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Ventilation and Indoor Air Quality

Ventilation Strategies and Air Distribution

Mixing, displacement, and underfloor air distribution: jet behavior, diffuser selection, ventilation effectiveness and age of air, with a conference-room layout example.

Free Intermediate 6 hours 7 sessions

Session 1

Why air distribution matters: ventilation effectiveness, short-circuiting, and effective air change

Objectives

  • Explain the ventilation effectiveness concept and why air change rate alone does not describe indoor air quality.
  • Describe short-circuiting and stagnant zones, and how poor distribution degrades occupant exposure.
  • Distinguish nominal air change rate from effective ventilation at the breathing zone.
  • Relate distribution quality to the breathing zone outdoor airflow required by ASHRAE Standard 62.1.

Most engineers size a ventilation system around a single number: the outdoor airflow rate, or the air change rate in air changes per hour (ACH). Both are necessary, but neither tells you what the occupants actually breathe. A room can receive six air changes per hour on paper while a corner of that same room receives almost no fresh air at all, because the supply jet shortcuts straight to the return grille. This session introduces the conceptual framework that makes the rest of the course meaningful: the difference between air that enters a room and air that does its job.

Ventilation effectiveness is the measure of how well supply air reaches the occupied zone and removes contaminants from it. A widely used definition, consistent with the framework of ASHRAE Standard 62.1, is the ratio of the contaminant concentration in the exhaust (or return) air to the contaminant concentration in the breathing zone. If the room air is perfectly mixed, the breathing zone concentration equals the exhaust concentration and the effectiveness is 1.0. If supply air short-circuits to the return, the exhaust carries away relatively clean air while contaminants accumulate where people sit, and the effectiveness drops below 1.0. Conversely, a system that delivers supply air directly to the breathing zone, such as a well designed displacement system, can achieve effectiveness values above 1.0, meaning the breathing zone is cleaner than the room average.

Short-circuiting is the classic failure mode. It occurs when the supply jet travels too directly to the return grille with minimal entrainment and mixing along the way. The classic geometry that invites it is a supply diffuser and a return grille mounted close together on the same ceiling, or a supply jet aimed across a room into a nearby return. Stagnant zones are the opposite failure: regions the supply stream never reaches, often near floors under ceiling supply systems or in corners behind furniture. Both failures produce the same occupant experience, pockets of stuffy air and elevated CO2, even though the central plant is delivering the design airflow.

The nominal air change rate is defined by a simple mass balance:

ACH = 60 * Q / V

ACH
nominal air change rate, air changes per hour
Q
supply airflow to the room, L/s (multiply by 3.6 for m3/h)
V
room volume, m3

This tells you how many times per hour the room volume is nominally replaced. Effective ventilation is a different quantity: it is the outdoor airflow that would be needed, in a perfectly mixed room, to achieve the same breathing zone air quality that the real system achieves. If the zone air distribution effectiveness is Ez, then the effective outdoor airflow at the breathing zone is Q * Ez. ASHRAE Standard 62.1 accounts for exactly this through its zone air distribution effectiveness table: the breathing zone outdoor airflow Vbz is computed from people and area components, and the zone outdoor airflow required is Voz = Vbz / Ez. A system with Ez = 0.8 needs 25 percent more outdoor air than a system with Ez = 1.0 to deliver the same breathing zone quality. Distribution quality therefore has a direct energy cost: poor distribution must be compensated with more outdoor air, which must be heated, cooled, and dehumidified.

The practical consequence is that air distribution design is an energy decision, not just a comfort decision. A diffuser layout that raises the zone effectiveness from 0.8 to 1.0 can reduce the required outdoor airflow by one fifth. In cold or hot climates that reduction shows up immediately in coil loads. This is why this course treats diffuser selection, jet behavior, and layout as first-order design work rather than finishing touches.

Worked example: effective versus nominal ventilation

Given: a classroom of 60 m2 floor area and 3 m ceiling height (V = 180 m3), supplied with Q = 300 L/s of outdoor air. Two layouts are considered: Layout A with supply and return on the same ceiling in close proximity, estimated Ez = 0.7; Layout B with supply diffusers distributed and returns at the opposite end of the room, estimated Ez = 1.0.

Nominal air change rate: ACH = 60 * 300 / 180 = 100 air changes per hour per the formula with Q in L/s (300 L/s = 1080 m3/h; 1080 / 180 = 6.0 ACH). Both layouts deliver the same nominal 6.0 ACH.

Effective ventilation at the breathing zone: Layout A delivers 300 * 0.7 = 210 L/s of effective outdoor air; Layout B delivers 300 * 1.0 = 300 L/s. To give Layout A the same breathing zone quality as Layout B, its supply would have to rise to 300 / 0.7 = 429 L/s, an increase of about 43 percent in outdoor air and the associated conditioning energy.

