Satellites: Orbits and Energy — Question 6

Section 13-7 · Physics pages 2022–2023

Question 6 A two-burn transfer must match the outer circular speed at arrival A coplanar transfer from a circular orbit of radius r to one of radius 4r uses an ellipse tangent to both, with two prograde burns. Let v0 = √ µ/r. Use v2 = µ(2/rlocal −1/a) and T = 2π √ a3/µ. Transfer ellipse shares a focus with both circles and touches their opposite sides. (a) Find both burn magnitudes in units of v0. (b) Find the transfer time in units of the initial circular period T0.
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Question 6 - Solution A two-burn transfer must match the outer circular speed at arrival (a) Derivation and calculation The transfer ellipse has at = r + 4r 2 = 5r 2 . Vis-viva at its two apsides gives v2 t,p v2 0 = 2 −2 5 = 8 5, v2 t,a v2 0 = 2 4 −2 5 = 1 10. Since vc,out = v0/2, ∆v1 v0 = √ 8/5 −1 ≃.264911 , ∆v2 v0 = 1 2 − 1 √ 10 ≃.183772 . (b) Result and interpretation The transfer takes half the elliptic period: t = π √ a3 t /µ, T0 = 2π √ r3/µ. t/T0 = 1 2(at/r)3/2 = 1 2(5/2)3/2 = 1.97642 . At arrival vt,a < vc,out, so a second prograde burn is required. Physical check Transfer angular momentum gives rvt,p = 4rvt,a, confirming both apsis speeds.

Question 6

A two-burn transfer must match the outer circular speed at arrival

A coplanar transfer from a circular orbit of radius rr to one of radius 4r4r uses an ellipse tangent to both, with two prograde burns. Let v0=μ/rv_0=\sqrt{\mu/r}. Use v2=μ(2/rlocal−1/a)v^2=\mu(2/r_{local}-1/a) and T=2πa3/μT=2\pi\sqrt{a^3/\mu}.

Diagram shown in the original SVG worksheet.

  1. Find both burn magnitudes in units of v0v_0.

  2. Find the transfer time in units of the initial circular period T0T_0.

Question 6 - Solution

A two-burn transfer must match the outer circular speed at arrival

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The transfer ellipse has at=r+4r2=5r2.a_t=\frac{r+4r}{2}=\frac{5r}{2}. Vis-viva at its two apsides gives vt,p2v02=2−25=85,vt,a2v02=24−25=110.\frac{v_{t,p}^2}{v_0^2}=2-\frac25=\frac85,\qquad \frac{v_{t,a}^2}{v_0^2}=\frac24-\frac25=\frac1{10}. Since vc,out=v0/2v_{c,\mathrm{out}}=v_0/2, Δv1v0=8/5−1≃.264911,\boxed{\frac{\Delta v_1}{v_0}=\sqrt{8/5}-1\simeq.264911}, Δv2v0=12−110≃.183772.\boxed{\frac{\Delta v_2}{v_0}=\frac12-\frac1{\sqrt{10}}\simeq.183772}.

(b) Result and interpretation

The transfer takes half the elliptic period: t=πat3/μ,T0=2πr3/μ.t=\pi\sqrt{a_t^3/\mu},\qquad T_0=2\pi\sqrt{r^3/\mu}. t/T0=12(at/r)3/2=12(5/2)3/2=1.97642.\boxed{t/T_0=\tfrac12(a_t/r)^{3/2} =\tfrac12(5/2)^{3/2}=1.97642}. At arrival vt,a<vc,outv_{t,a}<v_{c,\mathrm{out}}, so a second prograde burn is required.

Physical check

Transfer angular momentum gives rvt,p=4rvt,arv_{t,p}=4rv_{t,a}, confirming both apsis speeds.