1. Trang chủ
  2. » Giáo Dục - Đào Tạo

Development of estate level outdoor ventilation prediction models for HDB estates in singapore 1

437 347 0

Đang tải... (xem toàn văn)

Tài liệu hạn chế xem trước, để xem đầy đủ mời bạn chọn Tải xuống

THÔNG TIN TÀI LIỆU

Thông tin cơ bản

Định dạng
Số trang 437
Dung lượng 12,67 MB

Nội dung

DEVELOPMENT OF ESTATE LEVEL OUTDOOR VENTILATION PREDICTION MODELS FOR HDB ESTATES IN SINGAPORE LEE ROU XUAN @ LEE SEU QUIN (B.Sc. Building (Hons.), NUS; M.Sc. (Building Science), NUS) A THESIS SUBMITTED FOR THE DEGREE OF DOCTOR OF PHILOSOPHY DEPARTMENT OF BUILDING NATIONAL UNIVERSITY OF SINGAPORE 2013 ACKNOWLEDGEMENTS I would like to express my gratitude to all the people who helped me in completing this thesis. First and foremost, I want to thank my supervisor and mentor, Prof. Wong Nyuk Hien, for all his advice, guidance and encouragement during all the stages of this research. My thanks also go to Dr. Demetris Clerides, Mr. Peter Ewing and Mr. Kynan Maley from CD-Adapco for providing all the necessary technical support in the use of the Star-CCM+ software throughout my candidature here. My appreciation also goes to Mr. Komari Bin Tubi, from the School of Design and Environment (SDE) Wind Tunnel Laboratory, for his kind technical assistance in helping to prepare the equipment and sensors before actual experiments. Also, thanks to Mr. Tan Dong Xing, the student assistant for helping me to construct the scaled wind tunnel models and even took the trouble to come back during his exams period. Next, my heartfelt thanks goes to Mr. Clement Choo, the IT expert for helping me to tackle some of my computer hardware problems. I am grateful to Dr. Steve Kardinal Jusuf for answering many of my questions regarding research methodologies and for all his insightful comments and suggestions. Moreover, I would also want to thank my fellow course-mate Mr. Terrance Tan, for letting me use his more powerful computer to supplement my massive simulation studies; without which, the whole process might stretch out for another one year. Also many thanks go to my entire lab mates - Alex Tan, Erna Tan and also Kelvin Li, for making all these years a funnier and wackier experience to remember. From all the laughs and their suggestions with this research, this certainly contributed to the betterment of this study. Furthermore, I am certainly grateful to acknowledge the financial support that comes from the scholarship funding from the National University of Singapore i (NUS) that has helped to ease some of my financial burden during my study here. Next, I want to thank my parents for bringing me to this world, my siblings for all their love, encouragement and endless moral support. Special thanks goes to my late grandparents who came all the way from China to settle down in Singapore and also drummed us the belief that girls should be given an equal opportunity to study like boys. Lastly, I would like to thank my husband and best friend Soong Chee Keong for sharing his knowledge in CFD research, incredible support, encouragement, taking care of me and making me see light when everything else seems hopeless. ii TABLE OF CONTENTS ACKNOWLEDGEMENTS i  TABLE OF CONTENTS iii  SUMMARY xi  LIST OF TABLES . xiv  LIST OF FIGURES xxii  LIST OF ABBREVIATIONS . l  CHAPTER : INTRODUCTION 1  1.1 Background and Motivation 1.1.1 Reduction of Wind Speed . 