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How far the opening is below (or above) the level where inside and outside pressures are equal.
With openings spread evenly up a building the neutral plane sits near mid-height, so a door at floor level in a 12 m (39 ft) shed is about 6 m (20 ft) below it. Large openings low down pull the plane down towards them.
Sets the direction the air moves; the size of the pressure depends only on the height.
In a heated building air comes in below the neutral plane and goes out above it; in a building cooled below the outdoor temperature the flows reverse.
The air temperature inside the building.
For a warehouse, the temperature the heating holds; for a tall building, the average up its height.
The outdoor air temperature.
The design winter temperature for a heating check, or the day's temperature for a diagnosis.
How much of the ideal flow a real opening passes — about 0.65 for a large opening.
It sets only the air speed row; the pressure does not depend on it.
Stack pressure across the opening
5.21 Pa
Outside air is pushed in through this opening: the building is warmer than outside and the opening is below the neutral plane, or cooler and above it. The pressure grows in a straight line with the height from the neutral plane and with the temperature difference.
- The same pressure in inches of water gauge (in. w.g.)
- 0.02 in. w.g.
- Outdoor air density
- 0.08 pcf
- Air speed through the opening at this discharge coefficient
- 362.08 ft/min
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Stack Effect Pressure Calculator: 5.21 Pa — shown in imperial, US market. The link sets both, so the result they see is the one on your screen.
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How this was calculated
Formula source(s)
- ASHRAE Handbook—Fundamentals, Chapter 16, Ventilation and Infiltration: stack pressure Δp = ρo × g × (H_NPL − H) × (Ti − To) ÷ Ti, temperatures absolute; flow through a large opening with a discharge coefficient of about 0.65
- Outdoor air density from the ideal gas law: ρ = 101,325 Pa ÷ (287.055 J/kg·K × T), dry air at standard pressure
Inputs used
- Height of the Opening From the Neutral Pressure Plane
- 19.5 ft
- Where the Opening Is
- Below the neutral plane — a door, a low vent
- Inside Temperature
- 64.4 °F
- Outside Temperature
- 28.4 °F
- Discharge Coefficient of the Opening
- 0.65
Intermediate steps
- The same pressure in inches of water gauge (in. w.g.)
- 0.02 in. w.g.
- Outdoor air density
- 0.08 pcf
- Air speed through the opening at this discharge coefficient
- 362.08 ft/min
Confidence note: Outside air is pushed in through this opening: the building is warmer than outside and the opening is below the neutral plane, or cooler and above it. The pressure grows in a straight line with the height from the neutral plane and with the temperature difference.
What this calculation does not cover
- The neutral plane's position is an estimate: mid-height for evenly spread openings, lower when the large openings are low. Wind adds its own pressures on top, and on an exposed door it can dominate.
- The air speed is an order-of-magnitude figure. Discharge coefficients vary with the opening's shape, and flow through a large door is two-way — out at the top while it comes in at the bottom.
- Mechanical ventilation that holds the building above or below outside pressure moves the neutral plane and can reverse the flow at a given opening.
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This result is a specification — 5.21 Pa — not a quantity. Put the thing it sizes into your project: how many, what you call it, and your supplier’s price.
Computed in your browser — nothing you enter is uploaded. Presented in US customary units and US trade terminology. Where a formula follows a published standard, that standard and its edition are cited beside it on this page; where none governs, the page says so. Local amendments override model codes — verify against the code in force where you build.
Sources checked 2026-09-22 · v1.0.0
Regulatory standards & verification citations2
- ASHRAE Handbook—Fundamentals, Chapter 16, Ventilation and Infiltration: stack pressure Δp = ρo × g × (H_NPL − H) × (Ti − To) ÷ Ti, temperatures absolute; flow through a large opening with a discharge coefficient of about 0.65
- Outdoor air density from the ideal gas law: ρ = 101,325 Pa ÷ (287.055 J/kg·K × T), dry air at standard pressure
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