№ 40 · engineering

Why rockets drop stages

A rocket throws part of itself backwards to move forwards. One equation says how much speed that buys, and its shape is the reason every orbital rocket is built to fall apart on the way up.

What the equation says

A rocket engine pushes exhaust gas out of the back at some speed. Call that the exhaust speed, ve. The gain in the rocket's own speed, written Δv and said "delta-vee", depends on only two things: the exhaust speed, and the ratio of the rocket's mass with its tanks full to its mass with them empty.

Δv = ve · ln(mfull / mempty)

The "ln" is the natural logarithm. For this piece, all you need to know about it is that it grows very slowly: doubling the mass ratio adds the same fixed amount of Δv every time, whether you go from 2 to 4 or from 32 to 64. The result is named for Tsiolkovsky, and it is exact for a rocket in empty space with nothing pulling on it.

Why it forces the design

Read the equation backwards. To get twice the Δv you do not need twice the propellant. You need the mass ratio squared. Each extra kilometre per second costs a multiplied, not added, amount of fuel. NASA's worked example uses an engine with a specific impulse of 390 s, which is an exhaust speed of about 3.8 km/s. Reaching low Earth orbit takes an ideal Δv of 30,000 ft/s, about 9.1 km/s, once you add back what gravity, air drag and the climb itself steal on the way up. That demands a mass ratio of 11: about 91% of the rocket at lift-off has to be propellant.

Here is the wall. Tanks, engines and structure typically weigh 10 to 20% of the propellant they hold. NASA's single-stage rocket with 10% hardware and a mass ratio of 11 lifts off at 110,000 lb, burns 100,000 lb of propellant, and arrives in orbit weighing 10,000 lb: exactly its own hardware. There is nothing left over for a payload.

Interactive Set the exhaust speed and the propellant fraction of each stage, then switch between one stage and two; the same lift-off mass either reaches the orbit line or does not.

exhaust speed 3.8 km/s propellant fraction 88 %
The rocket equation and nothing else: Δv = ve · ln(mfull/mempty), summed over the stages that burn. Lift-off mass is the same in both designs, and the payload is fixed at 2 % of it. Propellant fraction is the share of each stage that is propellant; the rest is that stage's tanks, engine and structure, and it is carried until the stage is dropped. With two stages the split between them is chosen to give the most Δv; with identical engines that split is always about 86 % to 12 % of lift-off mass, so only the block heights change as you slide. The default exhaust speed, 3.8 km/s, is the 390 s specific impulse of NASA's worked example. The orbit line is the ideal Δv that example uses for a 100-mile orbit, 30,000 ft/s ≈ 9.1 km/s, which already includes an allowance for drag, the climb and gravity loss. The curves themselves are ideal: no gravity loss, no drag, no steering.

Dropping the tank resets the ratio

The fix is to notice what "empty mass" means. Halfway up, the rocket is hauling a big tank that is now hollow. Every bit of Δv still to come is being paid for against that dead weight, because it sits in mempty and shrinks the ratio.

So cut it loose. A stage is a self-contained engine-plus-tank that can be discarded. When the first stage runs dry you drop it, and the second stage starts as a brand new, much smaller rocket whose own tanks are full. Its mass ratio begins fresh. Two modest ratios multiplied together give a large one, but you never had to carry the first stage's hardware through the second burn.

In the interactive, the payload is fixed at 2% of the lift-off mass and both designs weigh the same on the pad. Slide the propellant fraction and watch: with one stage, the Δv curve crawls toward the orbit line and, at 3.8 km/s, only reaches it once each stage is about 93% propellant; with two stages the same total mass clears it from about 82%. Nothing about the engine changed. Only what the rocket is allowed to throw away.

In short

Speed gained is the exhaust speed times the logarithm of the full-to-empty mass ratio. Because the logarithm grows slowly, each extra bit of speed costs a multiplied amount of fuel, and a single tank runs into its own structural weight before it reaches orbit. Dropping an empty stage removes that dead weight from the ratio and lets the next stage start over. That is why rockets are stacked, and why they shed pieces on the way up.

Where this comes from

  1. Multistage Rocket Optimization, Geophysics, and the Spacefaring Envelope of Habitable Super-Earths reuse permitted with attribution
    Sanjoy M. Som · arXiv:2607.02691 · 2026
    arxiv.org/abs/2607.02691
  2. Ideal Rocket Equation — Beginner's Guide to Aeronautics linked only, not reproduced
    Nancy Hall (ed.), NASA Glenn Research Center · 2023
    www1.grc.nasa.gov/beginners-guide-to-aeronautics/ideal-rocket-equation/
  3. Exploring in Aerospace Rocketry, 11: Launch Vehicles (NASA TM X-52398) linked only, not reproduced
    Arthur V. Zimmerman · 1968
    ntrs.nasa.gov/citations/19680010821