1.1.2 Research Motivation . 1.1.3 Developments in this Research Area 1.1.4 Design Standards for Optimal Ventilation 1.1.4.1 Singapore – HDB Present Situation . 1.1.4.2 Other Countries’ Situation . 1.2 Research Objectives . 11 1.3 Structure of Thesis . 12 CHAPTER : LITERATURE REVIEW 15  2.1 Effects of Wind 15 2.2 Effects of Urban Environments on Wind Flow . 15 2.3 Description of Airflow Phenomenon . 20 2.3.1 Indicator of Good Ventilation . 20 2.3.2 Parameters that Affect Wind Flow in Urban Environments . 21 2.3.2.1 Important Findings from Previous Researches 22 2.3.2.2 Other Factors that Affect Wind Flow 40  iii 2.4 Experimental Designs Adopted for Airflow and Ventilation Studies . 41 2.4.1. Computational Fluid Dynamics (CFD) 42 2.4.1.1 Points to Note in CFD Simulations 43 2.4.1.2 Turbulence Models 47 2.4.1.3 Near-wall Treatment 52 2.4.2 Wind Tunnel Studies . 53 2.5 HDB Building Designs and Site Planning . 54 2.6 Research Gap . 57 CHAPTER : HYPOTHESIS AND METHODOLOGY 59  3.1 Hypothesis 59 3.2 Methodology 60 3.2.1 Scenarios or Cases Adopted 63 3.2.1.1 Orientation of Canyon (ORIENT) . 65 3.2.1.2 Building Shape (BS) 66 3.2.1.3 Geometry (GEO) 67 3.2.1.4 Gross Building Coverage Ratio (GBCR) . 70 3.2.1.5 Permeability (PERM) . 73 3.2.1.6 Buildings’ Height Variation (HV) . 78 3.2.1.7 Staggering of Blocks Arrangement (STAG) 81 3.2.2. Computational Fluid Dynamics Simulations . 83 3.2.2.1 Model Description . 83 3.2.2.2 Model Assumptions and Limitations . 84 3.2.2.3 Computational Domain 86 3.2.2.4 Boundary Conditions . 88 3.2.2.5 Meshing Type and Size 91 iv 3.2.3 Wind Tunnel Studies . 93 3.3 Conclusion . 98 3.4 Importance and Potential Contribution of the Research 99 CHAPTER : WIND TUNNEL STUDY 103  4.1 Introduction 103 4.2 Wind Tunnel Testing . 103 4.2.1 Testing Facilities . 103 4.2.2 Simulation of the Atmospheric Boundary Layer (ABL) 105 4.2.3 Wind Tunnel Blockage and Model Span 107 4.2.4 Similarity Parameters 109 4.2.5 Locations of the Sensor Taps 112 4.2.6 Selected Cases . 113 4.2.7 Assumptions 115 4.2.8 Results . 115 CHAPTER : PARAMETRIC STUDY OF THE INFLUENCE OF MORPHOLOGICAL VARIABLES ON ESTATE LEVEL VENTILATION .121 5.1 Introduction 121 5.2 Parametric Approach . 122 5.3 Findings from Parametric Study 122 5.3.1 Gross Building Coverage Ratio (GBCR) 122 5.3.1.1 Point Blocks . 125 5.3.1.1.1 Point Blocks, Pedestrian Level . 125 5.3.1.1.1.1 Point Blocks, Pedestrian Level - Random Configuration 127 5.3.1.1.1.2 Point Blocks, Pedestrian Level - Group Configuration . 128 5.3.1.1.1.3 Point Blocks, Pedestrian Level - Courtyard Configuration . 130 v 5.3.1.1.2 Point Blocks, Mid-Level . 132 5.3.1.1.2.1 Point Blocks, Mid-Level - Random Configuration 133 5.3.1.1.2.2 Point Blocks, Mid-Level - Group Configuration . 134 5.3.1.1.2.3 Point Blocks, Mid-Level - Courtyard Configuration . 136 5.3.1.2 Slab Blocks 137 5.3.1.2.1 Slab Blocks, Pedestrian Level . 137 5.3.1.2.1.1 Slab Blocks, Pedestrian Level - Random Configuration . 