Every lesson so far quietly assumed one fuel: Jet-A. What breaks, and what gets better, when you change it?
The answer is a tour of the whole course, because every concept we built depends on some property of the fuel.
Aviation produces roughly 2.5% of global CO₂ emissions, and a larger share of its total climate effect once contrails and high-altitude NOₓ are counted. The industry has committed to net-zero CO₂ by 2050. Getting there means changing what burns inside the combustors of both today's fleet and tomorrow's aircraft. For a combustion engineer this is not a chemistry footnote: it reaches into atomization, stability, heat transfer, acoustics and emissions.
What makes Jet-A the benchmark
| Property | Jet-A (typical) | Why the combustor cares |
|---|---|---|
| Lower heating value | 43.2 MJ/kg | Energy per kilogram carried |
| Density | ~800 kg/m³ | Energy per litre of tank |
| Flash point | > 38 °C | Handling safety |
| Freeze point | < −40 °C (Jet A-1: −47 °C) | Cold-soak operability at altitude |
| Viscosity at −20 °C | ≤ 8 mm²/s | Atomization quality, cold relight (Lesson 6) |
| Aromatics | ~15–20 vol% | Soot and flame radiation (Lessons 8–9), seal swell |
| Thermal stability | High | Fuel used as a heat sink without coking |
Change the fuel and every row moves, and each move lands on a lesson you've already done.
Sustainable aviation fuels: nearly drop-in
Sustainable aviation fuelKerosene-like fuels from non-fossil feedstocks (e.g. HEFA, Fischer–Tropsch), certified as blends with Jet-A. are liquid hydrocarbons made from non-fossil feedstocks, engineered to be close enough to Jet-A to blend into today's engines and infrastructure without modification.
HEFA-SPK (hydroprocessed esters and fatty acids) is the most mature pathway: waste oils, fats and vegetable oils are hydrotreated into a paraffinic kerosene. Fischer–Tropsch SPK is built up from syngas (CO + H₂), which can come from biomass or, in power-to-liquid routes, from captured CO₂ and green hydrogen. Both are currently approved as blends of up to 50% with conventional fuel.
What changes in the combustor?
- Far less soot. These fuels have almost no aromatics, the main soot precursors. Particle emissions fall substantially, a large reduction in particle number in flight tests, and with them the contrail ice crystals that form on soot.
- A gentler flame for the liner. Less soot means less flame radiation (Lesson 8). A cleaner fuel is literally easier on the hardware.
- Slightly less energy per litre. Paraffinic fuels are less dense, so a full tank carries a little less energy.
- The seal problem. Aromatics make the elastomer seals in older fuel systems swell to seal properly. Remove them entirely and seals can shrink and leak. This is one reason for the 50% blend limit and a driver of work toward 100% SAF certification.
Hydrogen: a different kind of flame
Hydrogen is not a drop-in. It rewrites the design rules, because its combustion properties are extreme in almost every direction:
- Flame speed: a stoichiometric H₂–air flame travels at ~2–2.5 m/s, peaking near 3 m/s in slightly rich mixtures. That is roughly six to seven times kerosene (whose ~0.4 m/s is close to methane's).
- Flammability: from φ ≈ 0.1 to about 7, compared with about 0.5–3 for kerosene.
- Ignition: tiny minimum ignition energy and short ignition delays.
- Products: only water. No CO₂, no CO, no soot.
Now run each property back through the course.
Stability (Lesson 5): lean blowout almost vanishes as a concern. The loop is enormous. The problem flips: a hydrogen flame is hard to put out, and it wants to burn where you don't want it.
Flashback (Lesson 2): here is the central problem. A premixed flame propagates upstream wherever the flow is slower than the flame, and in every premixer there is a region where the flow is slow: the boundary layer, right next to the wall.
With natural gas or kerosene vapour, the near-wall flow outruns the flame before the wall stops quenching it. With hydrogen, the slow layer is wide enough for the flame to crawl upstream along the wall, into hardware never designed to hold a flame. No practical premixer velocity fixes it. The emerging answer is to abandon large premixers altogether for MicromixA hydrogen combustor concept using thousands of tiny, fast jets and compact flames to avoid flashback. concepts: thousands of tiny, fast hydrogen jets, each mixing and burning in a small, compact flame.
NOₓ (Lesson 9): hydrogen's stoichiometric flame is hotter and faster than kerosene's, so a careless hydrogen combustor could make more NOₓ. But its enormous lean stability lets it run at φ ≈ 0.3–0.5, far leaner than any hydrocarbon flame could survive, so well-designed lean hydrogen combustors have demonstrated very low NOₓ.
Acoustics (Lesson 7): faster chemistry shortens the time lags and shifts the flame's phase response, so a combustor that was quiet on natural gas can sing on hydrogen blends.
Water vapour: hydrogen produces about 2.6 times more water per unit energy than kerosene. Its contrail and cirrus effects at altitude are an active research question.
Storing hydrogen: the aircraft problem
The combustor is only half of it. Liquid hydrogen boils at −253 °C and holds about 8.5 MJ per litre, against ~35 MJ/L for Jet-A. Even as a cryogenic liquid it needs roughly four times the tank volume, in heavily insulated tanks that don't fit in wings. It is lighter per unit energy, but the tanks, insulation and boil-off management claw much of that back. That is an aircraft-architecture problem more than a combustor one, and it is why hydrogen timelines are longer than SAF timelines.
Fuel flexibility
The most immediate engineering challenge is a combustor that behaves well across a family of fuels: Jet-A, various SAF blends and, eventually, hydrogen-enriched fuels. It must tolerate:
- Different heating values and densities: fuel-flow control must keep the right equivalence ratio.
- Different viscosity and volatility: the injector must atomize them all acceptably (Lesson 6).
- Different flame speeds and ignition delays: shifting flashback margins, stability loops and acoustic time lags (Lessons 5 and 7).
- Different sooting tendencies: changing liner heat loads (Lesson 8) and particle emissions (Lesson 9).
- SAF (HEFA, Fischer–Tropsch) are near drop-ins: far less soot and flame radiation, slightly less energy per litre, and a seal-swell reason for today's 50% blend limit.
- SAF's carbon benefit is in the lifecycle, not the combustor: CO₂ per kilogram burned is nearly unchanged.
- Hydrogen flips the design rules: lean blowout almost disappears, but boundary-layer flashback makes conventional premixers unsafe, pushing designs toward micromix.
- Hydrogen's wide limits allow very lean flames and very low NOₓ, but careless designs can make more.
- Fuel flexibility means tolerating shifts in heating value, spray, flame speed, sooting and acoustics all at once.
You now have every piece. The final lesson hands you the whole machine: pick a mission and design a combustor that passes every test at once.