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Chapter 1 · Class 11 Physics

Gravitation — Important Questions

34 questions With answers CBSE format

SUMMARY: This chapter covers the universal law of gravitation and its applications in understanding the motion of celestial bodies and phenomena related to gravity.
KEY TOPICS: Universal law of gravitation, gravitational constant, acceleration due to gravity, motion of planets, Kepler's laws, gravitational potential energy, escape velocity, satellites, weightlessness, variation of g with altitude and depth.

Q1 1 Mark

Newton's law of universal gravitation states that F is proportional to:

Am₁m₂
Bm₁m₂/r
Cm₁m₂/r²
Dm₁/m₂
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Correct answer: Option 3 — m₁m₂/r²
Q2 1 Mark

The acceleration due to gravity at the surface of Earth is approximately:

A4.9 m/s²
B9.8 m/s²
C19.6 m/s²
D98 m/s²
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Correct answer: Option 2 — 9.8 m/s²
Q3 1 Mark

The gravitational force between two masses is independent of:

AThe product of the masses
BThe distance between them
CThe medium between them
DAll of these
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Correct answer: Option 3 — The medium between them
Q4 1 Mark

The escape velocity from the surface of the Earth is approximately:

A7.9 km/s
B11.2 km/s
C15.6 km/s
D30 km/s
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Correct answer: Option 2 — 11.2 km/s
Q5 1 Mark

A satellite in a stable orbit around the Earth has:

AConstant speed
BConstant velocity
CZero acceleration
DZero gravitational force on it
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Correct answer: Option 1 — Constant speed
Q6 3 Marks

State Newton's law of universal gravitation.

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Every particle in the universe attracts every other particle with a force directly proportional to the product of their masses and inversely proportional to the square of the distance between their centres. F = G m₁m₂/r² where G = 6.67 × 10⁻¹¹ N·m²/kg² is the universal gravitational constant. The force acts along the line joining the centres.
Q7 3 Marks

Define gravitational field intensity and write its formula.

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Gravitational field intensity at a point is the gravitational force experienced per unit mass placed at that point. E = F/m = GM/r² (for a point mass M at distance r). It is a vector quantity directed toward the source mass. SI unit: N/kg or m/s² (same as acceleration due to gravity).
Q8 3 Marks

Derive the expression for escape velocity from the surface of a planet.

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Escape velocity v_e: minimum velocity to escape gravitational pull (reach infinity with zero KE). Total energy at surface = total energy at infinity (= 0 for marginal escape). (1/2)mv_e² − GMm/R = 0. So v_e = √(2GM/R) = √(2gR) (using g = GM/R²). For Earth: v_e = √(2 × 9.8 × 6.4 × 10⁶) ≈ 11.2 km/s.
Q9 3 Marks

State Kepler's three laws of planetary motion.

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K1 (Law of orbits): each planet moves in an elliptical orbit with the sun at one focus. K2 (Law of areas): the line joining a planet to the sun sweeps equal areas in equal time intervals — implies angular momentum conservation. K3 (Law of periods): T² ∝ a³ where T is orbital period and a is semi-major axis — i.e. T²/a³ is the same for all planets around the same central body.
Q10 3 Marks

Calculate the gravitational force between two 5 kg masses placed 0.5 m apart. (G = 6.67 × 10⁻¹¹ N·m²/kg²)

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F = G m₁m₂/r² = (6.67 × 10⁻¹¹)(5)(5)/(0.5)² = (6.67 × 10⁻¹¹)(25)/0.25 = 6.67 × 10⁻⁹ N. Extremely small — gravitational forces between everyday objects are negligible compared to other forces.
Q11 6 Marks

Derive the expression for the orbital velocity and time period of a satellite revolving close to the Earth's surface.

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For a satellite in orbit at radius r the gravitational force provides the centripetal force: GMm/r² = mv²/r ⇒ v = √(GM/r). For an orbit close to Earth's surface r ≈ R: v_orbit = √(GM/R) = √(gR) (since g = GM/R²) ≈ √(9.8 × 6.4 × 10⁶) ≈ 7.9 km/s. Time period: T = 2πr/v = 2π√(R/g) ≈ 84 minutes — the famous low Earth orbit period.
Q12 6 Marks

State and prove the law of conservation of mechanical energy for a body falling under gravity from height h.