139 5.3.1.2.1.2 Slab Blocks, Pedestrian Level – Group Configuration 140 5.3.1.2.1.3 Slab Blocks, Pedestrian Level – Courtyard Configuration 142 5.3.1.2.2 Slab Blocks, Mid-Level 145 5.3.1.2.2.1 Slab Blocks, Mid-Level - Random Configuration . 146 5.3.1.2.2.2 Slab Blocks, Mid-Level - Group Configuration 148 5.3.1.2.2.3 Slab Blocks, Mid-Level - Courtyard Configuration 149 5.3.2 Buildings’ Height Variation (HV) 150 5.3.2.1 Point Blocks . 152 5.3.2.1.1 Point Blocks, Pedestrian Level . 152 5.3.2.1.1.1 Point Blocks, Pedestrian Level - Random Configuration 153 5.3.2.1.1.2 Point Blocks, Pedestrian Level - Stratified Configuration . 154 5.3.2.1.2 Point Blocks, Mid-Level . 156 5.3.2.1.2.1 Point Blocks, Mid-Level - Random Configuration 157 5.3.2.1.2.2 Point Blocks, Mid-Level - Stratified Configuration 158 5.3.2.2 Slab Blocks 160 5.3.2.2.1 Slab Blocks, Pedestrian Level . 160 5.3.2.2.1.1 Slab Blocks, Pedestrian Level - Random Configuration . 161 5.3.2.2.1.2 Slab Blocks, Pedestrian Level - Stratified Configuration 163 vi 5.3.2.2.2 Slab Blocks, Mid-Level 165 5.3.2.2.2.1 Slab Blocks, Mid-Level - Random Configuration . 166 5.3.2.2.2.2 Slab Blocks, Mid-Level - Stratified Configuration 167 5.3.3 Permeability (PERM) 168 5.3.3.1 Point Blocks . 171 5.3.3.1.1 Point Blocks, Pedestrian Level . 171 5.3.3.1.1.1 Point Blocks, Pedestrian Level – Ground Floor Only Permeability 172 5.3.3.1.1.2 Point Blocks, Pedestrian Level – Ground Floor and Mid-height Permeability . 173 5.3.3.1.1.3 Point Blocks, Pedestrian Level – Mid-height Only Permeability 175 5.3.3.1.2 Point Blocks, Mid-Level . 177 5.3.3.1.2.1 Point Blocks, Mid-Level – Ground Floor Only Permeability 179 5.3.3.1.2.2 Point Blocks, Mid-Level – Ground Floor and Mid-height Permeability . 181 5.3.3.1.2.3 Point Blocks, Mid-Level – Mid-level Only Permeability 183 5.3.3.2 Slab Blocks 185 5.3.3.2.1 Slab Blocks, Pedestrian Level . 185 5.3.3.2.1.1 Slab Blocks, Pedestrian Level – Ground Floor Only Permeability 187 5.3.3.2.1.2 Slab Blocks, Pedestrian Level – Ground Floor and Mid-height Permeability . 187 5.3.3.2.1.3 Slab Blocks, Pedestrian Level – Mid-level Only Permeability . 190 5.3.3.2.2 Slab Blocks, Mid-Level 191 5.3.3.2.2.1 Slab Blocks, Mid-Level – Ground Floor Only Permeability . 192 5.3.3.2.2.2 Slab Blocks, Mid-Level – Ground Floor and Mid-height Permeability . 195 5.3.3.2.2.3 Slab Blocks, Mid-Level – Mid-Height Only Permeability 197 vii 5.3.4 Geometry (GEO) . 199 5.3.4.1 Point Blocks . 202 5.3.4.1.1 Point Blocks, Pedestrian Level . 202 5.3.4.1.1.1 Point Blocks, Pedestrian Level – Geometrical Height Variation (H) 203 5.3.4.1.1.2 Point Blocks, Pedestrian Level – Geometrical Width Variation (W) 205 5.3.4.1.1.3 Point Blocks, Pedestrian Level – Combined Results of Geometric Height (H) and Width (W) Variation . 208 5.3.4.1.2 Point Blocks, Mid-Level . 210 5.3.4.1.2.1 Point Blocks, Mid-Level – Geometrical Height Variation (H) 211 5.3.4.1.2.2 Point Blocks, Mid-Level – Geometrical Width Variation (W) 213 5.3.4.1.2.3 Point Blocks, Mid-Level – Combined Results of Geometric Height (H) and Width (W) Variation . 217 5.3.4.2 Slab Blocks 219 5.3.4.2.1 Slab Blocks, Pedestrian Level . 219 5.3.4.2.1.1 Slab Blocks, Pedestrian Level – Geometrical Height Variation (H) 220 5.3.4.2.1.2 Slab Blocks, Pedestrian Level – Geometrical Width Variation (W) 222 5.3.4.2.1.3 Slab Blocks, Pedestrian Level – Combined Results of Geometric Height (H) and Width (W) Variation . 