Systems with Varying Mass: A Rocket — Question 1

Section 9-11 · Physics pages 1352–1353

Question 1 Deriving thrust from a short momentum balance An ideal rocket moves along +x. At an instant its mass is m and velocity is v. In time dt it expels positive mass dµ backward at speed u relative to the rocket. External force is zero; ignore terms of second order. +x exhaust m(t) Ideal one-dimensional rocket; exhaust is directed backward relative to the rocket. (a) Derive the rocket acceleration and thrust in terms of q = dµ/dt > 0. (b) Explain why setting d(mv)/dt = 0 for the rocket alone fails even though the full system is isolated.
Show solutionHide solution
Question 1 - Solution Deriving thrust from a short momentum balance +x exhaust m(t) (a) Derivation and calculation Follow the fixed collection consisting of the rocket and the newly expelled mass. To first order, mv = (m −dµ)(v + dv) + dµ(v −u). 0 = m dv −u dµ + O(dµ dv) ⇒m˙v = uq , T = uq , q = dµ dt > 0. (b) Result and interpretation The remaining rocket has ˙m = −q, hence d(mv) dt = m˙v + v ˙m = uq −vq = q(u −v) . Its momentum is not generally constant because exhaust crosses its boundary. Conservation applies to the fixed isolated collection of rocket plus all exhaust. Physical check Thrust points forward even when the exhaust still moves forward in the laboratory.

Question 1

Deriving thrust from a short momentum balance

An ideal rocket moves along +x+x. At an instant its mass is mm and velocity is vv. In time dtdt it expels positive mass dμd\mu backward at speed uu relative to the rocket. External force is zero; ignore terms of second order.

Diagram shown in the original SVG worksheet.

  1. Derive the rocket acceleration and thrust in terms of q=dμ/dt>0q=d\mu/dt>0.

  2. Explain why setting d(mv)/dt=0d(mv)/dt=0 for the rocket alone fails even though the full system is isolated.

Question 1 - Solution

Deriving thrust from a short momentum balance

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Follow the fixed collection consisting of the rocket and the newly expelled mass. To first order, mv=(m−dμ)(v+dv)+dμ(v−u).mv=(m-d\mu)(v+dv)+d\mu(v-u). 0=mdv−udμ+O(dμdv)⇒mv̇=uq,T=uq,q=dμdt>0.0=m\,dv-u\,d\mu+O(d\mu\,dv)\Rightarrow\boxed{m\dot v=uq},\qquad\boxed{T=uq},\quad q=\frac{d\mu}{dt}>0.

(b) Result and interpretation

The remaining rocket has ṁ=−q\dot m=-q, hence d(mv)dt=mv̇+vṁ=uq−vq=q(u−v).\frac{d(mv)}{dt}=m\dot v+v\dot m=uq-vq=\boxed{q(u-v)}. Its momentum is not generally constant because exhaust crosses its boundary. Conservation applies to the fixed isolated collection of rocket plus all exhaust.

Physical check

Thrust points forward even when the exhaust still moves forward in the laboratory.