Satellites: Orbits and Energy — Question 8

Section 13-7 · Physics pages 2026–2027

Question 8 Slow orbital energy loss can lead to a higher eventual circular speed A satellite evolves slowly between nearly circular orbits under weak drag. Its initial kinetic energy is K0 and initial radius r0. The net orbital energy removed is .01K0. Compare circular endpoints; do not treat the entire change as one instantaneous impulse. r0 rf Weak drag leads to a smaller nearly circular orbit; the radius difference is exaggerated. (a) Find the final circular radius and speed relative to their initial values. (b) Explain why this does not mean the drag force accelerates the satellite forward.
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Question 8 - Solution Slow orbital energy loss can lead to a higher eventual circular speed r0 rf (a) Derivation and calculation For circular endpoints, E0 = −K0. Removing .01K0 gives Ef = E0 −.01K0 = −1.01K0. Since E = −µm/(2r), rf/r0 = 1/1.01 ≃.990099 , vf/v0 = √ r0/rf = √ 1.01 ≃1.00499 . (b) Result and interpretation The final circular kinetic and potential energies are Kf = 1.01K0, Uf = −2.02K0. Hence ∆K = +.01K0, ∆U = −.02K0, ∆E = −.01K0. Drag does negative work directly. During orbital contraction, the larger decrease in potential energy allows a higher eventual circular speed. Physical check This compares settled nearly circular states; it does not claim that the immediate drag acceleration points forward.

Question 8

Slow orbital energy loss can lead to a higher eventual circular speed

A satellite evolves slowly between nearly circular orbits under weak drag. Its initial kinetic energy is K0K_0 and initial radius r0r_0. The net orbital energy removed is .01K0.01K_0. Compare circular endpoints; do not treat the entire change as one instantaneous impulse.

Diagram shown in the original SVG worksheet.

  1. Find the final circular radius and speed relative to their initial values.

  2. Explain why this does not mean the drag force accelerates the satellite forward.

Question 8 - Solution

Slow orbital energy loss can lead to a higher eventual circular speed

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For circular endpoints, E0=−K0E_0=-K_0. Removing .01K0.01K_0 gives Ef=E0−.01K0=−1.01K0.E_f=E_0-.01K_0=-1.01K_0. Since E=−μm/(2r)E=-\mu m/(2r), rf/r0=1/1.01≃.990099,\boxed{r_f/r_0=1/1.01\simeq.990099}, vf/v0=r0/rf=1.01≃1.00499.\boxed{v_f/v_0=\sqrt{r_0/r_f}=\sqrt{1.01}\simeq1.00499}.

(b) Result and interpretation

The final circular kinetic and potential energies are Kf=1.01K0,Uf=−2.02K0.K_f=1.01K_0,\qquad U_f=-2.02K_0. Hence ΔK=+.01K0,ΔU=−.02K0,ΔE=−.01K0.\Delta K=+.01K_0,\quad\Delta U=-.02K_0,\quad \Delta E=-.01K_0. Drag does negative work directly. During orbital contraction, the larger decrease in potential energy allows a higher eventual circular speed.

Physical check

This compares settled nearly circular states; it does not claim that the immediate drag acceleration points forward.