225 5.3.4.2.2 Slab Blocks, Mid-Level 227 5.3.4.2.2.1 Slab Blocks, Mid-Level – Geometrical Height Variation (H) . 228 5.3.4.2.2.2 Slab Blocks, Mid-Level – Geometrical Width Variation (W) . 230 5.3.4.2.2.3 Slab Blocks, Mid-Level – Combined Results of Geometric Height (H) and Width (W) Variation . 231 5.3.5 Staggering of Blocks Arrangement (STAG) . 233 5.3.5.1 Point Blocks . 239 viii (48) Hall, R.C. (1996). Evaluation of modeling uncertainty – CFD modeling of near-field atmospheric dispersion. Project EMU final report, WS Atkins Consultants Ltd, UK. (49) Hall, R.C. (Ed.). (1997). Evaluation of modelling uncertainty. CFD modelling of near-field atmospheric dispersion. Project EMU final report, European Commission Directorate–General XII Science, Research and Development Contract EV5V-CT94-0531, WS Atkins Consultants Ltd., Surrey. (50) Han, H.W. (2005). A study of entrainment in 2-phase upward concurrent annular flow in a vertical tube. PhD Thesis, University of Saskatchewan. (51) Hang, J., Sandberg, M. and Li, Y.-G. (2009). Age of air and air exchange efficiency in idealized city models. Building and Environment, 44, 17141723. (52) Hefny, M.M. and Ooka, R (2009). CFD analysis of pollutant dispersion around buildings: Effect of cell geometry. Building and Environment, 44(8), 1699-1706. (53) Holmes, J.D. (1982). Techniques and Modelling Criteria for the Measurement of External and Internal Pressures. Proceedings of the International Workshop on Wind Tunnel Modeling Criteria and Techniques in Civil Engineering Applications, (April 1982, Gaithersburg, MD), T.A. Reinhold, Ed. Cambridge University Press, New York, 245256. (54) Hooser J.D., Wei, M., Newton, B.E. and Chiffoleau G.J.A. (2009). An approach to understanding flow friction ignition: A computational fluid dynamics (CFD) study on temperature development of high-pressure oxygen flow inside micron-scale seal cracks. Journal of ASTM International, 6(10), 1-15. (55) Hotchkiss, R.S. and Harlow, F.H. (1973). Air Pollution Transport in Street Canyons. Report by Los Alamos Scientific Laboratory for US Environmental Protection Agency, EPA-R4-73-029, NTIS PB-233 252. (56) Housing and Development Board (HDB). (2004). Proposed Public Housing Development Under the Design, Build and Sell Scheme Particulars and Conditions of Tender. HDB, Singapore. (57) Housing and Development Board (HDB) (2005). Building Group, Public housing design guide: principles and practice. Singapore: Housing and Development Board. (58) Housing and Development Board (HDB) (2006). Universal design guide for public housing in Singapore. Singapore: Housing and Development Board. 369 (59) Housing and Development Board (HDB) (2007). Green housing book: HDB’s approach to sustainable development. Singapore: Housing and Development Board. (60) Hoydysh, W.G. and Dabberdt, W.F. (1988). Kinematics and dispersion characteristics of flows in asymmetric street canyons. Atmospheric Environment, 22(12), 2677-2689. (61) Hu, C.H. and Wang, F (2005). Using a CFD approach for the study of street-level winds in a built-up area. Building and Environment, 40(5), 617-631. (62) Huang, H., Akutsu, Y., Arai, M. and Tamura, M. (2000). A