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<strong>Air</strong> <strong>conditioning</strong> <strong>using</strong> <strong>displacement</strong> <strong>ventilation</strong> <strong>to</strong> <strong>maximize</strong> free cooling<br />

David Butler*<br />

*David Butler is a Principal Consultant in BRE’s Environmental Engineering Centre.<br />

Summary<br />

Displacement <strong>ventilation</strong> uses air supplied at a temperature, typically around 19°C for<br />

offices, which is only slightly cooler than the design temperature of the occupied zone.<br />

This is a much higher temperature than used for conventional mixed flow <strong>ventilation</strong><br />

systems and creates opportunities for <strong>using</strong> fresh-air based “free cooling” for a large<br />

proportion of the year.<br />

Conventional <strong>displacement</strong> <strong>ventilation</strong> design practice suggests that the cooling capacity<br />

of <strong>displacement</strong> <strong>ventilation</strong> in commercial offices with normal floor <strong>to</strong> ceiling heights (up<br />

<strong>to</strong> 3 m) is limited <strong>to</strong> around 25 W/m 2 . For this reason it is fairly common in the UK <strong>to</strong><br />

specify chilled ceilings in conjunction with <strong>displacement</strong> <strong>ventilation</strong> <strong>to</strong> meet typical office<br />

heat loads. However, recent BRE research has shown that <strong>displacement</strong> <strong>ventilation</strong> on<br />

its own <strong>using</strong> appropriate diffusers can deal with heat loads of around 50-55 W/m 2 in<br />

typical office environments without ca<strong>using</strong> thermal discomfort outside the outflow zone.<br />

This opens up the possibility of <strong>using</strong> fresh-air free cooling for large parts of the year.<br />

Displacement compared with mixed flow <strong>ventilation</strong><br />

Displacement <strong>ventilation</strong> is essentially a buoyancy driven "<strong>displacement</strong>" process.<br />

"Fresh" <strong>ventilation</strong> air is introduced at low velocity and at low-level in<strong>to</strong> the occupied<br />

zone at a temperature typically around 19°C, slightly cooler than the design room air<br />

temperature. <strong>Air</strong> is extracted at ceiling level. The supply air spreads out across the floor<br />

forming a reservoir of cool fresh air, as shown in Figure 1. Any heat source in the room,<br />

such as a person sat at a desk, will generate a positively buoyant thermal plume rising<br />

upwards. This plume will draw air from the reservoir of cool fresh air at low level in the<br />

room. If the source of heat also represents a pollutant source, these pollutants will also<br />

be transported up out of the occupied zone.<br />

1


2<br />

Return grill Return grill<br />

Figure 1 Displacement <strong>ventilation</strong> – typical room air flow<br />

Extensive investigations elsewhere (1-6) have shown that generally two distinct stratified<br />

layers of air form, an upper zone containing warm polluted air and a lower zone<br />

containing cooler cleaner air separated by a boundary layer. This causes a vertical<br />

temperature gradient <strong>to</strong> develop (typically 5-6°C between supply and extract), resulting<br />

in higher temperatures at ceiling level than with standard mixing <strong>ventilation</strong> systems.<br />

Displacement <strong>ventilation</strong> strategies exploit this vertical temperature gradient by<br />

maintaining the lower occupied zone at comfort conditions while allowing the upper<br />

hotter zone <strong>to</strong> increase <strong>to</strong> temperatures in excess of accepted comfort limits. A risk with<br />

such a strategy is, however, that significant vertical temperature gradient between feet<br />

and head height can lead <strong>to</strong> discomfort and this must be considered when designing<br />

such a system.<br />

Mixed flow <strong>ventilation</strong> is essentially a "mixing" process in which stale warm room air is<br />

continually diluted by cooled fresh air. The air in the room is fully mixed and therefore air<br />

temperature and pollutant concentrations are uniform throughout the space. Fresh air is<br />

normally introduced and removed at ceiling level and the interaction of upward warm air<br />

currents and horizontal supply air jets below the ceiling causes mixing and circulation <strong>to</strong><br />

lower areas with relatively high air speeds (see Figure 2). This can lead <strong>to</strong> draughts and<br />

discomfort in the occupied area. Because air is supplied and extracted at ceiling level<br />

some of the supplied ‘fresh’ air may short circuit by being drawn in<strong>to</strong> the extract grilles<br />

which effectively reduces its cooling and pollutant dilution potential.


3<br />

supply grill Return grill<br />

Figure 2 Mixed flow <strong>ventilation</strong> – typical room air flow<br />

The air supply temperature for <strong>displacement</strong> <strong>ventilation</strong> systems is typically 19°C<br />

compared <strong>to</strong> 13°C <strong>to</strong> 14°C for most conventional mixing systems. Figure 3 shows the<br />

variation in room air temperature for “ideal” <strong>displacement</strong> <strong>ventilation</strong> in a typical office<br />

environment compared with mixing <strong>ventilation</strong>. Note that in this example there is<br />

approximately 2°C air temperature pick-up between the supply and room air close <strong>to</strong> the<br />

floor due <strong>to</strong> room air entrainment.<br />

Supply air temperature<br />

= 14 o C<br />

9 o C<br />

<strong>Air</strong> temperature near<br />

head height for seated<br />

occupants = 23 o C<br />

Supply air temperature<br />

= 19 o C<br />

Room & extract air<br />

temperature = 23 o C<br />

7 o C<br />

Mixing<br />

<strong>ventilation</strong><br />

12 14 16 18 20 22 24 26 28 30 o C<br />

Extract air temperature<br />

= 26 o C<br />

Displacement<br />

<strong>ventilation</strong><br />

Figure 3 Supply and extract air temperatures for mixed flow and <strong>displacement</strong><br />

