influence of floor plenum on energy performance of
TRANSCRIPT
1
Influence of floor plenum on energy performance of buildings with 1
UFAD systems 2
Yan Xue1 and Qingyan Chen2,1* 3
4 1School of Mechanical Engineering, Purdue University, West Lafayette, IN 47907, USA 5
2School of Environmental Science and Engineering, Tianjin University, Tianjin 300072, China 6 *Tel. (765)496-7562, Fax (765)494-0539, Email: [email protected]
8
Abstract 9
10
The heat transfer through the floor slab in buildings with Under-Floor Air Distribution (UFAD) 11
systems may have a negative impact on the energy performance of these buildings, although very 12
few studies have been reported in the literature. By using an energy simulation program, 13
EnergyPlus, this investigation compared the energy use in a Philadelphia office building with a 14
UFAD system to that with a well-mixed ventilation system. When the heat transfer through the 15
floor slab was taken into consideration, the thermal load of the building with the UFAD system 16
was higher than with the well-mixed system. On the other hand, the higher supply air 17
temperature of the UFAD system enables the use of more free-cooling. The annual energy 18
consumption by the chillers in the building with the UFAD system was 16%-27% lower than 19
with the well-mixed system, but energy consumption by the boiler was 12%-30% higher, and the 20
energy consumption by the fan was 22-50% higher, depending on the manner in which the heat 21
was supplied to the floor plenum. When the UFAD system was used with an un-ducted floor 22
plenum and without heating coils under the diffusers, it consumed slightly more energy than the 23
well-mixed system. 24
25
1. Introduction 26
27
Unlike conventional overhead well-mixed systems, UFAD systems provide directly conditioned 28
air to the occupied zone through diffusers in a raised floor, as shown in Figure 1. Thermal 29
buoyancy causes temperature stratification in the occupied zone, and the air temperature in the 30
lower part of the zone is lower than that in the upper part. Therefore, UFAD systems are believed 31
to use less energy for cooling [1,2]. In addition, the thermal stratification in a room with a UFAD 32
system can create better indoor air quality than in a room with a well-mixed air distribution 33
system [3,4]. A UFAD system also allows individual control of airflow rate in order to meet the 34
thermal comfort requirements of different occupants [5,6] and can thus provide a more 35
comfortable environment than overhead well-mixed systems [7]. However, if the air supply and 36
return in the plenums are un-ducted or un-insulated, the air temperature in the floor plenum is 37
very low during the cooling mode, while the ceiling plenum is very warm. The temperature 38
Xue, Y. and Chen, Q. 2014. “Influence of floor plenum on energy performance of buildings
with UFAD systems,” Energy and Buildings, 79, 74-83.
2
difference between the floor plenum and downstairs ceiling plenum leads to heat transfer across 39
the floor slab, as shown in Figure 1,which may have an impact on energy use. 40
41
Studying the influence of the floor plenum on cooling load and energy use requires that the 42
energy flow between the occupied zone and the floor plenum also be considered, so do the 43
thermal stratification in the occupied zone [8]. Many previous researchers have analyzed the 44
thermal stratification, and various models have been developed to predict the air temperature 45
stratification in rooms with UFAD systems [9-15]. Air flow and heat transfer in the floor plenum 46
contribute further complexity to the simulations. Linden [16] determined that there was a 47
significant air temperature differential and air velocity variation in the floor plenum. These non-48
uniform air temperature and flow distributions could affect heat transfer in the floor plenum. 49
50
In regard to the impact of the floor plenum on the energy performance of a UFAD system, 51
Bauman et al. [17] found that the heat transfer in the floor plenum can be as high as 30%-40% of 52
the room cooling load. However, this conclusion was made on the basis of a simplified first-law 53
model that may not be accurate. Schiavon et al. [8] indicated that the presence of a raised floor 54