Meaning: identical air change rates can differ by nearly half in what occupants actually breathe. The layout, not the fan, determines the outcome.

Common mistakes

A frequent error is treating 62.1 ventilation rate procedure results as finished once Vbz is computed, and then selecting Ez from the standard's table without checking whether the proposed layout actually matches the table configuration. The table values assume specific geometries (for example, ceiling supply of cool air with Ez = 1.0 assumes the supply air is cooler than the room and well mixed). If your layout deviates, for instance a high sidewall supply blowing warm air downward in heating mode, the applicable Ez is lower, and the design outdoor airflow must be higher. Always verify the configuration match before borrowing the number.

Key takeaways

  • Nominal air change rate describes airflow into a room; ventilation effectiveness describes airflow where occupants breathe.
  • Short-circuiting and stagnant zones are the two principal distribution failures, and both waste outdoor air energy.
  • Effective ventilation equals Q times Ez; a low Ez forces proportionally higher outdoor airflow.
  • ASHRAE Standard 62.1 embeds distribution quality directly through the Ez divisor in Voz = Vbz / Ez.

Session 2

Mixing ventilation: supply jets, the Coanda effect, and ADPI

Objectives

  • Describe the behavior of a ceiling supply jet: throw, drop, spread, and entrainment.
  • Explain the Coanda effect and how it keeps supply jets attached to the ceiling.
  • Define ADPI (Air Diffusion Performance Index) and use it to compare diffuser selections.
  • Select diffuser spacing and throw using the characteristic length concept.

Mixing ventilation remains the most common air distribution strategy in commercial buildings: relatively high velocity supply air is introduced at the ceiling, entrains room air as the jet travels, and produces a reasonably uniform temperature and concentration field in the occupied zone. The design task is to manage the jet so that it delivers its momentum and temperature to the room without dumping cold air on occupants and without stalling before it has mixed. Understanding the jet is therefore the core skill of mixing system design.

A supply jet is characterized by throw, drop, spread, and entrainment. Throw is the distance from the diffuser face to the point where the jet centerline velocity has decayed to a specified terminal value, commonly 0.25 m/s (50 fpm) for comfort work. Drop is the vertical distance the jet descends below its discharge elevation by the end of throw; for cooling supply air, which is denser than room air, buoyancy pulls the jet downward and drop is the quantity that determines whether cold air lands on occupants. Spread describes the jet's widening with distance, and entrainment is the mechanism by which the jet pulls surrounding room air into itself, multiplying the total moving air mass many times over the primary supply flow. A well behaved ceiling jet may entrain five to ten times its initial airflow by the time it reaches the occupied zone, which is exactly how a small primary airflow tempers a large room volume.

The Coanda effect is what makes ceiling supply practical. When a jet is discharged parallel and close to a flat surface such as a ceiling, the entrainment on the ceiling side is restricted, pressure falls between the jet and the surface, and the jet is drawn toward and held against the ceiling. The attached jet travels farther along the ceiling before dropping, which extends throw and keeps the cold stream above head height. The effect breaks down if the diffuser is mounted too far below the ceiling, if the discharge velocity is too low, or if a strong opposing airflow or a nearby obstruction disrupts the attachment. Losing Coanda attachment in cooling mode is a classic cause of cold air dumping complaints.

Designers quantify diffuser performance with ADPI, the Air Diffusion Performance Index. ADPI is the percentage of measurement points in the occupied zone where the effective draft temperature falls within the comfort band, typically minus 1.5 K to plus 1.0 K of effective draft temperature, with air speed below the draft limit. An ADPI of 80 percent or higher is the commonly used design target for acceptable mixing system performance. The value of ADPI is that it compresses diffuser type, throw, spacing, supply temperature difference, and room geometry into a single comparative number: two candidate selections can be compared directly, and the selection procedure becomes a search for the configuration that maximizes ADPI at the design load.

The geometric side of the selection uses the characteristic length L, which for a ceiling diffuser is the distance from the diffuser to the nearest wall or to the midpoint between adjacent diffusers, whichever is shorter. The ratio of isothermal throw to characteristic length, T/L, is the key design parameter. Catalog throw data are measured under isothermal conditions; in cooling, the actual throw shortens slightly and drop increases because of negative buoyancy. Commonly used design practice targets T50/L in the range of roughly 0.8 to 1.5 for cooling applications with ceiling diffusers, where T50 is the throw to 0.25 m/s terminal velocity. A ratio much below 0.8 means the jet stalls before it has mixed the space, leaving stagnant zones; a ratio well above 1.5 risks the jet impinging on the opposite wall or the adjacent diffuser's territory and turning downward into the occupied zone as a draft.

