Boom Prize / Research
Research thread / 7 queries / Boom Prize

Five seconds past Mach 1on air alone.

A 25 kg aircraft, no rockets, level flight through the transonic wall. This is what the literature says actually gets you there, and what it says does not.

Real mesh: KJ66 assembly by Akash Jangid, Turbo3D, MIT
25 kgMax takeoff weight, fuel and gear included
5 sContinuous supersonic, each flight
M 1.02Indicated margin for uncertainty
2 flightsOne day, reciprocal headings
0 rocketsAir-breathing thrust only
$750,000Cash, plus $50,000 in Boom stock

The short version

The thread opened on a turbojet-boosted ramjet that hands off below Mach 1. The evidence pulled it somewhere plainer: a bought micro turbojet, a short augmentation burst, and an airframe shaped around transonic drag. The hard part is not the engine. It is keeping thrust margin from Mach 0.8 to 1.1.

Source: Consensus.app thread "Turbojet Boosted Ramjet Propulsion"Cited papers linked inlineReal 3D meshes, credited below
01Query 1

The rules are
the design brief.

A qualifying attempt is two flights by the same aircraft between sunrise and sunset of one day, watched by the judges. The prize goes to the first verified attempt. Every rule below removes a shortcut.

SpeedMach 1.0+ for 5 continuous seconds

True airspeed above the local speed of sound, on each of the two flights. The supersonic legs must be flown on reciprocal headings, 180 degrees plus or minus 10.

Mass25 kg

55 lb max takeoff weight, including fuel and landing gear. Only fuel may be shed in flight.

AccelerationNo dives

Mach 0.8 to past Mach 1 in level or climbing flight. Altitude may not drop more than 10 m below the highest point since that phase began.

ReuseFly it again

Controlled landing, wheels or belly, then fly again the same day. Refuel, recharge, minor repairs only. No new wings, fuselage, engine or flight computer.

ProofM 1.02 indicated

Calibrated pitot-static plus total air temperature, sealed loggers, GPS, ground weather data, and the raw files. The margin covers measurement uncertainty.

AirframeFixed wing, mostly home-built

Lift from aerodynamic surfaces. The team must build the majority of the airframe, in the spirit of FAA amateur-built rules (14 CFR 21.191(g)). Bought engines, servos and avionics are fine and do not count against that majority. Kits and target-drone derivatives are out.

ControlHuman in the loop

Autopilot is allowed, but a remote pilot keeps command authority and an immediate abort on every flight.

TurbojetTurbofanRamjetPulsejetElectric ducted fanAny combination RocketsOnboard oxidizerStored high-pressure gas or steamSolid propellantGliders and dynamic soaring

Liquid fuel only, with gaseous hydrogen and nitromethane allowed as exceptions. Open to U.S. persons; minors need a parent or guardian co-signature. No venture capital, sponsors or grants; personal funds and no-equity crowdfunding are fine. Contest runs until it is awarded or December 31, 2030. This is the summary pasted into the thread; the binding text is at boomsupersonic.com/prize.

02Query 4

Two loopholes,
closed by email.

The question, Oct 15

  • Can an external ground launcher release the aircraft below Mach 0.8, with everything after that done on air-breathing thrust? The ideas were a motorcycle engine or something like SpinLaunch.
  • Can a pressurized CO2 cold-gas thruster handle attitude control during takeoff?
The aircraft must take off under its own power, so an external ground launcher is not permitted. ... Thrust from stored high pressure gas is prohibited, as is any non air-breathing thrust at any point in flight.

Boom Supersonic Prize Team reply, Oct 16, as quoted in the thread.

So the aircraft has to get itself off the ground and through Mach 0.8 to 1 on its own engine. Cold gas is out even for attitude control. That leaves the fixed-wing micro turbojet path from Query 3 as the strongest option.

03Query 1

Why the ramjet
idea broke.

The first answer proposed a turbojet that hands off to a ramjet around Mach 0.6 to 0.8. The papers put every real ramjet handoff far to the right of the contest window. Plot them on one axis and the problem is obvious.