changed the cooling load profile greatly, and the peak cooling load could vary in the range of −7 55
to + 40% as compared to the load without the raised floor. However, their study did not address 56
heating. Lee et al. [18] simulated a three-floor office building with a UFAD system on two 57
design days: a summer day and a winter day. They found that thermal decay in the floor plenum 58
could result in a higher supply airflow rate and greater use of energy by the fans and chiller. 59
However, the non-uniform flow in the floor plenum was not taken into account in their study. 60
The current investigation systematically studied the influence of heat transfer through a floor 61
slab on the energy performance of an office building with a UFAD system. The objective was to 62
accurately simulate the thermal load and energy use as influenced by the floor plenum and to 63
assess the impact of non-uniform flow in the floor plenum on energy modeling. 64
65
2. Method 66
67
2.1. Load and energy simulations for an office building 68
69
To accurately study the impact of the floor plenum on energy performance, this investigation 70
used EnergyPlus [19] as the main tool with the implementation of a room air stratification model. 71
To simplify the study, this investigation simulated a typical middle floor, Floor N, in a multi-72
floor building, as shown in Figure 2, rather than an entire building. Accurate simulations must 73
take into account (1) the vertical air temperature stratification in the room air and (2) the non-74
uniform air distribution in the floor plenum. 75
76
3
2.2. Vertical air temperature stratification in the simulated room 77
78
Because the EnergyPlus program did not calculate the room air distribution, the air temperature 79
model from Lin et al. [12], implemented into the program by Liu et al. [20], was applied to 80
calculate the vertical air temperature profiles in the room. The model predicts the vertical 81
temperature profiles by simulating the buoyancy plumes from internal heat sources and the jets 82
from air supply diffusers. The buoyancy plumes generate the air stratification and the jets lead to 83
air mixing. 84
85
2.3. Non-uniform air distribution in the floor plenum 86
87
Along with the air temperature stratification in the room, non-uniform air velocity and air 88
temperature in the floor plenum also contribute additional complexity to the simulation[16]. To 89
simulate the non-uniform flow in the floor plenum, Computational Fluid Dynamics (CFD) can be 90
used in combination with the energy calculation [21,22], but doing so is too computationally 91
demanding. Instead, this investigation used a multizone model [23] to simulate the non-uniform 92
air distribution in the floor plenum for coupling with EnergyPlus. The floor plenum was divided 93
into several subzones according to the temperature distribution determined by CFD simulation. 94
The air velocity and temperature differences among these subzones represented the non-uniform 95
air temperature in the floor plenum. The simulation results of the multizone model were then 96
compared to a single zone model in which the floor plenum had uniform air distribution. The 97
difference between them could indicate the impact of the non-uniform air distribution on the 98
energy modeling. 99
100
2.4. Validation of the computer models 101
102
The computer models described above use a number of approximations, and coupling them with 103
EnergyPlus can lead to additional errors. The models needed to be validated before they could be 104
used to simulate the cooling load and energy use in the building. This investigation used an 105
environmental chamber as shown in Figure 3 to measure the air and surface temperatures in the 106
floor plenum and the surface temperatures in the room. 107
108
This chamber had dimensions of 4.80 m in length, 4.20 m in width, and 2.73 m in height, 109
including a floor plenum with a height of 0.30 m. The room contained several pieces of furniture, 110
lighting fixtures, and heated boxes that were used to simulate internal loads such as electrical 111
appliances, occupants, etc. The supply air duct was connected to the floor plenum, and two linear 112
grille diffusers were installed in the floor. The walls and ceiling were well insulated with a 113