<strong>ventilation</strong> (ideal situation)


“Free cooling” opportunities<br />

Supplying air at 19°C <strong>to</strong> a <strong>displacement</strong> <strong>ventilation</strong> system opens up the possibility of<br />

<strong>using</strong> fresh air “free-cooling” for large parts of the year. “Free cooling” is rather a<br />

misleading term as energy will always be needed for fan (and in some cases pump)<br />

operation. In cold weather a heat reclaim thermal wheel or heat exchanger is essential<br />

in order <strong>to</strong> minimise the need for pre-heating of the fresh-air supply. Where there is a<br />

requirement for dehumidification in warm weather a separate low temperature coil may<br />

be required, possibly in conjunction with heat pipe heat recovery and pre-cooling, or face<br />

and bypass dampers.<br />

A bin analysis of annual outdoor dry bulb temperature allows the potential of fresh air<br />

free-cooling <strong>to</strong> be investigated. Figure 4 shows the number of hours occurrence of<br />

outdoor air temperatures for normal working hours (0700 <strong>to</strong> 1800) during a whole year,<br />

based on the average of the five year period 1976 <strong>to</strong> 1980. The effect of a year with a<br />

hot summer is also shown by plotting hours occurrence for 1976 which had an<br />

exceptionally long hot summer. The data can be interpreted more easily by converting it<br />

<strong>to</strong> an accumulated frequency “s-curve”, shown in Figure 5. This allows the proportion of<br />

the <strong>to</strong>tal hours that were at and below a certain threshold temperature <strong>to</strong> be read directly<br />

from the graph. To take account of heat pick up from the air distribution fan (assumed <strong>to</strong><br />

result in a 1°C rise in the air stream) it is appropriate <strong>to</strong> take 12°C for a conventional<br />

mixing <strong>ventilation</strong> system and 18°C for a <strong>displacement</strong> system. The s-curve therefore<br />

shows that fresh-air free-cooling can be used for 85% of the time for a <strong>displacement</strong><br />

system but only 53% of the time for a conventional mixing <strong>ventilation</strong> system.<br />

4<br />

Total hours occurence<br />

350<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

0<br />

-8<br />

Five year average, 1976<br />

<strong>to</strong> 1980<br />

-5<br />

-2<br />

1<br />

Dry Bulb T (07:00 - 18:00)<br />

Kew 1976 <strong>to</strong> 1980<br />

4<br />

7<br />

10<br />

13<br />

16<br />

19<br />

22<br />

Dry Bulb Temperature (oC)<br />

Figure 4 Bin analysis of outdoor dry bulb air temperature<br />

25<br />

28<br />

31<br />

34


5<br />

Accumated frequency (% hours occurrence)<br />

110%<br />

100%<br />

90%<br />

80%<br />

70%<br />

60%<br />

50%<br />

40%<br />

30%<br />

20%<br />

10%<br />

0%<br />

85%<br />

53%<br />

Dry bulb temperature (whole year, 0700 <strong>to</strong> 1800 hrs)<br />

12 o C 18 o C<br />

-5 0 5 10 15 20 25 30 35<br />

Dry bulb temperature (oC)<br />

1977 cool summer<br />

1976 hot summer<br />

1976 <strong>to</strong> 1980


Figure 5 S-curves for occurrence of outdoor dry bulb temperatures<br />

Additional s-curves for years with a hot summer (1976) and a cool summer (1977) have<br />

also been plotted. These show that a hot summer would reduce the time that fresh air<br />

can be used for the <strong>displacement</strong> system from 85% <strong>to</strong> about 78% of the time. A cool<br />

summer would increase the proportion of the year that free-cooling is available <strong>to</strong> about<br />

90% of the <strong>to</strong>tal time.<br />

Thermal comfort requirements<br />

Thermal comfort requirements place limitations on the design parameters and the<br />

maximum cooling performance achievable with <strong>displacement</strong> <strong>ventilation</strong>. For sedentary<br />

occupancy such as office work, BS EN ISO 7730:1995 (7) recommends that air velocity<br />

on<strong>to</strong> people should not normally exceed 0.15 <strong>to</strong> 0.2 m/s, depending on air temperature<br />

and turbulence intensity. The maximum ankle <strong>to</strong> head temperature gradient (between<br />

0.1 m and 1.1 m above the floor) should not normally exceed 2°C <strong>to</strong> 3°C in summer.<br />

The dry resultant temperature in the occupied region should also normally be between<br />

23°C and 26°C. For <strong>displacement</strong> <strong>ventilation</strong> systems air velocity is principally a function<br />

of the air supply volumetric flow rate and temperature, and the degree of room air<br />

entrainment at the diffuser. The ankle <strong>to</strong> head temperature gradient is also a function of<br />

the supply air volumetric flow rate and the degree of room air entrainment at the diffuser.<br />

