This MCQ module is based on: Keplers Laws Universal Gravitation
Keplers Laws Universal Gravitation
This assessment will be based on: Keplers Laws Universal Gravitation
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Keplers Laws Universal Gravitation
7.1 Introduction
Early humans gazed at the night sky and wondered why the Sun, Moon and stars do not fall down. Ancient Indian astronomers, the Greeks, and later Renaissance scientists each built models to explain celestial motion. Aristotle taught that heavenly bodies move in perfect circles because they are made of a special "fifth element". A heliocentric model placing the Sun at the centre was proposed by Aryabhata in India, and rediscovered in Europe by Nicolas Copernicus in 1543. Detailed observations by Tycho Brahe and analysis by Johannes Kepler finally produced the three empirical laws that paved the way for Newton's law of universal gravitation.
7.2 Kepler's Laws
Tycho Brahe (1546–1601) recorded planetary positions with the naked eye for decades. His assistant Johannes Kepler (1571–1630) spent years analysing the Mars data and extracted three beautifully simple laws.
7.2.1 Law of Orbits (First Law)
7.2.2 Law of Areas (Second Law)
This means a planet moves faster when it is close to the Sun (perihelion) and slower when far away (aphelion). The areal velocity \(\frac{dA}{dt}\) is constant. We can derive this from angular momentum:
Because gravity is a central force, the torque on a planet about the Sun is zero, so its angular momentum \(L\) is conserved. This is exactly Kepler's Second Law in disguise.
7.2.3 Law of Periods (Third Law)
| Planet | a (×10¹⁰ m) | T (years) | T²/a³ (×10⁻³⁴) |
|---|---|---|---|
| Mercury | 5.79 | 0.241 | 2.95 |
| Venus | 10.8 | 0.615 | 2.99 |
| Earth | 14.96 | 1.000 | 2.96 |
| Mars | 22.79 | 1.881 | 2.98 |
| Jupiter | 77.83 | 11.86 | 3.01 |
| Saturn | 142.7 | 29.46 | 2.98 |
The remarkable constancy of T²/a³ across the solar system confirms Kepler's Third Law to high precision.
Interactive Simulation: Kepler's Third Law Calculator
Adjust the semi-major axis \(a\) (in AU) and instantly see the orbital period \(T\) via \(T^2 = a^3\) (Earth units).
Period T = 1.00 years
(Try a = 5.2 for Jupiter or a = 19.2 for Uranus)
7.3 Universal Law of Gravitation
Sir Isaac Newton (1665–1687) realised that the same force which makes an apple fall also keeps the Moon in orbit. He showed that to produce Kepler's Third Law with circular orbits, the force must vary as the inverse square of distance.
The force is always attractive and acts along the line joining the two masses. In vector form, the force on mass 1 due to mass 2 is:
The negative sign shows it points from 1 toward 2 (attraction). For an extended body like Earth, we may treat its entire mass as concentrated at its centre when computing the force on an external particle — this is the powerful Shell Theorem.
7.3.1 Cavendish's Experiment — Measuring G
In 1798 Henry Cavendish suspended a light rod with two small lead spheres at its ends from a fine quartz fibre. Two large lead spheres were brought near the small ones. The gravitational attraction caused the rod to rotate; the twist of the fibre measured the tiny force, yielding the first value of G.
Worked Example 1: Force between two students
Two friends of masses 60 kg and 55 kg stand 0.5 m apart. Find the gravitational force between them.
Worked Example 2: Earth–Moon force
Earth mass M = 6.0×10²⁴ kg, Moon mass m = 7.4×10²² kg, distance r = 3.84×10⁸ m. Find F.
Materials: Cardboard, two pins, string loop, pencil.
- Stick two pins about 10 cm apart on the cardboard.
- Loop a string of length 20 cm loosely around both pins.
- Pull the string taut with a pencil tip and move the pencil all around — keeping the string tight.
Observation: The pencil traces an ellipse. The two pins are the foci. As the pins move closer, the ellipse becomes more like a circle; as they move farther apart (with fixed string length), the ellipse flattens.
Conclusion: An ellipse is the locus of points whose distances from two fixed foci sum to a constant. For a circle, the two foci coincide. Planetary orbits are ellipses with small eccentricity — close to circles but not exactly.
Competency-Based Questions
Q1. According to Kepler's Third Law, the orbital period of Kalpana-X is approximately:L3 Apply
Q2. At which point does Kalpana-X move with the highest orbital speed?L2 Understand
Q3. True or False: Kepler's Third Law applies only to planets in our solar system. Justify.L5 Evaluate
Q4. Fill in the blank: Kepler's Second Law is a direct consequence of conservation of __________.L1 Remember
Q5. HOT: Design an experiment a high-school student could perform on Earth to estimate G using everyday materials.L6 Create
Assertion–Reason Questions
(A) Both true, R explains A. (B) Both true, R does NOT explain A. (C) A true, R false. (D) A false, R true.
A: A planet moves faster at perihelion than at aphelion.
R: Angular momentum of the planet about the Sun is conserved.
A: The gravitational constant G depends on the medium between the two masses.
R: G is a universal constant having the same value everywhere in the universe.
A: Kepler's laws apply to artificial satellites orbiting the Earth.
R: Newton's law of gravitation governs all gravitational orbits, of which Kepler's laws are a special case.