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How do you fly faster than sound without a sonic boom?

Model · simplified shock merging, not a CFD result

The jet flies right, high above a town (not to scale). Glowing lines are its shock waves; the house flashes at each one it meets. Top left: the pressure a person on the ground feels. Drag the jet's nose to stretch it.

1 See

An ordinary supersonic jet hits the ground with a sharp double boom. NASA's X-59 flies just as fast, but it is shaped so that people below should hear only a soft thump. How do you fly faster than sound without a sonic boom?

2 Change

3 Understand

The 45-second film · Watch with transcript
Watch the 45-second film
Model notes and sources

Model. A supersonic jet pushes the air aside, and every place where its cross-section or its lift grows (nose, canopy, inlet, wings, tail) starts a pressure wave. In G. B. Whitham's theory the jet is summed up by its F-function, F(y) = (1/2π) ∫ A″(ξ) / √(y − ξ) dξ, where A is the equivalent area: the jet's cross-section plus a lift term β W / (2q), with β = √(M² − 1), weight W and dynamic pressure q. Far below, the overpressure is Δp / pv = γ M² F(y) / √(2βr) (γ = 1.4, pv the air pressure at the jet). Each point of the wave travels a little faster the stronger it is: its position shifts by k F(y) S, with k = (γ + 1) M⁴ / √(2β³). In uniform air the age S would be √r; in the standard atmosphere (ISA: 6.5 K per km to 11 km, isothermal above) it is S = ∫ Z (pv/p) d√r with Z = √(ρc / ρvcv), which grows ever more slowly as the wave goes down into denser air. Where faster parts overtake slower ones, shocks form; the tool places them exactly with the equal-area rule, done as a lower convex hull (the Lax–Oleinik solution). At the ground the amplitude is multiplied by Z and by 1.9 for the reflection.

Why ordinary jets boom twice. The shocks from the front of the jet have stronger air behind them, so they catch up with the ones ahead and merge into a single bow shock; at the back the same happens to the tail shocks. What reaches the ground is an N-wave: a sudden jump up, a steady fall, and a sudden jump back, heard as “boom-boom”. The basics of the Mach cone and the boom carpet are in our Sonic Boom Lab.

The two shapes. Both weigh 24,000 lb (assumed; Lockheed Martin gives the X-59's take-off weight as about 25,000 lb, other sources up to about 32,300 lb). The ordinary jet is 19.5 m long; its equivalent area is built from its parts (a 3.5 m pointed nose, a bubble canopy, a belly inlet, a wing carrying all the lift, the tail) and its F-function computed from that. At Mach 1.4 and 55,000 ft the model gives it an N-wave of about 0.8 psf that lasts about 135 ms (Carlson's simplified method gives a similar size for a jet like this). The X-59 end is 30.4 m long (the X-59 is 99.7 ft, almost a third of it nose). Its F-function is a designed low-boom one, as NASA's designers worked backwards from a target signature: five small steps (nose, canard, canopy, wing, engine) on a gentle ramp, spaced so they cannot catch up before the ground at the design point, then a slow expansion and recovery at the back. The engine on top matters because the wing shields the ground from its inlet's shock; the long nose spreads the front compression over a longer distance. In between the two ends the tool smooths the ordinary jet's F-function and blends it into the X-59's. The lift part of the X-59's F-function scales with speed and altitude.

Loudness. NASA rates booms in perceived level, PLdB (Stevens' Mark VII). This tool uses a simpler stand-in: the A-weighted sound exposure of the modelled ground signature, with each shock's rise time set to 1 ms × (1 psf / jump), as weak shocks are thicker. A constant is added so the X-59 shape at Mach 1.4 and 55,000 ft reads 75 PLdB, NASA's target. The ordinary jet then reads about 92, and the X-59 shape's pressure takes about 15 ms to build instead of about 1 ms. NASA gives Concorde's boom as about 105 PLdB; Concorde was more than ten times heavier (about 185 t at take-off) and two to three times as long as these jets, so the Mach 2 preset is only its speed.

Mach cutoff. If the jet moves over the ground slower than sound travels in the warm air at the ground (about 340 m/s), its shock waves bend back up before they land and no boom reaches the ground. The tool applies this for still air in the standard atmosphere, below about Mach 1.15 at 55,000 ft.

