HVAC ComparingVAVDuctDesigns
Transcript of HVAC ComparingVAVDuctDesigns
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FINAL REPORTNCEMBT070315
COMPARING VAV DUCT DESIGNS
Brian J. Landsberger, Ph.D.
Liangcai (Tom) Tan, Ph.D.
University Of Nevada, Las Vegas
Davor Novosel
National Center for Energy Management and Building Technologies
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FINALREPORTNCEMBT-070315
NATIONAL CENTER FOR ENERGY MANAGEMENT
AND BUILDING TECHNOLOGIES TASK 3:
COMPARING VAV DUCT DESIGNS
MARCH 2007
Prepared B :y
Brian J. Landsberger, Ph.D.
Liangcai (Tom) Tan, Ph.D.
University Of Nevada, Las Vegas
Davor Novosel
National Center for Energy Management and Building Technologies
Prepared For:
U.S. Department of Energy
William Haslebacher
Project Officer / Manager
This report was prepared for the U.S. Department of Energy
Under Cooperative Agreement DE-FC26-03GO13072
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NOTICE
This report was prepared as an account of work sponsored by an agency of the United States government. Neither the
United States government nor any agency thereof, nor any of their employees, makes any warranty, express or
implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any
information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned
rights. Reference herein to any specific commercial product, process, or service by trade name, trademark,
manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by
the United States government or any agency thereof. The views and opinions of authors expressed herein do not
necessarily state or reflect those of the United States government or any agency thereof.
NATIONAL CENTER FOR ENERGYMANAGEMENT AND BUILDINGTECHNOLOGIES CONTACT
Davor Novosel
Chief Technology Officer
National Center for Energy Management and Building Technologies
601 North Fairfax Street, Suite 250
Alexandria VA 22314
703-299-5633
www.ncembt.org
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TABLE OF CONTENTS
ACKNOWLEDGEMENTS.......................................................................................................................................... ix
EXECUTIVE SUMMARY.............................................................................................................................................1
1 PROJECT OBJECTIVE.............................................................................................................................................2
2 BACKGROUND.....................................................................................................................................................32.1 Duct Design Issues .......................................................................................................................................3
2.2 Performance Issues ......................................................................................................................................4
2.3 Installation Problems....................................................................................................................................5
3 METHODOLGY......................................................................................................................................................6
3.1 General Approach.........................................................................................................................................6
3.1.1 Identifying the Knowledge Gap ..............................................................................................................6
3.1.2 Design of the Experiment (DoE)..............................................................................................................6
3.1.3 Development of Laboratory and Test Procedures ....................................................................................7
3.1.4 Testing and Industry Guidance...............................................................................................................7
3.2 Aligning project scope with the knowledge gap..............................................................................................8
3.2.1 Installation Variations Identified From Literature Review.........................................................................8
3.2.2 Expert Committee Recommendations ....................................................................................................8
3.2.3 DOE Peer Review of the VAV Duct Design Variations Test Plan ...............................................................11
3.3 System performance characterization and measurement .............................................................................12
3.4 Design of the Experiment ............................................................................................................................14
3.4.1 Parameter Selection............................................................................................................................14
3.4.2 Test Matrix Selection and Modification ................................................................................................16
3.5 Laboratory Design and Instrumentation......................................................................................................20
3.5.1 Laboratory System Modifications And Capabilities ...............................................................................20
3.5.2 Laboratory Instrument Modifications and Capabilities..........................................................................23
3.5.3 Test Conditions, Measurement Setup and Procedures ..........................................................................27
3.5.4 Experimental Error...............................................................................................................................28
3.6 Analysis Procedures...................................................................................................................................29
3.6.1 Parameter Effects On Performance ......................................................................................................30
3.6.2 Airflow Distribution Performance .........................................................................................................30
4 RESULTS ...........................................................................................................................................................31
4.1 Energy Efficiency For Square and Slot Diffusers ...........................................................................................31
4.2 Noise Generation For Square Diffusers ........................................................................................................32
4.3 Air Distribution Variations Resulting From Installation Variations For Square and Slot Diffusers ....................33
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5 DISCUSSION .....................................................................................................................................................34
5.1 Energy Efficiency.........................................................................................................................................34
5.1.1 Square Diffusers .................................................................................................................................34
5.1.2 Slot Diffusers ......................................................................................................................................35
5.2 Sound Levels..............................................................................................................................................36
5.3 Air Distribution ...........................................................................................................................................366 CONCLUSIONS ..................................................................................................................................................38
7 REFERENCES.....................................................................................................................................................39
APPENDIX A - ENERGY EFFICIENCY TEST RESULTS .................................................................................................40
A1. Test Conditions and Results ........................................................................................................................41
A2. Parameter Main Effects Analysis .................................................................................................................45
APPENDIX B - NOISE GENERATION TEST RESULTS.................................................................................................47
B1. Test conditions and Results ........................................................................................................................48
B2. Parameter Main Effects Analysis .................................................................................................................50APPENDIX C - AIR DISTRIBUTION VARIATION TEST RESULTS ..................................................................................52
C1. Airflow Around Diffusers:Square Diffusers...................................................................................................53
C2. Airflow Around Diffusers:Slot Diffusers ........................................................................................................62
C3. Room Airflow Between Diffusers: Square Diffusers.......................................................................................71
C4. Room Airflow Between Diffusers: Slot Diffusers ...........................................................................................89
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LIST OF FIGURES
Figure 1. Schematic of typical branch installation variations ....................................................................................9
Figure 2. Different types of diffusers that are used in terminal duct installations. Top: two 4-foot slot diffusers, one
with a 8 inch round adaptor and one with a 10-inch oval adaptor. Bottom right: typical 2 by 2-foot louvered square
diffuser. Bottom right: Plaque type 2 by 2-foot square diffuser. ..............................................................................10
Figure 3. Schematic of non-ideal energy transformation in the target system ..........................................................12
Figure 4. Schematic of air distribution modifications for VAV system.......................................................................21
Figure 5. Picture of duct showing a hard turn in the duct and a 3-foot vertical entry into the diffuser (low state of
Parameter 4) ........................................................................................................................................................22
Figure 6. Picture of duct showing a 3-foot vertical duct section attached to the diffuser (high state of Parameter 3) .22
Figure 7. Picture of duct showing the duct running horizontal right before attachment to the diffuser (low state of
Parameter 3) ........................................................................................................................................................23
Figure 8. Test room diffuser locations and measurement scan pattern for square diffusers (left) and slot diffusers
(right). ..................................................................................................................................................................24
Figure 9. Measurement scan patterns for slot (upper) and square (lower) diffusers..................................................25
Figure 10. Directional sensitivity for the HT-412 velocity probe. For= 0o, flow is at a right angle to the direction ofthe probe shaft. ....................................................................................................................................................26
Figure 11.Traversing mechanism sensor ................................................................................................................27
Figure 12. Main effects plots for square (left) and slot (right) diffusers for the five test parameters and where the
performance measure is airflow rate ratio..............................................................................................................31
Figure 13. Noise criteria means for square diffusers when noise criteria levels have been adjusted to that estimated
for a standard airflow rate .....................................................................................................................................32
Figure 14. Airflow distribution from the test diffuser for condition 1 and 4 for square diffusers at 100% design airflow
............................................................................................................................................................................33
Figure 15. Airflow rate ratio means for square diffusers..........................................................................................45
Figure 16. Signal to noise ratio for airflow rate ratio for square diffusers. ................................................................45
Figure 17. Airflow rate ratio means for slot diffusers...............................................................................................46
Figure 18. Signal to noise ratio for airflow rate ratio for slot diffusers .....................................................................46
Figure 19. Noise criteria means for square diffusers without adjustment to a standard airflow rate .........................50
Figure 20. Noise criteria means for square diffusers when noise criteria levels have been adjusted to that estimated
for a standard airflow rate .....................................................................................................................................51
Figure 21. Signal to noise ratio for noise criteria for square diffusers when noise criteria levels have been adjusted to
that estimated for a standard airflow rate ..............................................................................................................51
Figure 22. Test condition 0 airflow velocity from diffuser measured in a 2 by 2 foot square pattern around the diffuser.
