25.6: Kepler’s Laws
( \newcommand{\kernel}{\mathrm{null}\,}\)
Elliptic Orbit Law
I. Each planet moves in an ellipse with the sun at one focus.
When the energy is negative, E<0, and according to Equation (25.3.14),
ε=(1+2EL2μ(Gm1m2)2)12
and the eccentricity must fall within the range 0≤ε<1. These orbits are either circles or ellipses. Note the elliptic orbit law is only valid if we assume that there is only one central force acting. We are ignoring the gravitational interactions due to all the other bodies in the universe, a necessary approximation for our analytic solution.
Equal Area Law
II. The radius vector from the sun to a planet sweeps out equal areas in equal time.
Using analytic geometry in the limit of small Δθ , the sum of the areas of the triangles in Figure 25.9 is given by
ΔA=12(rΔθ)r+(rΔθ)2Δr

The average rate of the change of area, ΔA, in time, Δt, is given by
ΔA=12(rΔθ)rΔt+(rΔθ)2ΔrΔt
In the limit as Δt→0,Δθ→0, this becomes
dAdt=12r2dθdt
Recall that according to Equation (25.3.7) (reproduced below as Equation ???), the angular momentum is related to the angular velocity dθ/dt by
dθdt=Lμr2
and Equation ??? is then
dAdt=L2μ
Because L and μ are constants, the rate of change of area with respect to time is a constant. This is often familiarly referred to by the expression: equal areas are swept out in equal times (see Kepler’s Laws at the beginning of this chapter).
Period Law
III. The period of revolution T of a planet about the sun is related to the semi-major axis a of the ellipse by T2=ka3 where k is the same for all planets.
When Kepler stated his period law for planetary orbits based on observation, he only noted the dependence on the larger mass of the sun. Because the mass of the sun is much greater than the mass of the planets, his observation is an excellent approximation.
In order to demonstrate the third law we begin by rewriting Equation ??? in the form
2μdAdt=L
Equation ??? can be integrated as
∫orbit 2μdA=∫T0Ldt
where T is the period of the orbit. For an ellipse,
∫orbit dA=πab
where a is the semi-major axis and b is the semi-minor axis (Figure 25.10).

Thus we have
T=2μπabL
Squaring Equation ??? then yields
T2=4π2μ2a2b2L2
In Appendix 25B, Equation (25.B.20) gives the angular momentum in terms of the semimajor axis and the eccentricity. Substitution for the angular momentum into Equation (25.5.11) yields
T2=4π2μ2a2b2μGm1m2a(1−ε2)
In Appendix 25B, Equation (25.B.17) gives the semi-minor axis which upon substitution into Equation (25.5.12) yields
T2=4π2μ2a3μGm1m2
Using Equation (25.2.1) for reduced mass, the square of the period of the orbit is proportional to the semi-major axis cubed,
T2=4π2a3G(m1+m2)