CBSE • Class 11 • Physics
Gravitation
Universal gravitation, gravitational potential, satellites, and escape speed.
Chapter 7
Verified Curriculum Topic
What is Gravitation?
Universal gravitation, gravitational potential, satellites, and escape speed.
Gravitation matters because it connects theory, equations, and real physical behaviour. At Class 11 level, students are typically expected to explain concepts precisely, apply laws correctly, and interpret numerical or experimental questions with confidence.
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Summary
The One Thing
Gravitation is a universal attractive interaction whose inverse-square force governs falling objects, planetary motion and satellite orbits. Gravitational potential and energy determine whether an object remains bound to a celestial body or can escape its gravitational field.
Reactions, Processes and Experiments
| What happens | Equation or process | What you observe | Type |
|---|---|---|---|
| Two masses attract one another. | F = Gm1m2/r^2 | The force is always attractive and acts along the line joining the centres of the two masses. | Universal gravitation |
| A mass falls freely under the gravitational influence of a spherical body. | g = GM/r^2 | The object accelerates toward the centre of the body. | Acceleration due to gravity |
| Gravitational acceleration is considered at Earth’s surface. | g = GM_E/R_E^2 | Near Earth’s surface, g is approximately 9.8 m s^-2. | Surface gravity |
Gravitational acceleration is considered at height h above Earth’s surface. | g_h = g[R_E/(R_E + h)]^2 | Gravitational acceleration decreases as height increases. | Variation of gravity with height |
Gravitational acceleration is considered at depth d below Earth’s surface, assuming uniform density. | g_d = g(1 - d/R_E) | Gravitational acceleration decreases with depth and reaches zero at the centre in this model. | Variation of gravity with depth |
| A small test mass is brought from infinity to a point in a gravitational field without changing its kinetic energy. | V = -GM/r | The potential is negative when infinity is taken as zero. | Gravitational potential |
A mass is located at distance r from a mass M. | U = mV = -GMm/r | The potential energy is negative, indicating a bound state relative to infinity. | Gravitational potential energy |
| Gravity moves a mass between two points. | Work done by gravity is independent of the path followed. | The work depends only on the initial and final positions. | Conservative force |
| A spherically symmetric shell attracts an external object. | The shell theorem states that the shell attracts an external object as though all its mass were concentrated at its centre. | The external gravitational effect is the same as that of a point mass at the centre. | Shell theorem |
| A test mass is located inside a spherically symmetric shell. | The shell theorem states that the net gravitational field inside the shell is zero. | The net gravitational field inside the shell is zero. | Shell theorem |
| A satellite moves in a circular orbit when gravitational attraction supplies the required centripetal force. | GMm/r^2 = mv^2/r | The satellite continually falls toward Earth but its tangential velocity causes it to keep missing Earth’s surface. | Circular satellite orbit |
A satellite travels in a circular orbit of radius r. | v_o = √(GM/r) | A lower orbit has greater orbital speed than a higher orbit. | Orbital velocity |
| Orbital velocity is expressed using surface gravity near Earth. | v_o = √(gR_E) | The required orbital speed depends on the gravitational field and orbital radius. | Orbital velocity near Earth |
| A satellite completes a circular orbit. | T = 2π√(r^3/GM) | A higher orbit has a longer time period; T^2 is proportional to r^3. | Orbital period |
| The total mechanical energy of a satellite in a circular orbit is determined. | E = -GMm/(2r) | The negative total energy shows that the satellite is gravitationally bound. | Total orbital energy |
| An object is given the minimum speed required to escape a celestial body. | v_e = √(2GM/R) = √(2gR) | The object reaches infinity with zero final speed, if air resistance and rotation are neglected. | Escape speed |
| Escape speed and orbital speed are compared near the surface of the same celestial body. | v_e = √2 v_o | Escape speed is greater than orbital speed by a factor of √2. | Escape speed and orbital velocity |
| An object escapes a celestial body. | Escape speed does not depend on the mass of the escaping object, if air resistance and rotation of the body are neglected. | Objects of different masses require the same escape speed from the same body. | Escape speed |