............................................................................................................................................................................53
Figure 23. Test condition 1 airflow velocity from diffuser measured in a 2 by 2 foot square pattern around the diffuser.
............................................................................................................................................................................54
Figure 24. Test condition 2 airflow velocity from diffuser measured in a 2 by 2 foot square pattern around the diffuser.
............................................................................................................................................................................55
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Figure 25. Test condition 3 airflow velocity from diffuser measured in a 2 by 2 foot square pattern around the diffuser.
............................................................................................................................................................................56
Figure 26. Test condition 4 airflow velocity from diffuser measured in a 2 by 2 foot square pattern around the diffuser.
............................................................................................................................................................................57
Figure 27. Test condition 5 airflow velocity from diffuser measured in a 2 by 2 foot square pattern around the diffuser.
............................................................................................................................................................................58
Figure 28. Test condition 6 airflow velocity from diffuser measured in a 2 by 2 foot square pattern around the diffuser.............................................................................................................................................................................59
Figure 29. Test condition 7 airflow velocity from diffuser measured in a 2 by 2 foot square pattern around the diffuser.
............................................................................................................................................................................60
Figure 30. Test condition 8 airflow velocity from diffuser measured in a 2 by 2 foot square pattern around the diffuser.
............................................................................................................................................................................61
Figure 31. Test condition 0 airflow velocity from diffuser measured across the face from 6 inches away from the
diffuser.................................................................................................................................................................62
Figure 32. Test condition 1 airflow velocity from diffuser measured across the face from 6 inches away from the
diffuser.................................................................................................................................................................63
Figure 33. Test condition 2 airflow velocity from diffuser measured across the face from 6 inches away from thediffuser.................................................................................................................................................................64
Figure 34. Test condition 3 airflow velocity from diffuser measured across the face from 6 inches away from the
diffuser.................................................................................................................................................................65
Figure 35. Test condition 4 airflow velocity from diffuser measured across the face from 6 inches away from the
diffuser.................................................................................................................................................................66
Figure 36. Test condition 5 airflow velocity from diffuser measured across the face from 6 inches away from the
diffuser.................................................................................................................................................................67
Figure 37. Test condition 6 airflow velocity from diffuser measured across the face from 6 inches away from the
diffuser.................................................................................................................................................................68
Figure 38. Test condition 7 airflow velocity from diffuser measured across the face from 6 inches away from the
diffuser.................................................................................................................................................................69
Figure 39. Test condition 8 airflow velocity from diffuser measured across the face from 6 inches away from the
diffuser.................................................................................................................................................................70
Figure 40. Airflow distribution between diffusers for test condition 0, Square diffusers, at 100% design airflow......71
Figure 41. Airflow distribution between diffusers for test condition 0, Square diffusers, at 50% design airflow. ......72
Figure 42. Airflow distribution between diffusers for test condition 1, Square diffusers, at 100% design airflow......73
Figure 43. Airflow distribution between diffusers for test condition 1, Square diffusers, at 50% design airflow. .......74
Figure 44. Airflow distribution between diffusers for test condition 2, Square diffusers, at 100% design airflow......75
Figure 45. Airflow distribution between diffusers for test condition 2, Square diffusers, at 50% design airflow. .......76
Figure 46. Airflow distribution between diffusers for test condition 3, Square diffusers, at 100% design airflow......77
Figure 47. Airflow distribution between diffusers for test condition 3, Square diffusers, at 50% design airflow. .......78
Figure 48. Airflow distribution between diffusers for test condition 4, Square diffusers, at 100% design airflow. ....79
Figure 49. Airflow distribution between diffusers for test condition 4, Square diffusers, at 50% design airflow. .......80
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Figure 50. Airflow distribution between diffusers for test condition 5, Square diffusers, at 100% design airflow......81
Figure 51. Airflow distribution between diffusers for test condition 5, Square diffusers, at 50% design airflow. .......82
Figure 52. Airflow distribution between diffusers for test condition 6, Square diffusers, at 100% design airflow......83
Figure 53. Airflow distribution between diffusers for test condition 6, Square diffusers, at 50% design airflow. .......84
Figure 54. Airflow distribution between diffusers for test condition 7, Square diffusers, at 100% design airflow......85
Figure 55. Airflow distribution between diffusers for test condition 7, Square diffusers, at 50% design airflow. .......86Figure 56. Airflow distribution between diffusers for test condition 8, Square diffusers, at 50% design airflow. .......87
Figure 57. Airflow distribution between diffusers for test condition 8, Square diffusers, at 50% design airflow. .......88
Figure 58. Airflow velocity between diffusers for test condition 0, Slot diffusers, at 100% design airflow..................89
Figure 59. Airflow velocity between diffusers for test condition 0, Slot diffusers, at 50% design airflow....................90
Figure 60. Airflow velocity between diffusers for test condition 1, Slot diffusers, at 100% design airflow. ................ 91
Figure 61. Airflow velocity between diffusers for test condition 1, Slot diffusers, at 50% design airflow....................92
Figure 62. Airflow velocity between diffusers for test condition 2, Slot diffusers, at 100% design airflow..................93
Figure 63. Airflow velocity between diffusers for test condition 2, Slot diffusers, at 50% design airflow....................94Figure 64. Airflow velocity between diffusers for test condition 3, Slot diffusers, at 100% design airflow..................95
Figure 65. Airflow velocity between diffusers for test condition 3, Slot diffusers, at 50% design airflow....................96
Figure 66. Airflow velocity between diffusers for test condition 4, Slot diffusers, at 100% design airflow..................97
Figure 67. Airflow velocity between diffusers for test condition 4, Slot diffusers, at 50% design airflow....................98
Figure 68. Airflow velocity between diffusers for test condition 5, Slot diffusers, at 100% design airflow..................99
Figure 69. Airflow velocity between diffusers for test condition 5, Slot diffusers, at 50% design airflow..................100
Figure 70. Airflow velocity between diffusers for test condition 6, Slot diffusers, at 100% design airflow................101
Figure 71. Airflow velocity between diffusers for test condition 6, Slot diffusers, at 50% design airflow..................102
Figure 72. Airflow velocity between diffusers for test condition 7, Slot diffusers, at 100% design airflow................103
Figure 73. Airflow velocity between diffusers for test condition 7, Slot diffusers, at 50% design airflow..................104
Figure 74. Airflow velocity between diffusers for test condition 8, Slot diffusers, at 100% design airflow................105
Figure 75. Airflow velocity between diffusers for test condition 8, Slot diffusers, at 50% design airflow..................106
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LIST OF TABLES
Table 1. Possible Standardized Input Conditions ...................................................................................................11
Table 2. Parameter list for the experimental design following Department of Energy review .....................................15
Table 3. Taguchi Orthogonal L8 Array ....................................................................................................................16Table 4. Parameter List for Test Array ....................................................................................................................16
Table 5. Test Array with One 4-Level Parameter, Four 2-Level Parameters And One Noise Parameter........................17
Table 6. Expected effect of parameter variation on output ......................................................................................19
Table 7. Vertical locations of the traversing mechanism sensors .............................................................................25
Table 8. Airflow Rate Ratio predictions with parameter levels set at levels for high and low performance for square
diffusers ............................................................................................................................................................... 35
Table 9. Airflow Rate Ratio predictions with parameter levels set at levels for high and low performance for slot
diffusers ............................................................................................................................................................... 35
Table 10. Test conditions and results for square diffuser tests ...............................................................................41Table 11. Test conditions and results for square diffuser tests (continued) .............................................................42
Table 12. Test conditions and results for slot diffuser tests.....................................................................................43
Table 13. Test conditions and results for slot diffuser tests (continued)..................................................................44
Table 14. Test conditions and sound results for square diffuser tests......................................................................48
Table 15. Test conditions and sound results for slot diffuser tests...........................................................................49
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ACKNOWLEDGEMENTS
The authors obtained help and guidance from many outside sources during the course of this project. The
collaboration of those people steered this project in the productive direction toward filling essential
industry knowledge gaps and keeping the project focused on those goals. They also were very helpful in
applying practical knowledge on experimental techniques that are particular to ductwork and room
airflow testing. The expert committee members: Ted Carnes, Steve Kimmel, Richard John, Robert
Browning, and Michael Mamayek, contributed their expertise and guided the project team. Also, Dan
Int-Hout contributed multiple times to the success of the experiment testing.