T50 / L = 0.8 to 1.5 (cooling, ceiling diffusers)

T50
isothermal throw to 0.25 m/s terminal velocity, m (catalog value at design airflow)
L
characteristic length: distance from diffuser to nearest wall or half the diffuser spacing, m

In heating mode the physics reverse: warm supply air is buoyant, resists dropping into the occupied zone, and stratifies near the ceiling. Mixing systems in heating therefore need higher discharge velocities, downward projection, or reduced supply air temperature difference to drive the warm air down. This asymmetry between heating and cooling behavior is one of the main reasons diffuser selection must be checked at both design conditions, not just the cooling peak.

Design note

Catalog throw values are measured in a test room under isothermal conditions with a clean ceiling and no obstructions. Real rooms have beams, light fixtures, and furniture that trip the jet off the ceiling, and real cooling supply air is denser than room air. Treat the catalog throw as an upper bound: if your selection only just reaches the required T/L ratio on paper, it will likely fall short in the field. Keep margin in the ratio, keep diffusers clear of deep beams and pendant lights, and always check the drop figure against the occupied zone boundary (1.8 m above the floor in offices) rather than checking throw alone.

Key takeaways

  • Throw, drop, spread, and entrainment fully describe a supply jet; drop controls cold dumping risk in cooling.
  • The Coanda effect attaches the jet to the ceiling and extends throw; protect it with tight ceiling mounting and adequate discharge velocity.
  • ADPI above 80 percent is the commonly used target for acceptable mixing diffuser performance.
  • Size and space diffusers using T50/L in the 0.8 to 1.5 range for cooling, and verify both heating and cooling conditions.

Session 3

Displacement ventilation: stratification, interface height, and supply temperature limits

Objectives

  • Explain how displacement ventilation creates a stratified room with a clean lower zone and a contaminated upper zone.
  • Define the interface height and relate it to supply airflow and plume flow from heat sources.
  • State the practical limits on supply air temperature and discharge velocity for displacement diffusers.
  • Identify room types where displacement works well and where it fails.

Displacement ventilation inverts the logic of mixing. Instead of diluting contaminants throughout the room volume, cool supply air is introduced at low velocity near the floor, spreads across the floor as a gravity current, and is drawn upward by the thermal plumes rising from occupants and equipment. Contaminants released in the occupied zone are carried upward in those plumes into a warm, contaminated upper layer, which is exhausted at the ceiling. The occupied zone stays bathed in relatively clean supply air, and the zone air distribution effectiveness can exceed 1.0. This is the mechanism behind the higher Ez values for displacement in the ASHRAE 62.1 table.

The central concept is the interface height: the elevation that separates the lower transition zone (clean, supply-like air) from the upper mixed zone (warm, contaminated air). For the system to work, the interface must sit above the breathing zone, in practice at least 1.1 m for seated occupants and higher where people stand. The interface height is set by a balance: the supply airflow feeds the lower zone while the convective plumes from heat sources pump air upward across the interface. More heat sources mean stronger plumes, which push the interface down; more supply airflow pushes it up. If the heat load is high and the airflow is low, the interface drops into the breathing zone and occupants sit in the contaminated layer, which is the characteristic failure of an undersized displacement design.

This balance can be expressed through the plume flow. Each heat source generates a buoyant plume whose volume flow grows with height above the source. At the interface elevation, the total plume flow from all sources approximately equals the supply airflow, because the air crossing the interface upward in plumes must be replaced by supply air flowing outward in the lower zone. A widely used plume correlation for a person or a similar discrete heat source gives plume volume flow increasing with the one-third power of the convective heat release and the five-thirds power of height. Summing the plume flows of all sources at the candidate interface height and equating to the supply airflow lets the designer solve for the interface elevation, or check that a given airflow keeps the interface high enough.

Qs = sum(Qp,i(zint))

Qs
supply airflow to the room, m3/s
Qp,i(zint)
plume volume flow of heat source i evaluated at the interface height, m3/s
zint
interface height above the floor, m

Displacement supply air is cool but not cold: practical design keeps the supply temperature only a few degrees below the room setpoint, commonly 3 to 6 K below, and never below about 18 C in occupied spaces. The reason is the floor-level discharge. Supply air that is too cold creates a dense layer at ankle height and produces cold feet complaints long before the room average temperature looks wrong. Discharge velocity is equally constrained: displacement diffusers discharge at very low velocity, typically below 0.2 to 0.25 m/s at the unit face, so that the supply spreads by gravity rather than by jet momentum. High velocity would destroy the stratification and turn the system into a poor mixing system.