Boom window Where the evidence sits Original claim, not supported Risk band
Mach ladderMach number ranges for propulsion evidence compared with the Boom Prize window of Mach 0.8 to 1.1.
Ramjets need compression.A review of ramjet compression systems says they are inoperable when velocity is too low for adequate compression, identified there as below about Mach 2. Ramjet work in the later corpus starts operation around Mach 2.5. Veeran 2018
TBCC switches late.Modeled turbine-to-ramjet transitions sit at Mach 2.5 to 3.2, and controlling the thrust gap is hard even there. Reviews describe turbojet-to-ramjet transition at Mach 3 to 4. Liu 2024Lv 2022Urzay 2018
Even detonation does not reach down.A hydrogen detonation ramjet showed positive effective thrust starting around Mach 1.3. Better than a plain ramjet, still already supersonic. Ivanov 2021
04Query 1

Five ways to make thrust,
ranked by evidence.

Ranked for a Boom-scale aircraft, by how much small-scale testing backs each one, not by how exciting it sounds.

01

Turbojet + afterburner or duct burner

Most plausible

Small-engine augmentation is directly studied. Variable nozzles and short-burst thrust gains fit a 5 second requirement. Apke 2012Shea 2024

02

Turbojet + ejector nozzle

Helper, not the answer

Compact, no moving parts, but the gain falls off strongly with airspeed. Mostly a takeoff and low-speed benefit. Schmidt 2021

03

Turbojet + ramjet (TBCC)

Long shot, distinctive

Mature as a concept, but the evidence centers on Mach 2.5+ transition, not a subsonic or transonic handoff. Liu 2024Lv 2022

04

Pulsejet / ram-pulsejet

Too risky for Mach 1

Simple and light, with low efficiency and poor thrust density. No paper here shows a practical small supersonic aircraft on one. Piancastelli 2018Geng 2007

05

Air-breathing detonation

Unique but premature

Promising thrust in rigs and wind tunnels. Nothing yet closes the gap to repeatable small-aircraft supersonic flight. Frolov 2019Meng 2022Ivanov 2021

05Queries 1, 6, 7

Inside the engine
you should buy.

A real, open KJ66 micro turbojet model. The thread describes the JetCat P140 class as representative of the sub-500 N, KJ66-derived architecture. Chachurski 2024 Each marker ties a part to what the research says about it.

Drag to orbit / pinch or wheel to zoom
Loading mesh
    06Queries 1, 5, 7

    The short-burst
    augmentation stack.

    Keep the turbine core and add thrust only where the drag rise needs it. These are the add-ons with real test or design work behind them, and what each one costs you.

    Afterburner + variable nozzle50%thrust increase targeted on a 200 N-class mini turbojet

    A Colorado mini-turbojet project paired an afterburner with a variable-area convergent nozzle to run wet and dry efficiently. A related concept paired afterburning with nozzle control for a Mach 1.4 class vehicle. Apke 2012Walter 2012 Modular afterburners for JetCat-class engines are an active design topic. Shea 2024

    Cost: thermal and pressure-loss management. The thread supports its plausibility more than a verified micro-engine gain number.

    Afterburner diffuser<5%pressure loss in optimized micro-afterburner layouts

    Reshaping the tail cone and using 2.5 degree struts reduced swirl while keeping diffuser pressure loss under 5%. Lee 2025

    Cost: this is a subsystem result, not a flight result.

    Nozzle ejector2.5 to 6.1%measured thrust gain on a JetCat P80, high-load regimes

    SFC dropped about 2.5 to 5.5% in the same tests. Silivestru 2025

    Cost: benefit drops significantly with airspeed, so it helps takeoff and early climb, not the final push. Schmidt 2021

    Compact combustor~30%shorter combustor, up to 12% better thrust-to-weight

    Gear-shaped high-g combustor work on micro turbojets keeps combustion performance at the same thrust while shortening the chamber. Huang 2024

    Cost: integration maturity is still low.

    Pulse detonation add-on180 to 200 Nground-tested air-breathing thrust modules

    Real, ground-tested hardware. Frolov 2019

    Cost: integration and sensitivity to pressure losses.

    07Query 7

    Which turbine
    to actually buy.

