, 1 Galaxies
1.1 Types of galaxies
There are two types of galaxies; elliptical galaxies and spiral galaxies. In elliptical galaxies stars orbit
all around the galaxy. In spiral galaxies stars orbit in a plane around the center.
2 Gravity
2.1 Basics of gravity
To describe the motion of objects under gravity we use the following equations:
F⃗ (⃗x) = −m∇Φ(⃗x) (1)
∇2 Φ(⃗x) = 4πGρ(⃗x) (2)
We will be using these two equations to describe stars and galaxies. We will not need general or
special relativity as the speeds we are working with are well below the speed of light.
The point-mass potential is given by:
GM
Φ(r) = − (3)
r
This is also the potential outside any spherical mass distribution. It does not matter how it is
distributed inside that boundary.
The circular velocity, also known as Keplerian velocity, is described by:
r
GM
vc (r) = (4)
r
This equation is equivalent to Kepler’s third law. Equation 4 implies that when vc is constant, the
mass of a galaxy M is proportional to its radius r. However we know that the mass does not increase
with the radius, so we are missing a component; dark matter.
The time it takes to complete an orbit at a given circular velocity is given by the dynamical or crossing
time:
2πr
tdyn = (5)
vc
The dynamical time of the Milky Way is approximately 225 Myrs, which is short compared to the age
of the Universe. This means there has been enough time for galaxies to reach dynamical equilibrium.
If the dynamical time long, we would see galaxies as they were forming.
3
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