AstrophysicsBinary Stars and Exoplanets

Exoplanet Transits

A transit's depth (R_p/R_*)² gives the planet's size, and its period gives the orbit.

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A planet that crosses in front of its star is a tiny eclipsing binary in which one member is dark. You met the idea in Finding Planets Around Other Stars, and the geometry of eclipsing binaries carries over. NASA's Kepler and TESS missions found thousands of planets this way by watching stars dim on a schedule.

Why it works

The star's disk has area $\pi R_\star^2$ and the planet covers $\pi R_p^2$ of it. If the disk were uniformly bright, the fraction of light lost would be the ratio of areas: $$\delta = \frac{\pi R_p^2}{\pi R_\star^2} = \left(\frac{R_p}{R_\star}\right)^{2}.$$ The repeat time is the orbital period, and Kepler's third law turns it into the orbit's size: $a^3 = M_\star P^2$ (AU, years, solar masses). During a central transit the planet moves a distance $2R_\star$ at its orbital speed $2\pi a/P$, which gives the transit's length.

Key idea

Depth $\delta = (R_p/R_\star)^2$, so $R_p = R_\star\sqrt{\delta}$. Period gives $a = (M_\star P^2)^{1/3}$, and a central transit lasts about $t \approx PR_\star/(\pi a)$.
A dark planet with one-tenth of the star's radius blocks one-hundredth of its light: $(0.1)^2 = 1\%$.
Depths an observer far away would see. Earth-size planets around Sun-like stars dim them by less than one part in 10,000.
Planet crossing the Sun$R_p/R_\odot$Depth
Jupiter$0.103$about 1%
Neptune$0.035$about 0.13%
Earth$0.0092$about 84 ppm

Worked examples

Worked example: An Earth-size planet

A star of $0.90\,R_\odot$ dims by 100 parts per million during each transit. How big is the planet? ($R_\odot = 109\,R_\oplus$.)
  1. $R_p/R_\star = \sqrt{1.00 \times 10^{-4}} = 0.0100$.
  2. $R_\star = 0.90 \times 109 = 98\,R_\oplus$.
  3. $R_p = 0.0100 \times 98 = 0.98\,R_\oplus$.

Answer: About the size of Earth.

Worked example: Orbit and duration

A planet transits a $1.0\,M_\odot$, $1.0\,R_\odot$ star every 3.5 days. Find its orbital radius and how long a central transit lasts ($1\text{ AU} = 215\,R_\odot$).
  1. $P = 3.5/365.25 = 9.58 \times 10^{-3}$ yr, so $a = (1.0 \times (9.58 \times 10^{-3})^2)^{1/3} = 0.0451$ AU.
  2. In solar radii, $a = 0.0451 \times 215 = 9.70\,R_\odot$.
  3. $t \approx PR_\star/(\pi a) = (84\text{ h})(1.0)/(\pi \times 9.70) = 2.8$ h.

Answer: $a \approx 0.045$ AU (a "hot Jupiter" distance, far inside Mercury's 0.39 AU), and each transit lasts about 2.8 hours.

Worked example: What is it made of?

Another transiting planet has a radius of $1.5\,R_\oplus$, and the wobble it gives its star yields a mass of $5.0\,M_\oplus$. Find its mean density. (Earth's mean density is 5.51 g/cm³.)
  1. Density scales as mass over radius cubed: $\rho = 5.51 \times 5.0/1.5^3$ g/cm³.
  2. $1.5^3 = 3.375$, so $\rho = 5.51 \times 1.48$.

Answer: About 8.2 g/cm³, denser than Earth: a rocky planet, probably with a large iron core. Combining transits (size) with wobbles (mass) is how astronomers tell rocky worlds from gas-rich ones.

Common mistake

Taking the depth to be $R_p/R_\star$ instead of its square. A dip of 1% does not mean the planet is 1% of the star's radius; it means $R_p/R_\star = \sqrt{0.01} = 0.1$, ten times larger. The light lost depends on the area covered. Check: Jupiter, about one-tenth of the Sun's radius, would cause a 1% dip, not a 10% one.

Practice

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Sources and further reading

  • OpenStax Astronomy 2e, section 21.4 (Planets beyond the Solar System: Search and Discovery)
  • NASA Exoplanet Exploration, Ways to Find a Planet: Transit
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