Obtaining higher cooling performance with <strong>displacement</strong> <strong>ventilation</strong><br />

Conventional design practice and BRE investigations suggest <strong>displacement</strong> <strong>ventilation</strong><br />

systems in offices (with floor <strong>to</strong> ceiling heights below 3 m) are limited <strong>to</strong> around 20/25<br />

W/m 2 cooling capacity. To increase cooling capacity either the supply air temperature<br />

has <strong>to</strong> be reduced, or the volumetric air supply rate must be increased. Reducing the air<br />

supply air temperature below the normal 19°C is not an option when the aim is the<br />

maximisation of free-cooling, and could lead <strong>to</strong> unacceptable thermal discomfort in the<br />

ankle region. Raising the volumetric air supply rate allows a 19°C supply air<br />

temperature <strong>to</strong> be maintained, but increases the risk of high air speed in the occupied<br />

space. Fan power and duct sizing will also be increased and therefore a life cycle<br />

analysis of this compared with the reductions in cooling energy must be undertaken as<br />

part of specific system designs.<br />

Types of <strong>displacement</strong> diffuser<br />

A wide range of diffusers can be used for <strong>displacement</strong> <strong>ventilation</strong>, including the<br />

following:<br />

6<br />

• Wall mounted diffusers<br />

• Corner mounted diffusers<br />

• Free-standing "bin" diffusers<br />

• Floor mounted swirl diffusers<br />

• Fabric “sock” diffusers.<br />

Figure 6 shows typical air outflow profiles with these diffusers. Fabric sock diffusers are<br />

not yet widely used and are rare in offices in the UK. Wall, corner and free-standing<br />

diffusers typically consist of a perforated plate with an internal baffle <strong>to</strong> promote even air


discharge through the perforated plate face. The active surface areas are usually quite<br />

large without taking up excessive amounts of floor space.<br />

Floor mounted diffusers can normally provide either vertical or horizontal discharge.<br />

Horizontal discharge is usually used for <strong>displacement</strong> applications and this typically<br />

produces a horizontal circular swirling jet. These diffusers are often 150 mm or 200 mm<br />

diameter. This restricted size leads <strong>to</strong> relatively higher discharge or face velocities than<br />

the other types of diffuser.<br />

7<br />

Corner <strong>displacement</strong><br />

diffuser<br />

Wall mounted<br />

<strong>displacement</strong> diffuser<br />

Free standing “bin”<br />

<strong>displacement</strong> diffuser<br />

Figure 6 Outflow air profiles of typical <strong>displacement</strong> <strong>ventilation</strong> diffusers<br />

Floor mounted swirl<br />

<strong>displacement</strong> diffuser<br />

Floor diffusers appear <strong>to</strong> be a very popular choice for new commercial office buildings,<br />

despite the fact that their relative small size conflicts with the <strong>displacement</strong> <strong>ventilation</strong><br />

requirement for air <strong>to</strong> be introduced at low velocity. Their apparent popularity may be<br />

due <strong>to</strong> the installation flexibility offered by floor terminals in conjunction with raised floors,


although there is a risk of low level thermal discomfort if occupants sit <strong>to</strong>o close <strong>to</strong> them.<br />

Limitations of conventional <strong>displacement</strong> diffusers<br />

The primary limitation of <strong>displacement</strong> <strong>ventilation</strong> in dealing with heat loads has been<br />

shown <strong>to</strong> be the amount of air that can be supplied through conventional wall or floor<br />

mounted <strong>displacement</strong> diffusers without ca<strong>using</strong> discomfort due <strong>to</strong> draughts.<br />

The design procedure for the specification of <strong>displacement</strong> <strong>ventilation</strong> diffusers generally<br />

involves defining the distance from the diffuser at which the air speed has decreased <strong>to</strong><br />

between 0.15 and 0.2 m/s (the usual threshold for acceptable thermal comfort), and may<br />

be measured at around 0.1 m above the floor.<br />

BRE has tested a range of conventional <strong>displacement</strong> <strong>ventilation</strong> diffusers including a<br />

swirl <strong>displacement</strong> diffuser and a floor-standing “bin” diffuser. The swirl diffuser had an<br />

active area of 0.125 m 2 (overall diameter = 0.25 m) at a range of air supply volumetric<br />

rates. The results for air speed at 1.07 m from the center of the diffuser are shown in<br />

Figure 7. This shows that the diffuser air supply limit for acceptable thermal comfort<br />

(maximum air speed of 0.15 m/s at 1.07 m from the diffuser and 0.05m above the floor)<br />

is about 30 l/s. Assuming that the diffuser is installed in a space with 3.0 m spacing<br />

between diffusers (9 m 2 floor area per diffuser) and a supply and extract air differential of<br />

6°C (19°C air supply, 25°C extract and about 24°C in the occupied region) the cooling<br />

performance would be 24 W/m 2 .<br />

8<br />

Height (m)<br />

0.30<br />

0.25<br />

0.20<br />

0.15<br />

0.10<br />

0.05<br />

Variation of mean air speed with height at 1.07 m from centre of diffuser<br />

(0.25 m dia floor swirl)<br />

maximum air<br />

speed for<br />

acceptable<br />

thermal comfort<br />

Diffuser A, 10 l/s<br />

Diffuser A, 30 l/s<br />

Diffuser A, 50 l/s<br />

0.00<br />

0.00 0.05 0.10 0.15 0.20<br />

Mean air speed (m/s)<br />

0.25 0.30 0.35 0.40<br />

Figure 7 Swirl diffuser – air speed at 1.07 m from diffuser centre (0.05 m above the<br />

floor)