Limits. The vertical scale is squeezed (the ground is 17 km below a 30 m jet), and the spread of the shocks is squeezed with depth so the picture fits. The model ignores refraction other than the cutoff, wind, turbulence (which roughens real shocks), atmospheric absorption, the jet's exhaust plume and three-dimensional flow near the jet; the X-59's real shape was designed with CFD and wind-tunnel tests. Numbers from the model are approximate; the 75 and 105 PLdB figures are NASA's.

The X-59. NASA and Lockheed Martin Skunk Works built the X-59 for NASA's Quesst mission. It first flew on 28 October 2025, went supersonic in June 2026 and reached Mach 1.53 (about 1,010 mph) in September 2026, NASA says. Its long nose blocks the view ahead, so the pilot sees forward through a camera and screen, the eXternal Vision System. A year after its first flight, after more than 40 flights, it flew across the country via El Paso and Fort Worth to Kennedy Space Center. Next, NASA plans acoustic tests and then flights over US communities to ask people what they hear. Civil supersonic flight over US land has been banned since 1973 (14 CFR 91.817); in July 2026 the FAA proposed replacing the ban with a limit of 0.11 psf on the boom's pressure at the ground; the rule is not final.

The pictures. Everything on the stage is drawn in code from the model. The film also shows three short pieces of real footage, picture only, each credited on screen: the X-59 landing at Naval Air Station Joint Reserve Base Fort Worth on 28 October 2026 and taking off from there the next day, filmed by spotter @LensOfMae (take-off), shown whole with her watermark; and NASA's AirBOS schlieren image of two T-38s flying supersonic, their shock waves made visible (NASA Armstrong, YouTube, 2019), cropped to leave out NASA's caption. The T-38s are ordinary jets, not the X-59. The Concorde in the film is drawn in code.

Sources: NASA, How is the X-59 designed to quiet the boom?; NASA, Low-Boom Flight Demonstrator lithograph (99.7 ft, Mach 1.4, 55,000 ft, shock waves kept apart); NASA, NASA awards contract to build quieter supersonic aircraft (2018: 75 PLdB, “as loud as a car door closing”); NASA Armstrong, Sonic boom heads for a thump (Concorde 105 PLdB); NASA Quesst blog, X-59 completes record six flights in one week (Mach 1.53); AIN, X-59 heads to Florida as NASA marks first-flight anniversary (30 Oct 2026); S. Doebler and colleagues (NASA), X-59 sonic boom simulation and case study (75 PL design, reflection factor 1.9); G. B. Whitham, The flow pattern of a supersonic projectile (1952); H. W. Carlson, Simplified sonic-boom prediction (NASA TP-1122, 1978; used to check the N-wave's size); DLA Piper, Proposed FAA rule would allow civil supersonic flight (the 1973 ban and the July 2026 proposal); The Engineer, NASA and Lockheed Martin unveil quiet supersonic aircraft (2024: nose almost a third of its length, engine on top); Wikipedia, Sonic boom and International Standard Atmosphere.

An ExplainerTools Original. After NASA's X-59 and its Quesst mission (NASA and Lockheed Martin Skunk Works). Model after G. B. Whitham's theory of supersonic flow (1952).

Learn more

Learn more about quiet supersonic flight

The X-59 still makes shock waves; its shape keeps them apart. The guide explains what PLdB and psf mean, how the nose and engine help, where the X-59 has flown, and where this model stops.

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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

N-wave

Heard from the ground, an ordinary supersonic jet’s boom is an N-wave: the pressure jumps up at the bow shock, falls steadily below normal, then jumps back at the tail shock, so the ear hears two bangs, “boom-boom”. Each jump takes only about a millisecond, which is what makes it sound so sharp. In the tool, the ordinary jet at Mach 1.4 and 55,000 ft lands an N-wave whose first jump is about 0.8 psf (pounds per square foot: about 38 pascals, or 1/2,700 of the air’s pressure) and whose two bangs come about 135 ms apart, close to what NASA’s simplified Carlson method gives for a jet that size.

Related research H. W. Carlson, Simplified sonic-boom prediction (NASA TP-1122, 1978)Sonic boom (Wikipedia)

See also Sonic Boom Lab: the Mach cone and the boom carpetJournal: What makes a sonic boom?Whip Crack Lab: a sonic boom you can hold

Shock merging

A pressure wave doesn’t keep its shape over a long trip: where the air is squeezed harder it is slightly hotter and already moving forward, so that part runs a little faster and catches up with the weaker part ahead. Where it overtakes, a shock forms, and a stronger shock behind swallows a weaker one in front. G. B. Whitham’s 1952 theory, which the tool uses, follows every part of the wave down from the jet; over the 17 km below 55,000 ft, an ordinary jet’s shocks from nose, canopy, inlet, wings and tail have time to pile into two. The denser air near the ground slows this down, so a shape designed to keep its shocks apart can land with them still apart.

