Technical note

Air density correction, the selection step people skip

Almost every published fan curve is drawn for standard air at 1.2 kg/m3. Almost every real installation moves something else. Here is the arithmetic that turns one into the other, and the three failure modes it prevents.

The basis

Standard air is a laboratory convention

Catalogue curves are measured in a test chamber, not on a roof. The convention behind most of them – the basis shared by the laboratory methods used for certified ratings – is air at about 20 C and 101.3 kPa at low altitude, which lands at 1.2 kg/m3. It is a good convention because it makes machines comparable. It is a poor assumption because nobody buys a fan to run in a laboratory.

Formula
Density = absolute pressure divided by (287.05 x absolute temperature in kelvin)
287.05
The specific gas constant for dry air, in J per kg per kelvin
Standard air
1.2 kg/m3, the usual catalogue basis
What density changes
Pressure the fan makes, and power absorbed. Volume airflow is essentially unaffected

Altitude

Altitude: the quiet 10 per cent

Ambient pressure falls with elevation. The usual engineering approximation for the lower atmosphere is a barometric relation, and the numbers are worth memorising at round figures.

Sea level
101.3 kPa, about 1.20 kg/m3 at 20 C
500 m
About 95.5 kPa, roughly 1.13 kg/m3
1,000 m
About 89.9 kPa, roughly 1.07 kg/m3
1,500 m
About 84.5 kPa, roughly 1.00 kg/m3
2,000 m
About 79.5 kPa, roughly 0.94 kg/m3

At 1,500 m you are 17 per cent short of the density the curve assumes. A machine selected from the catalogue as written will make about 17 per cent less pressure than the plant needs, and the ventilation contractor will discover this after the ducting is in place. The fix is not a bigger motor. The fix is a machine selected on the corrected duty.

Worked: a plant at 1,200 m needs 30,000 m3/hr against 1,400 mmWC of cool air at 25 C. Absolute pressure there is about 87.2 kPa and density is 87,200 divided by 287.05 x 298.15, which is about 1.02 kg/m3. The equivalent standard-air pressure is 1,400 x (1.2 / 1.02) = about 1,647 mmWC. Select on 30,000 m3/hr at 1,650 mmWC standard air – then check the power the wheel actually absorbs on the site gas, which will be lower than the cold test suggests, but which must still be quoted against the motor that is going to be bought.

Temperature

Hot gas: the same rule, bigger consequences

Temperature divides rather than subtracts, and the kelvin scale is not optional. Density at 350 C with the site at or near atmospheric pressure is 101,325 divided by 287.05 x 623.15, or about 0.57 kg/m3. That is 47 per cent of standard air. A fan that looks ample on a cold curve is a small machine on hot duty, and it is the most common single cause of an underperforming ID fan.

Two errors, one after the other

First error: taking the required static pressure from a cold commissioning measurement. Second error: reading the mass flow as if it were volume. The gas at 350 C carries about half the mass per cubic metre, so a duty quoted in kg/hr needs a volume conversion before it touches a fan curve at all.

Where density is not the whole story

Above roughly 30 kPa of rise, compressibility correction enters. High pressure blowers and air-duty machines are the usual place this shows up, and the works quotes it explicitly rather than assuming a cold-air curve.

Composition

The gas is not air

Specific gas constant changes with molecular weight, so composition changes density at the same temperature and pressure. Rough values against air at 28.96 as a molecular-weight yardstick:

Biogas, roughly 60 per cent methane
About half the density of air at the same temperature, and flammable
Flue gas, mostly N2 and CO2
Slightly heavier than air per molecule, typically treated as air for selection
Humid and saturated gas
Water vapour lowers the mean molecular weight, so warm damp air is lighter than dry air at the same temperature

Consequences

What else moves with density

Noise

Sound power tracks density through a twenty-times-log term, so lighter gas is quieter. That is a real relief on a hot exhauster, and a real problem on a cold aeration blower running the same mass duty at higher speed.

Velocity pressure and outlet losses

Dynamic pressure is half-density times velocity squared. Light gas makes less outlet loss and less duct regeneration loss, which is why a network designed on cold air does not balance hot.

Bearing and seal choice

Hot gas does not only change density. It changes shaft growth, lubricant life and which isolation method the drawing shows. Two consequences of the same number, and only one of them is on the curve.

Questions

Density questions

Does a fan at altitude move less air?

It moves the same volume at the same speed, and that volume weighs less. The pressure it can generate and the power it absorbs both fall with density. So a fan at 1,500 m is not starved of airflow, it is starved of pressure rise.

My catalogue gives standard m3/hr and actual m3/hr - which do I use?

Use actual cubic metres per hour on the fan, and standard cubic metres per hour when you are comparing to a process specification or an emission limit. The curve basis is the actual volume; the process number is usually mass expressed as volume.

How do I check a density figure I have been given?

Divide absolute pressure in pascals by 287.05 times kelvin. If the answer is above about 1.25 kg/m3 at atmospheric pressure someone has used a gauge pressure, and if it is near 1.20 for a hot gas someone has used 20 C.

Next

Use the worksheet

The sizing worksheet carries this arithmetic with the altitude and temperature inputs, and shows the corrected pressure and the fan-law consequence. It is the fastest way to make sure the number you send us is the number the works will select on.

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