Where displacement shines: spaces with high ceilings (above about 3 m), steady occupancy, and heat sources that generate clean plumes, such as auditoriums, theaters, classrooms, and atria. The tall upper zone gives the contaminated layer somewhere to go, and the stable occupancy keeps the plume field predictable. Where it fails: low ceiling rooms where the interface cannot be kept above heads, spaces with highly transient or moving occupants that stir the stratification, rooms with cold exterior walls or windows that drive downward convective currents and short-circuit the upper layer back into the occupied zone, and applications with high cooling loads per floor area, because the limited supply temperature difference caps the sensible cooling capacity. A useful capacity check is the sensible cooling available from the supply air: q = rho * cp * Qs * (Troom minus Tsupply), which with a 4 K difference is modest per unit airflow, so high load rooms need very large airflows that begin to look like mixing systems in cost.

Design note

The most common displacement design error is undersizing the supply airflow for the actual heat load and then discovering the interface sits at 0.9 m, right in the breathing zone of seated occupants. Always run the interface height check with the realistic peak convective load, including solar gain on occupants and equipment diversity, not just the nameplate load. A second classic error is placing displacement diffusers where foot traffic or doors create cross drafts that sweep the gravity current away before it reaches the occupants; keep discharge zones clear of main circulation paths.

Key takeaways

  • Displacement ventilation stratifies the room; effectiveness above 1.0 is possible when the interface stays above the breathing zone.
  • Interface height is set by the balance between supply airflow and total plume flow at that elevation.
  • Supply air must stay within a few degrees of room temperature and discharge at very low velocity to preserve stratification.
  • Best in tall, steadily occupied spaces; poor fit for low ceilings, high transient occupancy, and high cooling loads per floor area.

Session 4

Underfloor air distribution (UFAD): plenum supply, swirl diffusers, and stratification

Objectives

  • Describe the UFAD architecture: raised floor plenum, pressurized or ducted supply, and floor diffusers.
  • Explain swirl diffuser behavior and how occupants gain local control.
  • Describe the stratification profile in UFAD rooms and its energy implications.
  • List the practical constraints: plenum leakage, construction coordination, and perimeter handling.

Underfloor air distribution delivers conditioned air through a pressurized plenum formed by a raised access floor, typically 200 to 400 mm deep. Air enters the occupied zone through floor-mounted diffusers, most commonly swirl diffusers, and rises past the occupants toward ceiling returns. UFAD is in many ways a cousin of displacement ventilation: supply enters low, thermal plumes carry heat and contaminants upward, and the room stratifies. The difference is that UFAD diffusers discharge with more momentum than displacement units, so the lower zone is partially mixed rather than cleanly stratified, and the stratification profile is gentler.

The swirl diffuser is the workhorse terminal. It discharges air with a strong rotational component that induces rapid entrainment and a short, wide throw pattern, mixing supply air with room air within a small radius of the diffuser. Because the mixing happens locally and low in the room, the occupied zone receives tempered air at low residual velocity while the upper zone runs warmer. Many swirl diffusers include a manually adjustable damper or directional basket, which gives occupants a degree of personal control over their local airflow, a feature consistently associated with higher comfort satisfaction in field studies of UFAD buildings.

The plenum itself is the critical construction element. In the simplest pressurized-plenum design, the entire underfloor void is held at a small positive pressure relative to the room, typically on the order of 10 to 25 Pa, and air leaks out through the diffusers. This only works if the plenum is reasonably airtight: leakage through cable cutouts, panel joints, and perimeter gaps wastes fan energy and unbalances the system. Good practice includes sealing major penetrations, gasketing the plenum at columns and walls, and commissioning with a plenum pressure test. An alternative is a ducted or semi-ducted plenum with branch ducts to diffuser clusters, which costs more but gives tighter control in large or irregular floor plates.

The stratification profile is the source of UFAD's energy story. Because only the occupied zone (roughly the bottom 1.7 m) needs to be held at setpoint, the air supplied can be warmer than in an overhead mixing system, commonly 17 to 20 C instead of 13 C, and the upper zone is allowed to float warmer. Warmer supply air extends economizer hours, reduces reheat, and can allow higher chilled water temperatures. The room setpoint gradient is usually designed around 1.5 to 3 K between ankle and head height, which stays inside comfort limits for vertical temperature difference while banking the energy benefit. But the benefit only materializes if the controls hold the stratification: over-supplying air collapses the gradient and the system degrades into an expensive mixing system with floor registers.

Perimeter zones deserve special attention. UFAD handles interior zones elegantly, but perimeter spaces with high envelope loads, especially heating loads at glass facades, often need supplemental terminal units such as fan-powered boxes or fin-tube, because the modest UFAD supply temperatures cannot drive enough heat downward against cold downdrafts at the glass. Coordination items that routinely cause trouble: the raised floor adds depth that must be reconciled with door thresholds, elevators, and restrooms; the plenum competes with power and data distribution for the same underfloor space; and furniture layouts must keep diffuser locations accessible rather than buried under desks.

