Air Temperature Measurement
by Ghost Aviator
Table of Contents
- Introduction — Why Pilots Need Air Temperature
- Air Temperature Thermometers
- Total Air Temperature (TAT) Probe
- Errors
- Heating Error — Compression and Kinetic Heat
- Ram Rise and Recovery Factor — Worked Example
- Correction of TAT/RAT to SAT
- The Absolute (Kelvin) Temperature Scale & Accurate Formula
- Calibration and the ISA
- Practice Questions & Detailed Answers
1. Introduction — Why Pilots Need Air Temperature
A pilot must know the temperature of the surrounding air for the following reasons:
1.1 Avoidance of Icing Conditions
Ice formation on aircraft, particularly in cloud, can be very rapid and extremely dangerous. Icing effects include:
- Loss of lift and increase in drag — ice distorts the aerofoil shape
- Increase in mass — can be as much as ten tonnes on large aircraft with thick icing
- Freezing of control surfaces so they cannot be moved
- Loss of engine power or total engine failure due to intake or carburettor icing
- Ice shed from propellers striking the fuselage
1.2 Engine Power and Aircraft Performance
Aviation engines (jet and piston) require a correct fuel/air ratio for combustion. Dense (cold) air allows more fuel to be injected, producing more power. Less dense (warm) air reduces available power — this has significant effects on take-off performance calculations.
1.3 Measurement of Speed
Airspeed cannot be measured directly — dynamic pressure is measured instead. Dynamic pressure depends on both aircraft speed and air density. Since temperature affects density, temperature data is essential to compute True Airspeed (TAS).
1.4 Measurement of Altitude
The rate of pressure change with altitude varies with temperature. Altimeter indications contain a temperature error that can create potentially dangerous under-readings near high ground in cloud.
2. Air Temperature Thermometers
2.1 Direct Reading Thermometer
Operates on differential thermal expansion. A bimetallic strip bonds two metals with different coefficients of expansion:
- Invar — nickel-steel alloy; uniquely low coefficient of thermal expansion.
- Brass — higher coefficient of thermal expansion.
On heating, the brass expands more than the invar, causing the strip to curl. The amount of curl is proportional to temperature rise. The strip is drawn into a helix to amplify pointer movement. The probe protrudes through the windscreen or fuselage into the airstream; the dial is visible to the pilot.
2.2 Remote Reading Thermometer
Uses a sensor whose electrical resistance changes with temperature. The sensor is located anywhere suitable on the fuselage (away from boundary layer) and sends an electrical signal to a remote cockpit indicator and to other aircraft systems.
flowchart LR
A["Outside Air\n(TAT Probe)"] --> B["Platinum\nResistance Wire\n(sensor)"]
B --> C["Electrical\nSignal"]
C --> D["Cockpit\nIndicator"]
C --> E["Air Data\nComputer"]
C --> F["Other\nSystems"]
3. Total Air Temperature (TAT) Probe
The TAT probe is a small strut and air intake made of nickel-plated beryllium copper — chosen for good thermal conductivity and mechanical strength. It is fixed to the fuselage at a point that keeps it clear of the aircraft’s boundary layer.
3.1 Key Design Features
| Feature | Purpose |
|---|---|
| Right-angle airflow turn inside intake | Separates water particles from the airflow before they reach the sensing element (water cannot make the sharp turn) |
| Bleed holes in intake casing | Higher pressure inside the intake draws off boundary layer air, preventing it from contaminating the measurement |
| Pure platinum resistance wire sensor | Very high thermal conductivity; rapid response; precise and repeatable resistance-temperature relationship |
| Inbuilt heating element | Prevents ice formation. Self-compensating — as temperature rises, heater resistance increases, reducing current automatically |
3.2 Ground Temperature Measurement (Aspirated Probe)
Modern aircraft use reduced take-off power to protect engines from thermal stress (e.g. 93% power is a typical example, computed from runway length, weight, altitude and temperature). When stationary on the ground there is no natural airflow through the probe. An aspirator (air-to-air ejector) uses engine bleed air or APU bleed to create suction, drawing fresh outside air through the casing even when the aircraft is stationary — preventing heat-soaked stagnant air from being measured.
