# Newton's gravity formulas for ellipses

A few times I've come across formulas, which are identical for circular and elliptical orbits, except that for the second ones you substitute $r$ with $a$, where $r$ is the radius of a circular orbit and $a$ the semi-major axis of an elliptical orbit. For instance:

Third Kepler's law for circular orbits: $T^2=\frac{4\pi^2}{GM}r^3$,

Third Kepler's law for elliptical orbits: $T^2=\frac{4\pi^2}{GM}a^3$,

or

Mechanical energy of a satellite in a circular orbit: $E=-\frac{GMm}{2r}$,

Mechanical energy of a satellite in an elliptical orbit: $E=-\frac{GMm}{2a}$.

Such substituting is very convenient but also seems a bit too easy. I'm wondering: how can you justify it? Do you have to always prove everything and it just always happens, that you can swap those values, or maybe it's possible to justify it with a single claim?

Well, a circle is a special case of an ellipse, so if something is true of a general ellipse, it will be true of a circle.

In order to work out the rules for ellipses, the calculus is typically a bit more involved than what you see in your standard intro class, so the real, general case is usually reserved for sophomore year classical mechanics, where you basically solve ${\vec a} = -\frac{GM{\vec x}}{|{\vec x}|^{3}}$ for ${\vec x}$ in the general case.

• That means that from a formula for elliptical orbits I can always infer the formula for circular orbits. Is the opposite also always true? If not, could you please name an example? Jun 16, 2020 at 17:04
• @hm1912 all circles are ellipses, but not all ellipses are circles. Jun 17, 2020 at 16:10