thermal resistance of 5.45 m2-K/W. The raised floor panels were made of 0.1 m thick lightweight 114
concrete with a thermal resistance of 0.16 m2-K/W. A double-glazed window with dimensions of 115
4
4.65 m in width and 1.55 m in height and a thermal resistance of 0.25 m2-K/W was installed in 116
the east wall of the chamber. Table 1 shows the power levels of the internal heat sources. 117
118
Eight anemometers were placed in the middle of the floor plenum (0.15 m from the slab) for 119
measuring air temperature and velocity in the plenum. Temperatures of the different surfaces of 120
the floor plenum and room were measured by a number of T-type thermocouples. The 121
experiment was conducted under steady-state conditions in summer. The inlet temperature was 122
17.3°C, and the air change rate was 6 ACH. 123
124
3. Validation of the computer models and case setup 125
126
3.1. Validation of the computer models 127
128
The CFD simulations for this investigation were performed for the floor plenum using a 129
commercial software program FLUENT [24]. The CFD results provided greater understanding of 130
the temperature distribution in the floor plenum, which was the basis of the multizone model. 131
Figures 4 and 5 show the air velocity and temperature profiles, respectively, in two sections of 132
the floor plenum. The air supply was located on the bottom wall under Position 7, as shown in 133
Figure 6, and therefore Positions 3 and 7 were located in the jet region. As a result, the air 134
velocities measured at these positions were high, and the air temperatures were low. The 135
agreement between the CFD results and experimental data for air velocity and temperature is 136
quite good. Figure 6 shows a non-uniform air temperature distribution in the floor plenum. 137
138
Our EnergyPlus simulation divided the floor plenum into three subzones, as shown in Figure 6, 139
for studying the impact of the non-uniform air temperature distribution on the load. Figure 5 140
depicts the air temperature profiles calculated with the multizone model in the two sections of 141
the floor plenum, and again they are in good agreement with the measured data. The results 142
shown in Figures 5 and 6 have validated the computer models for calculating air temperature in 143
the floor plenum. 144
145
Table 2 further compares the air temperature from the diffusers, air temperature at the exhaust, 146
and EnergyPlus-simulated surface temperatures with the measured data. The columns of "Error" 147
show the percentage difference between the experimental measurements and simulation results. 148
Once again, agreement between the simulations and measurements is quite good. Therefore, the 149
EnergyPlus program with the multizone air models can be used to predict thermal load and 150
energy use in buildings. In addition, Table 2 shows the results obtained by EnergyPlus with the 151
assumption of uniform air temperature in the floor plenum (one subzone). The air temperature 152
with one subzone differed by only 0.5 K from that with three subzones, which was insignificant, 153
although the air temperature between zones can differ by 2 K, as shown in Figure 6. Thus, the 154
5
impact of the non-uniform air distribution in the floor plenum on the energy simulation was very 155
limited and our subsequent simulations used only one zone for the floor plenum. 156
157
3.2. Case description for a building with UFAD systems in Philadelphia 158
159
Using the validated EnergyPlus model, this investigation conducted energy simulations for a 160
mid-level floor of a multi-floor office building in Philadelphia. An office area with dimensions 161
of 30 m 40 m 3.7 m, as shown Figure 7, was divided into five thermal zones: a central zone 162
and four perimeter zones, because solar radiation would have a significant impact on the 163
perimeter zones. The perimeter zones had a width of 5.0 m [25]. The construction and material 164
information for the building envelope were taken from the default data for Chicago in 165
EnergyPlus Version 7. Figure 8 shows the internal load profiles for weekdays and Saturdays. 166
This study further assumed that the building was completely closed on Sundays, without an 167
internal heat load. 168
169
This investigation simulated three different scenarios for the office building, as shown in Figure 170