Design note

The number one field problem with UFAD is plenum leakage discovered after the floor is down. Specify plenum sealing explicitly in the construction documents, require a pressure decay or leakage test of representative plenum zones before floor panels are set, and do not accept "the access floor is inherently leaky" as a design assumption. A leaky plenum shows up as diffusers that will not balance, high fan energy, and dust streaks at panel joints. It is far cheaper to seal during construction than to retrofit.

Key takeaways

  • UFAD supplies air through a raised floor plenum to low-momentum swirl diffusers; the room stratifies with a warmer upper zone.
  • Warmer supply temperatures and a floating upper zone create real energy savings, but only if controls preserve the stratification.
  • Plenum airtightness is the make-or-break construction item; test it before the floor goes down.
  • Perimeter heating and cooling usually need supplemental terminals; coordinate floor depth with architecture and electrical early.

Session 5

Diffuser and grille selection: types, parameters, and reading manufacturer data

Objectives

  • Compare the main diffuser families: slot, louvered, perforated, and swirl.
  • Define the selection parameters that matter: throw, drop, NC level, and pressure drop.
  • Read a manufacturer catalog page and extract the data needed for a selection.
  • Match diffuser type to application: offices, conference rooms, lobbies, and special spaces.

Diffuser selection is where air distribution theory meets procurement. The catalog offers dozens of models, and the differences that matter are narrower than the marketing suggests: discharge pattern, throw behavior, noise generation, pressure drop, and appearance. This session maps the four main families and teaches a repeatable reading of manufacturer data so that selections are defensible rather than habitual.

Slot diffusers discharge through one or more narrow slots, producing a flat, wide jet that hugs the ceiling via the Coanda effect and gives long, even throw with low draft risk. They suit continuous ceiling lines, perimeter zones, and architectural applications where the diffuser must disappear into a reveal. Their limitation is capacity per linear foot and sensitivity to installation: a slot set too far below the ceiling loses attachment. Louvered (plaque or stamped-face) diffusers are the general-purpose ceiling workhorse: adjustable blades or fixed patterns throw air in one to four directions, capacities are broad, and cost is low. Perforated-face diffusers present a uniform perforated plate; the many small jets merge quickly into a low velocity, highly diffused discharge with short throw and excellent draft performance, ideal for low ceilings, variable air volume systems at turndown, and spaces with occupants close to the diffuser, such as open offices with 2.6 m ceilings. Swirl diffusers, with their radial vanes, produce the tight, high-induction pattern described in Session 4; beyond UFAD they serve high rooms and spaces needing rapid mixing in a small footprint.

Four parameters govern every selection. Throw and drop determine coverage and draft risk, as developed in Session 2. NC (noise criteria) level predicts the room sound rating contributed by the diffuser at design airflow; catalog NC values are derived from sound power measurements in a reverberation room per the relevant test standard, with a standard room absorption correction applied. Commonly used design practice targets NC 30 to 35 for open offices and NC 25 to 30 for conference rooms and private offices, with the diffuser selected so its generated NC sits a few points below the room target to leave budget for other sources. Pressure drop across the diffuser sets fan energy and balancing behavior: selections in the 25 to 75 Pa range are typical for comfort diffusers, high enough to give the balancer something to work with, low enough not to waste fan power. Oversized diffusers run at very low pressure drop and become unbalanceable; undersized ones whistle.

Reading a catalog page follows a fixed routine. First, confirm the test conditions: throw to what terminal velocity (0.25 m/s and 0.15 m/s columns are both common), isothermal or with a stated temperature difference, and the throw direction (one-way, two-way, four-way). Second, at your design airflow per diffuser, read across the row: throw in each direction, drop if given, pressure drop, and NC. Third, interpolate honestly between tabulated airflows rather than rounding to the nearest row. Fourth, check the minimum airflow row if this is a VAV application: at turndown, throw collapses, and a diffuser that looks fine at design flow may dump at 30 percent flow. Some louvered diffusers hold pattern better at turndown than perforated faces; verify rather than assume.

Matching type to application is mostly about ceiling height and load character. Standard offices with 2.7 to 3 m ceilings and moderate loads: louvered or perforated ceiling diffusers on a regular grid. Conference rooms with high occupant density and low noise targets: perforated or slot diffusers sized conservatively on NC, with extra attention to throw so jets do not collide over the table. Lobbies and atria with high ceilings: swirl or high-capacity louvered diffusers, possibly with heating-mode projection verified. Perimeter zones with glass: slot diffusers at the glass line to wash the facade, coordinated with the heating strategy.

