Engine Room

Supercharger vs Altitude

Engine Room · Demo

An engine is an air pump — here is how a blower keeps it breathing where the air runs out.

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Readout

Full throttle — starvingAbove the critical altitude the blower is flat out and the air is still thinning. From here the lapse takes over again.
Shaft power1006 hp
Air density (σ)67%
Manifold pressure1.16× sea level
Critical altitude2.5 km
Blower drive cost6% of power

The same 1,000 hp engine, three ways of breathing. Notice the supercharged curves RISE slightly toward their critical altitude — constant boost plus ever-colder intake air.

In plain terms

An engine is an air pump: its power is set by how much oxygen it can inhale per second, and by 9 km the air carries only about a third of its sea-level oxygen. A supercharger is a compressor geared to the crankshaft that squeezes the thin outside air back up to sea-level pressure before the cylinders drink it. It holds the engine at full strength up to its critical altitude — the height where the blower runs out of squeeze — and stacking a second stage lifts that ceiling by kilometres. That is how the Merlin kept Spitfires fighting at heights where an unblown engine would barely climb.

More detail

The atmosphere is the ISA troposphere, and a naturally aspirated engine follows the classical Gagg–Ferrar lapse with density ratio σ=ρ/ρ0\sigma = \rho/\rho_0:

PP0=σ0.1170.883\frac{P}{P_0} = \frac{\sigma - 0.117}{0.883}

A blower of pressure ratio PRPR per stage delivers manifold pressure pm=min(p(h)PRn,  pboost)p_m = \min(p(h)\cdot PR^{n},\; p_{boost}) — the knock-limited boost wins below the critical altitude, the atmosphere above it. Compression also heats the charge (imperfect intercooling leaves a PR0.28PR^{0.28} temperature penalty), so what the cylinders actually gain is charge density:

σcharge=pm/p0(T(h)/T0)PR0.28\sigma_{charge} = \frac{p_m/p_0}{(T(h)/T_0)\cdot PR^{0.28}}

and the blower itself taxes the crank a few per cent per stage. The model treats boost as knock-limited and constant below the critical altitude, folds charge cooling into that one exponent, and ignores ram rise and exhaust back-pressure — the textbook shapes, honestly simplified.