Systems with Varying Mass: A Rocket — Question 9

Section 9-11 · Physics pages 1368–1369

Question 9 A varying exhaust speed belongs inside the mass integral A force-free rocket burns from m0 to m0/2. Its relative exhaust speed depends on remaining mass as u(m) = u0(m/m0) with fixed backward direction. m/m0 u/u0 1/2 1 1/2 1 Exhaust-speed law over the burn interval; time runs from larger to smaller remaining mass. (a) Find the exact velocity gain. (b) Compare with assuming constant exhaust speed u0 and with using the arithmetic mean of the initial and final exhaust speeds in the logarithmic formula.
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Question 9 - Solution A varying exhaust speed belongs inside the mass integral m/m0 u/u0 1/2 1 1/2 1 (a) Derivation and calculation The mass-dependent exhaust speed remains inside the integral: ∆v = ∫m0 m0/2 u(m) m dm = u0 m0 ∫m0 m0/2 dm. ∆v = u0/2 . (b) Result and interpretation The two proposed substitutions give ∆vconst = u0 ln 2 = 0.6931u0, ∆vmean = 0.75u0 ln 2 = 0.5199u0. Both exceed the exact 0.5000u0. The correct effective exhaust speed is weighted by dm/m: ueff= ∫u(m) dm/m ln 2 = u0 2 ln 2. Physical check The exhaust speed falls from u0 to u0/2 during the burn.

Question 9

A varying exhaust speed belongs inside the mass integral

A force-free rocket burns from m0m_0 to m0/2m_0/2. Its relative exhaust speed depends on remaining mass as u(m)=u0(m/m0)u(m)=u_0(m/m_0) with fixed backward direction.

Diagram shown in the original SVG worksheet.

  1. Find the exact velocity gain.

  2. Compare with assuming constant exhaust speed u0u_0 and with using the arithmetic mean of the initial and final exhaust speeds in the logarithmic formula.

Question 9 - Solution

A varying exhaust speed belongs inside the mass integral

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The mass-dependent exhaust speed remains inside the integral: Δv=∫m0/2m0u(m)mdm=u0m0∫m0/2m0dm.\Delta v=\int_{m_0/2}^{m_0}\frac{u(m)}m\,dm=\frac{u_0}{m_0}\int_{m_0/2}^{m_0}dm. Δv=u0/2.\boxed{\Delta v=u_0/2}.

(b) Result and interpretation

The two proposed substitutions give Δvconst=u0ln⁡2=0.6931u0,Δvmean=0.75u0ln⁡2=0.5199u0.\Delta v_{\mathrm{const}}=u_0\ln2=0.6931u_0,\qquad\Delta v_{\mathrm{mean}}=0.75u_0\ln2=0.5199u_0. Both exceed the exact 0.5000u00.5000u_0. The correct effective exhaust speed is weighted by dm/mdm/m: ueff=∫u(m)dm/mln⁡2=u02ln⁡2.u_{\mathrm{eff}}=\frac{\int u(m)\,dm/m}{\ln2}=\frac{u_0}{2\ln2}.

Physical check

The exhaust speed falls from u0u_0 to u0/2u_0/2 during the burn.