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At height h: PE = mgh (taking ground as reference); KE = 0. While falling distance s velocity v = √(2gs) so KE at depth s below initial = (1/2)mv² = mgs; PE = mg(h − s). Total = mgs + mg(h − s) = mgh ✓. Conservation holds throughout the fall — only the partition between KE and PE changes. Total = mgh = constant.
Q13 6 Marks

Discuss the variation of acceleration due to gravity with altitude and depth.

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At Earth's surface: g₀ = GM/R². With altitude h above surface: g_h = GM/(R + h)² = g₀ R²/(R + h)². For small h ≪ R: g_h ≈ g₀ (1 − 2h/R) — decreases with altitude. With depth d below surface (assuming uniform density): g_d = g₀ (1 − d/R) — also decreases linearly, reaching zero at the centre. So g is maximum at the surface; both moving up AND moving down reduces it.
Q14 6 Marks

A satellite of mass 1000 kg is to be placed in orbit at an altitude of 800 km above the Earth's surface. Calculate (i) orbital velocity, (ii) period of revolution. (R = 6.4 × 10⁶ m, g_surface = 9.8 m/s²)

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Orbital radius r = R + h = 6.4 × 10⁶ + 0.8 × 10⁶ = 7.2 × 10⁶ m. Orbital velocity: v = √(gR²/r) = √(9.8 × (6.4 × 10⁶)²/(7.2 × 10⁶)) = √(9.8 × 6.4² × 10¹² / 7.2 × 10⁶) = √(5.57 × 10⁷) ≈ 7464 m/s ≈ 7.46 km/s. Period: T = 2πr/v = 2π × 7.2 × 10⁶ / 7464 ≈ 6062 s ≈ 101 minutes.
Q15 6 Marks

Define gravitational potential and gravitational potential energy. Derive expressions for both for a point mass M.

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Gravitational potential V at a point = work done per unit mass in bringing a unit test mass from infinity to that point. V = −GM/r (taking V = 0 at infinity; sign is negative because gravity is attractive). Gravitational potential energy U of a mass m at distance r from M is U = −GMm/r. Both quantities are negative because work must be done ON the system to separate the masses. Difference (V_b − V_a) is the work done per unit mass against gravity moving from a to b.
Q16 6 Marks

Differentiate between gravitational potential and gravitational potential energy in tabular form.

Q17 1 Mark

Assertion (A): All bodies near Earth's surface fall with the same acceleration g.

Reason (R): Newton's second law gives a = F/m = (GMm/R²)/m = GM/R² = g — independent of m.

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q18 1 Mark

Assertion (A): Kepler's second law (equal areas in equal times) is a consequence of conservation of angular momentum.

Reason (R): The torque of gravity about the central body (Sun) is zero since the force is along r — so angular momentum is conserved.

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q19 1 Mark

Assertion (A): Escape velocity is independent of the mass of the projectile.

Reason (R): v_e = √(2GM/R) where M is the mass of the planet — the projectile mass cancels out.

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q20 1 Mark

Assertion (A): An astronaut in a satellite feels weightless.

Reason (R): The astronaut and the satellite are both in free fall — there is no normal force from the satellite floor on the astronaut.

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q21 1 Mark

Assertion (A): g decreases below the surface of the Earth.

Reason (R): Only the mass within the spherical shell of radius r contributes to gravity at depth d — mass outside the shell exerts zero net gravity.

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q22 1 Mark

Statement 1: The gravitational force is always attractive.

Statement 2: F = G m₁m₂/r² with G > 0.

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Correct answer: Option 1 — Both statements are true.
Q23 1 Mark

Statement 1: Acceleration due to gravity is approximately 9.8 m/s² near Earth's surface.

Statement 2: g varies slightly with latitude and altitude.

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Correct answer: Option 1 — Both statements are true.
Q24 1 Mark

Statement 1: Kepler's third law: T² ∝ a³.

Statement 2: The constant of proportionality equals 4π²/(GM) where M is the mass of the central body.

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Correct answer: Option 1 — Both statements are true.
Q25 1 Mark

Statement 1: A geostationary satellite has a period of 24 hours.

