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6📖 Chapter Overview
Overview
Gravitation explains the attractive force between any two masses in the universe. Newton’s universal law gives this force as proportional to the product of masses and inversely proportional to the square of separation. This chapter connects falling bodies, planetary motion, satellites, tides, weightlessness and escape from planets. Kepler’s laws describe planetary orbits and are explained by Newton’s law. Acceleration due to gravity, g, changes with altitude, depth and Earth’s rotation. Gravitational potential and potential energy help solve energy-based problems, while escape velocity and orbital velocity explain rockets and satellites. For NEET, this chapter is highly scoring because formulas are direct and concepts are repeatedly tested in numerical and assertion-type questions.
- 1Gravitational force obeys inverse square law and superposition principle.
- 2The value of G is universal, while g depends on planet, location and height.
- 3Gravitational potential energy is negative when zero is taken at infinity.
- 4Orbital velocity near Earth is v_o = √(GM/R) and escape velocity is √2 times orbital velocity.
- 5Satellites are weightless because they and their occupants are in continuous free fall.
- 6Geostationary satellites have period 24 hours and appear fixed over the equator.
Gravitation Flow
Remember F-G-E-S: Force law, g variation, Energy-potential, Satellites.
Escape vs Orbit
Escape speed is √2 times close-orbit speed: escape needs extra energy to reach infinity.
Daily Life Example
A falling apple, Moon’s revolution around Earth, artificial satellites and ocean tides all involve gravitational attraction.
Quick NEET Check
If distance between two masses is doubled, gravitational force becomes one-fourth.
Confusing G and g
G is universal constant; g is local acceleration due to gravity and changes with planet and location.
Forgetting Negative Potential Energy
With zero at infinity, gravitational potential and potential energy near a mass are negative.
Thinking Satellite Weightlessness Means No Gravity
Gravity provides centripetal acceleration in orbit; weightlessness is due to continuous free fall.
Attractive gravitational force between two point masses separated by distance r.
Variables
F=Gravitational force
G=Universal gravitational constant
m1, m2=Interacting masses
r=Distance between centres of masses
Acceleration due to gravity at the surface of a planet of mass M and radius R.
Variables
g=Acceleration due to gravity
M=Mass of planet
R=Radius of planet
🌍 Universal Law of Gravitation
Overview
Newton’s universal law of gravitation states that 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 them. The force acts along the line joining the two masses and is always attractive. The proportionality constant G is called the universal gravitational constant and has the same value everywhere in the universe. Gravitation is a long-range central force and obeys the inverse square law. When many masses are present, the net gravitational force is found by vector addition using the superposition principle. This topic is a frequent source of NEET ratio-based questions.
- 1The law applies accurately to point masses and spherically symmetric bodies treated as masses concentrated at centres.
- 2Gravitational force between ordinary objects is weak because G is very small.
- 3The force on m1 due to m2 and force on m2 due to m1 are equal and opposite.
- 4Gravitational force does not depend on the medium between masses.
- 5Superposition principle means each mass exerts force independently.
- 6The inverse square nature is central to planetary and satellite motion.
Universal Law
Masses multiply, distance squares divide: F grows with masses and falls with r².
Force Nature
Gravity never pushes; it only pulls.
Ratio Example
If the distance between two masses becomes 3 times, force becomes F/9.
Numerical Example
Two 1 kg masses separated by 1 m attract with force F = 6.67 × 10^-11 N.
Using Surface Distance Instead of Centre Distance
For spherical bodies, r is the distance between centres, not distance between surfaces.
Forgetting Vector Addition
For many masses, gravitational forces must be added vectorially, not simply by magnitudes.
Confusing G with g
G is universal and constant; g is local acceleration due to gravity.
Magnitude of gravitational attraction between two point masses.
Variables
F=Gravitational force
G=Universal gravitational constant
m1, m2=Masses attracting each other
r=Separation between masses
Force is attractive; negative sign indicates force on one mass is toward the other.
