Formula & Calculator
Turbojet Thrust Equation
General thrust equation for an airbreathing jet engine including momentum and pressure-imbalance terms.
Interpretation
Turbojet thrust: F = ṁ·(V_e − V_0) + A_e·(p_e − p_0), where ṁ is mass flow, V_e exit velocity, V_0 flight speed, A_e exit area, p_e exit pressure, p_0 ambient. It is the general thrust equation. Example: ṁ=50 kg/s, V_e=400 m/s, V_0=250 m/s, p_e=1 atm, p_0=0.5 atm, A_e=0.3 m² → F = 50×150 + 0.3×(101325−50662.5) = 7500 + 15199 ≈ 22,699 N.
Variables
| Symbol | Quantity | Unit |
|---|---|---|
| F | Net thrust | N |
| mdot | Mass flow rate | kg/s |
| V_e | Exhaust velocity | m/s |
| V_0 | Freestream velocity | m/s |
| A_e | Exit area | m2 |
| p_e | Exit static pressure | Pa |
| p_0 | Ambient pressure | Pa |
What it means
The turbojet thrust equation is similar to the rocket equation but accounts for the incoming air momentum. It shows that thrust is produced by the change in momentum of the airflow plus the pressure thrust at the nozzle exit. For a jet engine, the mass flow includes air and fuel. This equation is used to calculate thrust for given engine conditions and flight speed. It is fundamental for engine performance analysis and for sizing the engine for a given aircraft. Understanding this equation is essential for propulsion engineers.
Worked example
Turbojet Thrust – Two Examples
Real‑World| Parameter | Value |
|---|---|
| ṁ | 50 kg/s |
| V_e | 600 m/s |
| V₀ | 230 m/s |
| Parameter | Value |
|---|---|
| ṁ | 80 |
| V_e | 650 |
| V₀ | 250 |
| A_e | 0.6 |
| p_e-p₀ | 175 |
Common mistakes
- Turbojet thrust equation: F = ṁ·(V_e − V₀) + A_e·(p_e − p₀).
- ṁ: Mass flow rate (kg/s).
- V_e: Exit velocity (m/s).
- V₀: Freestream velocity (m/s).
- A_e: Exit area (m²).
- p_e: Exit pressure (Pa).
- p₀: Ambient pressure (Pa).
- If nozzle is perfectly expanded, pressure term is zero.
Applications
The turbojet thrust equation, F = ṁ·(V_e − V_0) + A_e·(p_e − p_0), is the general thrust expression for a turbojet, accounting for momentum and pressure thrust. It is used to design and evaluate turbojet engines, to size nozzles, and to compute thrust at different flight conditions. Engineers use this to integrate the engine with the airframe, to assess installation effects, and to predict performance. By applying this equation, aerospace engineers can optimise engine design for specific mission profiles, achieving the required thrust with minimal fuel consumption.
- Turbojet engine design and performance prediction
- Nozzle sizing and expansion ratio optimisation
- Engine‑airframe integration and installation losses
- Thrust measurement and validation in test cells
- Performance analysis of gas turbine engines
Frequently Asked Questions
It is the general thrust equation for an airbreathing jet engine including momentum and pressure‑imbalance terms.
ṁ = mass flow rate through the engine (kg/s)
Ve = exhaust velocity (m/s)
V0 = freestream velocity (m/s)
Ae = nozzle exit area (m²)
pe = static pressure at exit (Pa)
p0 = ambient pressure (Pa)
It accounts for the thrust contribution from the difference between exit and ambient pressures. For an ideally expanded nozzle (pe=p0), it is zero.
- Dropping the pressure‑imbalance term entirely; it is small but not always negligible, especially for underexpanded nozzles.
- Using the wrong mass flow (e.g., core flow only vs. total flow).
- Confusing exit velocity with effective exhaust velocity.
ṁ = 50 kg/s, Ve = 600 m/s, V0 = 200 m/s, Ae = 0.5 m², pe = 1.1 atm, p0 = 1 atm. F = 50×(600−200) + (1.1−1)×101325×0.5 = 50×400 + 0.1×50662.5 = 20000 + 5066.25 = 25066.25 N.
As V0 increases, the momentum term decreases, reducing net thrust (for a fixed mass flow and exhaust velocity).
Afterburning increases Ve (by adding heat) and often increases mass flow, boosting thrust significantly, but at the cost of increased TSFC.
A higher pressure ratio (pc/p0) increases Ve and the pressure term, increasing thrust.
The ideal equation often neglects the pressure term and assumes fully expanded flow.
Exhaust velocity is difficult to measure directly; it is usually inferred from thrust and mass flow measurements.