β€”

Cross-section (to scale)

Design box β€” constraint checks

Brayton cycle β€” T-s diagram

The cycle's fingerprint: temperature vs entropy through the engine. Up-and-right legs cost you (compression heat, combustion), the down leg 4β†’5β†’8 pays you back. The rightward lean of the compression line is inefficiency (ideal compression would be vertical); the long orange leg is fuel heat; whatever temperature survives to leg 5β†’8 becomes jet velocity. A taller, wider loop = more work per kg of air.

Station conditions

The gas state at each numbered station (see the bubbles on the Design cross-section). Practical anchors: 3 is what your combustor and its o-rings must survive, 4 is the turbine material limit, 5 is what your EGT probe reads, and 8βˆ’0 pressure tells you whether the nozzle chokes.

StationWhereT [K]T [Β°C]P [kPa]

Pressure-ratio sweep (at your TIT β€” dot = your design)

The fundamental trade study: raising Ο€c buys specific thrust (blue, less air needed per newton) and fuel economy (orange TSFC falling). So why not max it out? Because compressor work rises with Ο€c, and work = tip speedΒ² β€” the RPM and wheel stress climb until the aluminum gives up. The curve also flattens: past ~3.5 you pay a lot of stress for little thrust.

TIT sweep (at your pressure ratio)

Hotter gas = more energy left after the turbine = more thrust per kg of air (blue, nearly linear). But EGT (red) tracks TIT almost 1:1 β€” and uncooled Inconel quits around 1050 K TIT / ~750 Β°C EGT. This chart is why turbine material, not aerodynamics, is the real thrust limit of a micro engine.

Throttle curve (first-order estimate, no compressor map)

Thrust vs spool speed. Note how steep it is: at 70% RPM you have only ~ΒΌ of full thrust β€” this is why turbine models need momentum management on landing. Real engines also show an EGT spike during fast accels that this steady-state estimate can't capture; a proper prediction needs the compressor map, which is why it's labeled an estimate.

Sensitivity β€” which knob matters most?

Each parameter nudged Β±3% while the rest hold still; bars show the resulting change in specific thrust. Long bars = high leverage β€” this is your build-effort priority list. Note how much the "boring" loss terms (intake recovery, nozzle Cv) matter: polishing a bellmouth is free thrust, while the faint mirror-image bars confirm the effect works both ways.

Energy accounting

Where the fuel's chemical power actually goes. Only a few percent becomes jet kinetic energy β€” the rest leaves as hot exhaust. This is normal at micro scale (low Ο€c, small parts, big relative clearances); compare the TSFC line against a full-size engine and appreciate why real aircraft engines are big.

3D preview (drag to orbit Β· scroll to zoom Β· double-click to reset β€” cutaway shows the gas path)

The STL is the full (non-cutaway) engine at your exact dimensions in mm β€” open it in any CAD package, slicer, or Windows 3D Viewer. It's a visualization mesh of the major components, not a machining model.

Build notes / bill of materials

PartSpecification~ cost

Rough 2026 hobby prices for bought parts and raw stock β€” excludes tools, fuel, and the inevitable second turbine wheel.

Export

The share link encodes your entire design in the URL β€” send it to a friend and they'll open JetStudio with your exact parameters loaded.

How a micro turbojet works

Intake β†’ Compressor β†’ Combustor β†’ Turbine β†’ Nozzle (0β†’2) (2β†’3) (3β†’4) (4β†’5) (5β†’8)

A single-spool turbojet is the Brayton cycle cast in metal: squeeze air (centrifugal compressor, pressure ratio ~1.8–4), burn kerosene in it at constant pressure (up to the turbine inlet temperature, TIT), expand it through a turbine that extracts exactly the work the compressor needs, then let the leftover pressure accelerate the gas out of a converging nozzle. Thrust = mass flow Γ— exit velocity (plus a pressure term if the nozzle chokes).

Micro engines are thermodynamically bad on purpose: low pressure ratio and small size give ~5–10% thermal efficiency and roughly 10Γ— the specific fuel consumption of a full-size engine. They trade efficiency for simplicity, cost, and robustness β€” the right trade at this scale.

The five core components

1 Β· Compressor β€” a turbocharger wheel, spun by you

The hobby standard is an automotive turbocharger compressor wheel (KKK/BorgWarner, Garrett), 54–76 mm tip diameter, cast or billet aluminum. Work scales with tip speed squared (w β‰ˆ ΞΌΒ·UΒ², ΞΌ β‰ˆ 0.75–0.80): pressure ratio 2.2 needs ~360–400 m/s of tip speed β†’ ~110,000 rpm on a 66 mm wheel. Behind the wheel a diffuser (wedge vanes or a drilled ring) converts swirl into pressure β€” the #1 home-build efficiency killer. Expect only 70–78% stage efficiency.