Related research G. B. Whitham, The flow pattern of a supersonic projectile (Communications on Pure and Applied Mathematics, 1952)NASA, How is the X-59 designed to quiet the boom?

See also Sonic Boom Lab: where the shock waves come fromSound by Bartosz Ciechanowski: how pressure waves travel through air

Low-boom design

What reaches the ground is set by how a jet’s cross-section and its lift grow along its length, which Whitham’s theory sums up as one curve, the equivalent area (lift counts because holding up the weight pushes air down). The X-59’s designers worked backward from the soft signature they wanted to a 99.7 ft (30.4 m) jet with a long, slender nose and its engine on top, so that each part’s small shock lands separately. In the tool that shape at Mach 1.4 and 55,000 ft lands five small steps, the biggest only 0.074 psf against the ordinary jet’s 0.79 psf at the same weight, and its pressure builds over about 15 ms instead of about 1. The long nose blocks the view ahead, so the pilot looks forward through cameras and a screen, NASA’s eXternal Vision System.

Related research NASA, How is the X-59 designed to quiet the boom?Lockheed Martin, X-59 media kit

See also Airfoil by Bartosz Ciechanowski: how a wing makes liftSonic Boom Lab: the ordinary boom it avoids

Perceived level (PLdB)

Two booms with the same peak pressure can sound very different: a sudden jump carries more of the higher frequencies the ear is most sensitive to, so it sounds louder than a gradual rise. NASA rates booms in perceived level, PLdB, a loudness scale for short sounds based on S. S. Stevens’ Mark VII method. By NASA’s figures Concorde’s boom was about 105 PLdB and the X-59 aims for about 75, “about as loud as a car door closing”, 30 dB less. The tool uses a simpler stand-in, calibrated so the X-59 shape reads 75 at its design point; the ordinary jet then reads about 92.

Related research NASA Armstrong, Sonic boom heads for a thumpNASA, NASA awards contract to build quieter supersonic aircraft (2018)

See also Sound Extinguisher Lab: what a decibel measuresSound by Bartosz Ciechanowski: what a sound wave is

Mach cutoff

Sound travels faster in warm air, so a boom heading down from the cold air at cruise height bends as it reaches the warmer air near the ground. If the jet moves over the ground slower than sound travels down there, about 340 m/s on a standard 15 °C day, its shock waves bend back up before they land and no boom reaches the ground. At 55,000 ft, where the standard air is −56.5 °C and sound travels about 295 m/s, that means flying below about Mach 1.15 in still air, where the tool’s “Just past Mach 1” preset sits. Wind and real temperatures move the threshold; NASA measured it in flight tests flown between about Mach 1.13 and 1.17.

Related research Cliatt, Hill & Haering (NASA Armstrong), Mach cutoff analysis and results from NASA’s Farfield Investigation of No-boom ThresholdsInternational Standard Atmosphere (Wikipedia)

See also Thunder Timer: sound is faster in warm airSonic Boom Lab: booms that never reach the groundTwinkle Lab: warm and cool air bend light too

Schlieren photography

Air is invisible, but where its density changes it bends light slightly, and schlieren methods photograph that bending, so a shock wave, a thin sheet of suddenly denser air, shows up as a sharp line. NASA’s AirBOS flights did it from a King Air flying around 30,000 ft, filming two supersonic T-38s about 30 ft apart from roughly 2,000 ft away at 1,400 frames a second and measuring how the ground behind them seemed to ripple. The 2019 images, seen in the film, show the two jets’ shocks bending where they meet; NASA built the system partly to check the X-59’s shocks in flight.

Related research NASA Armstrong, NASA captures first air-to-air images of supersonic shockwave interaction in flight (2019)Schlieren photography (Wikipedia)

See also Whip Crack Lab: the shadowgraph, schlieren’s simpler cousinTwinkle Lab: pockets of warm air bend starlight

About this tool

How do you fly faster than sound without a sonic boom?

Stretch a supersonic jet’s nose and watch its shock waves stop merging on the way down: the sharp double boom becomes a soft thump.

Subject
Science
Topics
supersonic flight · sonic booms · shock waves · NASA · aircraft design
Published
In the catalog
How do you fly faster than sound without a sonic boom?

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