    Published thrust for commercial engines that have test or modeling data behind them. The P300 class is the smallest with substantial experimental and CFD-validated support for serious transonic UAV work. Rhee 2020bLee 2023Lee 2024

    JetCat P80 class78 to 87 N measured max
    Too small for the safest path Ezgin 2025Vouros 2025
    JetCat P140 classabout 140 N
    Prototype scale only Chachurski 2024
    JetCat P300-RX / PRO257 to 300 N
    Best documented minimum Rhee 2020bLee 2023
    JetCat / AMT / PBSroughly 400 N up to 1.1 kN
    More margin, less open data Catană 2024Prisăcariu 2026
    0 N2755508251100 N

    Recommendation

    A P300-class engine is the floor. A P400-class or PBS TJ100 / TJ150-class engine is more likely to keep transonic thrust margin if the airframe stays under 25 kg. Rhee 2020bCatană 2024Prisăcariu 2026

    The reason is margin. The small-supersonic studies keep naming insufficient transonic thrust margin as the central risk. Mizobata 2016Dalman 2021Minato 2005 JetCat is the best documented brand in this set; PBS is described as especially mature for UAV integration. Prisăcariu 2026Catană 2024 Catalog thrust is not enough to size from: secondary air, lubrication fuel and off-design effects change thrust, SFC and temperatures, so pair test-stand data with a model. Aksoy 2026Vouros 2025Wu 2023Zhang 2025

    08Queries 1, 3, 5, 7

    The airframe matters
    more than the engine.

    The most repeated lesson across small supersonic test programs: getting supersonic depends on transonic drag reduction. Exotic combustion does not fix a draggy shape.

    • 5 to 20%Drag reduction from area-rule shaping in Mach 0.8 to 1.2 analyses of Muroran's small supersonic testbed. Mizobata 2016
    • 57 countsDrag cut at Mach 1.1 from a sharpened conical nose and a large-radius bottleneck. Mizobata 2024
    • CancelledThe area-rule benefit on some configurations, once an intake was added. Design the inlet with the fuselage from the start. Mizobata 2024Mizobata 2025
    • 61 to 66°Sweep of the cranked-arrow wing with a 6% diamond section used on the Muroran flight-test vehicles. Mizobata 2025Mizobata 2024
    • 0.5 to 0.85%Supersonic drag penalty for enforcing low-speed stability in RANS-based optimization. Worth paying, because it has to take off and land. Seraj 2025
    • 13.41 kgSmallest feasible supersonic UAV in one conceptual design framework. No feasible vehicles hit Mach 1.1 at 6 km. Aim for the mid-teens to low 20s. Dalman 2021

    What that means for the shape

    One slender fixed-wing airframe built only for this mission: small thin wing, high sweep, a waisted fuselage around the wing, and no VTOL requirement. Jacob 2021Mizobata 2005Mizobata 2014 The engine install is a primary design task, so inlet and exhaust nozzle are redesigned around the engine instead of bolted on. Compton 2021Hutchinson 2021

    Control risk lives in the subsonic and transonic range. Directional stability degrades at large angles of attack and sideslip, elevon roll inputs can cause adverse yaw, and roll reversal can appear without coordinated rudder. Mizobata 2016Mizobata 2025 That is why groups fly subsonic prototypes first and check them against 6-DOF or point-mass predictions. García 2024Mizobata 2011aMizobata 2011b

    For design tools, VLM stays useful for fast iteration while full CFD handles the harder supersonic features. Joshi 2023García 2024Jacob 2021

    Drag to orbit / pinch or wheel to zoom
    Loading mesh
      09Queries 2, 3

      The detour:
      a 590 km/h quadcopter.

      The SQ-2 speed quad brief was the starting design. It is a serious build, and it is limited by the wrong physics for Mach 1. Patel 2026

      590km/h predicted top speed
      657.6km/h official record; the brief puts SQ-2 about 10% short of it
      <3%estimated chance of clearing the practical ~700 km/h bar
      1.67×useful power per unit drag area needed for 700 vs 590 km/h
      Drag to orbit / pinch or wheel to zoom
      Loading mesh

        What is actually limiting it

        At 590 km/h the advance ratio is about J = 2.2 and the blade sections are near zero lift, so thrust only comes back if rpm keeps climbing. The binding limits are high-advance-ratio propeller thrust, drag area, and motor thermal margin. A 900 KV motor swap was already rejected on energy and thermal grounds, and aggressive rewinding did not fix the system. Patel 2026

        Hall-effect and ion thrusters are not an option. They produce mN to N of thrust, carry their own propellant, need high-voltage supplies, and are not air-breathing, so they cannot push a 25 kg aircraft through Mach 0.8 to 1 and would not qualify anyway.