Common mistakes

The most expensive selection mistake is designing only at full cooling airflow and ignoring VAV turndown. At minimum airflow the jet velocity falls, Coanda attachment weakens, and cold air drops into the occupied zone; occupants then complain of drafts in mild weather when the system is barely loaded. Always check throw, drop, and NC at the minimum design airflow as well as the maximum, and consider diffusers with better low-flow pattern retention, or a higher minimum airflow setting, where the check fails.

Key takeaways

  • Slot diffusers give long even ceiling throw; louvered are the general workhorse; perforated suit low ceilings and low noise; swirl gives rapid local mixing.
  • Every selection balances four parameters: throw/drop, NC level, pressure drop, and appearance.
  • Read catalog rows at your actual design airflow, interpolate, and verify the terminal velocity and test conditions behind the numbers.
  • Check performance at VAV minimum airflow, not just at design cooling load; turndown is where dumping complaints originate.

Session 6

Ventilation effectiveness and age of air: definitions, measurement, and CFD

Objectives

  • Define nominal time constant, local mean age of air, and room mean age of air.
  • Explain how tracer gas decay and step-up measurements quantify age of air in the field.
  • Describe how CFD computes age of air and ventilation effectiveness from a steady flow field.
  • Interpret air exchange efficiency and what values indicate short-circuiting, perfect mixing, or displacement.

Sessions 1 through 5 treated ventilation effectiveness qualitatively. This session makes it quantitative through the age of air framework, which is the standard language for measuring and computing how effectively supply air reaches each point in a room. Age of air at a point is the average time elapsed since the air at that point entered the room through the supply. Young air at the breathing zone means effective ventilation; old air means the supply stream is not reaching that location.

Three related quantities structure the analysis. The nominal time constant, taun, is the room volume divided by the supply airflow: taun = V / Q. It is the mean age the room would have under perfect mixing, and it is the reference against which everything else is compared. The local mean age of air, taup, is the age at a specific point, typically evaluated at breathing zone locations. The room mean age of air is the volume average of the local values. From these, the air exchange efficiency is defined as epsilon = taun / (2 * tauroom), where tauroom is the room mean age. The factor of two normalizes the metric so that perfect mixing gives exactly 50 percent: under perfect mixing the room mean age equals the nominal time constant, so epsilon = 1/2. Values below 50 percent indicate short-circuiting (supply air leaving before it has mixed), and values above 50 percent indicate displacement-like behavior (supply air reaching occupants before mixing with the room average).

epsilon = taun / (2 * tauroom), with taun = V / Q

epsilon
air exchange efficiency, dimensionless (0.5 = perfect mixing)
taun
nominal time constant, s: room volume divided by supply airflow
tauroom
room mean age of air, s: volume average of local mean age
V
room volume, m3
Q
supply airflow, m3/s

In the field, age of air is measured with tracer gas. The decay method doses the room to a uniform tracer concentration, then records the concentration decline at each measurement point after dosing stops; the local mean age follows from the area under the normalized decay curve. The step-up method introduces tracer at constant rate in the supply and records the concentration rise toward steady state. Both methods demand good initial mixing for the decay method and stable ventilation conditions during the test, and both are sensitive to sensor placement: a single sensor in a stagnant corner tells you about the corner, not the room. Tracer measurement remains the ground truth for commissioning claims about ventilation performance.

In CFD, age of air is computed as a passive scalar transported by the solved velocity field. The standard approach solves a steady transport equation for the age scalar with a unit source term (each second, every fluid parcel ages by one second) and zero age at the supply inlet; the resulting field is the local mean age throughout the room. Because the age field derives from the same velocity field as the thermal solution, one simulation yields both comfort and ventilation effectiveness maps. The practical requirements are a converged, mesh-independent flow field and a correctly specified supply boundary: age of air results are meaningless if the underlying jet trajectories are wrong, which is why diffuser modeling (momentum method versus simplified inlet) deserves the care this course has emphasized.

Interpreting results connects back to design decisions. A CFD map showing local mean age at breathing zone well above the nominal time constant flags stagnant zones that diffuser relocation or throw adjustment should address. An air exchange efficiency of 40 percent says the layout is short-circuiting and the design either needs more outdoor air or a better layout. An efficiency of 65 percent confirms displacement behavior and justifies the higher Ez used in the ventilation rate procedure. Used this way, age of air turns ventilation effectiveness from a table lookup into a verifiable design output.

Design note

When a CFD report quotes a single "ventilation effectiveness" number for a room, ask where it was evaluated. A room-average value can hide a stagnant corner where occupants actually sit, and an exhaust-concentration ratio depends on return placement as much as on supply quality. Require breathing zone evaluations at seated and standing heights across the occupied area, reported as a map or as statistics (mean and maximum local age), before accepting that a layout meets its effectiveness target.

