Gravitation Potential Energy — Question 2

Section 13-5 · Physics pages 1974–1975

Question 2 A subescape radial launch has a finite turning radius A particle is launched radially outward from radius R with speed .8vesc, where vesc = √ 2GM/R. Neglect atmosphere and source recoil. R v0 = .8vesc rmax Radial launch from the surface; the turning radius is schematic and to be determined. (a) Find its maximum radius and maximum altitude. (b) Explain why setting final potential to zero would be incorrect for this launch.
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Question 2 - Solution A subescape radial launch has a finite turning radius R v0 = .8vesc rmax (a) Derivation and calculation Let v0 = .8 √ 2GM/R. The conserved specific energy is ϵ = v2 0 2 −GM R = (.64 −1)GM R = −.36GM R . At a radial turning point v = 0: −GM rmax = −.36GM R , rmax = 25R 9 , hmax = 16R 9 . (b) Result and interpretation At infinity the potential is zero, which would require v2 ∞ 2 = ϵ = −.36GM R < 0. This is impossible for a real speed. Instead, at the finite turning point, Kmax r = 0, Umax r = E = −.36GMm R . Negative potential energy must be retained. Physical check For a general subescape factor k < 1, rmax = R/(1 −k2); it diverges as k →1−.

Question 2

A subescape radial launch has a finite turning radius

A particle is launched radially outward from radius RR with speed .8vesc.8v_{esc}, where vesc=2GM/Rv_{esc}=\sqrt{2GM/R}. Neglect atmosphere and source recoil.

Diagram shown in the original SVG worksheet.

  1. Find its maximum radius and maximum altitude.

  2. Explain why setting final potential to zero would be incorrect for this launch.

Question 2 - Solution

A subescape radial launch has a finite turning radius

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Let v0=.82GM/Rv_0=.8\sqrt{2GM/R}. The conserved specific energy is ϵ=v022−GMR=(.64−1)GMR=−.36GMR.\epsilon=\frac{v_0^2}{2}-\frac{GM}{R}=(.64-1)\frac{GM}{R}=-.36\frac{GM}{R}. At a radial turning point v=0v=0: −GMrmax=−.36GMR,rmax=25R9,hmax=16R9.-\frac{GM}{r_{\max}}=-.36\frac{GM}{R},\qquad \boxed{r_{\max}=\frac{25R}{9}},\quad\boxed{h_{\max}=\frac{16R}{9}}.

(b) Result and interpretation

At infinity the potential is zero, which would require v∞22=ϵ=−.36GMR<0.\frac{v_\infty^2}{2}=\epsilon=-.36\frac{GM}{R}<0. This is impossible for a real speed. Instead, at the finite turning point, Kmax⁡r=0,Umax⁡r=E=−.36GMmR.K_{\max r}=0,\qquad U_{\max r}=E=-.36\frac{GMm}{R}. Negative potential energy must be retained.

Physical check

For a general subescape factor k<1k<1, rmax=R/(1−k2)r_{\max}=R/(1-k^2); it diverges as k→1−k\to1^-.