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EXECUTIVE SUMMARY
This task compared the performance of conventional air distribution (CAD) systems, built according to
current design specifications and workmanship standards, with CAD systems that have been built with
common variations in construction and workmanship seen in typical field installations. Variations
examined in this task are those found in the ducted air distribution system from the variable air volume
(VAV) unit to the diffuser.
The results of this project testing revealed the quantitative differences in energy use, sound generation and
room air distribution due to variations in the installation of ductwork and diffusers after the VAV unit.
Specifically, for a constant supply air pressure:
Increasing flex-duct length from 6 to 35 feet decreased airflow by 11 percent
Decreasing diameter of the flex duct from 10 to 8 inches decreased airflow by 25 percent
One hard turn or a kink in the flex-duct near the diffuser decreased airflow by 11 percent andnoticeably increased noise level (5 dB)
The two standard types of diffuser tested had a 9 percent difference in airflow rate
For square diffusers, the absence of a vertical section in the flex-duct right above the diffuser (no
substantial length of vertical duct) actually resulted in a slight increase in airflow compared to aninstallation with a 40 inch vertical section but was accompanied by a significant (6 dB) increase
in flow generated noise and significant asymmetric diffuser discharge airflow.
A branch duct installed immediately after the VAV unit, compared to at least four duct diametersafter the VAV unit, in the square diffuser tests caused a slight decrease in airflow. The same
effect could not be determined from the slot diffuser tests.
Room air diffusion symmetry was affected primarily by the type of diffuser and the approach ofthe flex duct immediately before the diffuser. For square diffusers, the two levels of the flex duct
elbow near the diffuser condition, (1) three feet of vertical duct before the diffuser and (2) three
feet of horizontal duct with only 5 inches of vertical duct before the diffuser, gave significantly
different room air distribution patterns. Apparently the horizontal momentum of the airflow
carried through the diffuser creating an asymmetric airflow discharge pattern. For slot diffusers,which have an internal air plenum, the two levels of the flex duct elbow near the diffuser
condition did not result in significant differences in airflow discharge symmetry. The net effect
on room draft and air distribution performance index (ADPI) was not determined.
These effects were consistent for both the 100 percent design and 50 percent design airflowconditions tested
The tests were conducted in the new environmental systems room at UNLV under repeatable conditions
that replicated expected field installation variations. The test parameters and their test conditions were
determined with the help of the literature review, the advise of an expert panel and the advise of a
Department of Energy review panel. Quantitative effects were determined through the use of an
orthogonal test array. The orthogonal test array gives the main effect of parameter level variation under
both flow conditions in the fewest possible number of tests.
The results confirm many standard held beliefs and results of some previous testing by others, but the
results also show some standard held beliefs are not accurate. The main contribution of this research is
that it provides quantitative results that can be used to make energy efficiency and noise generation design
and installation decisions, and to predict the efficiency and noise levels of an installation.
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1 PROJECT OBJECTIVE
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1 PROJECT OBJECTIVE
This task compared the performance of conventional air distribution (CAD) systems, built according to
current design specifications and workmanship standards, with CAD systems that have been built with
common variations in construction and workmanship seen in typical field installations. Variations
examined in this task are those found in the ducted air distribution system from the variable air volume
(VAV) unit to the diffuser. A test protocol was developed and implemented in the UNLV Building
Technologies Laboratory (BTLab) to measure performance of CAD VAV systems with respect to energy
use, air distribution and acoustics. Test data were collected and analyzed to identify the sensitivity of
CAD systems to the typical variations.
The specific task objectives were:
Identify typical (with potential faults) field installations of ducted CAD VAV systems.
Conduct laboratory airflow, energy, and sound tests on selected typical installations of ductedVAV systems to develop a body of valid engineering design data for these systems.
Upgrade and modify the laboratory facilities at UNLV/CMEST to conduct airflow, energy, andsound tests on ducted CAD VAV systems.
Information gathered by the project team including guidance from the Department of Energy motivated
this research and guided formation of the specific project objectives. Those objectives cover gathering
information on past research that could be used to refine the project objectives and methodology,
identifying industry needs that will be used to define the project scope, design the experiment to fit the
project scope, develop a measurement protocol to meet the experimental design, develop analysis
methods used to determine the effects of installation variation on performance and disseminate this
information to the industry.
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2 BACKGROUND
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2 BACKGROUND
ASHRAE has sponsored several research projects for the purpose of updating friction loss coefficients for
duct fittings in rectangular, round, and flat oval ducts and for improving design methodologies for HVAC
air distribution systems in buildings. That research has helped to significantly improve the design of that
part of HVAC air distribution systems up to the point where branch ducts supply air to variable volume
terminal units and room air terminal devices (grills, registers, and diffusers). Design information on duct
design from variable volume terminal units to room air terminal devices is primarily anecdotal in nature,
and it is predicated on ideal system installations, which seldom if ever occur in field installations. There
are very little measured data concerning the effects on building air distribution, energy, and sound due to
variations in duct installations between air terminal units and room diffusers.
The installation of supply duct and VAV systems raises a number of issues that impact overall air
distribution system efficiency and performance. Although research information on specific details is
limited, there are established guidelines addressing common installation issues. The primary information
sources for VAV duct design are SMACNAs HVAC Systems Duct Design Manual (SMACNA 1990),
California Energy Commissions (CEC) Advanced Variable Air Volume Design Guide (Hydeman 2003),and the ASHRAE Handbook of Fundamentals (ASHRAE 2001). An additional important source is Mr.
Dan Int-Hout, Chief Engineer for Krueger. The purpose of this literature review was to extract published
information on the effect on the performance of the HVAC system of VAV terminal unit-to-diffuser duct
design and installation variations. Specific information sought included duct design issues, performance
issues, and installation problems.
2.1DUCTDESIGN ISSUES
The predominant duct design issues deal with duct leakage, noise and duct contamination.
