Gravitation — Exam Practice
Practice questions in CBSE, NEET, and JEE Main style covering Kepler’s laws, orbital velocity, escape speed, and satellite motion.
1CBSE Board Exam Style
At the exact centre, the mass of Earth surrounding that point pulls equally in all directions, cancelling out completely by symmetry — leaving a net gravitational field of zero.
Gravity supplies the centripetal force: GMm/R² = mv²/R.
Solving for v: v² = GM/R → v = √(GM/R). Since g = GM/R², this can also be written as v = √(gR).
(a) Escape velocity is the minimum launch speed for which total mechanical energy is exactly zero at infinity: ½mve² − GMm/R = 0 → ve = √(2GM/R).
(b) Since ve ∝ √(M/R), and R is unchanged while M doubles: ve,planet = ve,Earth × √2 = 11.2 × 1.414 ≈ 15.8 km/s.
2NEET Style (Single-Correct MCQ)
g decreases with height (farther from centre), decreases with depth (less enclosed mass), and varies slightly with latitude (Earth’s equatorial bulge and rotation effects).
A geostationary satellite’s period exactly matches Earth’s rotation period, so it stays fixed above one point on the equator.
U = −GMm/r — negative at every finite separation, reflecting that gravity is attractive and work must be done to pull the masses apart to infinity.
The square of the orbital period is proportional to the cube of the semi-major axis — later derived directly from Newton’s law of gravitation.
3JEE Main Style
Orbital radius r = R + R = 2R. v = √(GM/r) = √(GM/2R) = v₀/√2, since v₀ = √(GM/R).
The new orbital velocity is v₀/√2 ≈ 0.707v₀.
Gravity is only slightly weaker at typical orbital altitudes — the sensation of weightlessness comes from falling around Earth at the same rate as the spacecraft, not from an absence of gravity.
r = R + h = 6400 + 2000 = 8400 km = 8.4×10⁶ m. GM = gR² = 9.8×(6.4×10⁶)² ≈ 4.01×10¹⁴.
T = 2π√(r³/GM) = 2π√[(8.4×10⁶)³ / 4.01×10¹⁴] ≈ 2π×1216 ≈ 7640 s ≈ 127 minutes.

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