4. Errors in Air Temperature Measurement
| Error | Cause | Remedy |
|---|---|---|
| Instrument error | Manufacturing imperfections | Calibration; correction cards |
| Solar heating | Direct sunlight on the probe | Shielding within the probe strut |
| Ice accretion | Ice build-up on probe | Inbuilt electric heater |
| Heating error | Adiabatic (compression) + kinetic (friction) heating due to speed | Recovery factor & correction formulae |
5. Heating Error — Compression and Kinetic Heat
5.1 Kinetic Heating
Primary contributor in direct reading thermometers. As aircraft speed increases, more air molecules per second impact the probe surface, generating frictional heat at the surface.
5.2 Adiabatic (Compression) Heating
Primary contributor in remote reading (total head) thermometers. The high-speed airflow (potentially several hundred knots) is brought virtually to rest inside the platinum sensing chamber very rapidly. The kinetic energy of the moving air converts to temperature rise through adiabatic compression — analogous to pumping a bicycle pump (pressure energy converts to heat with no external flame).
The combined kinetic + adiabatic effect always totals a known quantity called the Total Ram Rise. Because no probe is perfectly efficient, the actually measured quantity is the Measured Ram Rise.
5.3 Temperature Definitions
| Term | Symbol | Definition |
|---|---|---|
| Static Air Temperature | SAT / Ts / COAT / OAT | Temperature of undisturbed air through which the aircraft is about to fly |
| Total Air Temperature | TAT / Tt / IOAT | Maximum temperature attainable when air is brought to rest adiabatically (theoretical maximum) |
| Ram Air Temperature | RAT | Temperature actually measured by the probe (less than TAT due to probe inefficiency) |
| Total Ram Rise | — | Temperature difference: TAT − SAT (theoretical) |
| Measured Ram Rise | — | Temperature difference: RAT − SAT (actual measured) |
| Recovery Factor | Kr | Fraction of Total Ram Rise actually recovered by the probe. Determined by flight test; published in aircraft operating instructions. |
SAT = COAT (Corrected Outside Air Temperature) = OAT (when used alone)
TAT = IOAT (Indicated Outside Air Temperature) — note: many gauges are labelled “TAT” but actually display RAT
TAT = SAT + Total Ram Rise RAT = SAT + Measured Ram Rise Measured Ram Rise = Total Ram Rise × Kr
6. Ram Rise and Recovery Factor — Worked Example
Worked Example — Recovery Factor Application (Source Example)
Given: SAT = −60°C, Total Ram Rise = 30°C, Kr = 0.9
| Step | Parameter | Value | Calculation |
|---|---|---|---|
| 1 | SAT | −60°C | Given |
| 2 | Total Ram Rise | +30°C | Given |
| 3 | (Theoretical) TAT | −30°C | SAT + Total Ram Rise = −60 + 30 |
| 4 | Recovery Factor Kr | 0.9 | Given |
| 5 | Measured Ram Rise | +27°C | 30 × 0.9 = 27 |
| 6 | RAT (gauge reading) | −33°C | SAT + Measured Ram Rise = −60 + 27 |
| 7 | Correction to get SAT | −27°C | SAT = RAT − Measured Ram Rise = −33 − 27 = −60 |
Conclusion: The gauge reads −33°C (RAT). A correction of −27°C is applied to obtain the true SAT of −60°C.
7. Correction of TAT/RAT to SAT
Methods to convert RAT to SAT (in order of exam relevance):
- Rapid formula (in-flight quick approximation — not for JAA/EASA/DGCA exams)
- CRP-5 navigation computer (blue scale — use in exams)
- Accurate Kelvin formula (most precise)
- Data Tables
- Air Data Computer (automatic, used in modern aircraft)
7.1 Rapid Formula (In-Flight Only)
| TAS (knots) | Ram Rise (Rapid Formula) | Ram Rise (CRP-5) |
|---|---|---|
| 200 | 4°C | 4°C |
| 300 | 9°C | 9°C |
| 400 | 16°C | 17°C |
| 500 | 25°C | 25°C |
7.2 CRP-5 Navigation Computer
On the slide-rule face there is a blue scale: outer ring = TAS in knots; inner ring = Ram Rise in °C. Set TAS on the outer scale, read Ram Rise on the inner scale.