        OptionEvidence-based upsideMain problem
        Custom high-pitch propLargest single lever in the brief. Higher pitch moves thrust and efficiency toward higher advance ratio. One CFD-plus-optimization study raised cruise efficiency from 82.3% to 87.1%; multi-point design cut required power about 4% at high speed versus a commercial APC prop. Patel 2026Czyz 2021Wu 2024Sanchez-Carmona 2025New blade design, spin rig, validation at very high rpm.
        EDF redesignCompact, high thrust per diameter, possible high-speed integration advantages. Gains over open rotors are most consistent at low speed. Urbán 2023Espinoza Quesada 2025Niță 2026Li 2023Jedamski 2023Darrah 2020Effectively a new aircraft: new ducts and inlets, a new drag problem.
        Hall / ion / plasmaNone in the aircraft literature.Not air-breathing; thrust far too low.

        The real answer from Query 3: stop iterating the quad. Fixed-wing removes the propeller advance-ratio ceiling and cuts drag, and nearly every small supersonic program is built around a micro gas turbine, not distributed electric propulsors. Patel 2026Jacob 2021Compton 2021Mizobata 2005 The Dart-80 in the airframe viewer above is an open-source EDF delta, shown as a reference for what an EDF fixed-wing layout looks like.

        10Query 6

        Custom turbofan and
        generative design?

        It can help, if the fan stays low-bypass and topology optimization goes into parts, not the whole jet.

        Engine cycle

        Afterburning gives more augmentation in low-bypass turbofans than in turbojets, because the mixed stream is cooler and keeps more free oxygen, but fuel burn climbs sharply. Fetahi 2021 Overall pressure ratio and turbine inlet temperature dominate afterburning cycle performance, so set those first. Williams 2023Ighodaro 2022 Use reheat briefly to cross the drag rise; it can get through Mach 1 faster despite the fuel flow. Fetahi 2021Ighodaro 2022Apke 2012 Keep bypass very low; in the wet cases studied, thrust-specific performance falls as bypass ratio rises. Fetahi 2021Goulos 2018

        Scaling is the trap. Very small turbojets already run only 5 to 10% overall efficiency, and one study argues a true tiny turbofan gets too complex and expensive to downscale cleanly. Schmidt 2021 Converting an existing micro turbojet with a fan, possibly geared or CVT-driven, is still a major propulsion project. Large 2018Kelly 2020 Curved after-bodies did not beat simple conical ones by much, though they can shorten length. Goulos 2018

        Where topology optimization pays

        PartMethodReported result
        Rotor blisk / diskCFD-FEM topology optimization for mass and forced response Bandini 2024~32% lighter
        Turbine blade interiorGraded lattice / TPMS core Alkebsi 202133-40% lighter
        26-49% less stress
        Engine mounts, fittingsRegulation-constrained TO Munk 2019Min-weight parts
        Whole wingGigavoxel morphogenesis Aage 2017only 2-5%

        Across these papers, topology optimization reliably cuts weight and can move resonances away from forcing frequencies, and additive manufacturing makes the shapes buildable. Munk 2019Bandini 2024Berrocal 2018 Point it at the rotor, hot-section internals, mounts and weight-critical structure. Fetahi 2021Shea 2024Boccini 2019 The bigger Mach 1.1 gains still come from cycle matching, nozzle control, diffuser losses and local mass cuts. Minato 2005Goulos 2018

        11Query 7

        Buy the hot core.
        Make everything around it.

        CNC, metal printing and PA6-CF, PC-CF and PEEK printing are real advantages, but the literature says to aim them at the integration, not the rotating hot section.

