3.3.8Rocket Propulsion

Effective exhaust velocity c = v_e + (P_e − P_a)A_e - ṁ

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WHAT is cc?


HOW: Derive thrust from first principles

Step 1 — Momentum thrust (Newton's 2nd/3rd law). Take the rocket as our system. In time dtdt it ejects mass dm=m˙dtdm = \dot m\, dt backward at speed vev_e (relative to rocket).

Why this step? Force = rate of change of momentum. The gas gains rearward momentum, so by reaction the rocket gains equal forward momentum.

Fmom=dpgasdt=vedmdt=m˙veF_{\text{mom}} = \frac{d p_{\text{gas}}}{dt} = \frac{v_e\,dm}{dt} = \dot m\, v_e

Step 2 — Pressure thrust (a force balance on the gas at exit). Consider the exit plane, area AeA_e. Inside the exit the gas pushes outward with pressure PeP_e; outside, ambient air pushes inward with PaP_a.

Why this step? Pressure is force per unit area. Over the exit ring the net outward push is (PePa)(P_e - P_a) acting on AeA_e. This force is not cancelled by anything (there's no wall there), so it becomes thrust.

Fpres=(PePa)AeF_{\text{pres}} = (P_e - P_a)\,A_e

Step 3 — Add them.

F=m˙vemomentum+(PePa)AepressureF = \underbrace{\dot m\, v_e}_{\text{momentum}} + \underbrace{(P_e - P_a)A_e}_{\text{pressure}}

Step 4 — Absorb everything into one velocity cc. We define cc so that F=m˙cF = \dot m\, c. Divide the whole thing by m˙\dot m:

c=Fm˙=ve+(PePa)Aem˙c = \frac{F}{\dot m} = v_e + \frac{(P_e - P_a)A_e}{\dot m}

Why bother? Because now every rocket equation (F=m˙cF=\dot m c, Isp=c/g0I_{sp}=c/g_0, Tsiolkovsky Δv=cln(m0/mf)\Delta v = c\ln(m_0/m_f)) uses ONE number.

Figure — Effective exhaust velocity c = v_e + (P_e − P_a)A_e - ṁ

Special cases (Forecast-then-Verify)


Common mistakes


Active Recall

Recall Quick self-test (hide and answer)
  • Why does a rocket produce pressure thrust?
  • When is c=vec = v_e exactly?
  • Does cc go up or down as the rocket climbs? Why?
  • What is the sign of the correction if Pe<PaP_e < P_a, and what is that condition called?
Recall Feynman: explain to a 12-year-old

Imagine blowing up a balloon and letting it go. The air rushing out backward shoves the balloon forward — that's the "speedy gas" push. Now imagine the balloon's mouth is a bit narrow so the air inside is still squeezed harder than the room's air right at the opening — that extra squeeze also shoves the balloon a little more. A rocket has both pushes. Instead of tracking two shoves, scientists pretend the gas came out at ONE make-believe speed, cc, that gives the exact same total push. High up in space there's no room-air pushing back, so the make-believe speed gets bigger and the rocket pushes harder!


Flashcards

Define effective exhaust velocity cc.
The single equivalent speed satisfying F=m˙cF=\dot m c, including momentum and pressure thrust: c=ve+(PePa)Ae/m˙c = v_e + (P_e-P_a)A_e/\dot m.
Write the full thrust equation before defining cc.
F=m˙ve+(PePa)AeF = \dot m v_e + (P_e - P_a)A_e.
When does c=vec = v_e?
When the nozzle is optimally expanded, i.e. Pe=PaP_e = P_a (pressure term vanishes).
Sign of the pressure term when underexpanded (Pe>PaP_e>P_a)?
Positive → c>vec>v_e (extra thrust).
Sign when overexpanded (Pe<PaP_e<P_a)?
Negative → c<vec<v_e (thrust penalty, risk of flow separation).
Why does cc increase with altitude for the same engine?
Because PaP_a decreases, making PaAe/m˙-P_aA_e/\dot m less negative; the exit pressure's push is opposed less by ambient air.
Where does pressure thrust physically come from?
The net outward force (PePa)(P_e-P_a) acting over the exit area AeA_e, which has no wall to cancel it.
Relation between cc and specific impulse?
Isp=c/g0I_{sp} = c/g_0, so c=Ispg0c = I_{sp}\,g_0.
Given cc, how do you recover raw exit velocity vev_e?
ve=c(PePa)Ae/m˙v_e = c - (P_e-P_a)A_e/\dot m.

Connections

  • Thrust Equation — this note's parent; F=m˙ve+(PePa)AeF=\dot m v_e + (P_e-P_a)A_e.
  • Specific ImpulseIsp=c/g0I_{sp}=c/g_0; effective velocity in disguise.
  • Tsiolkovsky Rocket Equation — uses cc: Δv=cln(m0/mf)\Delta v = c\ln(m_0/m_f).
  • Nozzle Expansion (Under/Over/Optimal) — sets the sign of the pressure term.
  • Conservation of Momentum — origin of momentum thrust.
  • Atmospheric Pressure vs Altitude — why cc varies during ascent.

Concept Map

equals

equals

Newton 2nd/3rd law

net push on exit ring

divide by m-dot

definition

P_e = P_a

P_e greater than P_a

P_e less than P_a

used in

Total thrust F

Momentum thrust m-dot times v_e

Pressure thrust P_e minus P_a times A_e

Gas ejected at v_e

Exit area A_e

Effective exhaust velocity c

F = m-dot times c

Optimal: c = v_e

Underexpanded: c > v_e

Overexpanded: c < v_e

I_sp and Tsiolkovsky delta-v

Hinglish (regional understanding)

Intuition Hinglish mein samjho

Dekho, rocket ko do tarah se thrust milta hai. Pehla hai momentum thrust — gas peeche ki taraf tez speed vev_e pe nikalti hai, aur Newton ke third law se rocket ko aage dhakka milta hai, jiska maan m˙ve\dot m v_e hota hai. Doosra hai pressure thrust — nozzle ke exit pe gas ka pressure PeP_e aur bahar ki hawa ka pressure PaP_a same nahi hote. Is difference (PePa)(P_e - P_a) ko exit area AeA_e se multiply karo, aur wo bhi ek real force banta hai jo thrust me add hota hai.

In dono ko alag-alag track karna jhanjhat hai, isliye scientists ne ek smart trick nikali: ek "as if" velocity define kar di jise effective exhaust velocity cc kehte hain, taaki thrust simply F=m˙cF = \dot m c ban jaye. Formula hai c=ve+(PePa)Ae/m˙c = v_e + (P_e - P_a)A_e/\dot m. Jab nozzle perfect ho (Pe=PaP_e = P_a), tab pressure term zero, aur c=vec = v_e.

Sabse important baat: jaise-jaise rocket upar jaata hai, bahar ka PaP_a kam hota jaata hai (space me toh zero). Isliye PaAe/m˙-P_a A_e/\dot m wala penalty kam ho jaata hai aur cc badh jaata hai. Yahi wajah hai ki same engine ka vacuum IspI_{sp} sea-level se zyada hota hai. Exam me galti mat karna — cc aur vev_e ko blindly barabar mat maano, pehle check karo ki Pe=PaP_e = P_a hai ya nahi.

Go deeper — visual, from zero

Test yourself — Rocket Propulsion

Connections