Every megatall development has an atrium — a hotel lobby, a retail galleria, a sky lounge — and every atrium is a compartment the fire code was not written for. Its whole purpose is that it is not divided, so the ordinary defence of compartmentation does not apply and the building must instead prove, by calculation, that smoke will stay above people's heads for long enough to get them out. The arithmetic is unforgiving: a 5 MW fire in a 20 m atrium drops the clear layer from the ceiling to 5.7 m in five minutes. Holding it there needs 33 m³/s of exhaust — and, far more awkwardly, 32 m² of make-up air opening, because the replacement air must arrive slowly enough not to blow the smoke plume sideways.

1 · Why an atrium is a special case

2 · Interactive: how fast the smoke layer descends

With no exhaust running, the smoke layer descends as the plume fills the volume from the top down. NFPA 92 gives a correlation for a steady fire in a uniform space[1]:

\[ \frac{z}{H} \;=\; 1.11 - 0.28\,\ln\!\left(\frac{t\,\dot{Q}^{1/3} / H^{4/3}}{A/H^{2}}\right) \]

with \(z\) the clear height, \(H\) the atrium height, \(A\) the plan area, \(\dot Q\) the fire heat release rate and \(t\) time. Note that \(A\) and \(H\) both help and \(\dot Q\) hurts only as the cube root — you cannot exhaust your way out of a fire that is too big, but a generous volume genuinely buys time.

Smoke layer descent with no exhaust
NFPA 92 filling correlation for a steady fire in a uniform-section space. Valid roughly for A/H² between 0.9 and 14 and for z/H above 0.2 — outside that range it is indicative only.
Floor to the underside of the smoke reservoir.
Cross-sectional area of the atrium volume.
Sprinkler-controlled retail ≈ 2–5 MW; unsprinklered or high fuel load far more.
Above the highest occupied level in the atrium — often 2 m above the highest walking surface.
Clear layer at 2 min
10.9 m
At 5 min
5.7 m
Time to limit
9.0 min
A/H²
5.0
Verdict

A 5 MW fire in a 20 m, 2,000 m² atrium leaves only 9 minutes before the smoke reaches head height with no exhaust running. That is the number the whole strategy is measured against: if the required safe egress time exceeds it, you need exhaust, and if it does not, natural filling may be enough. Drag the fire size and watch how weakly it matters — doubling the fire barely moves the curve, because the plume entrains as the cube root of heat release. Then drag the height: volume is what buys time, and it is an architectural gift rather than an engineering one.

3 · The plume — the calculation everything rests on

The mass of smoke arriving at the layer is almost entirely entrained air, not combustion products. For an axisymmetric plume above the flame tip[1][2]:

\[ \dot m \;=\; 0.071\,\dot Q_c^{1/3} z^{5/3} + 0.0018\,\dot Q_c, \qquad z_l = 0.166\,\dot Q_c^{2/5} \]

with \(\dot Q_c\) the convective heat release (typically 70 % of total) and \(z\) the height from the fire to the smoke layer. The \(z^{5/3}\) is the critical term: entrainment grows faster than linearly with height. Hold the layer at 12 m instead of 6 m in the same atrium and the exhaust needed more than doubles — which is the counter-intuitive result that a higher clear layer is much more expensive than a lower one, and why designers fight for every metre of permitted smoke reservoir depth.

Smoke exhaust required to hold a given clear layer
Axisymmetric plume mass flow, layer temperature from T = T₀ + Qc/(ṁ·cp), volumetric rate from the smoke density at that temperature.
Open Fan power as a calculator
Total heat release rate; 70 % taken as convective.
Height from the fire to the underside of the smoke layer.
Share of heat release carried in the plume rather than radiated away.
Atrium air temperature before the fire.
Plume mass flow
27.7 kg/s
Layer temperature
147 °C
Exhaust volume
33 m³/s
Flame height
4.3 m
If layer at 12 m
71 m³/s

A 5 MW fire with the layer held at 6 m needs 33 m³/s of exhaust, at a layer temperature of about 147 °C. Raise the clear layer to 12 m and it becomes 71 m³/s — more than double, for a layer that is only twice as high. Note also what happens to the temperature: the deeper the layer sits, the hotter and more buoyant the smoke, which makes the system easier to run. A cool, thin, high smoke layer is the hardest thing to extract and the most likely to destratify — which is why systems designed for a very high clear layer in a very tall atrium are the ones that fail in CFD.