        Buy

        • The core turbojet, with ECU support and research precedent Prisăcariu 2026Catană 2024
        • Servos, avionics, standard hardware (excluded from the amateur-built majority by the rules)

        Hot sections need Inconel or refractory steels, and durability problems sit in thermal fatigue, combustion stability and manufacturing repeatability. Prisăcariu 2026 Metal AM fatigue is hard to qualify because defects, residual stress and anisotropy drive life. Sanaei 2020Javidrad 2024Liu 2023

        Make

        • Inlet lip and intake duct
        • Engine mounts and nozzle shrouds
        • Fuel tank internals, avionics trays, fairings
        • Experimental add-ons: ejectors, afterburners, diffusers, manifolds, never compressor or turbine rotors Silivestru 2025Wattenbarger 2025
        Printed polymerWhat the papers foundUse it for
        PA6-CFAbout 96 MPa tensile in favorable XY builds, but interlayer strength stays in the high-20 MPa range. Dul 2021Cool structure, oriented with the load
        PC-CFBetter thermal stability and conductivity, still process-sensitive and orthotropic. Gupta 2022Gupta 2020Cool structure
        PEEKStrong fatigue for a printed polymer, but higher temperature and frequency cut life through defects and self-heating. Alhashmi 2025Warm-adjacent brackets, not hot hardware
        All FFF compositesAnisotropic; properties depend on print direction and process; temperature or cyclic self-heating degrades fatigue. Goh 2020Peng 2020Gupta 2020Design for the weak axis
        12Queries 1, 7

        Proving it, and
        surviving it twice.

        Winning needs a Mach number the judges accept and a vehicle that comes back through the transonic range intact, twice in one day.

        FlutterM 0.90 to 0.94estimated dangerous flutter range for typical control surfaces

        Right inside the window you must cross. Safronov 2023 Active flutter suppression has extended margin past predicted onset in flight tests, but on far slower demonstrators. Vanek 2025 Clear margins with ground vibration testing, engine-on vibration tests and stepwise envelope expansion. Heidersbach 2023González-Cabrera 2026Sampath 2025

        Design rule: spend as little time as possible in the drag-rise and flutter window. A strong core plus a short burst fits that better than a delicate mode switch in the same range. Liu 2024Xi 2023

        Air dataM 1.02indicated, the margin the judges require

        Transonic and supersonic airspeed calibration depends on precise pressure and temperature data. Uncertainty drops with careful onboard calibration, reverse-heading logic and temperature-aware pressure correction. Zolovcik 1950Cooper 2014 Calibrate pitot-static with GPS-based methods before any high-speed claim, because installed pressure errors can corrupt Mach. Foster 2010Jurado 2024Zhang 2024

        Engine bench too: measure thrust, fuel flow, EGT, pressure ratio and transient response, since catalog thrust is not enough. Rhee 2020bFernandes 2024Chachurski 2024Ezgin 2025

        13Queries 5, 7

        Nine steps
        to a Mach 1.1 attempt.

        The staged path the successful programs follow: bench first, slow prototype second, supersonic last. Apke 2012Shea 2024Lee 2025García 2024Mizobata 2014

        01

        Buy engine

        P300 class minimum

        02

        Model thrust margin

        Installed, not catalog

        03

        Shape airframe

        Area rule, inlet with fuselage

        04

        Bench test

        Engine, afterburner, diffuser, nozzle

        05

        Low-speed prototype

        Check handling vs models

        06

        Full-scale taxi

        Self-powered takeoff

        07

        Subsonic flight

        Air-data calibration

        08

        Transonic build-up

        Flutter margins, stepwise

        09

        Mach 1.1 attempt

        Two flights, one day

        The build the evidence points to

        Micro turbojet core P300 class or larger Variable-area nozzle Short afterburner burst Area-ruled, 15 to 25 kg Ramjet ducting last, if ever

        Single engine, fixed wing, thin swept wing, slender area-ruled fuselage, and add-on ejector or afterburner only after the dry engine is characterized. Dalman 2021Rhee 2020bMizobata 2016 Most published small-supersonic programs are still at design, wind-tunnel or low-speed prototype stage, so this is a plan with a clear risk, not a recipe.

        Open question

        Can a commercial 300 to 400 N engine keep enough net installed thrust, after inlet, nozzle and drag penalties, to hold a compliant self-launched Mach 1.1 segment at the final takeoff mass?

        14References

        Sources and
        3D credits.

