Systems with Varying Mass: A Rocket — Question 4

Section 9-11 · Physics pages 1358–1359

Question 4 Gravity loss depends on how long the engine burns A rocket already free of its launch support burns vertically upward from rest in uniform gravity g = 9.8 m/s2. Its mass falls from 1000 to 800 kg in 20 s at a constant rate. Relative exhaust speed is u = 2000 m/s; ignore air resistance. rocket T = uq mg 20 s: q = 10 kg/s 40 s: q = 5 kg/s Thrust opposes weight; longer burns accumulate a larger gravitational velocity loss. (a) Find initial acceleration and burnout velocity. (b) Compare with a 40 s burn using the same mass endpoints and exhaust speed. Check that both initially accelerate upward.
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Question 4 - Solution Gravity loss depends on how long the engine burns rocket T = uq mg 20 s: q = 10 kg/s 40 s: q = 5 kg/s (a) Derivation and calculation For the 20 s burn, q = (1000 −800)/20 = 10 kg/s: ai = uq mi −g = 20 −9.8 = 10.2 m/s2 . Integrating ˙v = uq/(mi −qt) −g gives vf = u ln(mi/mf) −gtb = 2000 ln 1.25 −196 = 250.29 m/s . (b) Result and interpretation For 40 s, q = 5 kg/s and ai = 10 −9.8 = 0.20 m/s2 > 0, vf = 2000 ln 1.25 −392 = 54.29 m/s . Both initially accelerate upward. The slower burn loses an additional g(40 −20) = 196 m/s to gravity. Physical check The ideal propulsive term is unchanged because the mass endpoints are identical.

Question 4

Gravity loss depends on how long the engine burns

A rocket already free of its launch support burns vertically upward from rest in uniform gravity g=9.8m/s2g=9.8\,\mathrm{m/s^2}. Its mass falls from 10001000 to 800kg800\,\mathrm{kg} in 20s20\,\mathrm s at a constant rate. Relative exhaust speed is u=2000m/su=2000\,\mathrm{m/s}; ignore air resistance.

Diagram shown in the original SVG worksheet.

  1. Find initial acceleration and burnout velocity.

  2. Compare with a 40s40\,\mathrm s burn using the same mass endpoints and exhaust speed. Check that both initially accelerate upward.

Question 4 - Solution

Gravity loss depends on how long the engine burns

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For the 20 s burn, q=(1000−800)/20=10q=(1000-800)/20=10 kg/s: ai=uqmi−g=20−9.8=10.2m/s2.\boxed{a_i=\frac{uq}{m_i}-g=20-9.8=10.2\ \mathrm{m/s^2}}. Integrating v̇=uq/(mi−qt)−g\dot v=uq/(m_i-qt)-g gives vf=uln⁡(mi/mf)−gtb=2000ln⁡1.25−196=250.29m/s.\boxed{v_f=u\ln(m_i/m_f)-gt_b=2000\ln1.25-196=250.29\ \mathrm{m/s}}.

(b) Result and interpretation

For 40 s, q=5q=5 kg/s and ai=10−9.8=0.20m/s2>0,a_i=10-9.8=0.20\ \mathrm{m/s^2}>0, vf=2000ln⁡1.25−392=54.29m/s.\boxed{v_f=2000\ln1.25-392=54.29\ \mathrm{m/s}}. Both initially accelerate upward. The slower burn loses an additional g(40−20)=196g(40-20)=196 m/s to gravity.

Physical check

The ideal propulsive term is unchanged because the mass endpoints are identical.