twodimensional air quality model in an urban street canyon: evaluation and sensitivity analysis. Atmospheric Environment, 34(5), 689-698. (63) Hunter, L.J., Watson, I.D. and Johnson, G.T. (1990/1991). Modeling air flow regimes in urban canyons. Energy and Buildings, 15-16(3-4), 315324. (64) Hunter, L.J., Johnson, G.T. and Watson, I.D. (1992). An investigation of three-dimensional characteristics of flow regimes within the urban canyon. Atmospheric Environment, 26B(4), 425-432. (65) Hussain, M. and Lee, B.E. (1980). An Investigation of Wind Forces on Three-dimensional Roughness Elements in a Simulated Atmospheric Boundary Layer Flow – Part II. Flow Over Large Arrays of Identical Roughness Elements and the Effect of Frontal and Side Aspect Ratio Variations. Report No BS 56, Department of Building Sciences, University of Sheffield. (66) Jeong, S.J. and Andrews, M.J. (2002). Application of the k-e turbulence model to the high Reynolds number skimming flow field of an urban street canyon. Atmospheric Environment, 36(7), 1137-1145. (67) Johnson, G.T., Hunter, L.J. and Arnfield, A.J. (1990). Preliminary field test of an urban canyon wind flow model. Energy and Buildings, 15(3-4), 325-332. (68) Johnson, W.B., Ludwig, F.L., Dabberdt, W.F. and Allen, R.J. (1973). An urban diffusion simulation model for carbon monoxide. Journal of the Air Pollution Control Association, 23(6), 490-498. (69) Kastner-Klein, P. and Plate, E.J. (1999). Wind-tunnel study of concentration fields in street canyons. Atmospheric Environment, 33, 3973-3979. (70) Khoo, H. and Su, V. (2007). Scaling New Heights. Urban Redevelopment Authority (URA) - Skyline (A bi-monthly Newsletter), Mar/April, 6-8. 370 (71) Kim, J.-J. and Baik, J.-J. (2001). Urban street-canyon flows with bottom heating. Atmospheric Environment, 35(20), 3395-3404. (72) Kim, J.-J. and Baik, J.-J. (2004). A numerical study of the effects of ambient wind direction on flow and dispersion in urban street canyons using the RNG k-εturbulence model. Atmospheric Environment, 38(19), 3039-3048. (73) Kim, S.E., Choudhury, D. and Patel, B. (1997). Computations of Complex Turbulent Flows Using the Commercial Code ANSYS FLUENT. In Proceedings of the ICASE/LaRC/AFOSR Symposium on Modeling Complex Turbulent Flows. Hampton, Virginia. (74) Kubota, T., Miura, M., Tominaga, Y. and Mochida, A. (2008). Wind tunnel tests on the relationship between building density and pedestrianlevel wind velocity: Development of guidelines for realizing acceptable wind environment in residential neighborhoods. Building and Environment, 43(10), 1699-1708. (75) Lakas, B.D. (1988). Wind Tunnel Simulation of the Texas Tech Field Research Laboratory: Effects of Terrain Features and Building Orientation. Masters Thesis. Texas Tech University. (76) Lee, I.Y., Shannon, J.D. and Park, H.M. (1994). Evaluation of Parameterizations for Pollutant Transport and Dispersion in an Urban Street Canyon using a Three-dimensional Dynamic Flow Model. Proceedings of the 87th Annual Meeting and Exhibition of the American Meteorological Society, June 19-24, 1994, Cincinnati, Ohio. (77) Li, X.-X., Liu, C.