        Every paper the Consensus thread cites, with its Consensus link. Patel 2026 is the uploaded SQ-2 technical brief. One paper (Wang) appears in the thread only as "+1 more" with no year.

        Aage 2017Gigavoxel computational morphogenesis for structural...Aksoy 2026Performance modelling and efficiency analysis of a micro...Alhashmi 2025Fatigue behaviour of peek fabricated by material...Alkebsi 2021Design of graded lattice structures in turbine blades...Andrei 2016Study of the turbojet engines as propulsion systems for the...Apke 2012Demonstration of an afterburner and nozzle in a mini...Astakhov 2020Problems of ensuring the acceleration dynamics of...Bandini 2024Improving aeromechanical performance of compressor...Berrocal 2018Topology optimization and additive manufacturing for...Boccini 2019Toward the integration of lattice structurebased...Catană 2024Thermodynamic analysis and performance evaluation of...Chachurski 2024Ground testing of a miniature turbine jet engine for...Chu 2025Static aeropropulsion experiment of an electric ducted...Compton 2021Propulsion systems integration for transonic unmanned...Cooper 2014Calibrating airborne measurements of airspeed pressure...Czyz 2021Wind tunnel performance tests of the propellers with...Dalman 2021Conceptual design methods for smallscale...Darrah 2020Electric ducted fan design and testing for high...Davidović 2020Study of innovative subsonic ramjet...Dul 2021Highperformance polyamidecarbon fiber composites for...Ebus 2021Experimental and numerical studies on small...Espinoza Quesada 2025Analysis of the propulsion and aerodynamics of a hybrid quesada...Ezgin 2025Analysis of energy and emission metrics for an...Fernandes 2024Experimental and analytical analysis of a jetcat p300pro...Fetahi 2021A parametric analysis of a turbofan engine with...Foster 2010A gpsbased pitotstatic calibration method using global...Frolov 2019Airbreathing pulsed detonation thrust module numerical...García 2024Design and testing of the multipurpose uncrewed fixedwing...Geng 2007Experimental and numerical investigation of an 8cm...Goh 2020Processstructureproperties in polymer additive...González-Cabrera 2026Structural vibration analysis of uavs under ground engine gonzlez cabrera...Goulos 2018Civil turbofan engine exhaust aerodynamics impact of...Gupta 2020Processing mechanical characterization and micrography...Gupta 2022Thermal characterization of short carbon fiber...Harris 2003Miniature turbojet development at hamilton sundstrand...Heidersbach 2023Safe flutter flight testing of an unmanned aerial vehicle...Huang 2024Gearshaped highg combustion chamber for micro turbojet...Hutchinson 2021Conceptual design and integration of a propulsion system...Ighodaro 2022Offdesign modelling of a turbo jet engine with operative...Ivanov 2021Hydrogen fueled detonation ramjet conceptual design and...Jacob 2021Proposed design of a transsonic unmanned aircraft system...Javidrad 2024Fatigue performance of metal additive manufacturing a...Jedamski 2023Distributed electric propulsion and vehicle integration...Joshi 2023Review of vortex lattice method for supersonic aircraft...Jurado 2024Noncooperative fullenvelope calibration of a supersonic...Kelly 2020Design of a geared turbofan module for small unmanned...Large 2018Investigation of micro gas turbine systems for high speed...Lee 2023A study on the implementation of a micro turbojet...Lee 2024A study of an integrated analysis model with secondary flow...Lee 2025Study on the design and performance analysis of an...Li 2023Aerodynamic design optimization and analysis of ducted...Liu 2023Review on fatigue of additive manufactured metallic...Liu 2024Simple model of turbinebased combined cycle propulsion...Lv 2022Mode transition analysis of a turbinebased combinedcycle...Mathesius 2019Manufacturing methods for a solid rocket motor propelling...Meng 2022Airbreathing rotating detonation fueled by liquid...Minato 2005Offdesign performance of turbojet engine for subscale...Mizobata 2005Development study on a smallscale supersonic flight...Mizobata 2011aDesign of a smallscale supersonic flight experiment...Mizobata 2011bDevelopment of a smallscale supersonic flight experiment...Mizobata 2014Development of a smallscale supersonic flight experiment...Mizobata 2016Aerodynamics and flight capability of a supersonic flight...Mizobata 2024Drag reduction on the basis of the area rule of the...Mizobata 2025Aerodynamics caused by rolling rates of a smallscale...Motsyk 2015Design of a solid rocket motor for a transonic...Munk 2019On the benefits of applying topology optimization to...Niță 2026Prototyping an innovative ducted fan system with...Patel 2026SQ-2 Speed Quadcopter: Executive Technical Brief, Rev. A (uploaded)Peng 2020Investigation of processing parameters on tensile...Peters 2023Materials design for hypersonics...Piancastelli 2018Feasibility study and preliminary design of a rampulsejet...Prisăcariu 2026A review of micro gas engines for uav propulsion...Rhee 2020aTrends of micro turbojet engines within thrust range up to...Rhee 2020bPerformance test and evaluation of micro turbojet engine...Safronov 2023Method of estimating the dangerous range of transonic...Sampath 2025Flutter prediction for unmanned long endurance aircraft...Sanaei 2020Defects in additive manufactured metals and their effect...Sanchez-Carmona 2025Multipoint design of optimal propellers for remotely sanchez carmona...Schmidt 2021Design and numerical simulation of ejector nozzles for...Seraj 2025Aerodynamic shape optimization of a supersonic transport...Shea 2024Design of a modular afterburner system for the jetcat...Shi 2024Rapid design method of heavyloaded propeller for...Silivestru 2025Micro turbojet engine nozzle ejector impact on the...Ueba 2019Design and tests of guidance and control systems for...Urbán 2023Effect of electric ducted fans structural arrangement on...Urzay 2018Supersonic combustion in airbreathing...Vanek 2025Flight testing active flutter suppression technologies...Veeran 2018Ramjet compression system for a hypersonic air...Vernacchia 2021Lowthrust solid rocket motors for small fast aircraft...Vouros 2025Experimental testing and optimizationbased performance...Vu 2026Numerical and experimental analysis of electric ducted...Walter 2012Gojett a supersonic unmanned aerial flight system...Wang (n.d.)A conceptual design and optimization approach for...Wattenbarger 2025Development of a microturbojet engine control unit...Williams 2023Design of an efficient turbofan engine with afterburners...Wu 2023An analysis approach for micro gas turbine engines...Wu 2024Multifidelity neural networkbased aerodynamic...Xi 2023Design of thrust augmentation control schedule during...Xiang 2018An improved propeller design method for the electric...Zhang 2024A study of data processing and error analysis in airspeed...Zhang 2025Fullflow simulationbased analysis and experimental...Zolovcik 1950A method of calibrating airspeed installations...