9: a well-mixed ventilation system, a UFAD system without heating coils in the diffusers, and a 171
UFAD system with heating coils in the diffusers [26]. For each of the two UFAD scenarios, three 172
cases were simulated with different floor plenum configurations: completely ducted floor 173
plenums; partially ducted floor plenums (ducted floor plenums in the perimeter zones and an un-174
ducted core zone); and completely un-ducted floor plenums. The arrangement led to a total of 175
seven simulation cases, as shown in Table 3. All of the cases used the same HVAC system, 176
which incorporated an electric chiller and a gas boiler. The system used variable-air-volume 177
control and an economizer. The thermostat in the occupied zone was set at 21°C during the 178
winter and 24°C during the summer. The minimum fresh air rate was 0.3 L/(s·m2), in accordance 179
with ASHRAE Standard 62.1-2010 for indoor air quality [27]. For mixed ventilation, the supply 180
air temperature was 13°C for cooling and 32°C for heating [28]. In the UFAD system without 181
heating coils in the diffusers, the supply air temperature was 17°C [1,29] for cooling and 32°C 182
for heating. In the UFAD system with heating coils, the air supply temperature from the HVAC 183
system was 17oC all year round. When heating was called for, the air was heated to 32°C by the 184
heating coils. The HVAC system operated from 6:00 to 22:00. 185
186
4. Results 187
188
In order to explain the effects of the heat transfer through slabs on the energy performance of 189
buildings, this section will show the heat flux profiles across slabs and analyze their influence on 190
the thermal loads. Then the year-round energy consumption results will be reported. 191
192
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4.1. Thermal load simulations for the building 193
194
Figure 10 shows the heat flux at the two surfaces of the floor slab in the office building on July 195
21, the summer design day in EnergyPlus. The sum of the heat transfer at the two surfaces is 196
equal to the thermal storage in the slab. For cooling, the heating coils in the diffusers were not 197
activated, and thus the two UFAD scenarios were identical. For the well-mixed system, from 198
8:00 to16:00, heat was transferred from the occupied zone to the slab, as shown in Case 1 of 199
Figure 10(a, b). In the perimeter zones as shown in Figure 10(a), this heat transfer was caused by 200
the high level of radiation from the direct sunlight on the floor slab and the internal heat sources, 201
With the UFAD systems, however, the radiation from the sun and the internal load had no direct 202
impact on the slab. Thus, the heat transfer profiles in these cases were very different from those 203
with the well-mixed system. In the thermal zones with ducted floor plenums, there was a small 204
amount of heat transfer across the floor slabs. As for the un-ducted UFAD systems, cool air was 205
supplied to the floor plenum, and the downstairs ceiling plenum was warm. The significant 206
temperature difference between the two sides of the floor slab led to a high heat transfer rate 207
from the downstairs ceiling plenum to the floor slab and further to the floor plenum. In the well-208
mixed system, from 6:00 to 8:00 and 18:00 to 22:00, when the internal load and solar radiation 209
were small, heat was transferred from the floor slab to the room air as a result of the high floor 210
slab temperature. In the UFAD system, however, the total air supply was lower during these two 211
periods than during the occupied hours, and thus the heat transfer from the floor plenum to the 212
slab was smaller. 213
214
Despite the drastic difference in heat transfer profiles between the well-mixed ventilation and 215
UFAD, the cooling loads of these systems had similar shapes on the summer design day, as 216
shown in Figure 11. 217
218
For the winter heating, the heat transfer between the well-mixed system and UFAD system could 219
be different but the heating load is also very similar as shown in the cooling scenario. Due to 220
limited space in this paper, the detailed results are not presented here. 221
222
4.2. Annual energy consumptions of the building 223
224