Variables
F_12=Force on mass 1 due to mass 2
r_hat=Unit vector from source to field point as chosen
r=Distance between masses
🪐 Kepler's Laws
Overview
Kepler’s laws describe how planets move around the Sun. The first law states that planets move in elliptical orbits with the Sun at one focus, not at the centre. The second law says the line joining the planet and Sun sweeps equal areas in equal intervals of time; this means a planet moves faster near the Sun and slower when far away. The third law states that the square of orbital period is proportional to the cube of semi-major axis: T² ∝ a³. Newton later explained these laws using universal gravitation and centripetal force. NEET commonly asks statements, area law interpretation and period-radius comparison.
- 1The Sun is at a focus of the ellipse, not at the centre.
- 2The semi-major axis decides the time period in Kepler’s third law.
- 3Equal area law means areal velocity is constant.
- 4Kepler’s laws apply to satellites around planets also, with the central mass replacing the Sun.
- 5For planets orbiting the same star, T²/r³ is constant.
- 6The law of areas is connected to zero torque under central gravitational force.
Kepler 1-2-3
1 shape, 2 sweep, 3 period: ellipse, equal areas, T² proportional to a³.
Area Law
Near Sun, run; far Sun, slow.
Period Ratio Example
If orbital radius becomes 4 times for circular orbit, T² becomes 64 times, so T becomes 8 times.
Concept Example
A comet moves fastest at perihelion because it is closest to the Sun and must sweep equal area in equal time.
Putting Sun at Centre of Ellipse
Kepler’s first law places the Sun at one focus, not at the centre.
Using Radius Instead of Semi-Major Axis for Ellipse
For elliptical orbit, Kepler’s third law uses semi-major axis a.
Assuming Speed Is Constant in Ellipse
Planetary speed varies in elliptical orbit; areal velocity remains constant.
Square of time period is proportional to cube of semi-major axis of elliptical orbit.
Variables
T=Orbital time period
a=Semi-major axis of orbit
Time period of a small body orbiting a central mass M in a circular orbit.
Variables
r=Orbital radius
M=Mass of central body
G=Universal gravitational constant
🌎 Acceleration due to Gravity
Overview
Acceleration due to gravity, g, is the acceleration acquired by a body falling freely under Earth’s gravitational pull. At Earth’s surface, it is obtained by equating weight mg with gravitational force GMm/R², giving g = GM/R². Unlike G, g is not universal; it changes with altitude, depth, latitude and Earth’s rotation. At height above Earth, g decreases according to inverse square law. Inside Earth, assuming uniform density, g decreases linearly with depth and becomes zero at the centre. Earth’s rotation reduces effective gravity, most at the equator and least at the poles. Weightlessness occurs when normal reaction becomes zero, such as in free fall or orbiting satellites.
- 1G is constant everywhere, but g varies from place to place.
- 2g decreases with altitude because distance from Earth’s centre increases.
- 3g decreases with depth because only mass inside that radius effectively contributes.
- 4g is maximum near poles and minimum near equator due to rotation and shape of Earth.
- 5Apparent weight is N, not mg; in free fall N = 0.
- 6Astronauts in orbit are weightless, not gravityless.
Altitude vs Depth
Altitude uses square law; depth uses straight line law.
Rotation Effect
Earth spins fastest effectively at equator, so g is least there.
Altitude Example
At height h = R above Earth, g_h = g(R/2R)² = g/4.
Depth Example
At depth d = R/2, g_d = g(1 - 1/2) = g/2.
Weightlessness Example
A freely falling lift has apparent weight zero because the normal reaction on a person is zero.
Assuming g Is Constant Everywhere
g is approximately constant only near Earth’s surface for small height changes.
Saying Gravity Is Zero in Satellite
Gravity is present in orbit; apparent weight is zero due to free fall.
Using Depth Formula for Altitude
Depth and altitude have different formulas; do not interchange them.
Acceleration due to gravity at the surface of a spherical planet.
Variables
g=Acceleration due to gravity
G=Universal gravitational constant
M=Mass of planet
R=Radius of planet
Gravity at height h above planet surface.
Variables
g_h=Acceleration due to gravity at height h
h=Height above surface
Approximate formula when h is much smaller than R.
