Two more measurements feed the air-data computer alongside the pressures: the temperature of the air, and the angle at which it meets the wing. This lesson returns to the outside air temperature the first module promised and finds that measuring it in flight is subtler than it sounds, then turns to the angle-of-attack sensors whose data guards the aircraft against the stall, and what happens when that data goes wrong.
OAT, SAT and TAT
Three names, two temperatures:
Outside air temperature (OAT) — the actual temperature of the undisturbed air the aircraft flies through; measured properly it is the same thing as the static air temperature (SAT), the term the instruments and computers prefer.
Total air temperature (TAT) — what a probe on a fast aircraft actually feels: air arriving at the probe is compressed and brought nearly to rest, and compression heats it, so the probe senses the static temperature plus a heating due to speed.
The relationship mirrors the pressure family deliberately: as total pressure is static plus dynamic, total temperature is static plus the ram rise.
Ram rise, and converting TAT to SAT
The ram rise is the difference TAT − SAT: the temperature added by bringing the moving air to rest against the probe. For a given air temperature it depends only on the Mach number, growing with its square, negligible for a light aircraft and around 25 to 30 degrees for a jet at cruise. With temperatures in kelvin the conversion is one line, written for a probe that captures the whole ram rise (called full recovery, which modern TAT probes very nearly achieve):
TAT from SAT (temperatures in kelvin, full recovery)