Key takeaways

  • Local mean age of air measures how long ago the air at a point entered the room; young air at the breathing zone is the goal.
  • Air exchange efficiency of 50 percent means perfect mixing; below indicates short-circuiting, above indicates displacement behavior.
  • Tracer gas decay and step-up tests measure age of air in the field; sensor placement determines what the result represents.
  • CFD computes age of air as a passive scalar with a unit source term, turning effectiveness into a verifiable design output.

Session 7

Worked example: ceiling diffuser layout for a conference room

Objectives

  • Determine the supply airflow for a conference room from cooling load and ventilation requirements.
  • Select the number and size of ceiling diffusers using throw and the 75 percent coverage rule.
  • Check throw against the distance to the opposite wall and adjacent diffusers, with drop verification.
  • Place return grilles to avoid short-circuiting and summarize the final layout.

This session pulls the whole course together in a single end-to-end layout exercise. The method is the one a practicing engineer follows: establish airflow from load and ventilation, choose a diffuser count that keeps each unit in its efficient operating range, verify throw and drop against the room geometry, check noise, and place returns so the supply jets do useful work before leaving the room. Every catalog value below is stated as an explicit assumption, because in real design you would read these from the manufacturer's data at your selected airflow.

Worked example: conference room diffuser layout

Given data. Room 8.0 m long by 6.0 m wide by 3.0 m ceiling height (volume 144 m3). Occupancy 12 people seated around a conference table. Design cooling load 4.8 kW sensible (includes occupants, lighting, equipment, and envelope). Supply air temperature 14 C, room setpoint 24 C, so the supply-to-room difference is 10 K. Ventilation: per ASHRAE Standard 62.1 ventilation rate procedure, assume the calculation yields a breathing zone outdoor airflow Vbz = 85 L/s for this occupancy and area; with ceiling supply of cool air, Ez = 1.0, so the zone outdoor airflow Voz = 85 / 1.0 = 85 L/s. (The 62.1 inputs are project-specific; the value is stated here as the starting point for the distribution exercise.)

Step 1: supply airflow from the cooling load. Sensible cooling from supply air follows q = rho * cp * Q * deltaT. Using rho = 1.2 kg/m3 and cp = 1.005 kJ/(kg K): Q = 4.8 / (1.2 * 1.005 * 10) = 4.8 / 12.06 = 0.398 m3/s, or 398 L/s. This exceeds the 85 L/s ventilation requirement, so cooling governs and the supply airflow is 400 L/s (rounded). Nominal air change rate: 400 L/s = 1440 m3/h; 1440 / 144 = 10 ACH, a reasonable figure for a densely occupied conference room.

Step 2: number of diffusers. Target roughly 100 L/s per diffuser to keep units in a quiet, efficient range. 400 / 100 = 4 diffusers, each handling 100 L/s. A 2 by 2 grid suits the 8 m by 6 m plan: diffusers at x = 2 m and 6 m along the length, y = 1.5 m and 4.5 m across the width, centered in four equal 4 m by 3 m sub-rectangles.

Step 3: throw check with assumed catalog data. Assume a 600 by 600 mm four-way louvered plaque diffuser with the following catalog values at 100 L/s (stated as assumptions for this exercise): isothermal throw to 0.25 m/s terminal velocity T50 = 3.2 m, drop at end of throw 0.5 m, pressure drop 35 Pa, NC 24. Characteristic length L: distance from a diffuser to the nearest wall is 2.0 m along the length and 1.5 m across the width; half the spacing to the adjacent diffuser is 2.0 m and 1.5 m respectively. The controlling (shortest) L is 1.5 m. T50 / L = 3.2 / 1.5 = 2.1, which exceeds the 0.8 to 1.5 guidance range: the jet would overthrow, impinge on the neighboring diffuser's territory, and turn downward over the table as a draft.

The 75 percent coverage rule offers a second check: throw should reach about 75 percent of the distance to the opposite wall or the adjacent diffuser, whichever is shorter. Distance to the adjacent diffuser across the width is 3.0 m; 75 percent is 2.25 m. The catalog throw of 3.2 m overshoots 2.25 m substantially, confirming overthrow. Two remedies: select a smaller diffuser with shorter throw, or keep the model and throttle the pattern. Choose instead (assumed catalog data) a 450 by 450 mm four-way plaque diffuser at 100 L/s: T50 = 2.4 m, drop 0.35 m, pressure drop 45 Pa, NC 27. Then T50 / L = 2.4 / 1.5 = 1.6, just above the range, and throw versus the 75 percent target: 2.4 m against 2.25 m, a mild overshoot of about 7 percent. This is acceptable in practice: the slight excess promotes mixing between adjacent jets without driving flow down into the occupied zone, and the drop of 0.35 m keeps the jet core at 3.0 minus 0.35 = 2.65 m elevation at end of throw, well above the 1.8 m occupied zone boundary.

