Engine Lab

The Ideal Rocket

Engines · Rocket · Demo

Pick a real engine, load a stage with propellant, and burn it — then watch one logarithm decide whether you reach orbit.

dry 26%prop 74%t = 0 s / 166 sa = 1.7 m/s² (0.17 g)246810km/s0%25%50%75%95%propellant burned, share of pad massorbit ≈ 9.4 km/s (incl. losses)needs 96% →Δv = ve · ln(m₀/m) — ve = 2.98 km/sburnout 4.0 km/s

Real engines

Saturn V (5 engines) · RP-1 / LOX, gas generator. Five F-1s lifted the 2 900 t Saturn V with a liftoff TWR of about 1.2 — the biggest single-chamber engine ever flown, burning 2.6 t of kerosene and oxygen per second each.

Burn

The on-screen burn is compressed; the physics clock next to the rocket runs at the stage's real burn time. Scrub the slider to inspect any instant.

Readout

Flies, but falls short of orbitIdeal Δv 4.0 km/s is 43% of the orbit budget. One stage at this Isp needs 95.7% propellant — which is exactly why real launchers stage.
Thrust at liftoff33.25 MN
Effective Isp263 s SL → 304 s vac
T/W liftoff → burnout1.175.2
Burn time166 s
Masses (pad / prop / dry)2,900 t / 2,146 t / 754 t
Ideal Δv (Tsiolkovsky)4.02 km/s
vs orbit budget (~9.4)43%
Δv if propellant ×2only +41%

That last row is the tyranny in one number: doubling the propellant at the same dry mass never doubles Δv, because the logarithm pays out less for every tonne you add — and the new tonnes must themselves be accelerated. The escape from the log is not more fuel; it is throwing empty tanks away.

In plain terms

propellantpayloadthrow mass left ← · → get pushed right
A rocket is mostly tank: it throws mass one way to go the other, and gets lighter — and quicker — as it burns.

A rocket is the only machine that carries everything it pushes against. It throws its own propellant backwards at enormous speed, and momentum conservation shoves the vehicle forwards. That simple trade has a cruel bookkeeping rule — the rocket equation — which says speed is bought with exponentially more propellant. This demo runs the honest numbers for four real engines.

More detail

How it works

It only pushes against itself

No air, no road, no water — thrust is pure momentum exchange: F = ṁ·ve, mass flow times exhaust velocity. That is why rockets work in vacuum, and why every gram thrown backwards matters twice: once as push, once as weight you no longer carry.

Two numbers rule the mission

Tsiolkovsky’s equation, Δv = ve·ln(m0/m1), says the speed a stage can gain depends only on its exhaust velocity and its full-to-empty mass ratio. Not on thrust, not on burn time, not on size. Everything else in rocketry is a fight to improve one of those two numbers.

The logarithm is a tyrant

Because the mass ratio sits inside a logarithm, doubling the propellant never doubles Δv — the extra tanks full of fuel must themselves be accelerated. Reaching orbital speed on one kerosene stage demands a vehicle that is ~95% propellant, which is why rockets stage.

Thrust for the pad, Isp for the mission

Δv does not care about thrust — but gravity does. A rocket must out-lift its own weight (T/W > 1) or it simply sits there burning. Hydrogen engines have superb Isp but modest thrust; that is why hydrolox stacks so often leave the pad strapped to solid boosters.

Key numbers

Δv to low orbit, incl. losses≈ 9.4 km/s
Best flown chemical IspRS-25 — 452 s vacuum
F-1 sea-level thrust6.8 MN per engine
Falcon 9 propellant share≈ 94% of pad mass
Saturn V liftoff T/W≈ 1.2