The bin diffuser was constructed from perforated steel plate and had a height of 0.61 m<br />

and a diameter of 0.20 m, giving an active face area of 0.38 m 2 . Figure 8 shows air<br />

speed at a distance of 1.07 m from the center of the diffuser for a range of air volumetric<br />

supply rates. It is clear that for acceptable thermal comfort (based on air speed in the<br />

space at 0.05 m above the floor) the limit of this diffuser is 50 l/s. It is very unlikely that<br />

in a commercial office space free-standing diffusers could be as close as the 3 m<br />

spacing assumed for the swirl diffusers. Assuming a wider spacing of 4 m and the same<br />

assumptions for air temperatures as for the swirl diffuser the limit on cooling<br />

performance is about 20 W/m 2 . Larger free-standing diffusers would allow higher air<br />

volume supply rates and therefore provide a higher cooling performance than this but<br />

would take up greater floor area.<br />

9<br />

Height (m)<br />

0.30<br />

0.25<br />

0.20<br />

0.15<br />

0.10<br />

0.05<br />

Variation of mean air speed with height at 1.07 m from centre of diffuser<br />

(0.61 m (h) x 0.2 (d) "bin" diffuser)<br />

maximum air<br />

speed for<br />

acceptable<br />

thermal comfort<br />

Diffuser C, 30 l/s<br />

Diffuser C, 50 l/s<br />

Diffuser C, 100 l/s<br />

0.00<br />

0.00 0.05 0.10 0.15 0.20<br />

Mean air speed (m/s)<br />

0.25 0.30 0.35 0.40<br />

Figure 8 “Bin” diffuser – air speed at 1.07 m from diffuser centre (0.05 m above<br />

the floor)<br />

A typical wall diffuser, shown in Figure 9, (dimensions 1.2 m high and 0.75 m wide) has<br />

been tested. The diffuser was supplied with 130 l/s of air at 19°C and the thermal load in<br />

the 7.5 m x 5.5 m test cell was 1000 W or 24 W/m 2 .


Figure 9 Typical perforated plate wall diffuser<br />

Figure 10 shows the vertical variation of air speed at various distances from the diffuser<br />

and Figure 11 shows the vertical variation of dry bulb air temperature (along a traverse<br />

line perpendicular <strong>to</strong> the diffuser). <strong>Air</strong> speed exceeds 0.2 m/s at 0.1 m height above the<br />

floor within 2.7 m from the diffuser. Vertical air temperature gradient between ankle and<br />

seated head height exceeds 3°C close <strong>to</strong> the diffuser but is 3°C or lower further away.<br />

Height above floor (m)<br />

10<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

3.36 m from end of room<br />

Maximum air<br />

speed for<br />

acceptable<br />

thermal comfort<br />

0.5m from side wall<br />

1.2m from side wall<br />

2.2m from side wall<br />

2.7m from side wall<br />

3.2m from side wall<br />

4.5m from side wall<br />

0<br />

0 0.05 0.1 0.15 0.2<br />

<strong>Air</strong> speed ( m/s)<br />

0.25 0.3 0.35 0.4<br />

Figure 10 Wall diffuser (130 l/s) – air speed


height above floor (m)<br />

11<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0.5m from side wall<br />

1.2m from side wall<br />

2.2m from side wall<br />

2.7m from side wall<br />

3.2m from side wall<br />

4.5m from side wall<br />

3.36 m from end of room<br />

dT ~ 3 K<br />

0<br />

18 19 20 21 22<br />

<strong>Air</strong> temperature (oC)<br />

23 24 25 26<br />

Figure 11 Wall diffuser (130 l/s) – dry bulb air temperature<br />

A higher thermal load would require another diffuser. An earlier test with the same<br />

diffuser in a 3.2 m x 6.5 m test cell with a similar thermal load but a smaller floor area<br />

(equivalent <strong>to</strong> 54 W/m 2 ) showed similar results, and that acceptable thermal comfort<br />

could be achieved in the space outside the diffuser outflow zone. However, with a<br />

smaller test cell floor area the relative size of the outflow zone is larger which reduces<br />

the area that has acceptable thermal comfort for sedentary office work.<br />

Displacement <strong>ventilation</strong> diffuser air entrainment<br />

The degree of room air entrainment in the diffuser outflow is an important characteristic<br />

of <strong>displacement</strong> <strong>ventilation</strong> diffusers and affects the volume and velocity of the outflow<br />

beyond approximately 1 m from the diffuser face. For example, floor swirl diffusers and<br />

wall diffusers with small perforations tend <strong>to</strong> produce higher levels of room air<br />

entrainment. The outflow air volume for a typical perforated panel diffuser is shown in<br />

Figure 12. Each hole creates a small jet, which entrains some room air. For a given<br />

supply volumetric airflow rate reducing the degree of perforation increases the level of<br />

entrainment and therefore the volume of the air outflow at 1 m from the diffuser.<br />

The effect of entrainment is <strong>to</strong> increase the amount of mixing between supply and room<br />

air and this raises the temperature of the low level cool air pool. High levels of<br />

entrainment can allow a lower air supply temperature without significantly increasing the<br />

risk of cold temperatures around the legs and feet. However, the resulting higher levels<br />

of room air mixing will tend <strong>to</strong> disrupt the stratified <strong>displacement</strong> <strong>ventilation</strong> room airflow<br />

pattern and result in a largely mixed lower zone. This may cause a reduction in air<br />

quality, and there may also be a risk of draught discomfort due <strong>to</strong> higher air speeds and<br />

air turbulence intensity.


