ATPL aircraft performance · Lesson 6 of 15

Density altitude and take-off distance

A hot day at a high airfield makes the air thin. The aeroplane behaves as if the airfield were higher still. This lesson shows how to put a number on that, and what it does to the runway you need.

An example lesson built by Chalkwork Labs from public sources, to show the shapes. Your course is drafted from your material and checked by you.

The aeroplane in this lesson is a generic light single-engine piston aeroplane with illustrative performance figures. It is not any real type, and its own figures are not from any flight manual. The wind, slope, surface and safety factors are the CAA's figures from CAP 698 and Safety Sense Leaflet 7. The physics of density altitude follows the FAA Pilot's Handbook of Aeronautical Knowledge (see Sources).

1. Why the aeroplane cares about air density

Air density is the mass of air in a given volume. Thin air has low density. Thin air hurts a piston aeroplane three times over at take-off:

Two things make air thin: low pressure and high temperature. Height gives low pressure. Heat makes the air expand. A hot, high airfield has both.

The aeroplane does not know the airfield's elevation. It only feels the density of the air. Every performance number in the manual is tied to density.

2. Pressure altitude

Performance tables need one standard to compare against. The International Standard Atmosphere (ISA) is that standard. It is a model of an average atmosphere: hPa and °C at sea level, with the temperature falling by about °C for every 1,000 ft of height.

The pressure altitude is the height in the ISA at which the pressure equals today's pressure at the airfield. It is what the altimeter reads when you set hPa. To find it from the airfield elevation and today's QNH (the sea-level pressure the tower gives you), use the ATPL rule of ft per hPa (PA is the pressure altitude):

PA = elevation + (1013 − QNH) × 27

Low pressure means a higher pressure altitude. On a day with QNH 1003 hPa, a 2,000 ft airfield has a pressure altitude of ft. PPL teaching rounds the rule to ft per hPa, which would give ft. The UK ATPL question bank is set with 27 ft per hPa, so use 27 ft in the exam.

Pressure altitude (ft)ISA temperature (°C)

The ISA temperature at each pressure altitude, from °C minus °C per 1,000 ft.

3. Density altitude

The pressure altitude fixes the pressure. The temperature still varies. The density altitude is the height in the ISA at which the air has today's density. The FAA handbook defines it as "pressure altitude corrected for nonstandard temperature".

The correction uses the ISA deviation: today's outside air temperature (OAT) minus the ISA temperature at that pressure altitude. Every degree warmer than ISA adds about ft of density altitude. This is the exam rule (DA is the density altitude):

ISA temp  = 15 − 2 × (PA ÷ 1,000)
deviation = OAT − ISA temp
DA        = PA + 120 × deviation

A warm day gives a positive deviation and a higher density altitude. A cold day gives a negative deviation, and the density altitude can fall below the pressure altitude. The aeroplane then performs better than the elevation suggests.

1. Exam style. An airfield has a pressure altitude of ft. The OAT is °C. What is the density altitude?

4. Take-off distance against density altitude

The take-off distance is the ground run plus the climb to a screen height of 50 ft. For our illustrative aeroplane it is m at sea level, ISA, maximum weight, on a level dry paved runway with no wind. Two rules then stretch it:

Move the three sliders. The dot is today's take-off. The dashed line is the take-off distance available (TODA), m at this airfield. Find the hottest day on which the take-off still fits at maximum weight.

–
density altitude (ft)
–
ISA deviation (°C)
–
take-off distance (m)
–
against 800 m available
Take-off distance to 50 ft against density altitude, for the weight you set. The grey dashed curve is maximum weight. Above the runway line the take-off does not fit.

At the starting settings the density altitude is ft and the distance is m, which fits. Warm the day to 40 °C and the density altitude rises to ft. The distance becomes m. Now load to maximum weight and it becomes m. That is longer than the runway.

The shape matters. The curve bends upward. The same 1,000 ft of density altitude costs more metres at the top of the chart than at the bottom. Hot and high is not a sum of two small effects. It is a product.

2. Nothing else changes, but the take-off weight goes up by 10%. By about how much does the take-off distance grow?

5. Correcting for wind, slope and surface

The chart above assumes a level, dry, paved runway and no wind. Real runways differ. Each difference multiplies the distance by a factor:

The first bar is today's distance from the chart above. Each later bar applies one more correction. Try a 10 kt tailwind. Then switch the safety factor on.

–
book distance (m)
–
corrected distance (m)
–
against 800 m available
Positive wind is a headwind. The wind bar uses half of a headwind and 150% of a tailwind, as CAP 698 requires. Positive slope is uphill. The corrections multiply, so their order does not change the final bar.

3. Same airfield, same aeroplane, same weight. Which day gives the shortest take-off distance?

6. Worked example

Airfield elevation ft. QNH hPa. OAT °C. Take-off weight kg. Headwind kt, upslope %, . Runway available m.

  1. Pressure altitude. − = hPa, times = ft. Pressure altitude = ft.
  2. ISA temperature. − × = °C.
  3. ISA deviation. − = °C.
  4. Density altitude. + × = + = ft.
  5. Book distance. Density factor = . Weight factor ( ÷ )² = . Distance = × × = m.
  6. Wind. The reported headwind is kt. CAP 698 allows % of it: kt. (( − ) ÷ )² = . Distance = m.
  7. Slope. × = m.
  8. Surface. × = m. This does not fit the m runway, even before the safety factor. It is m over.
  9. Safety factor. × = m. The shortfall grows to m.

Even the unfactored number says no. The factored number says no by a wide margin, and it is the one to trust. Notice the trap: with the full kt headwind the unfactored distance would be m and would look as if it fitted. That is why the exam takes only half the headwind: the wind will not always blow. The fix is to wait for a cooler hour, take less fuel, or use a longer runway. Press the "Set the worked example" button to see the same case on the charts.

7. Step through the calculation

Show the working in code

Optional. The same calculation as Python you can step through.

The block below is real Python that runs in this page. You do not write or edit it. Press Next step and watch each variable appear. The last two steps compare the exam rule with the exact ISA formula.

Block 1: Density altitude, by the rule and exactly

Step through the worked example. Check that each printed value matches section 6.

  1. Set the pressure altitude and the OAT from the worked example.
  2. Find the ISA temperature at that pressure altitude.
  3. Find the ISA deviation.
  4. Apply the exam rule: 120 ft per degree.
  5. Compute the exact ISA density ratio and turn it into a height.
  6. Compare the two answers.

4. The rule gives ft and the exact formula gives ft. What should you take from that?

What to remember

Sources