2 Β· Combustor β€” annular, with vaporizer sticks

An annular flame tube of 0.5 mm stainless with rows of carefully sized holes: primary zone (recirculating, near-stoichiometric flame), secondary (burnout), dilution (mix down to a TIT the turbine survives). Hobby engines don't atomize fuel β€” they boil it inside hooked vaporizer tubes sitting in the flame. Rules of thumb: reference velocity 15–25 m/s, residence time 4–6 ms (sets length ~80–100 mm), pressure loss 5–8%.

3 Β· Turbine β€” the part that wants to die

A ring of nozzle guide vanes accelerates the gas onto a single axial rotor of cast Inconel 713C (usable to ~900–950 Β°C metal temperature). There is no blade cooling at this scale, so TIT above ~1050 K means creep: blades stretch until they rub. Buy the cast wheel β€” it is one of two parts you should never improvise (the other is the compressor wheel).

4 Β· Shaft & bearings

Two angular-contact hybrid bearings (ceramic Si₃Nβ‚„ balls) with light spring preload, lubricated by ~5% turbine oil mixed into the fuel and misted through the shaft tunnel. Speed metric: DN = bore(mm) Γ— rpm β€” keep under ~2.0–2.5 million. The shaft must stay below its first bending critical speed: short and stiff wins.

5 Β· Nozzle

A simple converging cone, often over a center bullet. At hobby pressure ratios it is just barely choked or unchoked (exit 300–450 m/s). Exit area is a live tuning knob: too big β†’ cold and weak; too small β†’ hot and surgy.

The design box β€” what limits you

ConstraintHobby limitIf exceeded
Compressor tip speed~450 m/s cast Β· ~520 billetwheel burst
TIT (uncooled Inconel 713)~1000–1050 Kblade creep, rub, burst
EGT continuous600–750 Β°CECU cuts fuel; nozzle suffers
Bearing DN (fuel-mist lube)~2.0–2.5 M mmΒ·rpmbearing cooks, shaft whip
Ο€c, one centrifugal stage2–3 realistic, 4.5 maxtip speed the alloy can't take
Combustor loading15–25 m/s, β‰₯4 msblowout, flame in the turbine
Shaft speed< 1st bending modedestructive whirl

The design loop this app automates: pick thrust β†’ cycle gives mass flow & compressor work β†’ wheel diameter sets rpm β†’ check every limit β†’ iterate.

Reference engines

EngineThrustRPMΟ€cMass flowClaim to fame
Schreckling FD3/67~25 N~85k~1.9~0.10 kg/s1992 original; plywood compressor
KJ6675–92 N110–128k~2.2~0.23 kg/sTHE homebuild reference, plans available
P100 class~100 N~150k~2.6~0.26 kg/smodern commercial sport engine
P160/P180 class160–180 N~125k~3+~0.4 kg/s2 m sport jets

Fuel, starting, control

  • Fuel: kerosene / Jet-A1 (43.1 MJ/kg, ~0.80 kg/L) + 4–5% turbine oil (Mobil Jet II, AeroShell 500). Budget 150–400 ml/min at full thrust for KJ66-class.
  • Starting: electric starter spins the rotor β†’ ignite propane/butane pre-heat gas (or a kerostart glow vaporizer) β†’ ramp to self-sustain (~45–60 krpm idle) β†’ transition to kerosene. Failed starts that pool fuel cause the classic tailpipe fireball β€” purge before retrying.
  • ECU/FADEC: monitors rpm + EGT, drives the fuel pump, enforces limits (max EGT, max rpm, flameout detection, auto-cooldown). Use an off-the-shelf ECU (Xicoy, JetCat-style, Orbit); do not run open-loop needle-valve control.

Safety β€” non-negotiable

  • A turbine wheel failure at 120,000 rpm releases several kilojoules of shrapnel (see your design's rotor energy on the Build Sheet). First runs: engine bolted to a test stand, bystanders out of the rotor plane, barrier between you and the engine.
  • Kerosene pools burn. COβ‚‚ or dry-powder extinguisher within arm's reach; never fuel near the hot section.
  • Hearing protection β€” >120 dB close up. The exhaust is ~700 Β°C for a meter behind the nozzle.
  • Follow your national model-flying body's turbine code of practice (e.g. the GTBA's). Check insurance.

A sensible build path

  1. See one run first. Attend a jet meet or find a local turbine flyer.
  2. Build from proven plans β€” KJ66 or a GTBA-published design. Buy the compressor wheel and the cast Inconel turbine wheel; machine the housings, shaft, diffuser, and combustor yourself.
  3. Instrument from day one: EGT + rpm minimum, ECU strongly recommended.
  4. Only after a proven runner, iterate your own aero: diffuser, combustor holes, NGV angles, nozzle area. Change one thing at a time; log everything.

Sources and further reading are in RESEARCH.md next to this app β€” including Kurt Schreckling's book (the classic), GTBA design pages, KJ66 documentation, and papers on wheel tip speeds, Inconel 713 limits, and kerosene-lubricated hybrid bearings.