Figure 12 <strong>Air</strong> flow pattern with perforated panel diffusers<br />

12<br />

Little air is entrained in<br />

the primary flow<br />

<strong>Air</strong> is is entrained entrained at at the the the<br />

the<br />

boundary surface between the<br />

outflowing air and the room air.<br />

Figure 13 <strong>Air</strong> flow pattern with filter-mat or fabric type diffuser<br />

An alternative <strong>to</strong> perforated plates is <strong>to</strong> use fabric or filter mat based diffusers. Such<br />

diffusers create very little air entrainment at the diffuser face, entraining a small volume<br />

of room air at the boundary surface between the outflowing air and the room air. Overall<br />

they produce low levels of room air entrainment which results in lower air speed and<br />

turbulence in the occupied region (see Figure 13). However, because of the lack of<br />

mixing with room air, the cool pool of air at floor level will be closer <strong>to</strong> the supply air<br />

temperature, which may result in discomfort at foot/ankle level. This may be increased if<br />

the supply air temperature is reduced or the volumetric supply rate is raised <strong>to</strong> increase<br />

cooling performance.<br />

The effect of varying diffuser room air entrainment on the air temperature in the lower<br />

occupied zone is shown in Figure 14. High entrainment increases the temperature rise<br />

of the supply air as it is discharged from the diffuser. This mixing reduces the “undertemperature”<br />

of air within the diffuser outflow zone. Under-temperature is defined as the<br />

temperature difference between the air within the diffuser outflow zone and room


temperature (in the occupied region). However, when the aim is <strong>to</strong> supply the air at the<br />

highest possible temperature <strong>to</strong> maximise free cooling a high entrainment diffuser is<br />

undesirable as it raises the air temperature in the lower occupied zone. To maximise<br />

free cooling it is therefore preferable <strong>to</strong> use a low entrainment diffuser.<br />

13<br />

height above floor (m)<br />

3.0<br />

2.5<br />

2.0<br />

1.5<br />

1.0<br />

0.5<br />

Supply air<br />

temperature<br />

Little entrainment<br />

Moderate entrainment<br />

A lot of entrainment<br />

Room air<br />

temperature<br />

Extract air<br />

temperature<br />

0.0<br />

18 19 20 21 22 23 24 25 26 27 28<br />

<strong>Air</strong> temperature (oC)<br />

Figure 14 Variation of room air temperature with height (for diffusers with varying<br />

room air entrainment) – based on practical experience<br />

Extending the cooling performance of <strong>displacement</strong> <strong>ventilation</strong> systems<br />

The results of BRE testing a range of existing <strong>displacement</strong> <strong>ventilation</strong> diffusers has<br />

demonstrated that as the air supply rate is increased, above 30 l/s for a floor swirl<br />

diffuser and 50l/s for a bin diffuser, the air velocities at approximately 1m from the<br />

diffuser exceeded the maximum air velocity acceptable for thermal comfort. Such supply<br />

airflow rates represent cooling loads of less than 25 W/m 2 for a practical office<br />

configuration and temperature differential. Higher cooling loads could be met by<br />

increasing the number of diffusers for a given floor area but this would reduce the usable<br />

floor area with acceptable thermal comfort.<br />

Tests with a conventional wall diffuser showed that 24 W/m 2 could be achieved without<br />

ca<strong>using</strong> discomfort in the occupied space outside the diffuser outflow zone. Space<br />

permitting a second diffuser could be used <strong>to</strong> allow the thermal load <strong>to</strong> be increased <strong>to</strong><br />

around 50 W/m 2 . The diffuser is nevertheless fairly large and takes up a significant<br />

amount of wall space, and has a relatively large outflow zone in which occupants are<br />

likely <strong>to</strong> experience thermal discomfort when involved in sedentary office work. A wall<br />

diffuser would also be unsuitable for large open plan areas and in such situations<br />

appropriately designed bin diffusers would need <strong>to</strong> be used instead.<br />

Based on these results, therefore, the generally held belief that <strong>displacement</strong> <strong>ventilation</strong><br />

is only applicable <strong>to</strong> commercial buildings with modest cooling loads is only partially true.