-H., Leung, D.Y.C. and Lam, K.M. (2006). Recent progress in CFD modeling of wind field and pollutant transport in street canyons. Atmospheric Environment, 40(29), 5640-5658. (78) Lim, L. (2001). Fifty-storey HDB Blocks for Tanjong Pagar, Singapore. The Straits Times, August. (79) Liu, H. (1990). Wind Engineering (A Handbook for Structural Engineers). University of Missouri-Columbia. Prentice Hall, Englewood Cliffs, New Jersey. (80) Louka, P. (1998). Measurements of air flow in an urban environment. PhD Thesis. University of Reading. (81) Louka, P., Belcher, S.E. and Harrison, R.G. (1998). Modified street canyon flow. Wind Engineering and Industrial Aerodynamics, 74-76, 485-493. (82) MacDonald, R.W., Griffiths, R.F. and Hall, D.J. (1998). An improved method for the estimation of surface roughness of obstacle arrays. Atmospheric Environment, 32(11), 1857-1864. 371 (83) Melbourne, W.H. (1982). Wind Tunnel Blockage Effects and Corrections. Proceedings of the International Workshop on Wind Tunnel Modeling Criteria and Techniques in Civil Engineering Applications, (April 1982, Gaithersburg, MD), T.A.Reinhold, Ed. Cambridge University Press, New York, 197-216. (84) Ministry of National Development (MND), Housing and Development Board (HDB) and Urban Redevelopment Authority (URA) (2002). Duxton Plain Public Housing – international architectural design competition. Singapore: Urban Redevelopment Authority (URA). (85) Mochida, A., Tominaga, Y., Murakami, S., Yoshie, R., Ishihara, T. and Ooka, R. (2002). Comparison of various k-ε model and DSM applied to flow around a high-rise building – report on AIJ cooperative project for CFD prediction of wind environment. Wind and Structures, 5(2–4), 227– 244. (86) Mohammadi, B. (1991). Etude du modele k-ε de la turbulence pour les ecoulements compressibles. PhD thesis. Universite Paris VI. (87) Nakamura, Y. and Oke, T.R. (1988). Wind, temperature and stability conditions in an E-W oriented urban canyon. Atmospheric Environment, 22(12), 2691-2700. (88) Ng, E. (2009). Policies and technical guidelines for urban planning of high-density cities – air ventilation assessment (AVA) of Hong Kong. Building and Environment, 44, 1478-1488. (89) Ng, E. and Cheng V. (2012). Urban human thermal comfort in hot and humid Hong Kong. Energy and Buildings, 55, 51-65. (90) Nicholson, S.E. (1975). Air pollution model for street-level air. Atmospheric Environment, 9(1), 19-31. (91) Nunez, M. and Oke, T.R. (1976). Long wave radiative flux divergence and nocturnal cooling of the urban atmosphere. II. Within an urban canyon. Boundary Layer Meteorology, 10(2), 121-135. (92) Oke, T.R. (1982). Overview of interactions between settlements and their environments. WMO experts meeting on Urban and building climatology, WCP-37, WMO, Geneva. (93) Oke, T.R. (1987). Boundary Layer Climates. Methuen, London. (94) Oke, T.R. (1988). Street design and urban canopy layer climate. Energy and Buildings, 11(1-3), 103-113. (95) Pearlmutter, D., Bitan, A. and Berliner, P. (1999). Microclimatic analysis of ‘compact’ urban canyons in an arid zone. Atmospheric Environment, 33(24), 4143-4150. 