Lesson 10 of 11

Alternative Fuels

What happens when the fuel changes underneath everything: sustainable aviation fuels as near drop-ins, hydrogen as a whole new combustion problem, boundary-layer flashback, and what a fuel-flexible combustor must solve.

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The question

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

PropertyJet-A (typical)Why the combustor cares
Lower heating value43.2 MJ/kgEnergy per kilogram carried
Density~800 kg/m³Energy per litre of tank
Flash point> 38 °CHandling safety
Freeze point< −40 °C (Jet A-1: −47 °C)Cold-soak operability at altitude
Viscosity at −20 °C≤ 8 mm²/sAtomization quality, cold relight (Lesson 6)
Aromatics~15–20 vol%Soot and flame radiation (Lessons 8–9), seal swell
Thermal stabilityHighFuel 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.

CompareWhat changes when the fuel changes
Energy per kg (MJ/kg)120.0
Energy per litre (MJ/L)8.5
Peak flame speed (m/s)2.90
Flammable range (φ)7.0
Aromatics → soot (%)0.0
Combustion CO₂ (g/MJ)0
white tick = Jet-A
SAME ENERGY ON BOARDJet-A1.00× volumeLiquid hydrogen4.06× volumefuel mass: 0.36× Jet-A(before adding a heavy insulated cryogenic tank)
Three times the energy per kilogram, a quarter per litre. Burns ~7× faster than kerosene over an enormous flammability range: no CO₂, no soot — and a whole new set of combustor problems.
Challenges0/1
  • Compare all five fuels. Which single property changes the most? (1/5)
Bars compare the selected fuel (bright) with Jet-A (outline). The tanks show the volume and mass needed to carry the same energy.

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.

ExploreWhy hydrogen creeps upstream
00.81.52.3300.10.20.30.40.5velocity (m/s) — zoomed to the slow near-wall layerdistance from wall (mm)flame speed 0.46 m/squench layer: 0.108 mm
0% H₂
rest is methane
40 m/s
0.60
Wall velocity gradient16.0k s⁻¹
Critical gradient4.3k s⁻¹S_L² / α — below this, flashback
Min. safe velocity11 m/s
Safe. Even right next to the wall, the flow outruns the flame before the wall stops quenching it.
Challenges0/2
  • Make a 70% hydrogen blend flash back at 40 m/s or more.
  • Burn pure hydrogen in this premixer without flashback.
Inside a premixer, the flow is fast in the core but must slow to zero at the wall. Near the wall there is always a thin layer where the gas is slower than the flame — the flame can crawl upstream through it unless the wall quenches it first (grey band).

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.

Check your intuition
Why is hydrogen's high flame speed a problem for lean premixed combustors, when it helps stability?

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).
Estimate first
How many litres of liquid hydrogen carry the same energy as one litre of Jet-A?
0.10110100
Drag along the line to place your guess — each tick is ten times the last.
Recap
What changes when the fuel changes
  • 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.

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