| An object escapes Earth. | Earth’s escape speed is approximately 11.2 km s^-1. | An initial speed of approximately 11.2 km s^-1 is required under the stated ideal conditions. | Escape speed from Earth |
| A satellite remains apparently stationary above Earth. | A geostationary satellite has a circular equatorial orbit, an eastward direction of revolution, and a period equal to Earth’s rotational period. | It appears stationary above a fixed point on Earth’s equator. | Geostationary orbit |
| A geostationary satellite orbits Earth. | The approximate geostationary orbital radius from Earth’s centre is 4.23 × 10^7 m, or about 36,000 km above Earth’s surface. | The satellite remains above the same equatorial location. | Geostationary satellite |
| Planets move around the Sun. | Kepler’s first law: planets move in elliptical orbits with the Sun at one focus. | The orbit is elliptical rather than necessarily circular. | Kepler’s first law |
| A planet moves along its orbit. | Kepler’s second law: the line joining a planet and the Sun sweeps out equal areas in equal intervals of time. | The planet moves faster when closer to the Sun and slower when farther away. | Kepler’s second law |
| Bodies orbit the same central mass. | Kepler’s third law: T^2/a^3 is constant for bodies orbiting the same central mass. | The square of the period is proportional to the cube of the orbit’s semi-major axis. | Kepler’s third law |
| A mass moves from one point in a gravitational field to another. | Gravity is a conservative force; work done by gravity is independent of the path followed. | Different paths between the same points give the same work. | Conservative gravitational field |
| A mass is moved from a gravitational field to infinity. | Escape requires enough kinetic energy to overcome the negative gravitational potential energy and reach zero total energy at infinity. | At the minimum escape condition, the object reaches infinity with zero final speed. | Escape by energy conservation |
| An object orbits Earth or another celestial body. | An orbiting satellite is continuously falling toward Earth, but its tangential velocity makes it keep missing Earth’s surface. | The object remains in orbit rather than colliding with the surface. | Orbital motion |
| An object is in free fall or orbiting in a spacecraft. | The normal reaction on the object becomes zero. | The object experiences weightlessness. | Weightlessness |
Key Terms
- Universal Law of Gravitation: The force between two masses is directly proportional to the product of their masses and inversely proportional to the square of the distance between their centres.
- Gravitational Constant: The constant
Gin Newton’s law of gravitation; its value is approximately6.67 × 10^-11 N m^2 kg^-2. - Gravitational Field: The region around a mass where another mass experiences gravitational force.
- Acceleration Due to Gravity: The acceleration produced in a freely falling object by a celestial body; near Earth’s surface, it is approximately
9.8 m s^-2. - Gravitational Potential: The work done per unit mass in bringing a small test mass from infinity to a point in a gravitational field without changing its kinetic energy.
- Gravitational Potential Energy: The energy possessed by a mass because of its position in a gravitational field; for a mass
mat distancerfrom a massM,U = -GMm/r. - Orbital Velocity: The tangential speed required for a satellite to remain in a circular orbit around a celestial body; near Earth’s surface,
v_o = √(GM/r). - Satellite: An object that revolves around a planet or another celestial body under the influence of gravity.
- Geostationary Satellite: A satellite that appears stationary above a point on Earth’s equator because it has an orbital period of about 24 hours and moves in Earth’s rotational direction.
- Escape Speed: The minimum initial speed required for an object to escape the gravitational field of a celestial body;
v_e = √(2GM/R). - Kepler’s Laws: Three laws describing planetary motion: orbits are elliptical, equal areas are swept in equal times, and the square of the period is proportional to the cube of the orbit’s semi-major axis.
- Weightlessness: The condition in which the normal reaction on an object becomes zero, such as during free fall or while orbiting in a spacecraft.
- Shell Theorem: A spherically symmetric shell attracts an external object as though all its mass were concentrated at its centre, while the net gravitational field inside the shell is zero.
