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The Kepler orbit equation is a conic: u=c(1+ecos⁡(φ−θ0)) with E=(μκ2/2J2)(e2−1)

Statement

Let μ>0, κ>0, U(ρ)=−κ/ρ on (0,∞), let r:I→R3 be a central-force trajectory for (μ,U) with constant angular momentum j=Je3, J>0 and constant energy E (Central-force trajectories: the central-force equation, angular momentum, energy and the effective potential), and let u:W→(0,∞), θ and σ be as in Binet's equation for the attractive inverse-square field: d2u/dφ2+u=μκ/J2 for u=1/ρ, with W=θ(I∘). Write c:=μκ/J2>0 and p:=1/c=J2/(μκ). Then:

  1. there are e≥0 and θ0∈R with u(φ)=c(1+ecos⁡(φ−θ0))(φ∈W), and for t∈I∘ accordingly ρ(t)=p/(1+ecos⁡(θ(t)−θ0));
  2. the energy and the eccentricity are related by E=μκ22J2(e2−1); consequently E<0  ⟺  e<1, E=0  ⟺  e=1 and E>0  ⟺  e>1.

Facts & Assumptions

Given: The inverse-square central-force trajectory with constant angular momentum j=Je3, J>0, constant energy E, the solution u of Binet's equation on the interval W, and the constants c=μκ/J2, p=1/c.

[L1]

Binet's equation and the auxiliary identities: u′′+u=μκ/J2=c on W, W is an interval, and E=J22μ((u′)2+u2)−κu on W (Binet's equation for the attractive inverse-square field: d2u/dφ2+u=μκ/J2 for u=1/ρ).

[L2]

Solutions of v′′+v=0 on an interval with at least two points are Acos⁡(φ−φ0)+Bsin⁡(φ−φ0) for fixed φ0 in that interval (Solutions of v′′+ω2v=0 are exactly the functions Acos⁡(ω(t−t0))+Bsin⁡(ω(t−t0)), Intervals of R: the nine order-convex forms, nondegeneracy, and length).

[L3]

Subtraction formula: cos⁡(α−ψ)=cos⁡αcos⁡ψ+sin⁡αsin⁡ψ; (t↦(cos⁡t,sin⁡t)) is a bijection [0,2π)→S1; sin⁡2+cos⁡2=1 (The subtraction formulas for sine and cosine, t↦(cos⁡t,sin⁡t) is a bijection from [0,2π) onto the real unit circle, Parity and the Pythagorean identity for sine and cosine).

Proof

technique · direct
1.1L1L2algebra

Note u′′+u=c is equivalent to (u−c)′′+(u−c)=0 on W by linearity of the second derivative. Since W is an interval and Binet's equation holds on it (it contains at least two points because I∘ has at least two points), [L2] gives reals A,B with u(φ)−c=Acos⁡(φ−φ0)+Bsin⁡(φ−φ0)(φ∈W) for a fixed φ0∈W.

2.1step 1.1L3algebra

Put R:=A2+B2≥0. If R>0, then (A/R,B/R) is a unit vector, so by [L3] there is ψ∈[0,2π) with cos⁡ψ=A/R, sin⁡ψ=B/R; if R=0 take ψ:=0. Then for every φ, [L3] gives Acos⁡(φ−φ0)+Bsin⁡(φ−φ0)=Rcos⁡(φ−φ0−ψ). Setting θ0:=φ0+ψ and e:=R/c=R J2/(μκ)≥0, step 1.1 becomes u(φ)=c+e ccos⁡(φ−θ0)=c(1+ecos⁡(φ−θ0)) on W, which is the first assertion; the polar form ρ=p/(1+ecos⁡(θ−θ0)) follows by inverting u=1/ρ on I∘.

3.1step 2.1L1L4algebra

Energy: by [L1] and step 2.1, with ψ(φ):=φ−θ0, u=c(1+ecos⁡ψ) and u′=−cesin⁡ψ (differentiate with [L4]); hence (u′)2+u2=c2(e2sin⁡2ψ+1+2ecos⁡ψ+e2cos⁡2ψ)=c2(1+2ecos⁡ψ+e2), and κu=κc(1+ecos⁡ψ). Substituting into [L1]: E=J2c22μ(1+2ecos⁡ψ+e2)−κc (1+ecos⁡ψ). With c=μκ/J2 one has J2c22μ=μκ22J2 and κc=μκ2J2, so E=μκ22J2[(1+2ecos⁡ψ+e2)−2(1+ecos⁡ψ)]=μκ22J2(e2−1).

4.1step 3.1algebra∎

Classification: since μκ2/(2J2)>0, the sign of E equals the sign of e2−1; with e≥0 this is negative exactly for e<1, zero exactly for e=1 and positive exactly for e>1.

Depends on

Dependency tree · 2 levels

Sources