Figures 12 and 13 illustrate the monthly energy consumption by the chiller and boiler, 225
respectively, in the HVAC system in year-round simulations. With the well-mixed ventilation 226
system, more energy was used by the chiller, especially during the shoulder seasons when the 227
outdoor air temperature was suitable for free-cooling. In the two UFAD scenarios, the levels of 228
electricity consumption by the chillers were almost identical. They were lower than that in the 229
well-mixed system by 27% for the ducted cases (Cases 2 and 5), 23% for the partially ducted 230
cases (Cases 3 and 6), and 16% for the un-ducted cases (Cases 4 and 7). The percentage numbers 231
are based on the UFAD systems. However, the natural gas consumption levels by the boiler with 232
7
the UFAD systems were higher than that with the well-mixed system. Without heating coils 233
under the diffusers, the boiler energy consumption in the UFAD system was higher than that in 234
the well-mixed system by 18% in the completely ducted case (Case 2), 21% in the partially 235
ducted case (Case 3), and 30% in the un-ducted case (Case 4). When there were heating coils 236
under the diffusers, the boiler energy consumption in the UFAD system was higher than that in 237
the well-mixed system by 12% in the completely ducted case (Case 5) and by 18% in the 238
partially ducted (Case 6) and the un-ducted (Case 7) cases. 239
240
The levels of electricity consumption by the fans in the building’s HVAC system were 22-50% 241
higher with the UFAD systems than with the well-mixed system by using the energy use of the 242
UFAD system as the reference, as shown in Figure 14. This difference occurred because the 243
supply air temperature in the UFAD systems was higher than that in the well-mixed ventilation 244
system, and a higher airflow rate is required in order to remove the same amount of heat. 245
246
A comparison of the different cases indicates that the ducting of floor plenums can reduce energy 247
consumption by the chiller and the boiler, and that this effect is more significant in perimeter 248
zones. Furthermore, during the heating mode, supplying warm air directly to the floor plenum 249
without ducts is not recommended because heat flow in the plenum would cause significant 250
energy loss. In addition to ducting of the floor plenums, the use of heating coils under the 251
diffusers is recommended in order to reduce energy use by the boiler. 252
253
Using the energy consumption data, this investigation conducted a cost analysis for these cases 254
with EnergyPlus. Table 4 shows the monthly price of natural gas [30]. The cost of electricity [30] 255
was calculated using the block method shown in Table 5. The tax rate was 8%, and the monthly 256
service fee for electricity was $8.81. Table 6 shows the annual electricity costs for the chiller and 257
fans and the gas costs for the boiler. For the same building, the use of electricity by lights and 258
electrical equipment was exactly the same with either the well-mixed ventilation or UFAD. 259
Variations in energy consumption arose from the HVAC systems. 260
261
Because only the perimeter zones of the building required heating and natural gas was much 262
cheaper than electricity, the gas costs for the boiler were much lower than the electricity costs for 263
the chiller. As discussed above, energy consumption by the chiller was greater with the well-264
mixed system than with the UFAD systems. Therefore, as shown in Table 6, chiller operation 265
was more expensive in the well-mixed case (Case 1) than in the UFAD cases (Cases 2-6). 266
Among the UFAD cases, those with un-ducted floor plenums (Cases 4 and 7) had higher 267
electricity costs than the other cases. However, the addition of heating coils under the diffusers 268
did not contribute significantly to the electricity costs. 269
270
Although chiller operation was cheaper in the UFAD cases, both the gas costs for the boiler and 271
the electricity costs for the fan were higher with the UFAD systems than with the well-mixed 272
8
system. These higher costs are consistent with the energy consumption levels shown in Figures 273
13 and 14. In the UFAD cases, the addition of heating coils under the diffusers (Cases 5-7) 274
reduced the gas cost for the boiler, especially in the cases with un-ducted floor plenums. The 275