Variables
h=Small height above surface
R=Planet radius
⚡Gravitational Potential & Energy
Overview
Gravitational potential at a point is the work done per unit mass by an external agent in bringing a small test mass from infinity to that point without changing kinetic energy. Taking potential zero at infinity, potential due to a mass M is V = -GM/r. Gravitational potential energy of mass m is U = mV = -GMm/r. The negative sign means the mass is bound to the gravitational field and energy must be supplied to take it to infinity. Gravitational field is related to potential by g = -dV/dr. Equipotential surfaces have the same potential everywhere, so no work is done in moving a mass along them. Potentials due to multiple bodies add algebraically.
- 1Potential is zero at infinity by convention.
- 2Gravitational potential is always negative near an isolated mass with infinity as zero.
- 3Potential energy depends on both source mass and test mass.
- 4Field is vector, but potential is scalar.
- 5For multiple bodies, add potentials directly without resolving directions.
- 6A spherical mass has equipotential surfaces as concentric spheres outside it.
Potential vs Field
Potential is scalar energy per kg; field is vector force per kg.
Negative Potential
Gravity binds, so with infinity as zero, gravitational potential is below zero.
Potential Example
At distance r from mass M, potential is -GM/r. At double distance, potential becomes -GM/(2r), closer to zero.
Multiple Bodies Example
If two equal masses M are each at distance r from a point, net potential is -GM/r - GM/r = -2GM/r.
Escape Energy Example
Energy required to take mass m from Earth surface to infinity is GMm/R, ignoring atmosphere and Earth rotation.
Adding Potential Vectorially
Potential is scalar. Add potentials algebraically, not by vector components.
Missing Negative Sign
V = -GM/r and U = -GMm/r when zero is taken at infinity.
Confusing Potential with Potential Energy
Potential is per unit mass; potential energy belongs to a specific mass m.
Potential at distance r from a point or spherical mass M.
Variables
V=Gravitational potential
G=Universal gravitational constant
M=Source mass
r=Distance from source mass
Potential energy of mass m at distance r from mass M.
Variables
U=Gravitational potential energy
m=Test mass
Gravitational field equals negative rate of change of potential with distance.
Variables
g=Gravitational field intensity
dV/dr=Potential gradient
🚀 Escape Velocity
Overview
Escape velocity is the minimum speed with which a body must be projected from the surface of a planet so that it can reach infinity with zero speed, without further propulsion. It is derived using conservation of mechanical energy: the initial kinetic energy must equal the energy needed to overcome gravitational binding. Thus, v_e = √(2GM/R) = √(2gR). Escape velocity depends on the mass and radius of the planet, but not on the mass of the escaping object or the direction of projection if air resistance and rotation are ignored. It is related to orbital velocity near the planet by v_e = √2 v_o. NEET often asks comparisons between planets.
- 1Escape velocity ignores air resistance unless stated.
- 2A heavier object does not require greater escape velocity than a lighter object.
- 3Larger planet mass increases escape velocity.
- 4Larger radius decreases escape velocity if mass is fixed.
- 5Escape requires total mechanical energy to be zero or positive.
- 6Rocket engines may provide energy gradually, so actual launch speed need not instantly equal escape velocity.
Escape Formula
Escape is root two times orbit: v_e = √2 v_o.
Mass Independence
A pebble and a rocket need the same ideal escape speed from the same planet.
Earth Example
Using g = 9.8 m/s² and R = 6.4 × 10^6 m, v_e = √(2gR) ≈ 11.2 km/s.
Planet Ratio Example
If a planet has same mass as Earth but twice the radius, its escape velocity becomes 1/√2 times Earth’s.
Previous Year Style
If orbital velocity near a planet is 8 km/s, escape velocity is 8√2 km/s.
Including Object Mass in Final Escape Velocity
Mass m cancels in derivation, so escape velocity does not depend on escaping body mass.
Confusing Escape Velocity and Orbital Velocity
Escape velocity is larger than orbital velocity by factor √2 near the surface.
Assuming Escape Means Infinite Speed at Infinity
Minimum escape velocity means speed becomes zero at infinity.
Minimum speed required from planet surface to escape gravitational field.
Variables
v_e=Escape velocity
G=Universal gravitational constant
M=Mass of planet
R=Radius of planet
Surface escape velocity written using surface gravity.