Duct leakage is a frequently raised issue. Leakage in all unsealed ducts varies considerably with thefabricating machinery used, the methods of assembly, and installation workmanship (ASHRAE 2001). In
the buildings investigated by Xu et al. (Xu 2002), the duct systems leaked more than what is specified by
ASHRAE for unsealed ducts. Air leakage not only increases fan energy consumption and run-time, but
also increases the induced cooling load by the extra heat generated by the fan (Xu 2002). For large
commercial buildings the complete elimination of air leakage from the ducts has an electricity energy
savings potential on the order of 10 kWh/m2 per year. (Modera 2001). However, SMACNA (SMACNA
1990) cautions on the impracticality of obtaining zero leakage.
Noise is also an important consideration in HVAC duct design. Ducts serve as transmitters of break-in
noise while flexible ducts are effective attenuators of upstream noise sources (Int-Hout 1996). Issues with
flexible duct connections at the inlet of the diffuser include increased pressure drop, increased sound
levels, and non-uniform air distribution from the diffuser (Int-Hout 1996). Concerning VAV terminal
design, discharge noise is rarely an issue if the unit has hard duct on the inlet, a lined outlet plenum andflex duct between the plenum and diffusers VAV units above acoustical ceilings should have radiated
Noise Criteria levels no more than ~5 NC above the desired room NC rating. (Hydeman 2003).
Contamination of the duct walls is another important consideration particularly with respect to indoor
environmental quality. According to Hydeman (Hydeman 2003), it is yet to be determined how
significant a health issue duct liner retention of dirt and moisture truly is. However, Foarde et al. (Foarde
1996) acknowledged the contamination of fiberglass duct materials due to soil and moisture. Their study
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results suggest that dust accumulation and/or high humidity should be properly controlled in any HVAC
duct to prevent the growth ofP. chrysogenum (a species of fungus) (Foarde 1996).
2.2PERFORMANCE ISSUES
Variable airflow, proper unit sizing, and minimum airflow settings of VAV systems are the main
performance issues.
The variability of the flow rates common to VAV systems appears in the literature as a common issue.
Diffusers are designed to optimally distribute the air at some particular load condition and air volume.
Thus, the performance of outlets with regard to throw, room velocity and noise levels will vary greatly
with the discharge volume (SMACNA 1990). An adequate diffuser for VAV systems should be able to
perform across the whole operational range of a VAV system. As one option, Linder generally
recommends only linear slot diffusers for VAV systems (Linder 1997). Unfortunately, diffusers are often
being selected without regard to the effect of VAV turn-down (Int-Hout 2001), which results in the
degraded performance of diffusers at very low flow rates (Hydeman 2003). Diffusers with perforated
faces tend to have short throws at high airflow rates and thus may be unacceptable for VAV applications
(Int-Hout 2004).
The California Energy Commission suggests designing the HVAC system to efficiently handle auxiliaryloads that operate during off hours. HVAC systems may operate at only one-half of the design airflow for
the bulk of the time. Recognizing that VAV systems seldom operate at their design capacity, a reasonable
balance between first costs and energy costs often results in designs using smaller duct sizes. This design
approach results in a friction rate (airflow friction loss per 100 ft) at maximum design capacity that is very
high compared to a system designed around maximum expected capacity (Hydeman 2003). On the otherhand, optimizing the system at a dominant part load operating condition results in cost savings (Kim
2002). In a separate article, Kim reported a 7% reduction in energy consumption using the optimized part
load design approach compared to the duct area over the T-method, and a higher reduction compared to
the equal friction and static regain method (Kim 2002b). When considering proper room air distribution,
SMACNA suggests designing with overthrow at maximum design volumes to achieve acceptable throwat part load volumes (SMACNA 1990).
Over-sizing of VAV terminals can lead to significant operational issues and generally results from using a
safety factor when sizing the equipment. The outcome is quite often a reduced turndown ratio and a more
expensive system (Linder 1997). Additionally, over-sizing a VAV unit significantly reduces the velocity
of the air passing the velocity sensor at the same air flow as a properly sized unit, resulting in a velocity
pressure that is below the sensing range of the VAV unit manufacturers velocity sensor (Simon 2002).
The California Energy Commission design guidelines suggest setting the minimum airflow set point to
the larger of the lowest controllable airflow set point allowed by the unit and the minimum ventilation
requirement. In California, the minimum ventilation rate for an office is 0.15 CFM/sq.ft. In contrast, it is
common practice to have the minimum airflow set point between 30% and 50% of the cooling maximum
airflow set point, well above the guidelines. The recommended approach is a dual maximum scheme that
allows reduction of flow when heating or cooling load is low. There are many buildings operating
comfortably with lower than 30% airflow minimums (Hydeman 2003). Some issues that drive highminimum set points are stratification, short-circuiting and dumping of cold air. Room temperature non-
uniformities can result from insufficient flow at low loads due to low unit flow (Linder 1997). Also, if the
airflow set point is below the working range of the velocity controller, the unit may cycle between closed
and partially open, causing some varying sound levels (Int-Hout 2003). Taylor has developed a
simulation that considers many of the above mentioned design factors and determined optimum design
total pressure drop for the VAV unit that is on the path with the highest pressure drop (Taylor 2004).
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2.3INSTALLATION PROBLEMS
Installation problems predominantly concern the length and type of the duct branch, how duct turns are
accomplished and how the duct approaches the diffuser.
The length of the duct branch, the type of duct, and its radius affect the air delivery characteristics from
the VAV unit to the diffuser. Without sufficient length to develop a uniform profile, the flow in ductbranches too close to the VAV terminal or a previous branch is non-uniform, and hence causes an
increase in pressure loss. SMACNA suggests a sufficiently long duct section before elbows. In addition,
it highly emphasizes the use of turning vanes in elbows. However, the installation of elbows with only
some vanes and with no vanes is common practice. Eliminating every other turning vane from the vane
runners is believed to decrease the pressure drop. Research results, however, have revealed that thispractice more than doubles elbow pressure losses, and is definitely not recommended. More astounding
is the total elimination of vanes in the installation of fittings. This may be due to the fact that some sheet
metal contractors have found that they do not get paid for furnishing expensive fittings, such as ones with
turning vanes that were not shown on the project mechanical drawing. Without turning vanes, especially
in fittings used for avoiding obstructions, good airflow in the duct system can be totally destroyed(SMACNA 1990).
The advantages of installing vanes in elbows are significant but their purpose will not be met without theproper alignment of the vane rails. Improper alignment is a common problem found in the field. Vane
rails need to be aligned tangent to the flow to maintain uniformity in the flow. If the flow, however,
approaching the elbow is non-uniform, the turning vanes will instead assist in maintaining non-uniformity
in the flow downstream, and hence cause a pressure increase in the system upstream. The position of
fittings with respect to each other is also important for the air distribution. Hydeman et al. suggest
avoiding consecutive fittings to reduce the pressure drop, noting that in fittings less than six hydraulic
diameters apart the flow pattern entering subsequent fittings differs from the flow pattern used to
determine loss coefficients (Hydeman 2003). Thus, accurate loss calculation may be difficult.
Roughness of the ducts also affects the airflow distribution, and hence the energy used. The higher the
friction factor, the more energy it takes to push the air through the ducts. Straighter and smoother ducts
result in lower energy consumption and first cost (Hydeman 2003). The friction factor substantially
increases for not fully extended flexible ducts. For a straight flex duct extended only 70% of full length a
400% increase of the friction factor is expected (ASHRAE 2001).