Statement 2: A geostationary satellite is at altitude ≈ 36000 km above the equator.

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Correct answer: Option 1 — Both statements are true.
Q26 1 Mark

Statement 1: Gravitational potential is negative for an attractive system.

Statement 2: Gravitational potential at infinity is taken as zero by convention.

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Correct answer: Option 1 — Both statements are true.
Q27 3 Marks
Two students of mass 60 kg each stand 1 m apart. They wonder whether the gravitational force between them is detectable. They calculate this force using G = 6.67 × 10⁻¹¹ N·m²/kg² and compare it with their weights.
  1. The gravitational force between them equals:
    A2.4 × 10⁻⁷ N
    B2.4 × 10⁻⁵ N
    C2.4 × 10⁻³ N
    D2.4 × 10⁻¹ N
  2. Compared with their weights (≈ 600 N each) this force is:
    AComparable
    BNegligible
    CGreater
    DCannot decide
  3. Why is gravity the weakest fundamental force yet dominant in cosmology?
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1. Option 1 — 2.4 × 10⁻⁷ N
2. Option 2 — Negligible
3. F = G m₁m₂/r² = (6.67 × 10⁻¹¹)(60)(60)/(1²) = 2.4 × 10⁻⁷ N. Their weights are 60 × 9.8 ≈ 588 N. Ratio: 2.4 × 10⁻⁷ / 588 ≈ 4 × 10⁻¹⁰. The gravitational force between two people is about 10⁻⁹ times their weight — utterly undetectable in everyday life. Gravity is the weakest of the four fundamental forces — but its long-range universal nature makes it dominant on astronomical scales.
Q28 3 Marks
A spacecraft is to be launched from the surface of the Moon. The Moon has mass 7.35 × 10²² kg and radius 1.74 × 10⁶ m. The mission engineer wants to compute the escape velocity from the Moon and compare it with that from Earth (≈ 11.2 km/s).
  1. The escape velocity from the Moon equals:
    A1.7 km/s
    B2.4 km/s
    C5.6 km/s
    D11.2 km/s
  2. Compared with Earth the escape velocity from the Moon is:
    ASame
    BLower
    CHigher
    DCannot decide
  3. Why is the escape velocity smaller on the Moon than on Earth?
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1. Option 2 — 2.4 km/s
2. Option 2 — Lower
3. v_e = √(2GM/R) = √((2)(6.67 × 10⁻¹¹)(7.35 × 10²²)/(1.74 × 10⁶)) = √(5.63 × 10⁶) ≈ 2374 m/s ≈ 2.4 km/s. Compared to Earth's 11.2 km/s the Moon's escape velocity is ~5× lower because the Moon is less massive and larger (per unit mass). This is why the Apollo lander could leave the Moon with just a small ascent stage but a giant Saturn V was needed to leave Earth.
Q29 3 Marks
A communications satellite is to be placed in a geostationary orbit. This means it must have a 24-hour period (matching Earth's rotation) so it stays above the same point on the equator. The engineer needs to find the altitude of the orbit and the orbital speed. Earth's mass = 5.98 × 10²⁴ kg radius = 6.4 × 10⁶ m G = 6.67 × 10⁻¹¹.
  1. The orbital radius of a geostationary satellite is approximately:
    A4.2 × 10⁷ m
    B3.0 × 10⁷ m
    C1.0 × 10⁸ m
    D6.4 × 10⁷ m
  2. The orbital speed of a geostationary satellite is approximately:
    A1.5 km/s
    B3.1 km/s
    C5.0 km/s
    D7.9 km/s
  3. Why is the geostationary altitude unique (≈ 36000 km)?
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1. Option 1 — 4.2 × 10⁷ m
2. Option 2 — 3.1 km/s
3. From T = 2π√(r³/(GM)) with T = 86400 s: r³ = T²GM/(4π²) = (86400² × 6.67e-11 × 5.98e24)/(4π²) ≈ 7.54 × 10²² m³ ⇒ r ≈ 4.22 × 10⁷ m. Altitude = r − R = 4.22e7 − 6.4e6 ≈ 35800 km. Orbital speed v = 2πr/T = 2π × 4.22e7 / 86400 ≈ 3070 m/s ≈ 3.1 km/s. Geostationary satellites are used for direct broadcast TV weather imaging and communications.
Q30 3 Marks