total energy cost for a building with a UFAD system could be lower than that with a well-mixed 276
system if the floor plenum was ducted. Unfortunately, ducting of the floor plenum is not a 277
common practice at present. 278
279
5. Conclusions 280
281
Using validated computer models, this investigation assessed the energy performance of a 282
building in Philadelphia with several different UFAD systems and with a well-mixed ventilation 283
system. The study led to the following major findings: 284
The airflow and air temperature distribution in the floor plenum can be highly non-285
uniform. The non-uniform air temperature distribution can be calculated with the use of a 286
simple subzone model. By comparing the supply air temperature, exhaust air temperature, 287
and enclosure surface temperatures between the multizone model and the single zone 288
model, this study found that the impact of the non-uniform air temperature distribution on 289
the energy modeling is small. 290
In cooling situations, the temperature difference between the cold air in the floor plenum 291
and the warm air in the downstairs ceiling plenum can result in significant heat transfer 292
through the floor slab in a building with a UFAD system. This heat transfer leads to a 293
slightly higher cooling load than with a well-mixed ventilation system. 294
In heating situations, when a UFAD system is used in the building without heating coils 295
in the air supply diffusers, the presence of warm air in the floor plenum can lead to a 296
higher heating load than that with the well-mixed ventilation system. This increased heat 297
load is again attributed to heat transfer from the plenum air to the floor slab. 298
By conducting an annual energy analysis for the building, this investigation found that 299
the chiller used 16%-27% less energy with the UFAD systems than with the well-mixed 300
system because of the use of free cooling during the shoulder seasons. However, the 301
boiler consumed 18%-30% more energy with the UFAD systems because of heat loss in 302
the floor plenum. The use of heating coils in the air supply diffusers and/or the utilization 303
of ducts for supplying air to the floor plenum can reduce energy use by the boiler. Finally, 304
because the UFAD systems had a higher supply air temperature for cooling, the total 305
supply airflow rate was higher than that with the well-mixed ventilation system. As a 306
result, energy consumption by the fans in the UFAD systems was 22-50% higher. 307
The total energy cost for a UFAD system with un-ducted floor plenums and without 308
heating coils under the diffusers could be slightly higher than that for a well-mixed 309
system. Either ducting the floor plenums or using the heating coils under the diffusers 310
would reduce the energy cost. However, ducting the floor plenums would increase the 311
9
initial investment and maintenance costs. Therefore, although the UFAD system with 312
completely ducted floor plenums and with heating coils (Case 5) had the lowest energy 313
costs, the partially ducted UFAD system with heating coils (Case 6) would be the most 314
favorable one. 315
316
Acknowledgement 317
318
This research was funded partially by the Energy Efficient Building Hub led by the Pennsylvania 319
State University and funded by the U.S. Department of Energy and other government agencies, 320
where Purdue University was a subcontractor to the grant. 321
322
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324
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393
394
11
Table 1.Power inputs of the lights and heated boxes. 395
Number Power [W]
Lighting
1 43.0 2 44.0 3 26.5 4 43.5
Heated boxes for manikins 1 93.3 2 84.0
Heated boxes for equipment 1 65.0 2 65.0 3 65.0
396
Table 2.Comparison of simulated and measured temperatures for the environmental chamber. 397
Locations
Experimental measurements
E+ simulation with1-zone floor plenum
(uniform air temperature)
E+ simulation with 3-zone floor plenum (non-uniform air
temperature)
℃ ℃ Error (%) ℃ Error (%) Air at the diffusers 20.2 19.9 1.5 20.4 1.0 Air at the exhaust 24.2 24.4 0.8 24.2 0.0 Slab surface (facing floor plenum)
23.7 23.6 0.4 23.6 0.4