The duct approach to the diffuser is also very important, since detrimental effects of improper duct
approach cannot be corrected by the diffuser itself. Both SMACNA and ASHRAE agree that for proper
diffusion, the velocity of the air stream must be as uniform as possible over the entire connection to the
duct and must be perpendicular to the outlet face. However, few outlets are installed in this manner. In
some cases, special devices can assist redirecting and stabilizing the airflow. Most ceiling outlets are
attached either directly to the bottom of horizontal ducts or to vertical take-off ducts that connect the
outlet with the horizontal duct (ASHRAE 2001; SMACNA 1990).
With respect to noise, SMACNA suggest placing the diffusers as far as possible from duct elbows and
branch take-offs to minimize noise transmission. For flexible ducts, SMACNA recommends to keep
bends as gentle as possible to diminish noise transmission, however, they also indicate the possibleneed for bends to assist in sound attenuation (SMACNA 1990). Moreover, direct duct connections to the
diffuser can result in noise levels by as much as 12 NC higher than catalog levels (Int-Hout 1996). An
offset of the flexible duct connection between the diffuser and the supply duct equal to the diffuser
diameter over a connection length equal to two diameters can increase the sound power level as much as
12 dB. Improperly used diffusers can also be a source of noise. Diffuser dampers cannot be used for
reducing high air volumes without inducing objectionable noise (SMACNA 1990).
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To meet the project objectives, a detailed investigation methodology was developed and followed. To
determine scope and design of the experiment, and develop test procedures, the investigation used
information gathered from published literature, advise from an industry expert committee, and review
comments from a Department of Energy peer review panel. The test laboratory was designed anddeveloped and test protocols were developed and followed to conduct experiments called for in the
experimental design.
3.1GENERALAPPROACH
3.1.1 Identifying the Knowledge Gap
The goal of this task was to develop useful information for the HVAC industry on duct installation
between a VAV box and the diffuser. Therefore, collecting customer needs is essential to determine the
best direction and scope of the investigation. Some of the customer needs were extracted from the
literature review. The major source of customer needs came from a group of design and installation
experts assembled specifically for this project. Specific guidance sought included:
1. Consensus on a best or industry standard installation
2. Typical variations from that standard seen in the field
3. Predominance of the different variations and the magnitude of the variation encountered inthe field
4. Performance expectations from an industry standard installation
5. Expert opinion on the effect and importance of various installation variations
The information collected was used to determine the different installation parameters and to prioritize the
list based on the anticipated performance effect of variation in each parameter.
3.1.2 Design of the Experiment (DoE)
The design of the experiment is the crucial process used to devise a method to economically and
accurately determine the effects of parameter variation on the performance of the system. The system
field-operating environment is realistically simulated in the laboratory by testing under various
environmental conditions expected in the field. Important inputs to the design are the environmental
conditions, the physical installation parameters, the expected system performance and the parameters
expected effect on performance. Specific objectives of the experimental design are to determine:
1. What are the significant environmental conditions in the field2. Which parameters have a significant effect on the system performance
3. Which significant parameters are likely to be controlled by design or installation practices
4. Which significant parameters are likely to be not controlled by design or installation practices
5. What is the significant performance parameters to measure
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6. What is the most economical test matrix that can be used to capture the main effects ofparameter variation and achieve the objective of the experiment.
3.1.3 Development of Laboratory and Test Procedures
Laboratory and test procedures are needed to effectively and reliably perform the testing called for in the
experimental design. Specific objectives of the laboratory and test procedures development include:
1. Create a stable and repeatable laboratory test environment
2. Controls for modifying the test environment as required by the testing
3. Procedures for performing the various duct installations called for in the experiment design.
4. Sufficient instrumentation to monitor the test environment and accurately capture the targetperformance.
5. Data recording equipment and data reduction procedures for analysis of the results.
6. Understand the source and magnitude or experimental error
3.1.4 Testing and Industry Guidance
Experiments were conducted as called for in the experimental design using the laboratory and test
procedures. Data analysis, conclusions and recommendations focus on producing useful information and
guidance for the industry. Specific objectives of the testing and analysis of results include:
1. Conduct airflow, energy, and sound tests on a HVAC system with common installationvariations from a typical industry standard system
2. Determine the main effects of those variations on significant performance measures
3. Determine the importance of each type of variation and the target value for best performance4. Determine the quantitative advantage of holding a parameter on target and the quality loss for
off target performance.
5. Disseminate this information in a practical and usable format for industry use
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3.2ALIGNING PROJECT SCOPE WITH THE KNOWLEDGE GAP
Valuable assistance from outside sources was used to obtain the voice of the customer concerning the
knowledge gap in duct design and installation. The literature review, the project expert panel and a
Department of Energy review panel made particularly significant contributions toward identifying theknowledge gap.
3.2.1 Installation Variations Identified From Literature Review
The literature identified rules for proper installation of ductwork and gave reasons for following the rules.
In general, installations that result in unsteady flow at a branch connection or diffuser should be avoided
due to increased airflow pressure drop, increased noise and unpredictable flow balancing. Common
installation variations are branches to close to the terminal unit or to each other, flex duct too short or with
hard bends, and duct approach to the diffuser offset from the diffuser center.
3.2.2 Expert Committee Recommendations
To ensure relevance with up to date installation practices and problems, an expert committee for advising
the project team was established. This committee met at UNLV during the initial project methodology
development to identify the state of the art of VAV-to-diffuser duct design and common constructionvariations found in the field. The panel members evaluated a range of construction variations with regard
to good workmanship, commonly accepted construction practices and potential detrimental impact on the
air distribution performance of the system. The panel also identified several possible test setups and the
variations that should be tested in this Task.
The identified variations were generally expected to disadvantageously affect the performance of the air
distribution system due to either added flow restrictions, creation of uneven or disturbed flow in the ducts
or added imbalance of the system. The effect of two variations, perforated face on the diffuser for squarediffusers and round or oval side or top plenum inlet for slot diffusers, was not clearly known and could
negatively or positively impact the performance of air distribution system.
For square diffuser systems, the panel identified the following common variations:
1. First branch too close to VAV terminal discharge
2. Short length to diffuser
3. Flex duct offset
4. Bad radius in flex duct
5. Short vertical length to diffuser
6. Flex duct too long
7. Factory supplied damper in the face of diffuser grill
8. Perforated face on the diffuser
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For slot diffuser systems:
1. First branch too close to VAV terminal discharge
2. Short duct length to diffuser
3. Flex duct offset
4. Small radius turn in flex duct
5. Flex duct too long
6. Round or oval, side or end plenum inlet.
A sketch of a duct layout showing a normal branch and six variations is shown in Figure 1. Two typical
slot diffusers and two square diffusers are shown in Figure 2.
VAV Unit
Branch too close to
VAV unit dischar geProper branch
installationBranch too
short
Proper installation
Radius in branch
turn too small
Side View
Vertical duct offset Vertical duct
too short
Branch too long
Figure 1. Schematic of typical branch installation variations
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Figure 2. Different types of diffusers that are used in terminal duct installations. Top: two 4-foot slot diffusers, one with a 8 inch
round adaptor and one with a 10-inch oval adaptor. Bottom right: typical 2 by 2-foot louvered square diffuser. Bottom right:
Plaque type 2 by 2-foot square diffuser.
The expert panel suggested a separate series of tests for square diffusers and slot diffusers due to the
different fundamental air distribution characteristics of the two types of diffusers. Two-foot and four-
foot slot diffusers were discussed for the testing. Originally, when the test plan called for four square
diffusers in the test room, using four two-foot end slot diffusers in the test room would give the best
comparison to the square diffusers and are a common size of slot diffusers used in that size of room.