Study Kepler's three laws of planetary motion:

LawStatement
1stEach planet moves in an elliptical orbit with the sun at one focus.
2ndThe line joining a planet to the sun sweeps equal areas in equal times.
3rdT² is proportional to a³ (T = period, a = semi-major axis).
  1. Which Kepler's law gives T² ∝ a³?
    A1st
    B2nd
    C3rd
    DAll three
  2. Kepler's 2nd law (equal areas) is equivalent to:
    AConservation of energy
    BConservation of momentum
    CConservation of angular momentum
    DConservation of mass
  3. Use Kepler's 3rd law to estimate the orbital period of Mars (a ≈ 1.52 AU).
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1. Option 3 — 3rd
2. Option 3 — Conservation of angular momentum
3. Kepler's three laws (early 1600s) describe planetary motion empirically; Newton later derived them from his law of universal gravitation. 1st law: orbits are ellipses (not perfect circles). 2nd law: a planet moves faster when closer to the sun (perihelion) and slower at apohelion — equivalent to angular momentum conservation. 3rd law: planets farther from the sun have longer years; T² ∝ a³ holds for all bodies orbiting the same primary.
Q31 3 Marks

Study the gravitational acceleration g at various locations:

Locationg (m/s²)
Earth surface9.8
Top of Mt. Everest9.78
Geostationary orbit (36000 km)0.22
Moon surface1.62
Mars surface3.71
Sun's surface274
Centre of Earth0
  1. The maximum value of g (other than centre) is at:
    AEarth surface
    BMoon surface
    CSun's surface
    DMars surface
  2. At the centre of Earth g is:
    AMaximum
    BZero
    CMinimum
    DAbout 9.8
  3. Why does g decrease both as we go up from the surface AND down into the Earth?
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1. Option 3 — Sun's surface
2. Option 2 — Zero
3. Acceleration due to gravity g varies with location. At surface: g = GM/R². On more massive bodies (Sun) g is much larger. With altitude: g decreases as 1/r². At centre: g = 0 (mass shell theorem — only mass within smaller radius contributes; mass closer to centre is zero). At satellite altitudes g is reduced; this is why astronauts feel weightless (they and the satellite are in free fall together).
Q32 6 Marks

Compute (i) the orbital velocity of a satellite at altitude 400 km above Earth, (ii) its time period. (Earth's mass M = 6 × 10²⁴ kg, R = 6.4 × 10⁶ m, G = 6.67 × 10⁻¹¹ N·m²/kg²)

QuantityValue
Altitude h400 km
Earth radius R6.4 × 10⁶ m
Earth mass M6 × 10²⁴ kg
G6.67 × 10⁻¹¹ N·m²/kg²
Q33 6 Marks

Compute the escape velocity from (i) Earth, (ii) Moon, (iii) Jupiter using v_e = √(2gR).

Bodyg (m/s²)R (m)
Earth9.86.4 × 10⁶
Moon1.61.74 × 10⁶
Jupiter24.87.0 × 10⁷
Q34 3 Marks

Study Kepler's elliptical orbit diagram and answer:

Gravitation figure
  1. According to Kepler's first law the Sun is located:
    AAt the centre of the ellipse
    BAt one focus
    CAt both foci
    DOutside the ellipse
  2. Kepler's second law (equal areas in equal times) is a consequence of:
    AConservation of energy
    BConservation of momentum
    CConservation of angular momentum
    DConservation of mass
  3. State Kepler's three laws and explain the physics behind the second law.
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1. Option 2 — At one focus
2. Option 3 — Conservation of angular momentum
3. Kepler's three laws: (1) Each planet moves in an elliptical orbit with the Sun at one focus. (2) The line joining a planet to the Sun sweeps equal areas in equal times — so a planet moves faster at perihelion (closer) and slower at aphelion (farther). This is equivalent to conservation of angular momentum L = mvr (since the gravitational force is along r, its torque about the Sun is zero, so L is conserved). (3) T² ∝ a³ where T is orbital period and a is the semi-major axis.

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