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Space · interactive

How does SpinLaunch throw rockets into space?

Model · circular motion, a = v²/r

The chamber seen from above, with the spin slowed so you can follow it. Tap the chamber or press Release to let go; drag the arm’s tip in or out to change its length.

1 See

SpinLaunch doesn’t light a fire to leave the ground. It spins a projectile on an arm inside a vacuum chamber and lets go at thousands of miles an hour. So what does that spin do to the payload?

2 Change

3 Understand

The 36-second film · Watch with transcript
Watch the 36-second film
Model notes and sources

Model. A payload of mass m rides at the tip of an arm of radius r, moving at speed v. Holding it on the circle takes an inward acceleration a = v²/r; the g-load is a / 9.80665 m/s². The spin rate is v / (2πr) × 60 rpm, and the pull on the arm is F = m·v²/r, shown in tonnes-force. Each kilogram leaves with v²/2 of kinetic energy (2.2 MJ at 2.1 km/s). At the exit, the air load is the dynamic pressure q = ½ρv², with ρ = 1.07 kg/m³ (the US Standard Atmosphere at about 1.4 km, the height of Spaceport America), shown in atmospheres (101,325 Pa); Mach = v / 340 m/s. “Speed for orbit” compares the release speed with 7.8 km/s.

The planned machine. SpinLaunch says its orbital accelerator would release at up to 4,700 mph (2.1 km/s) inside a vacuum chamber about 100 m across, with payloads built for up to about 10,000 g; the projectile’s own rocket would ignite at about 60 km and supply the rest of the speed. SpinLaunch has not published the arm’s length, so the 46 m arm here is our assumption (it fits inside a 100 m chamber). With it, the model gives about 9,780 g, 436 rpm and a pull of about 1,960 tonnes-force on a 200 kg payload, about 4.4 times the 447.7 t maximum takeoff weight of a Boeing 747-8. Half the speed gives a quarter of the g-load (about 2,440 g). Keeping a 2.1 km/s throw at 1,000 g would take an arm about 450 m long; at 100 g, about 4.5 km. The air at the exit presses about 23 atm on the nose at Mach 6.2.

The marks on the g-meter. Fighter pilots: about 9 g sustained, with a g-suit and straining. Washing machine: our example of a 1,400 rpm spin cycle on a drum of 25 cm radius (36.7 m/s), which gives 549 g. SpinLaunch: its stated 10,000 g. HARP gun: the 16-inch gun of the 1960s High Altitude Research Project fired at 2,164 m/s with up to 15,000 g at launch, about the same speed as SpinLaunch’s planned release.

Limits. The g-load is the steady load at full speed; the push along the circle while spinning up is small by comparison. The model ignores the arm’s own mass (which the arm must also hold against the spin), the counterweight, the time spent in the tube, the slowing and heating as the projectile climbs through the air, and the extra speed the rocket must make up for drag and gravity. The pressure right at a blunt nose is higher than q. The drawing is rescaled to fit, and the spin is shown slowed down by the factor on the stage.

Why it’s hard. The g-force grows with the square of the speed and falls only in proportion to the arm’s length, so a fast throw on a short arm is brutal: electronics can be hardened like artillery parts, but people can’t ride it. And all of that speed meets the thick air near the ground at once.

The pictures. Everything on the stage is drawn in code from the model. In the film, the opening shot (a projectile bursting through the launch tube’s membrane) and one picture-in-picture insert (the 33 m test machine, then a launch) are short excerpts of SpinLaunch test-flight video, picture only and credited on screen. Between them, the same test machine at Spaceport America, New Mexico, is drawn at dawn in slow motion, and the release is shown in slow motion where the stage says so. SpinLaunch flew 10 test flights from this machine from October 2021 (the first at 20% power) to September 2022, reaching about 30,000 ft; Flight Test 10 carried payloads from NASA, Airbus US, Cornell and Outpost. In September 2026 its planned Meridian satellite constellation split from SpinLaunch.

Neal Stephenson. On Core Memory, Neal Stephenson recalled the Slingatron, a spiral-track accelerator from the 1990s: “it’s a big gun, basically.” And “all big gun systems have got problems … around what happens when you meet the atmosphere.”

Sources: SpinLaunch (Wikipedia: 33 m test machine, test flights, 4,700 mph, 10,000 g, ignition near 60 km, payload mass, Meridian); Keeptrack, SpinLaunch deep dive (100 m chamber, 200–400 kg payloads); Meridian Space, Meridian splits from SpinLaunch; Space.com, Slingatron (Derek Tidman); Wikipedia, G-force (pilots sustain about 9 g); Wikipedia, Martlet 2 (the HARP 16-inch gun: 2,164 m/s, 15,000 g); Wikipedia, Boeing 747-8 (987,000 lb, 447.7 t maximum takeoff weight); Wikipedia, Spaceport America (elevation 1,401 m); US Standard Atmosphere; Neal Stephenson with Ashlee Vance, Core Memory episode 94 (chapter at 1:13:43) and the episode page.