Later, after a series of preliminary tests, a room configuration with only two diffusers, either square or
slot, was determined to be the best for room air distribution and for testing. The panel initially worked
out a series of tests that were based on having one condition at the extreme or bad setting while holding
the other conditions at nominal or the good setting. This testing sequence was modified in favor of a
more efficient orthogonal array test sequence, which is discussed in detail in section 3.4 Design of the
Experiment.
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A summary of a preliminary test plan was submitted back to the expert committee for their review and
comment. Changes suggested by several members of the committee were subsequently incorporated into
the test plan.
A focus of discussion between the panel members and the team was determination of the VAV unit input
parameters. Debate centered around maintaining constant airflow, pressure or energy into the VAV unit.
The advantages and disadvantages of each approach are shown in Table 1. Normally, as many units donot have airflow sensing, airflow through the VAV unit is controlled by predetermined positioning of the
inline damper. Therefore, the team decided to use two fixed damper positions for the two noise
conditions. Only two of the three parameters: pressure, airflow and damper position, are independent.
Thus, for each damper position, only pressure or airflow, but not both, can be held constant for different
variations in the ductwork. Alternately, energy can be held constant by adjusting airflow until the airflow
and pressure condition results in the same energy. The team decided to hold pressure constant and allow
airflow to vary. This is more representative of field conditions where several VAV units are attached to amain air supply. In such cases, supply pressure is held constant and flow requirements are met by use of
in-line dampers, such as in a VAV unit. By holding the supply pressure constant while varying
installation conditions, the airflow will vary off target. This airflow variation is expected to be small
compared to the airflow difference caused by the two damper positions.
Table 1. Possible Standardized Input Conditions
Advantage Disadvantage
Constant Airflow Easy to control May be inconsistent with actualbuilding system operating
conditions
Constant VAV Inlet Pressure Easy to control Similar to actual building system
operating conditions
Will require airflow scaling todetermine noise effects of
parameter variation
Constant Input Energy Similar to actual operating
conditions in some small systems
May be difficult to determine root
cause of output variation
High and low value of the test parameters were provided by the industry expert panel.
3.2.3 DOE Peer Review of the VAV Duct Design Variations Test Plan
A Department of Energy sponsored peer review panel was presented with the details of the test plan. The
panel made a few recommendations in the test parameters.
Following the DOE peer review panel recommendations, a test parameter of closed and open center face
design diffuser was added, while perforated face diffuser and end slot diffuser testing was dropped.These changes are based on the types of diffusers most commonly used in the commercial building
HVAC industry. From the original seven parameters, short length to diffuserandflex duct too long werecombined into one four level parameter, flex duct length to result in six parameters for both square and
slot diffusers.
The DOE panel also concurred with the test plan to measure isothermal throw from the diffusers.
Estimating ADPI from isothermal throw measurements is an industry accepted method. The different
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installations used in this project are expected to result in changes in total airflow and flow pattern from
the effected diffuser.
3.3SYSTEM PERFORMANCE CHARACTERIZATION AND MEASUREMENT
Good performance measures posses the important characteristics of a strong relation to the customer
needs and being identifiable as the result of an energy transformation from input to output. It is alsoadvantageous that the performance measure be a leading indicator of customer satisfaction. System
designers require sufficient information to design a system that will provide the desired thermal and
acoustic comfort as economically as possible. The common indicator of thermal comfort is ADPI, and of
acoustic comfort is the noise criteria (NC) level. The information needed to create a good system design
includes diffuser airflow, diffuser airflow pattern, the expected pressure drop and noise generated from a
given installation.
The energy transformation takes place in the target system from VAV unit to the test room. The input is
airflow at a given rate, temperature and pressure. The desired output is airflow into the room at a desired
rate, temperature and distribution. The intended energy transformation consists of redirection of the flow.
The unintended consequences of the transformation are airflow decrease, pressure loss, noise generation,
heat loss or gain, and undesired airflow distribution. A depiction of the energy flow is shown in Figure 3.
This project deals with isothermal flow so heat transfer is not considered. A strong effort was made to
avoid airflow loss due to leakage between the VAV unit and the diffuser. Airflow decrease due to
leakage was not used as a parameter and any loss was considered experimental error in this experiment.
As previously mentioned, at a given inline damper setting airflow and system pressure drop are inter-
dependent.
Energy Outputnergy InputfAirflow
Figure 3. Schematic of non-ideal energy transformation in the target system
For this experiment, the supply air pressure was held constant. For a given VAV damper setting, airflow
decreased due to increased airflow resistance in the ductwork including diffuser. Thus, changes in
airflow were a good measure of the efficiency of the energy transformation. Before reaching the VAV
unit, the supply air passed through several silencer like plenums, nearly 15 feet of lined metal duct with
perforated inner surface and about 30 feet of large diameter flex duct. At the VAV unit the flow had no
significant noise content. All noise created in the room was noise that was generated from the VAV unit
to the diffuser. Thus, noise measured in the room was a good indicator of unintended energy
transformation in the target system. Airflow entered the VAV unit through a 4-foot straight metal duct
and was presumed to be uniform. The distribution of the air into the room, uniform or otherwise was a
fAirflow Energy Transformationf Flow Distributionf Pressuref NoisefTemperaturef
Temperature
Unintended Energy Inputf Noise
f Heat Transfer
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combination of the intended and unintended consequence of the installation from the VAV unit to the
diffuser. Airflow distribution was a good measure of part of the energy transformation in the target
system. For this experiment, airflow rate, airflow pattern and room noise levels were measured as
performance parameters.
Airflow rates were measured at each diffuser before and after each test run. The performance parameter
used was the ratio of test diffuser airflow to the airflow measured during the nominal case run. This gavea direct measure of the relative efficiency of the installation.
Room noise level was measured at two elevations for all test points during all test runs. An average of the
readings from the microphone at mid level during a scan around the diffuser was used for the
performance measurement. The measurement was converted to the Noise Criteria (NC). Noise Criteria is
designed for measuring HVAC related noise and is commonly used by the industry. Because of
intermittent extraneous noise in the test room at the two lowest octave bands used for calculating NC, the
measurements at those bands were omitted. Therefore, the reported levels were modified NC levels.
Those omitted bands covered the low frequencies typically associated with rumble. Rumble is a
characteristic of large fan noise or unstable flow in large ducts and the generation of such noise was not
expected from the ductwork in this experiment. The modified NC was expected to be a good
representation of the actual NC due to the ductwork installation. For nearly all measurements, they were
in fact the same.
Room diffuser airflow pattern and throw characteristics were measured to determine air distribution
changes due to variations in ductwork installation. If a room air distribution system is designed with the
assumption of directionally symmetric diffuser performance, then any significant deviation from that
symmetry could be detrimental to the room ADPI. However, most room designs, including the test room
for this task, have inherent compromises in the diffuser design. Most notably, the characteristic length
used to select diffuser location may not be symmetrical in every direction. In the test room used in this
experiment, the square diffuser characteristic length varied from eight to eleven feet. It is possible that
matching asymmetry in diffuser throw with asymmetry in characteristic length could be beneficial. On
the other hand, random anti-symmetrical throw is likely to be especially detrimental to ADPI. Clearly,
APDI has dual dependency on both diffuser throw and room air distribution design. The Task goals were
to produce data that could be used for different room designs, and in a sense, be room independent.
Therefore, diffuser throw variation were deemed to be a better indicator of the effect of variations in the
test parameters than ADPI measurements. Some parameter variations may not affect throw symmetry,
but may affect the system balance and, as a result, the overall efficiency with or without system
rebalancing.
