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The Saturn V Burned 15 Tons of Fuel Per Second
On July 16, 1969, the Saturn V rocket that carried Apollo 11 to the Moon consumed roughly 15 metric tons of kerosene and liquid oxygen every second during its first stage burn. Five F-1 engines generated a combined 35,100 kilonewtons (7.89 million pounds-force) of thrust -- enough to lift a fully loaded vehicle weighing 2,970 tons off the launch pad. Nothing built since has matched that raw power, though SpaceX's Starship is designed to surpass it.
Thrust is the force that pushes an aircraft or rocket forward. It is not horsepower, though people often conflate the two. Understanding the difference -- and why engineers measure propulsion in newtons and pounds-force rather than horsepower -- explains a lot about how flight actually works.
Thrust vs. Horsepower: They Measure Different Things
Horsepower measures the rate of doing work. One horsepower equals 745.7 watts, or enough power to lift 550 pounds one foot per second. Your car engine is rated in horsepower because it describes acceleration capability.
Thrust measures force, period. A jet engine producing 10,000 pounds-force of thrust exerts that same push whether the airplane is sitting still on the runway or cruising at 600 mph. The relationship between them is:
Power = Thrust x Velocity
A fighter jet producing 20,000 lbf at 500 mph delivers about 26,800 horsepower. The same engine at rest on the tarmac -- same thrust -- delivers zero horsepower because velocity is zero. That is why rockets and jets are rated in thrust, not horsepower. Their useful power output changes constantly with speed, but the thrust stays roughly constant.
Use our kg to newtons converter for quick force unit translations.
Units of Thrust
Newtons (N)
The SI unit. One newton accelerates a one-kilogram mass at one meter per second squared. In everyday terms, an apple in your hand exerts about one newton of gravitational force. Aerospace companies outside the US report thrust in newtons or kilonewtons.
Pounds-Force (lbf)
The imperial unit, dominant in American aerospace. One pound-force is the gravitational pull on a one-pound mass at sea level. The FAA and most US military specifications use lbf.
Kilonewtons (kN)
For the enormous forces involved in jet and rocket propulsion, kilonewtons (1,000 N) keep the numbers manageable. A typical commercial jet engine produces 100-500 kN of thrust.
Conversions: 1 kN = 224.8 lbf = 1,000 N. For speed conversions when calculating performance, try our mph to kph converter.
How Jet Engines Make Thrust
A jet engine is a continuous-cycle air pump. It sucks in air, squeezes it, heats it, and blasts it out the back faster than it came in. Newton's Third Law does the rest.
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Intake: Air enters through the front. At subsonic speeds the inlet is a simple duct; at supersonic speeds, a shaped inlet slows the air to subsonic before it reaches the compressor.
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Compression: Spinning fan blades squeeze the air to 20-40 times atmospheric pressure. This compression also heats the air substantially.
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Combustion: Fuel sprays into the compressed air and ignites. Temperatures hit 1,400-2,000 degrees Celsius.
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Turbine: The hot gas expands through a turbine that extracts just enough energy to drive the compressor. The rest goes out the back.
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Exhaust: Gas exits at 1,500-2,000 mph, and the reaction to that rearward acceleration is thrust.
Modern commercial jets use turbofan engines where a large front fan pushes most air around the core rather than through it. This bypass air generates the majority of thrust while cutting noise and improving fuel efficiency. Bypass ratios range from 5:1 on older engines to 12:1 on the Rolls-Royce UltraFan.
Military fighters use turbojets or low-bypass turbofans, often with afterburners that inject extra fuel into the exhaust stream. Afterburners boost thrust by 50% or more but guzzle fuel -- they are reserved for takeoff, combat maneuvering, and supersonic dash.
How Rocket Engines Make Thrust
Rockets carry both fuel and oxidizer, which is why they work in the vacuum of space where there is no air to breathe.
The process is conceptually simpler than a jet engine: propellants flow into a combustion chamber, burn at extreme temperatures (often above 3,000 degrees C), and expand through a bell-shaped nozzle that accelerates them to 2,500-4,500 m/s. That is 5,600-10,000 mph of exhaust velocity.
Liquid rockets (SpaceX Merlin, RS-25 Space Shuttle engines) store fuel and oxidizer in separate tanks. They can throttle, shut down, and restart. Common propellant combinations:
- RP-1 kerosene + liquid oxygen (Falcon 9)
- Liquid hydrogen + liquid oxygen (SLS, Ariane)
- Methane + liquid oxygen (Starship Raptor)
Solid rockets (Space Shuttle SRBs, many missile boosters) mix fuel and oxidizer into a solid grain. Once ignited, they cannot be throttled or stopped. They are simpler, cheaper, and produce massive thrust, which makes them useful as strap-on boosters.
Famous Thrust Numbers
| Vehicle | Engine Type | Total Thrust | Thrust-to-Weight |
|---|---|---|---|
| Boeing 747 (4 engines) | Turbofan | 1,000 kN (225,000 lbf) | ~0.27 |
| F-22 Raptor (2 engines) | Turbofan + afterburner | 312 kN (70,000 lbf) | ~1.08 |
| Space Shuttle (launch) | Liquid + Solid | 30,580 kN (6.87M lbf) | ~1.5 |
| Falcon 9 (first stage) | 9x Merlin liquid | 7,607 kN (1.71M lbf) | ~1.3 |
| Saturn V (first stage) | 5x F-1 liquid | 35,100 kN (7.89M lbf) | ~1.2 |
The F-22's thrust-to-weight ratio exceeding 1.0 means it can point straight up and accelerate. A Boeing 747 at 0.27 cannot -- it relies on wings to generate lift. A rocket must exceed 1.0 at launch or it simply sits on the pad.
Thrust-to-Weight Ratio
This is the single most important performance number for any flying machine:
TWR = Thrust / Weight
- TWR < 1: Cannot lift off vertically. Commercial aircraft (TWR 0.25-0.35) need wings and runways.
- TWR = 1: Hovers. Impractical for real flight -- no margin for climbing.
- TWR > 1: Can accelerate straight up. Required for rockets and achieved by many fighter jets.
A rocket's TWR changes dramatically during flight. As propellant burns off, the vehicle gets lighter while thrust stays roughly constant. A Falcon 9 launches at TWR 1.3 but might reach 3.0 before stage separation. That is why rockets throttle back during "Max Q" -- the period of maximum aerodynamic stress -- to avoid tearing themselves apart.
Ion Engines: Tiny Thrust, Huge Patience
Not all propulsion is about brute force. Ion engines produce millinewtons of thrust -- roughly the force of a sheet of paper resting in your palm. But they do it for months or years at a time, using electrical energy to accelerate xenon ions to 30-50 km/s exhaust velocity (compared to 3-4 km/s for chemical rockets).
NASA's Dawn spacecraft used ion propulsion to visit both asteroid Vesta and dwarf planet Ceres on a single mission. The total velocity change (delta-v) exceeded what any chemical rocket of the same mass could have achieved. Ion engines are useless for launch -- TWR is laughably below 1 -- but unmatched for deep space missions where time is cheap and fuel is scarce.
Key Takeaways
Thrust measures force, not power. A jet engine's useful power depends on speed, but its thrust stays roughly constant. Jet engines compress and heat atmospheric air; rocket engines carry their own oxidizer. TWR above 1.0 enables vertical climb; below 1.0 requires wings. The Saturn V remains the most powerful rocket ever flown, though Starship aims to change that. And ion engines prove that sometimes the smallest push, sustained long enough, outperforms the biggest explosion.
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