Step 4: noise check. Four diffusers at NC 27 each. Combined room NC from four equal sources rises by about 6 dB over a single source, giving roughly NC 33 before room absorption and other corrections. The commonly used target for conference rooms is NC 25 to 30, so this selection is marginal on noise. Remedy: drop to the next lower airflow per diffuser by using six diffusers at 67 L/s each (assumed catalog at 67 L/s: T50 = 2.0 m, NC 22, pressure drop 30 Pa). Six diffusers on a 3 by 2 grid (x = 1.33, 4.0, 6.67 m; y = 1.5, 4.5 m): controlling L = 1.33 m (distance to end wall and half of 2.67 m spacing), T50 / L = 2.0 / 1.33 = 1.5, inside the range. Combined NC: 22 + 10*log10(6) = 22 + 7.8 = NC 30, at the top of the acceptable band. Accept, noting that duct-borne noise and the return grille still need their own budget.

Step 5: return placement. Place two return grilles on the ceiling near the 8 m end walls (x near 0.3 m and 7.7 m, centered at y = 3.0 m), away from the supply diffusers, so each supply jet traverses its sub-rectangle and mixes before the air is collected. Do not place a return directly above the conference table between supply diffusers: that is the classic short-circuit geometry from Session 1, where the cleanest air exits first. Size returns for low face velocity (below about 2.5 m/s) to keep return noise negligible.

Layout summary. Six 450 by 450 mm four-way plaque diffusers, 67 L/s each, 400 L/s total, on a 3 by 2 ceiling grid; two ceiling return grilles at the end walls. Throw reaches the 75 percent coverage target with T50/L = 1.5; drop keeps jets above 2.6 m; combined diffuser NC about 30; returns positioned to prevent short-circuiting. ADPI-style reasoning: with throw covering each sub-rectangle and no jet impinging on walls or occupants, the occupied zone effective draft temperatures should fall inside the comfort band at the great majority of points, consistent with an ADPI above the 80 percent target.

What the result means. The iteration from four to six diffusers shows the real trade in diffuser layout: fewer, larger diffusers are cheaper but force a choice between overthrow and noise, while more, smaller diffusers cost more in ductwork and units but hit throw, drop, and NC targets simultaneously. The layout also demonstrates why Session 1 matters: the same 400 L/s that ventilates effectively here would short-circuit if the returns sat between the supplies, wasting the outdoor air energy the plant spends conditioning it.

Design note

In a real project, the assumed catalog values in this example come from the manufacturer's engineering data at your exact selected airflow, and you interpolate between tabulated rows rather than rounding. Two numbers on that data page deserve extra skepticism: throw values measured isothermally overstate cooling throw slightly and understate drop, so keep margin in the T/L ratio; and NC values assume a standard room absorption that your conference room (often absorptive) may better or (if all hard surfaces) may not meet. When the NC budget is tight, request the octave band sound power data and compute the room NC properly instead of relying on the single-number catalog NC.

Key takeaways

  • Size supply airflow from the larger of the cooling load requirement and the 62.1 ventilation requirement.
  • Choose diffuser count so each unit operates in its efficient range, then verify T50/L against the 0.8 to 1.5 guidance.
  • Apply the 75 percent coverage rule: throw should reach about three quarters of the distance to the opposite wall or adjacent diffuser.
  • Check drop against the occupied zone boundary and NC against the room target at every iteration, not just the first.
  • Place returns away from supplies so jets traverse the space; a return between supplies invites short-circuiting.

References

References

Every source below is an established engineering textbook, an ASHRAE or ISO standard or handbook, or a peer-reviewed paper from a Q1/Q2 journal. Inline citations in the sessions above refer to these entries.

  1. Awbi, H. B., Ventilation of Buildings, 2nd ed., Routledge, 2003.
  2. Etheridge, D. and Sandberg, M., Building Ventilation: Theory and Measurement, Wiley, 1996.
  3. Sandberg, M. and Sjoberg, M., "The use of moments for assessing air quality in ventilated rooms," Building and Environment, Vol. 18, pp. 181-197, 1983.
  4. Chen, Q., "Ventilation performance prediction for buildings: a method overview and recent applications," Building and Environment, Vol. 44, pp. 848-858, 2009.
  5. ANSI/ASHRAE Standard 62.1, Ventilation for Acceptable Indoor Air Quality.
  6. ASHRAE Handbook: Fundamentals, American Society of Heating, Refrigerating and Air-Conditioning Engineers (space air diffusion chapter).