8. The Absolute (Kelvin) Scale & Accurate Formula
The Celsius scale changes sign at 0°C (freezing point of water), creating issues with mathematical ratios. The Kelvin (Absolute) scale starts from absolute zero — the theoretical point of no thermal energy, occurring at −273°C.
| Reference Point | Celsius (°C) | Kelvin (K) |
|---|---|---|
| Absolute zero | −273 | 0 |
| Freezing point of water | 0 | 273 |
| Boiling point of water | 100 | 373 |
Conversion: K = °C + 273 | One kelvin = one degree Celsius (same increment size, different baseline).
8.1 Accurate Formula
Variables: TAT = Total Air Temperature in Kelvin; Kr = Recovery Factor (dimensionless, from flight test data); M = Mach Number.
Worked Example — Accurate SAT Formula (Source Example)
Given: Indicated TAT = −20°C | Mach No = M 0.73 (typical B737 Long Range Cruise) | Kr = 0.98 (typical modern TAT probe)
Step 1: Convert TAT to Kelvin: −20 + 273 = 253 K
Step 2: Calculate denominator: 1 + (0.2 × 0.98 × 0.73²) = 1 + (0.2 × 0.98 × 0.5329) = 1 + 0.1044 = 1.1044
Step 3: SAT = 253 ÷ 1.1044 = 229 K
Step 4: Convert to Celsius: 229 − 273 = −44°C
Result: SAT = −44°C. The probe reads −20°C but true static air temperature is −44°C.
9. Calibration and the International Standard Atmosphere (ISA)
Due to the variable nature of the real atmosphere, a standard calibration model is used. All air data instruments are calibrated to the International Standard Atmosphere (ISA).
9.1 ISA Mean Sea Level (MSL) Values
| Parameter | ISA MSL Value |
|---|---|
| Pressure | 1013.25 hPa |
| Temperature | +15°C |
| Density | 1225 g/m³ |
9.2 ISA Atmospheric Layers
| Layer | Altitude Range | Temperature Behaviour |
|---|---|---|
| Troposphere | MSL to 11 km (36 090 ft) | Decreases at 6.5°C/km = 1.98°C/1000 ft |
| Lower Stratosphere (Isothermal) | 11 km to 20 km (36 090–65 617 ft) | Constant at −56.5°C |
| Upper Stratosphere | 20 km to 32 km (65 617–104 987 ft) | Increases at 1°C/km = 0.3°C/1000 ft |
Calibration is carried out with both increasing and decreasing readings to determine lag at calibration conditions. Any residual errors within agreed tolerances are listed as instrument errors over the operating range.
- Four reasons for temperature measurement: icing avoidance, engine performance, speed measurement, altitude accuracy.
- Direct reading = bimetallic helix (differential thermal expansion). Remote reading = platinum resistance wire (electrical).
- TAT probe: nickel-plated beryllium copper; right-angle airflow; bleed holes; platinum sensor; self-compensating heater (<1°C error).
- Aspirator = ground temperature device, uses bleed air suction to bring fresh outside air to the sensor.
- Dominant error = heating error (adiabatic + kinetic). Solar error remedied by shielding; icing remedied by heater.
- SAT + Total Ram Rise = TAT. SAT + Measured Ram Rise = RAT. Measured Ram Rise = Total Ram Rise × Kr.
- Quick formula: Ram Rise ≈ (TAS/100)² — NOT for exams. Use CRP-5.
- Accurate formula (Kelvin ONLY): SAT = TAT ÷ (1 + 0.2 Kr M²).
- ISA MSL: 1013.25 hPa, +15°C, 1225 g/m³. Lapse rate to 36 090 ft: 1.98°C/1000 ft. Isothermal: −56.5°C from 36 090 ft to 65 617 ft.
Practice Questions & Detailed Answers
- (a) COAT is another name for SAT itself, not the difference between SAT and TAT.
- (c) Recovery Factor (Kr) is a dimensionless ratio (0 to 1), not a temperature difference.
- (d) Hot ramp radiation is not a recognised aviation temperature term.
- (a) Electrical resistance is the principle of the remote reading thermometer, not the direct reading bimetallic type.
- (b) The bimetallic thermometer measures temperature, not pressure; airspeed pressure drives the ASI, not the thermometer.