        3D models

        All meshes are the original authors' geometry. I converted STEP and STL to GLB, decimated with meshoptimizer, and quantized positions. On the KJ66 assembly, six small stray bodies that sit far off the engine axis were removed. On the X-59, the flat triangular print-support web under the belly (a 3D-printing aid, not part of the aircraft) was removed. Nothing is procedural or invented. Materials and colors were assigned for this page.

        ModelAuthorSourceLicenseFile here
        KJ66 micro turbojet, full assembly (exploded layout)Akash Jangidgithub.com/Akash-9070/Turbo3DMITmodels/kj66-assembly.glb
        740 KB
        KJ66 compressor wheel (impeller)Akash Jangidgithub.com/Akash-9070/Turbo3DMITmodels/kj66-compressor-wheel.glb
        55 KB
        KJ66 combustion chamber casingAkash Jangidgithub.com/Akash-9070/Turbo3DMITmodels/kj66-combustion-chamber.glb
        265 KB
        NASA X-59 (printable model)NASA ARMD; Zachary Gwennap and Liam Brinton (NASA interns)www.nasa.gov/stem-content/x-59-3d-printing/NASA media, public domain in the U.S.models/nasa-x59.glb
        514 KB
        Dart-80 80 mm EDF delta jetCaio Cerda (caioplcerda)github.com/caioplcerda/dart-80CERN-OHL-S-2.0models/dart80-edf-delta.glb
        452 KB
        SQ-2 v3 speed quadcopter, 74-part CadQuery assembly (exploded)Aayushya Patelspeed-quad repo (not public)Own designmodels/sq2-v3.glb
        1402 KB