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3.4DESIGN OF THE EXPERIMENT
The design of the experiment determines how economically and accurately the effects of parameter
variation on the performance of the system are captured. Parameters that have a direct effect on the
energy transformation were chosen and grouped as either control, test or noise parameters. Followingparameter selection, the most efficient test matrix was chosen and parameter levels were adjusted to best
capture the main effects of parameter variation.
3.4.1 Parameter Selection
The expert panel identified seven different conditions and two different types of diffusers that most likely
would be installed in a typical VAV system. A full factorial design of experiment (DoE) for those seven
conditions and two diffuser types at just two levels would involve hundreds of tests. Alternately, a basic
vary-from-nominal one parameter at a time test for four configurations would require 26 tests at each
airflow level (48 for two airflow levels) and would not give any information in cases where more than one
parameter is different from nominal. Along with total number of tests, the required labor and thedifficulty of achieving test parameters must also be considered. Each test involves configuring the duct
system and diffuser according to the selected levels of the parameters, running the HVAC system until
conditions such as air velocity and temperature have stabilized, then measure air velocity, temperature
and sound at all the required positions in the test room.
To achieve the task objectives in the budget and time allotted, an efficient experimental design was
required.
A DoE based on the Taguchi Orthogonal Array is a very efficient tool used to derive relationships
between parameters and the results. The Taguchi method of experimental design has gained wide
acceptance in industry and applied research for quality improvement in product and process design. The
method is used to determine the relationships between different parameters such as ingredients, strength,
shape, length and smoothness, and the quality level achieved in the output. The orthogonal property ofthe test array allows for easy and accurate statistical analysis. For example, from the experimental results,
the designer can determine the best level for a parameter, the sensitivity of the output to that parameter
and the sensitivity of the output to noise (changes in uncontrolled conditions) at different parameter
levels. In this experiment, the relations obtained were for the main effects. A main effect was defined
as the impact a particular parameter had on the output. In contrast, an interaction was defined as any
change in the effect of a parameter caused by a change in the level of a different parameter. In other
words, an interaction was the change in the output that was not caused by the main effect. When the
Taguchi Orthogonal Array is used, any interaction is spread out evenly through all the output of the
experiment. Thus, the interaction is not measurable, but fortunately, due to the spreading out of any
interaction effects on the experimental output, the interaction has a minimum impact on the main effect.
The Taguchi Orthogonal Array was used to test the system for all the parameter variations. Along with
the conditions obtained from the expert panel, analysis of the literature suggested an additional condition
of VAV terminal variable flow rate. One of the conditions suggested by the expert panel, flex duct
vertical section above the diffuser is offset, was incorporated into short vertical section above diffuser.
Knowledge of the physics of the system suggested that both parameters have a similar effect and have
strong interaction. In fact, short vertical section above diffuser, is just the extreme case of duct offset.
The conditions and resulting parameters are listed in Table 2. The table also lists the form of energy
conversion associated with that parameter and the type of parameter as either test, control or noise.
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The type definitions are:
Test Parameter. A parameter that is a cause of variation and is tested a several levels.
Control Parameter. A parameter that can be controlled and eliminated as a source of variation.
May be tested to evaluate different design option.Noise Parameter. A parameter that cannot be controlled, or is preferred not to be controlled, in
actual system use. Therefore a good system should be robust to changes in the noiseparameter. This parameter may be varied in the experiment to test for system robustness.
Table 2. Parameter list for the experimental design following Department of Energy review
Condition Parameter Energy Form Type of Parameter
Duct branch close to VAV terminal or
previous branch
Distance from branch to
VAV unit or previous
branch
Flow disturbance Test Parameter (x)
Duct very short or very long Distance from branch todiffuser
Flow disturbance Test Parameter (x)
Short vertical section above diffuser Distance from elbow to
diffuser
Flow disturbance Test Parameter (x)
Small radius turn in flex duct Size of radius Flow resistance / noise Test Parameter (x)
Closed or open face diffuser (square
diffuser only)
Closed / open Flow resistance,
disturbance
Control Parameter (C)
Round / oval diffuser plenum inlet
(slot diffuser only)
Round / oval Flow disturbance Control Parameter (C)
VAV airflow volume Flow rate Flow resistance / noise
/disturbance
Noise Parameter (N)
Note that the type of parameter classification (test, control or noise) is dependent on where in the whole
process of HVAC system creation the evaluation is performed. For example, a system designer may not
specify the exact diffuser or duct but instead just the source of air for each diffuser and the expected flow
for the anticipated room load. To that designer, some of the control parameters listed in Table 2 become
noise parameters such as diffuser choices, and variations in duct installation and room conditions.
Alternately, to the installer that chooses the diffuser and duct products, and directs the installation, many
of the test parameters in Table 2 become control parameters. Possible noise parameters for the installer
would be parameters such as flow rate, room load, room furniture and partition arrangement, variations
within the products, and variations from the designated installation.
For this experiment, it was assumed that diffuser choices are controlled but that exact installationconditions are subject to variation. The seven parameters in Table 2 were determined to be acceptable
parameters for the DoE. One practical consideration was that, based on the available time for testing and
how the design sequence affected ease of changing between tests, the total number of tests would not
exceed 35. To the maximum extent possible, test parameters that were expected to have a strong
interaction or were essentially the same parameter at different levels were combined and varied together
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as one parameter. It was decided to include the control parameter, diffuser inlet or face type, as a test
parameter to capture the effects of changing the diffuser type.
3.4.2 Test Matrix Selection and Modification
For the experiment itself, there were a discrete number of arrays to choose from. Considering the number
of parameters and the desire to economize on the number of tests, the L8 array, requiring 8 tests andhaving the ability to evaluate the main effects of up to 7 parameters at two levels, or 5 parameters, 1 at
four levels and 4 at two levels was chosen. The array shown in Table 3 is the 5-parameter configuration.
The first test shown has all parameters at level one while all other tests have the parameters at mixed
levels. When the test is actually conducted the order of tests is randomized to help reduce uncontrolled
noise interference in the results. The array is balanced by choosing parameter levels such that any
condition of any parameter is tested with an equal number of high and low conditions of the other
parameters. For example, parameter 2, level 1 is tested with parameter 4, level 1 twice and level 2 twice.
This testing method reduces interaction effects in the output and exposes all parameters to the different
levels of the other parameters. This is an excellent array to determine main effects as long as interactions
are low and effects for the two level parameters are close to linear.
Table 3. Taguchi Orthogonal L8 Array
TESTCONDITION PARAMETERS
Test No.Branch to elbow
distance
Branch to VAV
unit distance
Elbow to diffuser
distance
Bend in duct
radius
Diffuser/duct
type
1 1 1 1 1 12 1 2 2 2 23 2 1 1 2 24 2 2 2 1 15 3 1 2 1 26 3 2 1 2 17 4 1 2 2 18 4 2 1 1 2
The list of the five parameters for the two diffuser cases is shown in Table 4.