- Gravitational Potential Reference: Gravitational potential is usually defined by taking its value at infinity as zero; its numerical value therefore depends on the chosen reference level.
- Gravitational Field Strength: The strength of a gravitational field decreases with distance according to an inverse-square relationship.
- Orbital Period: The time taken by a satellite to complete one orbit; for a circular orbit,
T = 2π√(r^3/GM). - Total Mechanical Energy: The sum of kinetic and potential energy; for a satellite in a circular orbit,
E = -GMm/(2r).
Easily Confused
- Gravitational potential and gravitational potential energy: Potential is work done per unit mass, measured in
J kg^-1orm^2 s^-2; potential energy is the energy of a particular mass and is measured in joules. - Orbital velocity and escape speed: Orbital velocity keeps an object in a bound orbit, whereas escape speed allows it to reach infinity with zero final speed.
- Weightlessness and absence of gravity: Weightlessness means that the normal reaction is zero; it can occur during free fall or orbital motion even though gravity is acting.
- Orbital speed in lower and higher orbits: A lower orbit has greater orbital speed and a shorter period than a higher orbit.
- Geostationary and ordinary satellites: A geostationary satellite must have a circular equatorial orbit, eastward motion and a period equal to Earth’s rotational period; these conditions are not required of every satellite.
- Gravitational force and centripetal force: Gravitational force is the physical attraction between masses; in a circular satellite orbit, it supplies the centripetal force.
- Gravitational potential energy and total orbital energy: Gravitational potential energy is
U = -GMm/r, whereas total mechanical energy in a circular orbit isE = -GMm/(2r). - Distance from Earth’s centre and height above Earth’s surface: The orbital formula uses the distance
rfrom Earth’s centre; height above the surface is represented byh, withr = R_E + h.
What Gets Asked
- State or apply Newton’s law of gravitation: Use
F = Gm1m2/r^2, withras the distance between the centres of the masses. Marks are lost by using surface separation instead of centre-to-centre distance or by omitting that the force is attractive. - Calculate gravitational acceleration at a surface, height or depth: Use
g = GM/r^2,g_h = g[R_E/(R_E + h)]^2, org_d = g(1 - d/R_E)as appropriate. Marks are lost by using the height expression for a depth question. - Calculate gravitational potential or potential energy: Use
V = -GM/randU = -GMm/r, taking infinity as zero. Marks are lost by omitting the negative sign, which indicates a bound state relative to infinity. - Derive or calculate orbital velocity and period: Equate gravitational force to centripetal force using
GMm/r^2 = mv^2/r, then usev_o = √(GM/r)andT = 2π√(r^3/GM). Marks are lost by confusing orbital radius with height above the surface. - Explain escape speed: Use
v_e = √(2GM/R) = √(2gR)and, for the same body,v_e = √2 v_o. Marks are lost by treating escape speed as dependent on the escaping object’s mass or by confusing it with orbital speed. - Describe geostationary satellites or apply Kepler’s laws: State the required circular equatorial orbit, eastward direction and approximately 24-hour period for geostationary motion, or identify elliptical orbits, equal areas in equal times and
T^2/a^3constant for Kepler’s laws.
Flashcards
Quick quiz
According to Newton's universal law of gravitation, how does the gravitational force between two masses depend on the distance between their centres?
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- Explain the core principle behind Gravitation in clear scientific language.
- Use the correct equations, symbols, and units when solving numerical questions.
- Interpret diagrams, graphs, or experiments linked to the topic.
- Connect conceptual understanding with the final answer instead of memorising formulas alone.
Common exam prompts
- State the law, principle, or definition behind Gravitation precisely.
- Apply the relevant equation to a short numerical problem with correct units.
- Explain a diagram, graph, or experiment related to Gravitation.
- Distinguish between conceptual understanding and memorised formula use in this chapter.
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What is Gravitation in CBSE Class 11 Physics?
Universal gravitation, gravitational potential, satellites, and escape speed.
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