Newton's Law of Gravitation
F = Gm₁m₂/r² — inverse-square force between two masses.
Notes coming soon — open the simulation for the live walkthrough.
Complete revision notes and formulas for Gravitation (Class 11). Curated for JEE, NEET, AP Physics, SAT, and CUET. Tap any topic to open the live simulation and full PYQ set.
F = Gm₁m₂/r² — inverse-square force between two masses.
Notes coming soon — open the simulation for the live walkthrough.
g(r) ∝ r inside, 1/r² outside — single curve across both regions.
Notes coming soon — open the simulation for the live walkthrough.
V(r) = −GM/r — well shape with smooth transition at the surface.
Notes coming soon — open the simulation for the live walkthrough.
v_esc = √(2GM/R) — launch a rocket with various v₀ and see if it escapes.
Notes coming soon — open the simulation for the live walkthrough.
v_orb = √(GM/r) — satellite at altitude h with period and g(h).
Notes coming soon — open the simulation for the live walkthrough.
Elliptical orbit with Sun at focus — equal-area sweep demonstrated live.
Notes coming soon — open the simulation for the live walkthrough.
Launch satellites into orbit, adjust velocities, and observe Kepler's laws in action with stunning visuals.
Newton's Law of Gravitation: Every mass attracts every other mass with force F = Gm₁m₂/r².
The gravitational constant G = 6.674 × 10⁻¹¹ N·m²/kg².
Orbital velocity of a satellite: v₀ = √(GM/r) = √(gR²/r), where r is the orbital radius.
Escape velocity from Earth's surface: vₑ = √(2gR) ≈ 11.2 km/s. It is √2 times the orbital velocity at surface.
Kepler's Third Law: T² ∝ r³ — the square of the period is proportional to the cube of the orbital radius.
Geostationary orbit: T = 24 hours, r ≈ 42,164 km from Earth's center, above the equator.
Total energy of an orbiting satellite: E = −GMm/(2r) — it is negative (bound state).
At the surface: g = GM/R². As you go up: g decreases as GM/(R+h)². Inside Earth: g decreases linearly.
Attractive force between two masses.
Speed needed for circular orbit at radius r.
Minimum speed to escape gravitational pull.
Period-radius relation for orbits.
Potential energy (zero at infinity).
Total energy of satellite in orbit.
Escape velocity is independent of the mass of the escaping object and the direction of projection.
If a satellite's speed is increased beyond orbital velocity but below escape velocity, it enters an elliptical orbit.
At exactly escape velocity, the orbit becomes parabolic. Above it, hyperbolic.
Inside a uniform spherical shell, gravitational field is zero — Shell Theorem.
Weightlessness in orbit is not absence of gravity — it's free fall. Gravity provides centripetal force.
For JEE: relate v_orbital, v_escape, and energy — they're deeply interconnected.
Three masses; drag a probe and see net F as the vector sum from each.
Net gravitational force on a body is the vector sum of forces from each other mass.
Always attractive — each force points from the test mass toward each source.
For continuous distributions, sum becomes an integral.
Vector sum.
At symmetric points (e.g. center of equilateral triangle of equal masses), forces cancel.
Inside a uniform spherical shell, F = 0 (shell theorem).
g points always toward masses — single mass and binary system fields.
Field lines point in the direction of the gravitational field g — always toward masses (always attractive).
Density of lines is proportional to |g|. Lines start at infinity and end on masses.
Lines never cross — at each point g has a unique direction.
Negative sign = attractive.
Unlike electric fields, gravitational fields have no sources of repulsion (no negative mass).
For two equal masses, midpoint field is zero — saddle point.
Tune altitude until T = 24h — satellite locks above the same point on Earth.
A satellite in circular equatorial orbit with period T = 24 h appears stationary above one point on Earth.
Required altitude ≈ 35,786 km above Earth's surface (radius from center ≈ 42,164 km).
Used for telecommunications, weather imaging, broadcast TV.
From T = 2π√(r³/GM).
≈ 3.07 km/s for geostationary.
Must be in equatorial plane; otherwise it traces a figure-8 (geosynchronous but not stationary).
Three geostationary satellites cover almost the entire planet (excluding polar regions).
Gravitation on sciphylab (also known as SciPhy, SciPhy Lab, SciPhy Labs). Free physics revision for Class 11, JEE Mains, JEE Advanced, NEET UG, AP Physics 1/2/C, SAT Subject Physics, and CUET-UG.