AstrophysicsGalaxies and Cosmology

Rotation Curves and Dark Matter

v(r) = √(GM(r)/r), so a flat rotation curve needs mass that grows in proportion to r.

Not started Jump to practice

How do you weigh a galaxy? The same way you weigh the Sun: watch something orbit it. In a spiral galaxy, stars and gas clouds circle the center, and Doppler shifts give their speeds at every radius. A plot of orbital speed against radius is a rotation curve. In Dark Matter you saw what it revealed; here you will do the calculation, using the shell theorem.

Why it works

For a roughly spherical distribution of mass, a body orbiting at radius $r$ feels only the mass $M(r)$ inside its orbit, as if it were at the center. A circular orbit needs $v^2/r = GM(r)/r^2$, so $$v(r) = \sqrt{\frac{GM(r)}{r}}, \qquad M(r) = \frac{v^2r}{G}.$$ If nearly all of the mass sat in the bright center, $M(r)$ would stop growing beyond it and orbital speeds would fall as $1/\sqrt{r}$, like the planets. Instead, from the 1970s Vera Rubin and Kent Ford and later radio astronomers found that the curves of spiral galaxies stay flat far beyond the visible disk.

Key idea

A flat rotation curve ($v$ constant) means $M(r) = v^2r/G$ keeps growing in proportion to $r$, out where there are few stars and little gas. Most of a galaxy's mass is invisible: dark matter, in a halo with density falling roughly as $1/r^2$.
Orbital speed against distance from the center. The dashed curve is what the visible stars and gas alone would produce; the measured curve stays flat.

Worked examples

Worked example: Weighing the Milky Way inside the Sun's orbit

The Sun orbits the galactic center at about 230 km/s, 8.2 kpc out. How much mass lies inside the Sun's orbit, and how long is one orbit? ($1\text{ kpc} = 3.09 \times 10^{19}$ m.)
  1. $$M = \frac{v^2r}{G} = \frac{(2.30 \times 10^{5})^2(2.53 \times 10^{20})}{6.67 \times 10^{-11}} = 2.0 \times 10^{41}\text{ kg}.$$
  2. In solar masses: $2.0 \times 10^{41}/1.99 \times 10^{30} \approx 1.0 \times 10^{11}$.
  3. Period: $2\pi r/v = 2\pi(2.53 \times 10^{20})/(2.30 \times 10^{5}) = 6.9 \times 10^{15}$ s.

Answer: About $10^{11}\,M_\odot$, and one "galactic year" of about 220 million years.

Worked example: What Kepler would predict

Stars 10 kpc out in a galaxy orbit at 220 km/s. If all the mass were inside 10 kpc, how fast would gas at 40 kpc orbit?
  1. Same mass: $v \propto 1/\sqrt{r}$.
  2. $v = 220\sqrt{10/40} = 220/2$.

Answer: 110 km/s. Measured curves stay near 220 km/s instead, so the mass inside 40 kpc is four times the mass inside 10 kpc.

Worked example: The dark halo's density

For a flat curve at 220 km/s, the density at radius $r$ is $\rho = v^2/(4\pi Gr^2)$. Evaluate it at 8 kpc.
  1. $$\rho = \frac{(2.20 \times 10^{5})^2}{4\pi(6.67 \times 10^{-11})(2.47 \times 10^{20})^2}$$
  2. $\rho \approx 9 \times 10^{-22}$ kg/m³, or about $0.014\,M_\odot$ per cubic parsec.

Answer: A thin haze: roughly half a proton's mass per cubic centimeter, but spread through an enormous volume.

Common mistake

Missing why a flat curve is a surprise. With visible matter alone, the mass would be nearly all inside the bright inner disk, and stars and gas farther out should orbit more slowly, $v \propto 1/\sqrt{r}$, as the outer planets do. A flat curve means the enclosed mass keeps growing with radius even where we see almost nothing. Check with numbers: $M(r) = v^2r/G$ doubles from 10 kpc to 20 kpc when $v$ stays the same.

Practice

Pass with 3 right answers, the last 2 in a row. Each right answer earns 2 XP.

Loading practice…

Builds on

Leads to

Sources and further reading

  • OpenStax Astronomy 2e, section 25.3 (The Mass of the Galaxy) and section 28.4 (The Challenge of Dark Matter)
  • MIT OpenCourseWare 8.282J Introduction to Astronomy (Spring 2006)
@teddyrookbook GitHub