Ceiling surface 24.3 24.7 1.6 25.4 4.5 North wall of floor plenum 23.8 22.7 4.6 23.7 0.4 South wall of floor plenum 22.7 22.7 0.0 23.0 1.3 West wall of floor plenum 23.5 22.7 3.4 23.0 2.0 East wall of floor plenum 22.7 22.7 0.0 23.0 1.3 North wall of room 25.1 25.2 0.4 25.5 1.6 South wall of room 24.1 25.2 4.6 25.5 5.8 West wall of room 24.7 25.2 2.0 26.4 6.9 East wall of room 25.4 25.2 0.8 25.5 0.4
398
Table 3.Simulated cases. 399
Case Ventilation system Floor plenum configuration
Heating coils under diffusers
1 Well-mixed N/A N/A 2 UFAD Completely ducted No
3 UFAD Ducted perimeter zones
Un-ducted core zone No
4 UFAD Completely un-ducted No 5 UFAD Completely ducted Yes
6 UFAD Ducted perimeter zones
Un-ducted core zone Yes
7 UFAD Completely un-ducted Yes 400
12
Table 4. Monthly natural gas price (unit: $/kWh). 401
Jan Feb Mar Apr May Jun
0.344 0.343 0.343 0.346 0.371 0.400
Jul Aug Sep Oct Nov Dec
0.391 0.386 0.376 0.375 0.322 0.331
402
Table 5.Electricity price (unit: $/kWh). 403
Summer (Jun – Sep)and Winter (Oct - May) Charge Energy [$/kWh] Transition [$/kWh] Distribution [$/kWh]
< 80 hrs. 0.1088 0.0669 0.0344 80-160 hrs. Summer: 0.0592
Winter: 0.0428 Summer:0.0319 Winter: 0.0205
Summer:0.0162 Winter: 0.0103
160-400 hrs. 0.0428 0.0205 0.0103 > 400 hrs. 0.0275 0.0095 0.0046
404
Table 6. Annual energy cost for the whole building in different cases. 405
Case Electricity cost for the chiller
($)
Electricity cost for the fans
($)
Gas cost for the boiler
($)
Total cost as a percentage of Case 1
(%) 1 4275 369 244 100.0 2 3425 481 300 86.1 3 3553 660 320 92.7 4 3797 756 372 100.7 5 3424 481 274 85.7 6 3553 659 290 92.4 7 3814 744 297 99.6
406
13
407
408
409
410
411
412
413
414
415
416
417
Figure 1.Schematics of well-mixed (left) and UFAD (right) systems. 418
419
420
421
422
423
424
425
426
427
428
429
430
431
432
433
434
435
436
Figure 2. Floor N in a multi-floor building with a UFAD system. 437
438
439
Floor plenum
Heat transfer
Troom= Tplenum
Ceiling plenum
Occupied zone
Ceiling plenum
Floor slab
Floor plenum
Room
Return plenum
Floor plenum
Room
Floor plenum
Return plenum
14
1 2 3 4
5 6 7 8
0.00
0.40
0.80
1.20
1.60
0 1 2 3 4 5
U[m/s]
x[m]
Experiment Simulation
0.00
0.40
0.80
1.20
1.60
0 1 2 3 4 5
U[m/s]
x[m]
Experiment Simulation
440
Figure 3.Schematic of the environmental chamber. 441
442
443
444
445
446
447
448
449
450
451
452
453
454
Figure 4. Comparison of CFD results with experimental data for air velocity in two sections of 455
the floor plenum (horizontal cross-section of the plenum at 0.15m above the floor). 456
457
ExhaustLights
Heated boxes
for manikin and
equipment
Diffusers
Conditioned air inlet
Floor plenum
Desk
Room
North
1 2
3
4
5 6
7
8 x
y
15
458
Figure 5. Comparison of measured air temperature with that computed by CFD and by the 459
multizone model in two sections of the floor plenum 460
461
462 Figure 6.Air temperature distribution at 0.15m above the floor slab as simulated by CFD, and 463
division of the plenum into three subzones. 464
465
17
18
19
20
21
22
23
24
25
0 1 2 3 4 5
T[ ]
x[m]
CFD Experiment E+ (three subzones)
17
18
19
20
21
22
23
24
25
0 1 2 3 4 5
T[ ]
x[m]
Experiment CFD E+ (three subzones)
(K)
16
466
467
468
469
470
471
(a). Top view of thermal zone layout. 472
473
474
475
476
477
(b). Side view of thermal zone layout. 478
Figure 7.Medium-sized office building in Philadelphia. 479
480
481
482
Figure 8.Internal heat load of the office building on weekdays (left) and Saturdays (right). 483
484
0
2
4
6
8
10
12
0:00
2:00
4:00
6:00
8:00
10:0
0
12:0
0
14:0
0
16:0
0
18:0
0
20:0
0
22:0
0
W/m2
Time/h
Internal heat on weekdaysElectric Lights Occupancy
0
1
2
3
4
5
6
0:00
2:00
4:00
6:00
8:00
10:0
0
12:0
0
14:0
0
16:0
0
18:0
0
20:0
0
22:0
0
W/m2
Time/h
Internal heat on SaturdaysElectric Lights Occupancy
Ceiling Plenum
Floor Plenum
Room
0.4m
3.0m
0.3m
N
W
S
E
40.0m
30.0m
5.0m
Central Zone
5.0m
5.0m
5.0m
Ceiling Plenum
Room
0.7m
3.0m
17
485
486
487
488
489
490
491
492
493
494
495
(a) (b) (c) 496
497
Figure 9. Simulated scenarios: (1) well-mixed ventilation system, (2) UFAD system without 498
heating coils in the diffusers, and (3) UFAD system with heating coils in the diffusers. 499
500
501
(a) (b) 502
-15
-10
-5
0
5
10
15
0:00
2:00
4:00
6:00
8:00
10:0
0
12:0
0
14:0
0
16:0
0
18:0
0
20:0
0
22:0
0
Hea
t flu
x [W
/m2 ]
Time[h]
Perimeter zonesHeat flux from room/floor plenum to slab
