/2. Find its escape velocity.
1
v_e = √(2GM/R_planet) = √(2GM/(R/2)) = √(4GM/R) = 2√(GM/R) = 2 Γ— 11.2 = 22.4 km/s
βœ“  v_e = 2 Γ— Earth's escape velocity = 22.4 km/s
MediumFind orbital velocity and time period of satellite at height R above surfaceβ–Ύ
Find orbital speed and period of a satellite orbiting at height h = R above Earth's surface.
1
Orbital radius r = R + R = 2R
2
v_o = √(gRΒ²/r) = √(gRΒ²/2R) = √(gR/2) = v_surface/√2 = 7.9/√2 β‰ˆ 5.6 km/s
3
T = 2Ο€r/v = 2Ο€(2R)/v_o. Using T = 2Ο€βˆš(rΒ³/GM): T = 2Ο€βˆš(8RΒ³/GM) = 2√2 Γ— T_surface
βœ“  v_o = 5.6 km/s, T = 2√2 Γ— 90 min β‰ˆ 4 hours
EAPCET LevelPlanet A has T = 8 years, planet B has T = 1 year. Find ratio of their orbital radii.β–Ύ
Two planets orbit the same star. Planet A has period T_A = 8 years, planet B has T_B = 1 year. Find r_A/r_B.
1
Kepler's 3rd Law: TΒ² ∝ rΒ³ β†’ (T_A/T_B)Β² = (r_A/r_B)Β³
2
(8/1)Β² = (r_A/r_B)Β³ β†’ 64 = (r_A/r_B)Β³
3
r_A/r_B = 64^(1/3) = 4
βœ“  r_A/r_B = 4 (Planet A is 4Γ— farther from the star)
Trap QuestionEscape velocity depends on the angle of launch β€” True or False?β–Ύ
An object is launched vertically at escape velocity. Would it also escape if launched at 45°? ⚠️ Common misconception.
1
The trap: Students think angle matters because the vertical component must overcome gravity.
2
Escape velocity is derived from energy conservation: Β½mv_eΒ² = GMm/R. Energy is a scalar β€” no direction.
3
The same minimum KE = GMm/R is needed regardless of launch direction.
4
At 45°, the object escapes along a parabolic path, but the minimum speed required is still v_e = √(2gR).
βœ“  False β€” escape velocity is the same in any direction (energy, not force condition)

Mistake DNA

4 gravitation errors from EAPCET distractor analysis.

πŸ“
Using g_h = g(1βˆ’2h/R) for Large Heights
This approximation is valid only when h β‰ͺ R. For h = R or more, use the exact formula g_h = gΒ·RΒ²/(R+h)Β².
❌ Wrong
g at h=R: g(1βˆ’2R/R) = g(βˆ’1) = βˆ’g βœ— (gives negative g!)
βœ“ Correct
g_h = gRΒ²/(R+h)Β² = gRΒ²/4RΒ² = g/4 βœ“ Always use exact for large h
The approximation (1βˆ’2h/R) is a first-order Taylor expansion valid for h/R β‰ͺ 1. For h = R, the exact formula gives g/4, not βˆ’g.
πŸš€
Confusing Escape Velocity and Orbital Velocity
v_escape = √2 Γ— v_orbital at the same radius. They are related but different.
❌ Wrong
v_e β‰ˆ 7.9 km/s (orbital) βœ— v_o β‰ˆ 11.2 km/s (escape) βœ— (swapped!)
βœ“ Correct
v_o = √(GM/R) β‰ˆ 7.9 km/s βœ“ v_e = √(2GM/R) β‰ˆ 11.2 km/s βœ“ v_e = √2 Γ— v_o
Orbital velocity keeps a satellite in circular orbit. Escape velocity breaks free from gravity entirely. v_escape/v_orbital = √2 β‰ˆ 1.41.
⬆️
Thinking g Increases as You Go Deeper Into Earth
g decreases linearly from surface to centre as depth increases β€” not increases.
❌ Wrong
Deeper = more gravity because more mass below βœ—
βœ“ Correct
g_d = g(1βˆ’d/R) βœ“ g decreases to zero at Earth's centre βœ“
Going deeper, the outer shell above contributes no net gravity (shell theorem). Only the mass of the sphere below the depth matters, and that decreases.
πŸͺ
Applying Kepler's 3rd Law to Different Stars
TΒ²/rΒ³ = constant holds only for planets orbiting the SAME central body. Different stars have different constants.
❌ Wrong
Planet of star A and planet of star B: TΒ²/rΒ³ same for both βœ—
βœ“ Correct
TΒ²/rΒ³ = 4π²/GM_star βœ“ Different stars β†’ different constants βœ“
The constant in Kepler's 3rd law is 4π²/GM where M is the mass of the central body. Only compare planets of the same star.

Chapter Intelligence

Gravitation connects directly to circular motion, energy, and SHM.

EAPCET Weightage (2019–2024)
Escape/orbital velocity
~8
g variation with height/depth
~6
Kepler's laws
~5
Gravitational PE & binding energy
~4
Satellites & geostationary orbit
~3
High-Yield PYQ Patterns
g at height nR above surfaceEscape velocity from another planetKepler's 3rd: ratio of r from TOrbital velocity at given heightg at depth dv_e = √2 Γ— v_orbital
Exam Strategy
  • For g variation: use exact formula g_h = gRΒ²/(R+h)Β² for height questions. Use approximate g(1βˆ’2h/R) only when explicitly told h β‰ͺ R.
  • Escape velocity questions often change planet mass or radius β€” use v_e = √(2GM/R) = √(2gR) and substitute what changed.
  • Kepler's 3rd Law: (T₁/Tβ‚‚)Β² = (r₁/rβ‚‚)Β³. Take the ratio β€” no need to know G or M of the star.
  • Satellites: orbital KE = GMm/2r, PE = βˆ’GMm/r, Total E = βˆ’GMm/2r. Total energy is negative and half the magnitude of PE.
  • Geostationary satellite: T = 24 hours (same as Earth's rotation), r β‰ˆ 42,000 km, v_o β‰ˆ 3.07 km/s. Fixed point in sky.
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