4 · Interactive: the make-up air problem

Whatever you exhaust must come back in, and NFPA 92 limits the velocity of that replacement air to about 1.02 m/s where it could reach the plume — because faster air deflects the plume, tears it, and mixes the smoke layer down into the clear layer.

Make-up air opening required, against what is usually provided
Free area = exhaust volume ÷ permitted make-up velocity. The dashed line is the area actually available in the design — doors, louvres and openings that can be opened on alarm.
From the plume calculation above.
NFPA 92 limit near the plume is 1.02 m/s. Higher only where the inlet cannot affect the plume, and that must be demonstrated.
Doors and louvres that will actually be open during a fire, at their free area.
More, smaller extract points reduce the risk of plugholing.
Area required
32.4
Area available
12
Actual velocity
2.75 m/s
Per exhaust point
8.3 m³/s
Status

This is where atrium smoke systems are lost. Holding a 6 m layer needs 33 m³/s, and at the 1.02 m/s limit that demands 32 m² of free make-up area — the equivalent of a dozen wide doorways, all of which must be open during the fire and none of which the architect wants. Provide the 12 m² that is typically available and the inrush runs at 2.75 m/s, well past the limit, and the CFD will show the plume being pushed off vertical and the layer mixing down. The resolutions are all architectural and all early: more openings, a dedicated mechanical make-up system with low-velocity diffusers, or a lower clear-layer requirement agreed with the fire engineer. Discover it late and the only remaining option is a bigger fan, which makes it worse.

5 · The strategy choices

Plugholing — the failure that looks like success If an individual extract point pulls too hard for the depth of smoke above it, it draws clear air up through the layer instead of smoke — plugholing. The fans then run at full duty, the instruments confirm the design flow, and the system is removing mostly clean air while the smoke layer descends anyway. The defence is to split the exhaust into more, smaller points and to check each against the layer depth and temperature. It is a calculation per extract point, not per system, and it is the single most common technical error in atrium smoke design.

6 · Design, installation & commissioning

7 · The design & installation checklist

The one-line summary Atrium smoke control is a performance calculation, not a code lookup: a 5 MW fire drops the clear layer in a 20 m atrium to head height in about nine minutes, and holding it at 6 m costs 33 m³/s of exhaust. The exhaust is the easy half. The hard half is that the same 33 m³/s has to come back in below 1 m/s, which means 32 m² of free opening — and that is an architectural decision that must be made at concept, because no fan can fix it later. Then remember that entrainment goes as z^{5/3}, so a higher clear layer is far more expensive than a lower one, and that splitting the exhaust into more, smaller points is what stops the system quietly extracting clean air while the smoke comes down anyway.

References & standards

  1. NFPA 92 — Standard for Smoke Control Systems: filling correlations, plume equations, make-up air velocity limits and plugholing criteria.
  2. Klote, J.H. & Milke, J.A. Handbook of Smoke Control Engineering (ASHRAE / SFPE / ICC) — atrium smoke management, plume models and design fires.
  3. SFPE Handbook of Fire Protection Engineering — fire plumes, entrainment, heat release rates and design fire selection.
  4. BS 7346-4 and BS 9999 — functional recommendations for smoke and heat exhaust ventilation systems, smoke reservoirs and channelling screens.
  5. EN 12101 series — smoke and heat control systems: natural and powered exhaust ventilators, and their temperature-time classification.
  6. Hansell, G.O. & Morgan, H.P. (BRE) — design approaches for smoke control in atrium buildings.
  7. International Building Code (IBC) and Saudi Building Code SBC 801 — atrium provisions and smoke control requirements.
  8. Hot smoke test protocols (for example AS 4391) — commissioning verification of smoke management performance.
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