It appears that appropriately designed and located diffusers are capable of meeting large<br />

cooling loads, albeit with some impact on space utilisation flexibility due <strong>to</strong> the space<br />

taken up by the diffusers and the impact on thermal comfort in the diffuser outflow<br />

zones. Thermal comfort in the diffuser outflow zones is especially critical for sedentary<br />

office work but may well be acceptable for circulation areas or areas around<br />

pho<strong>to</strong>copiers or drink dispensers which are only occupied for short times.<br />

Fabric diffusers<br />

Earlier work elsewhere (8) has shown considerable promise in the use of fabric diffusers<br />

<strong>to</strong> provide higher air flow rates without ca<strong>using</strong> thermal discomfort from draughts. The<br />

results suggested that fabric diffusers positioned along the bot<strong>to</strong>m of two opposite walls<br />

of a room could deal with heat loads of around 50 W/m 2 without ca<strong>using</strong> high air<br />

velocities in the occupied space. A recent case study (9) used fabric diffusers in a<br />

restaurant <strong>to</strong> overcome a high heat load from the occupants (56 W/m 2 ) and <strong>to</strong> provide a<br />

high fresh air flow rate <strong>to</strong> overcome indoor air pollution from smokers (30 l/s/person).<br />

Fabric diffusers were selected on the basis that they provided a high surface area <strong>to</strong><br />

supply a high flow rate without risk of excessive draught or noise.<br />

Fabric socks can be manufactured in virtually any shape and size. BRE has tested an<br />

experimental fabric sock that was manufactured from polyester/cot<strong>to</strong>n fabric with a<br />

quadrant cross section so that it would fit in<strong>to</strong> the skirting board position at the bot<strong>to</strong>m of<br />

a long wall, see Figure 15. The aim was <strong>to</strong> provide a large surface area <strong>to</strong> allow high<br />

supply-air volumetric flow rates without ca<strong>using</strong> excessively high discharge air speeds or<br />

noise, but without taking up <strong>to</strong>o much floor space. The sock dimensions were 4.25 m<br />

long, 200 mm high and 200 mm wide. It was retained in position by two sewn-in plastic<br />

beads which clipped in<strong>to</strong> channels fixed <strong>to</strong> the wall and floor. <strong>Air</strong> was supplied in<strong>to</strong> the<br />

sock through an opening at one end from a flexible duct. The fabric created sufficient<br />

internal pressure for the discharge air flow <strong>to</strong> be essentially constant along the length of<br />

the sock.<br />

Figure 15 Fabric sock diffuser (smoke visualisation of outflow shown on right)<br />

The sock was tested at two air flow rates, 130 l/s and 260 l/s and 19°C air temperature.<br />

At the higher air flow rate the test room heat load was 2000 W which was equivalent <strong>to</strong><br />

48 W/m 2 in a BRE mock-up of a typical office space.<br />

14<br />

200 mm<br />

200 mm


Figure 16 shows the vertical variation of air temperature at different distances from the<br />

sock following a floor traverse perpendicular <strong>to</strong> the sock and starting about 0.5 m from<br />

one end of the sock. The temperature gradient between ankle and head height (0.1 <strong>to</strong><br />

1.1 m for a seated person) was 3.5°C at 1.2 m from the sock and 2.5°C at 2.2 m from<br />

the sock. This is on the limit of what is recommended as being acceptable by BS EN<br />

ISO 7730 for normal office activity and clothing levels. The traverse from the centre of<br />

the diffuser showed a higher temperature gradient (4.5°C at 1.2 m and 3.0°C at 2.2 m).<br />

Therefore according <strong>to</strong> standard BS EN ISO 7730 occupants sitting close <strong>to</strong> the diffuser<br />

may experience some thermal discomfort.<br />

height above floor (m)<br />

15<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0.5m from diffuser<br />

1.2m from diffuser<br />

2.2m from diffuser<br />

2.7m from diffuser<br />

3.2m from diffuser<br />

4.5m from diffuser<br />

2.4m from end of room<br />

Traverse 0.5 m from end of diffuser<br />

dT ~ 3.5K @ 1.2 m<br />

(dT ~ 2.5K @ 2.2 m)<br />

0<br />

18 19 20 21 22 23 24 25 26 27 28<br />

<strong>Air</strong> temperature (oC)<br />

Figure 16 Variation of air temperature with height at 260 l/s (48 W/m 2 )<br />

BS EN ISO 7730 relates the maximum acceptable air velocity <strong>to</strong> the air temperature and<br />

turbulence intensity as well as the occupants' activity and clothing levels. Taking in<strong>to</strong><br />

account these fac<strong>to</strong>rs, and assuming typical office activity and clothing, the maximum<br />

recommended air velocity is between 0.15 and 0.2 l/s. Figure 17 shows that air speed is<br />

well within this limit.<br />

Overall the fabric sock diffuser has provided acceptable thermal comfort in most of the<br />

room for normal sedentary office work, apart from close <strong>to</strong> the centre of the diffuser.