1.Well-mixed2/5.UFAD (completed ducted)3/6.UFAD (ducted perimeter zones)4/7.UFAD (completed un-ducted)
-15
-10
-5
0
5
10
15
0:00
2:00
4:00
6:00
8:00
10:0
0
12:0
0
14:0
0
16:0
0
18:0
0
20:0
0
22:0
0
Hea
t flu
x [W
/m2 ]
Time[h]
Core zoneHeat flux from room/floor plenum to slab
1.Well-mixed2/5.UFAD (completed ducted)3/6.UFAD (un-ducted core zone)4/7.UFAD (completed un-ducted)
Diffuser Exhaust
Supply air
Return air
Diffuser
Exhaust
Supply air
Return air
Diffuser
Exhaust
Return air
Supply air Heating
coil
18
503 (c) (d) 504
Figure 10. Heat transfer across the floor slab of the office building on the summer design day - a 505
weekday. Refer to Table 3 for case descriptions. (a) Heat flux from the room/floor plenum to the 506
floor slab in perimeter zones, (b) Heat flux from the room/floor plenum to the floor slab in the 507
core zone, (c) Heat flux from the downstairs ceiling plenum to the floor slab in perimeter zones, 508
and (d) Heat flux from the downstairs ceiling plenum to the floor slab in core zones (right) 509
510
511
512 (a) Perimeter zones (b) Core zone 513
514
Figure 11. Cooling loads on the summer design day for the office building with different 515
ventilation systems. The numbers are for different cases as described in Table 3. 516
-15
-10
-5
0
5
10
15
0:00
2:00
4:00
6:00
8:00
10:0
0
12:0
0
14:0
0
16:0
0
18:0
0
20:0
0
22:0
0
Hea
t flu
x [W
/m2 ]
Time[h]
Perimeter zonesHeat flux from ceiling plenum to slab
1.Well-mixed2/5.UFAD (completed ducted)3/6.UFAD (ducted perimeter zones)4/7.UFAD (completed un-ducted)
-15
-10
-5
0
5
10
15
0:00
2:00
4:00
6:00
8:00
10:0
0
12:0
0
14:0
0
16:0
0
18:0
0
20:0
0
22:0
0
Hea
t flu
x [W
/m2 ]
Time[h]
Core zoneHeat flux from ceiling plenum to slab
1.Well-mixed2/5.UFAD (completed ducted)3/6.UFAD (un-ducted core zone)4/7.UFAD (completed un-ducted)
0
10
20
30
40
50
60
70
0:00
2:00
4:00
6:00
8:00
10:0
0
12:0
0
14:0
0
16:0
0
18:0
0
20:0
0
22:0
0
Coo
ling
load
[W
/m2 ]
Time[h]
Perimeter zones_cooling load1.Well-mixed2/5.UFAD (completed ducted)3/6.UFAD (ducted perimeter zones)4/7.UFAD (completed un-ducted)
0
10
20
30
40
50
60
70
0:00
2:00
4:00
6:00
8:00
10:0
0
12:0
0
14:0
0
16:0
0
18:0
0
20:0
0
22:0
0
Coo
ling
load
[W
/m2 ]
Time[h]
Core zone_cooling load1.Well-mixed2/5.UFAD (completed ducted)3/6.UFAD (un-ducted core zone)4/7.UFAD (completed un-ducted)
19
517
518
Figure 12.Monthly energy consumption by the chiller in the building’s HVAC system.The 519
numbers are for different cases as described in Table 3. 520
521
522 Figure 13.Monthly energy consumption by the boiler in the building’s HVAC system. The 523
numbers are for different cases as described in Table 3. 524
525
526
0
1000
2000
3000
4000
5000
6000
7000
8000
1 2 3 4 5 6 7 8 9 10 11 12
Ele
ctri
c C
onsu
mpt
ion
[kW
h]
Month
Chiller energy consumptionNo heating coils in diffusers
1.Well-mixed2.UFAD (completed ducted)3.UFAD (partially ducted)4.UFAD (completed un-ducted)
0
1000
2000
3000
4000
5000
6000
7000
8000
1 2 3 4 5 6 7 8 9 10 11 12
Ele
ctri
c C
onsu
mpt
ion
[kW
h]Month
Chiller energy consumptionWith heating coils in diffusers
1.Well-mixed5.UFAD (completed ducted)6.UFAD (partially ducted)7.UFAD (completed un-ducted)
0
500
1000
1500
2000
2500
3000
3500
4000
1 2 3 4 5 6 7 8 9 10 11 12
Gas
Con
sum
ptio
n [k
Wh]
Month
Boiler energy consumptionNo heating coils in diffusers
1.Well-mixed2.UFAD (completed ducted)3.UFAD (partially ducted)4.UFAD (completed un-ducted)
0
500
1000
1500
2000
2500
3000
3500
4000
1 2 3 4 5 6 7 8 9 10 11 12
Gas
Con
sum
ptio
n [k
Wh]
Month
Boiler energy consumptionWith heating coils in diffusers
1.Well-mixed5.UFAD (completed ducted)6.UFAD (partially ducted)7.UFAD (completed un-ducted)
20
527 Figure 14.Monthly energy consumption by the fans in the building’s HVAC system.The numbers 528
are for different cases as described in Table 3. 529
530
0
100
200
300
400
500
600
700
800
1 2 3 4 5 6 7 8 9 10 11 12
Ele
ctri
c C
onsu
mpt
ion
[kW
h]
Month
Fan energy consumptionNo heating coils in diffusers
1.Well-mixed2.UFAD (completed ducted)3.UFAD (partially ducted)4.UFAD (completed un-ducted)
0
100
200
300
400
500
600
700
800
1 2 3 4 5 6 7 8 9 10 11 12
Ele
ctri
c C
onsu
mpt
ion
[kW
h]
Month
Fan energy consumptionWith heating coils in diffusers
1.Well-mixed5.UFAD (completed ducted)6.UFAD (partially ducted)7.UFAD (completed un-ducted)