An ExplainerTools Original. Concept from Neal Stephenson’s conversation with Ashlee Vance on Core Memory (episode 94, October 2026).

Behind the film

Concepts in this film

The ideas the film moves through, with this model’s numbers, the research behind each one and where else it comes up.

All concepts, A to Z

Centripetal acceleration

Anything moving in a circle is always turning toward the centre, and that takes an inward acceleration a = v²/r. Speed counts twice: double it and the pull quadruples. The radius counts once: double the arm and the pull only halves. On the tool’s assumed 46 m arm, SpinLaunch’s planned 2.1 km/s release takes about 96,000 m/s², at 436 rpm; at half the speed it takes a quarter as much.

Related research OpenStax University Physics, 4.4 Uniform and Nonuniform Circular MotionSpinLaunch (Wikipedia)

See also Space Gun Lab: the same speed-squared law in a straight barrelNewton’s Cannon: gravity supplies the same pull for an orbitWays to space: the sling

G-force

A g-load compares an acceleration with gravity’s 9.81 m/s². At 2.1 km/s on the 46 m arm the payload feels about 9,780 g, so a 1 kg part presses on its mount like a 9.8-tonne weight. Fighter pilots sustain about 9 g in g-suits; a washing machine’s 1,400 rpm spin reaches 549 g. The arm feels it too: holding a 200 kg payload takes about 1,960 tonnes-force, about 4.4 fully loaded Boeing 747-8s.

Related research G-force (Wikipedia)SpinLaunch (Wikipedia)

See also Space Gun Lab: 6,000 g down to a few hundredWays to space: Could people ride SpinLaunch or a space gun?Journal: Why the speed hurts so much

Vacuum chamber

SpinLaunch spins its projectile inside a sealed chamber with the air pumped out. In air, a projectile at 2.1 km/s would meet about 23 atmospheres of pressure on its nose on every lap, and drag would brake and heat it, and the arm, long before release. With the air gone, the spin-up meets almost none. A membrane seals the end of the launch tube, and the projectile bursts through it on the way out: that is the film’s opening shot.

Related research SpinLaunch (Wikipedia)Keeptrack, SpinLaunch deep dive

See also Journal: Then the airWays to space: the sling

Dynamic pressure

Dynamic pressure, q = ½ρv², is the push of the air on something moving through it. The model uses air at 1.07 kg/m³, the density about 1.4 km up, where Spaceport America sits: at 2.1 km/s that is about 2.4 million pascals, 23 atmospheres, on the nose. The Mach number compares the speed with sound’s: 2,100 ÷ 340 m/s is Mach 6.2. Inside the chamber there was no air; at the exit all of it arrives at once, in the thickest air of the climb.

Related research NASA Glenn, Dynamic PressureMach number (Wikipedia)

See also Space Gun Lab: 340 atmospheres at Mach 22Tall Tower Launch: max QSonic Boom Lab: what Mach 1 and above look like

Hardened electronics

Electronics can be built to survive a hard shove. In the Second World War, proximity fuzes rode anti-aircraft shells through up to 20,000 g, their tiny radio valves packed in wax and oil to spread the stress. In the 1960s, Project HARP test-fired guidance and control parts to about 10,000 g. SpinLaunch says its payloads are built for about 10,000 g. People are another matter: nobody can ride this throw.

Related research Proximity fuze (Wikipedia)Martlet 2 (Wikipedia)

See also Space Gun Lab: what rugged satellites can takeJournal: Then the airWays to space: the gun

Slingatron

The Slingatron is an older way to throw a payload without a long arm. A spiral track is shaken around in small, fast circles (gyrated), and a projectile sliding along the spiral gains speed on every turn. Derek Tidman conceived it in late 1994; a 2013 demonstrator was meant to gyrate 40 to 60 times a second and throw a quarter-pound payload at 1 km/s. Stephenson remembered it on Core Memory: “it’s a big gun, basically.”

Related research Space.com, SlingatronPhys.org, Slingatron vision: payloads to orbit (2013)

See also Journal: The slingWays to space: the sling

Learn more

More ways to space

A sling is one of four launch ideas Neal Stephenson talked through on Core Memory. The guide compares all four, and the other three films are here.

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About this tool

How does SpinLaunch throw rockets into space?

Spin a payload on a 46 m arm to 4,700 mph, then let go. See why the g-force grows with the square of the speed, and what the air does at Mach 6.

Subject
Engineering
Topics
SpinLaunch · rockets · centripetal force · g-force · kinetic launch
Published
In the catalog
How does SpinLaunch throw rockets into space?

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