Variables
g=Acceleration due to gravity at surface
R=Planet radius
Initial kinetic energy equals gravitational binding energy.
Variables
m=Mass of escaping object
GMm/R=Energy needed to reach infinity
🛰️ Satellites & Orbital Motion
Overview
A satellite is a body revolving around a planet under gravitational attraction. In a circular orbit, gravity provides the required centripetal force, so GMm/r² = mv²/r. This gives orbital velocity v = √(GM/r), where r is distance from the planet’s centre. The orbital period is T = 2π√(r³/GM). Artificial satellites are launched for communication, weather monitoring, navigation, defence and scientific observation. A geostationary satellite has a 24-hour period, moves in the equatorial plane in the same direction as Earth’s rotation and appears fixed over one point. Polar satellites pass over poles and scan the entire Earth. Satellites and astronauts feel weightless because they are in continuous free fall.
- 1Orbital velocity is independent of satellite mass.
- 2Higher orbit means lower orbital speed but larger time period.
- 3Geostationary satellites must be equatorial, prograde and have period 24 hours.
- 4Polar satellites are useful for Earth mapping and weather observation.
- 5Weightlessness in satellites is due to free fall, not absence of gravity.
- 6Total energy of a bound satellite is negative.
Satellite Energy
For circular satellite: U is negative double of K, and total energy is negative K.
Geostationary Conditions
Geo-stationary means same Earth station: equatorial, eastward, 24-hour period.
Orbit Speed
Higher orbit means slower speed but longer period.
Orbital Velocity Example
Near Earth, v_o = √(gR) ≈ √(9.8 × 6.4 × 10^6) ≈ 7.9 km/s.
Energy Example
If a satellite has kinetic energy K in circular orbit, its potential energy is -2K and total energy is -K.
Period Concept
A satellite in a higher orbit has larger r, so from T = 2π√(r³/GM), its period is longer.
Using Earth Radius Instead of Orbital Radius
In satellite formulas, r is distance from Earth’s centre, equal to R + h.
Saying Orbital Velocity Depends on Satellite Mass
Satellite mass cancels, so orbital speed is independent of satellite mass.
Confusing Geostationary and Polar Satellites
Geostationary satellites stay above the equator; polar satellites pass near poles.
Assuming No Gravity in Orbit
Gravity is the centripetal force that keeps the satellite in orbit.
Speed needed for a circular orbit of radius r around mass M.
Variables
v_o=Orbital velocity
G=Universal gravitational constant
M=Mass of planet
r=Orbital radius from planet centre
Orbital velocity close to Earth’s surface ignoring atmosphere.
Variables
g=Surface acceleration due to gravity
R=Earth radius
Time taken by a satellite to complete one circular orbit.
Variables
T=Orbital period
r=Orbital radius
Kinetic energy of satellite in circular orbit.
Variables
K=Kinetic energy
m=Satellite mass
Formula Sheet
10Attractive gravitational force between two point masses separated by distance r.
Variables
F=Gravitational force
G=Universal gravitational constant
m1, m2=Interacting masses
r=Distance between centres of masses
Acceleration due to gravity at the surface of a planet of mass M and radius R.
Variables
g=Acceleration due to gravity
M=Mass of planet
R=Radius of planet
Gravitational potential at distance r from an isolated spherical mass M, taking zero at infinity.
Variables
V=Gravitational potential
M=Source mass
r=Distance from source mass
Minimum speed needed to escape a planet’s gravitational field without further propulsion.
Variables
v_e=Escape velocity
M=Mass of planet
R=Radius of planet
Magnitude of gravitational attraction between two point masses.
Variables
F=Gravitational force
G=Universal gravitational constant
m1, m2=Masses attracting each other
r=Separation between masses
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NEET PYQs — Gravitation
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The amount of work done to raise a mass 'm' from the surface of the Earth to a height equal to the radius of the Earth 'R' will be:
A body weighs 48 N on the surface of the earth. The gravitational force experienced by the body due to the earth at a height equal to one-third the radius of the earth from its surface is :
The radius of Martian orbit around the Sun is about 4 times the radius of the orbit of Mercury. The Martian year is 687 Earth days. Then which of the following is the length of 1 year on Mercury?
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