Table 4. Parameter List for Test Array
Parameter Low State Mid State High State
1. Branch to diffuser distance 6 (square), 9 (slot) feet 15 and 25 feet 35 feet
2. Branch to VAV unit distance 6 inches 54 inches
3. Elbow to diffuser distance 5 inches 40 inches
4. Bend in duct radius 5 inch radius, 120 degree
turn
30 inch radius, less than
90 degree turn
5. Diffuser design (square) Louvered Plaque
5. Duct size and connection (slot) 8-inch, round 10-inch, oval
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Table 3 is referred to as the inner array. The one noise test condition, airflow rate, still needed to be
added to the experiment. Noise conditions are added at the right of the matrix in what is called the outer
array. With only one noise condition, the outer array is just a one-row, two-column array. The complete
test array, inner and outer, for both diffuser types is shown in Table 5. One nominal test condition, listed
as test condition 0, was added to the array. Test parameters for this test condition were set at what are
considered standard installation practice levels and the more common diffuser was chosen. Test
condition 0 was not used in the calculations for main effects and signal to noise levels. It was included togive comparative information on the performance of a standard installation. The measured output for
each test is entered under each Noise Test Condition column. Thus, for each type of diffuser (square or
slot) there are eight test numbers, each done once for each noise condition. Because we have two diffuser
types, a total of 32 tests were required. The results of the experiment were used to determine the main
effects of the test parameters. The main effects were the average effects for that test parameter with the
other parameters at equal instances of all possible test levels and while exposed to the different noise
condition levels.
Using the main effects, it was possible to predict the results for all possible cases of parameter levels,
most of which were not tested. Also, for any given performance measure or combination of measures,
optimum settings of the test parameters can be determined. Parameters that can have continuous levels
(not just either/or) can be set at values between the extremes. Results for the 4-level parameter can shownon-linearity in the output and can show an optimum value between extremes. Because a noise parameter
is evaluated, robustness of the design to that noise condition can be evaluated. These results also can be
used to help with tolerance design.
Table 5. Test Array with One 4-Level Parameter, Four 2-Level Parameters And One Noise Parameter
TESTCONDITION PARAMETERS NOISETESTCONDITION
Test No. 1 2 3 4 5 1 21 1 1 1 1 12 1 2 2 2 23 2 1 1 2 24 2 2 2 1 15 3 1 2 1 26 3 2 1 2 17 4 1 2 2 18 4 2 1 1 20 Nominal 2 2 2 1
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Because the arrays are balanced and orthogonal, analysis of the results of the test is greatly simplified.
Analysis of the results produces values for the main effects (change in output when a parameter is
changed from one level to the other), and the signal-to-noise ratios (S/N), (the effect of noise and other
parameter variation on the output with the parameter at a given level). Those values are plotted for easy
parameter at all test levels. The main effects are calculated using the equation:
Al,i =j=1
j= n
Yl ,i,j
n(1)
where Al,i is the mean performance when parameter i is at level l, and Yl,i,j is the result for the j test
when parameteri is at level l. For example, for the mean when parameter 2 is at level 1, the results from
the four tests (numbered 1, 3, 5, and 7 in Table 5) are averaged.
The S/N calculation depends on the type of performance characteristic. The performance characteristic ofairflow is a larger the better characteristic and noise level is a smaller the better characteristic. The
signal-to-noise calculation uses the equation:
S/N= 10log10 MSD (2)
where MSD is the mean square deviation. For smaller the better:
MSDl ,i =j=1
j= n
Yl,i,j
2
n(3)
while for greater the better,
MSDl ,i =j=1
j= n
1/Yl,i,j2
n(4)
for level l of parameteri.
The mean gives the average performance when a test condition is at a specific level. Because the other
test parameters are equally balanced at all of their levels, this mean is the best indicator of expected
performance at that level. S/N, on the other hand, also measures the variation of performance when a test
condition is at a specific level. Because of the way S/N is calculated, the highest value of S/N is always
desirable in both larger and smaller the better performance measures. For the larger and smaller the better
performance measures, the mean and the S/N level normally indicate the same level as the best for any
given parameter. However, if performance has high variation at a specific parameter level, the S/N value
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may be lower than a level with a less desirable mean but lower variability. A designer then needs to
decide if the low variation is more desirable than the better mean. In many cases, low variation is chosen
and a different parameter is used to obtain a desirable mean. In the case of energy efficiency in ductwork,
the optimum mean may be chosen to maximize potential energy savings, while the lower variation may
be chosen so that performance can be better predicted.
Based on principals of physics and engineering experience, certain changes in performance were expectedfrom changes in the different parameters. Table 6 lists the expected change in different performance
characteristics with changes in the test parameter. This list was compiled before the experiment was run
to help build the design and measurement scheme so as to not miss those performance changes.
Table 6. Expected effect of parameter variation on output
ParameterExpected effect at
variation
Effect on
diffuser throw
symmetry
Effect on system
performance
Energy efficiency related
effect
Duct branch to diffuser distance Unstable flow Small to none Airflow balance
change
Resistance added by
balancing
Duct branch to VAV unitdistance Unstable flow Possibleasymmetry Airflow balancechange Resistance added bybalancing
Duct hard elbow to diffuser
distance
Flow velocity
direction
Significant
asymmetry
Flow noise
generation
Unknown
Bend in duct radius Flow restriction none Flow resistance Resistance added to
balance
Diffuser design (square
diffuser)
Throw pattern
variation, flow
resistance
Different throw
pattern
Possible resistance
change
Possible resistance change,
different balancing
Duct connection (slot diffuser) Flow resistance and
direction
Different throw
pattern
Possible resistance
change
Possible resistance change,
different balancing
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3.5 LABORATORYDESIGN AND INSTRUMENTATION
The UNLV test room was extensively modified to accommodate the requirements of this and other
NCEMBT projects. The modifications included new heat pumps for the room air system, rework and
extensive additions to the room ductwork, addition of a temperature control system for all test room
surfaces, the addition of extensive system monitoring instruments and new instruments for measuring theperformance characteristics.
3.5.1 Laboratory System Modifications And Capabilities
The laboratory system modifications that made this project possible were the addition of temperature
control of the room HVAC system and room surfaces, and the rework and extensive additions to the room
ductwork.
The room HVAC control was designed to supply air at a stable volume and temperature. The volume for
each test is maintained by a manually controlled fan run at a set speed. The supply air temperature was
conditioned by two multi-stage compressor heat pumps. Each heat pump was controlled by a variable
demand thermostat with a temperature sensor in the supply duct located just before the VAV unit. Tostabilize the supply air temperature, the air passed a heat exchanger with 15 gallons of circulating water
and glycol. The buffering effect of the heat exchanger reduced temperature changes in supply air to a rate
of less than 2F per minute under all operating conditions.
Temperature control of the room surfaces was accomplished by ducting conditioned air through a channelbetween layers in the walls, sub-floor and ceiling. Surface control was divided into thirteen
independently controlled zones. The zones could be heated or cooled to maintain the desired temperature
or heat transfer, on their respective surfaces. The four vertical surfaces (room walls) were covered with
1/4-inch wallboard backed by 1/8-inch of dense foam rubber like material. The wall covering added
sufficient insulation between the temperature control air ducting and the room interior surface to achieve
thermal buffering in the wall and create slower thermal convection through the wall. At the same time,
the control scheme for the surface temperature control was optimized to hold target and reduce
temperature variations. Tests indicate a temperature gradient along the walls of 4 F or less. Average
surface temperature variation was below 2 F. For this experiment, all the walls and ceiling were
maintained at 75 F to achieve isothermal conditions. Total heat load in the room was estimated at 150
watts from overhead florescent lighting, 80 watts from the instrument motion system, and 50 watts from
the instrumentation.
The room ductwork was modified to accommodate the CAD and under floor air distribution (UFAD)
testing. The UFAD tests were conducted under a separate NCEMBT task. A depiction of the supply
ductwork in the test room is shown in Figure 4. Starting with the main supply duct, a T-section with a
class III smoke damper on each