- (c) Adiabatic cooling does not apply to the bimetallic strip mechanism.
- (a) “Two metals” implies a bimetallic direct-reading type. The TAT probe uses a single platinum element.
- (c) Resistance in the platinum sensor changes with temperature, not pressure.
- (d) Capacitance principles are used in some fuel gauges, not TAT probes.
- (b) Physical protection from hailstones is not the purpose of shielding; the beryllium copper construction provides mechanical strength.
- (c) Icing is prevented by the inbuilt heater, not the shield.
- (d) Kinetic heating cannot be shielded against — it is an inherent consequence of speed, corrected by the recovery factor.
- (a) 50°C would result from TAS/10 — incorrect formula.
- (c) 5°C is TAS/100 = 5, without squaring.
- (d) 16°C corresponds to TAS = 400 kt: (400/100)² = 16.
- (a) Icing is prevented by the probe’s inbuilt electric heater.
- (c) Moisture compensation is not a function of the aspirator.
- (d) Solar radiation is mitigated by the probe strut’s shielding design.
- (b) The thermometer indicates RAT (not SAT). Adding the Measured Ram Rise to RAT gives nothing meaningful; TAT = SAT + Total Ram Rise.
- (c) Recovery Factor is dimensionless and cannot be subtracted from a temperature.
- (d) These are two different types of quantities and cannot be added to produce a temperature.
- (a) Omits Kr — assumes a perfect probe (Kr = 1.0) which does not exist in practice.
- (c) This is the formula for SAT from TAT (the inverse direction), not TAT from SAT.
- (d) A negative sign would make TAT less than SAT — physically impossible since compression always adds heat.
Master Reference Tables — Chapter 3
Numerical Values
| Value | Parameter | Section |
|---|---|---|
| <1°C | Maximum heater error in TAT probe | 3 |
| 93% | Example reduced take-off power setting | 3 |
| −273°C = 0 K | Absolute zero | 8 |
| 273 K | Freezing point of water (0°C) | 8 |
| M 0.73 | Typical cruise Mach number (B737 LRC) | 8 |
| 0.98 | Typical Kr for a modern TAT probe | 8 |
| 1013.25 hPa | ISA MSL pressure | 9 |
| +15°C | ISA MSL temperature | 9 |
| 1225 g/m³ | ISA MSL density | 9 |
| 36 090 ft (11 km) | ISA tropopause | 9 |
| −56.5°C | Isothermal temperature (tropopause to 65 617 ft) | 9 |
| 65 617 ft (20 km) | Top of isothermal layer (ISA) | 9 |
| 104 987 ft (32 km) | Top of upper stratosphere (ISA) | 9 |
| 1.98°C/1000 ft | ISA lapse rate (troposphere) | 9 |
| 0.3°C/1000 ft | ISA temperature rise rate (upper stratosphere) | 9 |
Formula Sheet
| Formula | Use |
|---|---|
TAT = SAT + Total Ram Rise | Basic temperature relationship |
RAT = SAT + Measured Ram Rise | What the probe actually measures |
Measured Ram Rise = Total Ram Rise × Kr | Apply recovery factor |
Ram Rise ≈ (TAS in kt / 100)² | Quick in-flight approximation ONLY |
SAT (K) = TAT (K) ÷ (1 + 0.2 Kr M²) | Accurate formula (Kelvin required) |
TAT (K) = SAT (K) × (1 + 0.2 Kr M²) | Rearranged accurate formula |
K = °C + 273 | Celsius to Kelvin conversion |
Mnemonics
| Mnemonic | Meaning |
|---|---|
| COAT = SAT | Corrected Outside Air Temperature = Static Air Temperature |
| IOAT = TAT | Indicated Outside Air Temperature = Total Air Temperature |
| TAT > RAT > SAT | Temperature hierarchy at speed (TAT is always highest) |
Source Answer Key
| Q1 | Q2 | Q3 | Q4 | Q5 | Q6 | Q7 | Q8 |
|---|---|---|---|---|---|---|---|
| b | d | b | a | b | b | a | b |
Reinforce Chapter 3: Air Temperature Measurement
Test your knowledge and practice actual exam questions for Navigation — Instrumentation.