AstronomyGravity and OrbitsHS-ESS1-4

Weighing Stars and Planets with Orbits

Newton's form of Kepler's third law, M = a³/P² in solar masses, AU and years, gives the mass at the center.

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Kepler's third law was a pattern; Newton explained it, and in doing so turned every orbit into a scale for weighing the body at the center. You know from Gravity: Mass and Distance that more mass means more pull. More pull means a faster orbit.

Why it works

Take a small body on a circular orbit of radius $a$ around a mass $M$. Gravity supplies the centripetal force: $\frac{GMm}{a^2} = \frac{mv^2}{a}$, so $v^2 = \frac{GM}{a}$. The small mass $m$ cancels. One orbit takes $P = \frac{2\pi a}{v}$, so $v = \frac{2\pi a}{P}$. Substituting: $\frac{4\pi^2 a^2}{P^2} = \frac{GM}{a}$, which gives $$M = \frac{4\pi^2 a^3}{G P^2}.$$ The same result holds for ellipses with $a$ the semi-major axis. In the Sun's units (AU, years, solar masses), Earth's orbit makes every constant equal to 1, leaving $M = \frac{a^3}{P^2}$. (Strictly, $M$ is the sum of both masses; a planet adds almost nothing.)

Key idea

Newton's form of Kepler's third law: $M = \dfrac{a^3}{P^2}$ with $M$ in solar masses, $a$ in AU and $P$ in years; in SI units, $M = \dfrac{4\pi^2 a^3}{G P^2}$. The orbit measures the mass at the center.
A planet at $1$ AU from a star of $2$ solar masses: its year is $\sqrt{1/2} = 0.71$ years. The heavier star pulls harder, so the orbit is faster.

Worked examples

Worked example: A star's mass

A planet orbits a distant star at $a = 2$ AU with a period of $2$ years. What is the star's mass?
  1. $M = \frac{a^3}{P^2} = \frac{2^3}{2^2} = \frac{8}{4}$.
  2. $M = 2$ solar masses.

Answer: $2$ solar masses.

Worked example: Weighing Jupiter

Jupiter's moon Io orbits at $4.22 \times 10^{8}$ m every $1.769$ days. Find Jupiter's mass.
  1. Period in seconds: $1.769 \times 86{,}400 = 1.528 \times 10^{5}$ s.
  2. $a^3 = (4.22 \times 10^{8})^3 = 7.52 \times 10^{25}\,\text{m}^3$.
  3. $M = \frac{4\pi^2 \times 7.52 \times 10^{25}}{6.674 \times 10^{-11} \times (1.528 \times 10^{5})^2} = 1.90 \times 10^{27}$ kg, about 318 Earth masses.

Answer: $1.90 \times 10^{27}$ kg.

Common mistake

It seems natural that a heavier satellite would orbit faster or slower, but the orbiting body's own mass cancels out of $\frac{GMm}{a^2} = \frac{mv^2}{a}$. A space station and a dropped bolt beside it orbit together. That is why an orbit weighs the central body. Check: the Moon (about $1\%$ of Earth's mass) and a tiny satellite at the Moon's distance would have almost exactly the same 27-day period.
This is how astronomers know the masses of the Sun, the planets with moons, distant stars with planets, and the black hole at the center of our galaxy.

Practice

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Sources and further reading

  • OpenStax, Astronomy 2e, section 3.3, Newton's Universal Law of Gravitation
  • OpenStax, Astronomy 2e, section 18.2, Measuring Stellar Masses
  • NGSS HS-ESS1-4
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