Height above floor (m)<br />

16<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

2.24 m from end of room<br />

Traverse 0.5 m from end of diffuser<br />

0.5m from diffuser<br />

1.2m from diffuser<br />

2.2m from diffuser<br />

2.7m from diffuser<br />

3.2m from diffuser<br />

4.5m from diffuser<br />

Maximum air<br />

speed for<br />

acceptable<br />

comfort<br />

0.15 <strong>to</strong> 0.2 m/s<br />

0<br />

0 0.02 0.04 0.06 0.08 0.1<br />

<strong>Air</strong> speed ( m/s)<br />

0.12 0.14 0.16 0.18 0.2<br />

Figure 17 Variation of air speed at 260 l/s (48 W/m 2 )<br />

BRE also tested an experimental fabric bin diffuser which was constructed from the<br />

same polyester/cot<strong>to</strong>n fabric as the sock, see Figure 18. The dimensions of the bin were<br />

700 mm diameter and 740 mm high which gave a similar active area as the fabric sock.<br />

Supply air was fed through the bot<strong>to</strong>m of the diffuser by a flexible duct run through the<br />

underfloor void. The bin was located in the centre of the room.<br />

The fabric bin was tested at the same air flow rates and supply air temperature as for the<br />

fabric sock, 130 l/s and 260 l/s and 19°C air temperature. At the higher air flow rate the<br />

test room heat load was 2000 W which was equivalent <strong>to</strong> 48 W/m 2 . <strong>Air</strong> speed and air<br />

temperature were measured throughout the room space by traversing with multiple<br />

transducer poles.


Figure 18 Fabric bin diffuser (smoke visualisation of outflow shown on right)<br />

Figure 19 shows the vertical variation of air temperature at various points along a<br />

traverse across the width of the test room. The middle of the traverse was<br />

approximately 1.5 m from the diffuser. The measured temperature gradient between<br />

ankle and head height (0.1 <strong>to</strong> 1.1 m for a seated person) at the closest position <strong>to</strong> the<br />

diffuser (1.5 m) was 3.2°C. This is just on the limit of what is recommended as being<br />

acceptable by BS EN ISO 7730 for normal office activity and clothing levels. However,<br />

elsewhere the temperature gradient was around 2°C which is within the comfort limit.<br />

17<br />

height above floor (m)<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0.5m from side wall<br />

1.2m from side wall<br />

2.2m from side wall<br />

2.7m from side wall<br />

3.2m from side wall<br />

4.5m from side wall<br />

2.4m from end of room<br />

Middle of traverse ~1.5 m from diffuser<br />

dT ~ 3K at point<br />

nearest <strong>to</strong> diffuser<br />

0<br />

18 19 20 21 22 23 24 25 26 27 28<br />

<strong>Air</strong> temperature (oC)<br />

Figure 19 Variation of air temperature with height at 260 l/s (48 W/m 2 )<br />

Figure 20 shows the vertical variation of air speed. <strong>Air</strong> speed was well below the<br />

recommended maximum value given by BS EN ISO 7730.


Figure 20 Variation of air speed at 260 l/s (48 W/m 2 )<br />

Comparison of the test results from these two diffusers showed that overall the fabric bin<br />

diffuser provided a higher level of thermal comfort in the test room than provided by the<br />

fabric sock diffuser. This was largely due <strong>to</strong> the greater vertical temperature gradient<br />

close <strong>to</strong> the middle of the sock diffuser. The regions of high temperature gradient shown<br />

<strong>to</strong> exist close <strong>to</strong> both of the diffusers are a direct result of the low levels of room air<br />

entrainment in this region. The air temperature at a height of 1.1m is relatively constant<br />

throughout each of the test mock-ups and is a function of supply airflow rate and thermal<br />

load in the space. Therefore, the vertical gradient is greatest in the diffuser outflow zone<br />

where the cool supply air enters the room and undergoes little mixing with the room air.<br />

The diffuser outflow zone is largest at the middle of the sock diffuser as it is essentially a<br />

single sided diffuser whereas the bin has an unrestricted radial discharge. This effect is<br />

illustrated in Figure 21 below.<br />

The size of the outflow zones, and therefore the size of the areas around the diffusers<br />

with relatively poor thermal comfort, would be smaller with lower cooling loads. The<br />

cooling load assumed in this study is 48 W/m 2 which is deliberately on the high side of<br />

the cooling loads found in typical office buildings.<br />

18<br />

Height above floor (m)<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

2.24 m from end of room<br />

Middle of traverse ~1.5 m from diffuser<br />

Maximum air<br />

speed for<br />

acceptable<br />

comfort<br />

0.15 <strong>to</strong> 0.20 m/s<br />

0.5m from side wall<br />

1.2m from side wall<br />

2.2m from side wall<br />

2.7m from side wall<br />

3.2m from side wall<br />

4.5m from side wall<br />

0<br />

0 0.05 0.1 0.15 0.2<br />

<strong>Air</strong> speed ( m/s)<br />

0.25 0.3 0.35 0.4


19<br />

Limit of zone with<br />

high vertical<br />

temperature gradient<br />

1.5 m<br />

Limit of zone with<br />

high vertical<br />

temperature gradient<br />

Figure 21 Outflow size from fabric sock and bin diffusers<br />

Conclusions<br />

It has been shown that the limitations of many existing <strong>displacement</strong> diffusers for<br />

meeting high cooling loads include the maximum volumetric air supply rate that can be<br />

achieved without ca<strong>using</strong> discomfort <strong>to</strong> the occupants, and the maximum number of<br />

diffusers that can be installed in a given space without reducing the area that can be<br />

occupied by people. Large wall diffusers have been shown <strong>to</strong> be capable of satisfying<br />

cooling loads as high as 50-55 W/m 2 without ca<strong>using</strong> thermal discomfort outside the<br />

diffuser outflow zone. However, the diffuser outflow zone will be relatively large and this<br />

would reduce the practicality of <strong>using</strong> such a diffuser for large loads, especially in<br />

buildings where the occupants were mainly involved in sedentary office type work.<br />

