D.1.1—Kepler’s three laws of orbital motion

Syllabus
First assessment 2025
Objective
Level
HL

Model Kepler’s Three Laws

State the three laws

  1. A planet follows an elliptical orbit with the star at one focus.
  2. The line from the star to the planet sweeps out equal areas in equal time intervals.
  3. For bodies orbiting the same central star, the square of the orbital period is proportional to the cube of the semi-major axis: T2a3T^2\propto a^3.

Interpret the geometry

The semi-major axis aa is half the longest diameter of the ellipse. In an elliptical orbit the planet is closer to the star at one focus-side end and farther away at the other. Equal swept areas mean the planet moves faster when it is closer to the star and slower when it is farther away.

Compare orbital systems

For two planets around the same star,
TYTX=(aYaX)3/2\frac{T_Y}{T_X}=\left(\frac{a_Y}{a_X}\right)^{3/2}
Use the semi-major axes, not automatically the instantaneous distance from the star. The third law comparison assumes the same central mass.

Common trap

The star is at a focus, not generally at the centre of the ellipse. Also, the second law refers to equal swept areas, not equal arc lengths or equal distances travelled.

D.1.1 Exam Analysis

Assessment in practice

1 marks
How it is assessed

Questions identify a correct Kepler statement or compare periods for planets orbiting the same star using the 3/2 power of the semi-major-axis ratio.

Command terms

Which is / What is

What earns marks

Match each statement to its law, distinguish semi-major axis from instantaneous radius, and use T²∝a³ only when comparing bodies around the same central star.

Watch for

Replacing the semi-major axis with the instantaneous orbital radius, or stating that the star lies at the centre of an ellipse.

Representative question

Question 1

[Maximum number: 1]

The relationship between the period of a planet's orbit T and the distance to the Sun R can be expressed as TnRmT^{\mathrm{n}} \propto R^{\mathrm{m}} where n and m are constants.

What is a possible pair of values for n and m ?

n

m

1.0

3.0

1.0

1.5

2.0

1.5

2.0

1.0

Retrieve the Core D.1 Gravitational Fields Model

D.1 core gravitational fields is secure when you can connect source mass, distance and field representation.

  • Kepler’s three laws describe orbital geometry and period
  • F=Gm1m2/r² for point-mass interactions
  • Point-mass approximation requires suitable size or symmetry conditions
  • g=F/m=GM/r² is a vector field strength
  • Field lines point toward mass and spread as the field weakens