Alternatively it might be possible <strong>to</strong> arrange for the outflow zones <strong>to</strong> be used for general<br />

circulation areas which have less stringent criteria for acceptable thermal comfort. A<br />

cooling performance of 50-55 W/m 2 would be sufficient for the cooling requirements in<br />

the core zones of most normal office buildings. Bin diffusers would have <strong>to</strong> be used<br />

instead of wall diffusers in large open plan areas and the space that they would take up<br />

would further reduce the usable floor area.<br />

Testing of a range of innovative fabric diffusers showed that a cooling performance<br />

around 50 W/m 2 could be achieved. This performance was in part achieved by utilising<br />

the low entrainment characteristic of fabric as part of the diffusers, which allows<br />

relatively high volumetric supply rates without ca<strong>using</strong> unacceptably high air speeds. A<br />

disadvantage of minimal mixing and entrainment of the room air with supply air at the<br />

diffuser is high ankle <strong>to</strong> head temperature gradients which could exceed the limit of<br />

acceptability for people engaged in sedentary office type work in quite a large floor area<br />

around the diffuser (the diffuser “outflow zone”).<br />

The degree of under temperature and the size of the diffuser outflow zone, as well as the<br />

air velocity are all issues that need <strong>to</strong> be addressed very carefully be designers when<br />

choosing a diffuser for an application. At present little information exists on the extent or<br />

range of acceptable under temperature regions and adoption of low air entrainment<br />

diffusers would require detailed physical mock-ups <strong>to</strong> confirm suitability before<br />

installation.<br />

The supply air temperature used throughout the testing was 19°C, which should allow<br />

free air cooling for about 85% of the year in south-east England. This might drop <strong>to</strong><br />

1.5 m


about 78% in a year with a very hot summer, but should be higher in more northerly UK<br />

locations.<br />

The improvement in <strong>displacement</strong> <strong>ventilation</strong> cooling performance was achieved by<br />

increasing the air supply volumetric rate, which entails increased <strong>ventilation</strong> fan power<br />

and larger duct sizes. This must be taken in<strong>to</strong> account when determining the overall<br />

benefit of <strong>using</strong> <strong>displacement</strong> <strong>ventilation</strong> for cooling.<br />

A practical consideration of <strong>using</strong> bin and sock fabric diffusers is the floor space taken<br />

up. In large open plan areas the bin diffuser could be located around structural columns,<br />

and there is no reason why fabric diffusers could not be located inside partition walls.<br />

Another possibility is <strong>to</strong> incorporate fabric in<strong>to</strong> floor grill type diffusers. Preliminary tests<br />

showed that this produces low entrainment air discharge and may offer a practical<br />

alternative <strong>to</strong> socks and bins.<br />

Acknowledgements<br />

Some of the work described in the paper has been supported by the DTI’s Partners in<br />

Innovation research programme and industry sponsors, including, Arup Research &<br />

Development, CIBSE, IPS Ventilation Ltd, Gilberts (Blackpool) Ltd, Hal<strong>to</strong>n Products Ltd,<br />

Hoare Lea, Oscar Faber, Troup Bywaters & Anders, Trox (UK) Ltd and Waterloo <strong>Air</strong><br />

Management PLC.<br />

References<br />

20<br />

1. Wyon D P and Standberg M. Thermal Manikin Prediction Of Discomfort Due To<br />

Displacement Ventilation. ASHRAE Trans., 96 (17), 67-75, 1990.<br />

2. Alamdari F, Bennett K M, Rose P M. Displacement Ventilation Performance –<br />

office space application. Technical Note TN 3/93, BSRIA, 1993.<br />

3. Alamdari F and Eagle N. Displacement Ventilation And Chilled Ceilings.<br />

Technical Note TN 2/96, BSRIA, 1996.<br />

4. Breum N O. Ventilation Efficiency In An Occupied Office With Displacement<br />

Ventilation – A Labora<strong>to</strong>ry Study. Environmental International, 18, 353-361,<br />

1992.<br />

5. Breum N O, Helbo F and Laustesen O. Dilution Versus Displacement Ventilation<br />

– An Intervention Study. Annals of Occupational Hygiene, 33(3), 321-329, 1989.<br />

6. Ørchede E, Breum N O and Skov T. Perceived And Measured Indoor Climate<br />

With Dilution Versus Displacement Ventilation: An Intervention Study In A<br />

Sewing Plant. Indoor <strong>Air</strong>, 1996.<br />

7. BS EN ISO 7730: 1995. Moderate thermal environments – Determination of the<br />

PMV and PPD indices and specification of the conditions for thermal comfort.<br />

British Standards Institute, London, 1995.<br />

8. Geens A J, Graham M S and Alamadari F. Displacement <strong>ventilation</strong> applications<br />

– an alternative view. 1997 CIBSE National Conference.<br />

9. Cullen N. High performance <strong>displacement</strong> <strong>ventilation</strong> <strong>using</strong> fabric diffusers – a<br />

case study. 2000 ASHRAE CIBSE joint conference, Dublin, 2000.

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