372 (96) Pernpeintner, A., Schnabel, P., Schuler, A. and Theurer, W. (1995). ‘Appendix 17: Qualifizierungsversuch’, WTG-Merkblattűber Windkanalversuche in der Gebäudeaerodynamik, in E. J. Plate (ed.), WTG-Berichte Nr. 3, Windtechnologische Gesellschaft WTG e.V., 292 pp. (97) Plate, E.J. (1999). Methods of investigating urban wind fields – physical models. Atmospheric Environment, 33(24), 3981-3989. (98) Rae, W.H. and Pope, A. (1984). Low-speed wind tunnel testing. (2nd Ed.). John Wiley and Sons, USA. (99) Rafailidis, S. (1997). Influence of building areal density and roof shape on the wind characteristics above a town. Boundary-layer Meteorology, 85(2), 255-271. (100) Raupach, M.R. (1992). Drag and drag partition on rough surfaces. Boundary-layer Meteorology, 60(4), 375-395. (101) Ricciardelli, F and Polimeno, S. (2006). Some characteristics of wind flow in the lower urban boundary layer. Journal of Wind Engineering and Industrial Aerodynamics, 94(11), 815-832. (102) Roberson, J.A. and Crowe, C.T. (1988). Engineering Fluid Mechanics. Wiley, USA. (103) Ruck, B. (1993). Wind-tunnel measurements of flow field characteristics around a heated model building. Journal of Wind Engineering and Industrial Aerodynamics, 50, 139-152. (104) Russell, M.B., Surendran, P.N. and Probert, S.D. (2002). Quantifying acceptable mesh dependencies for computational investigations of airflow within rooms. Applied Energy, 72(1), 409-425. (105) Santamouris, M. (2001). Energy and Climate in the Urban Built Environment. James and James (Science Publishers) Ltd, UK. (106) Santamouris, M., Papanikolaou, N., Koronakis, I., Livada I and Asimakopoulos, D.N. (1999). Thermal and air flow characteristics in a deep pedestrian canyon and hot weather conditions. Atmospheric Environment, 33(27), 4503-4521. (107) Scaperdas, A., Gilham, S. (2004). Thematic Area 4: Best practice advice for civil construction and HVAC. The QNET-CFD Network Newsletter, 2(4), 28-33. (108) Schlichting, H. (1979). Boundary Layer Theory. McGraw-Hill, New York. 373 (109) Shih, T.-H., Liou, W.W., Shabbir, A., Yang, Z. and Zhu, J. (1995). A new k-ε eddy viscosity model for high Reynolds number turbulent flows. Computer Fluids, 24(3), 227-238. (110) Shirasawa, T., Tominaga, T., Yoshie, R., Mochida, A., Yoshino, H., Kataoka, H. and Nozu, T. (2003). Development of CFD method for predicting wind environment around a high-rise building part 2: the cross comparison of CFD results using various k-models for the flow field around a building model with 4:4:1 shape. AIJ Journal of Technology and Design, 18, 169–174 (in Japanese). (111) Simiu, E. and Scanlan, R.H. (1986). Wind effects on structures. An introduction to wind engineering. 2nd Edition. John Wiley and Sons, New York. (112) Sini, J.F., Anquetin, S. and Mestayer, P.G. (1996). Pollutant dispersion and thermal effects in urban street canyons. Atmospheric Environment, 30(15), 2659-2677. (113) Snyder, W.H. (1981). Guidelines for Fluid Modeling of Atmospheric Diffusion. US Environmental Protection Agency, Office of Air Quality, Planning and Standards, Research Triangle Park, NC, EPA 600/8-81-009. (114) So, E.S.P., Chan, A.T.Y. and Wong, A.Y.T. (2005). Large-eddy simulations of wind flow and pollutant dispersion in a street canyon. Atmospheric Environment, 39, 3573-3582. (115) Sorensen, D.N. and Nielsen, P.V. (2003). Quality control of computational fluid dynamics in indoor environments. Indoor Air, 13(1), 2-17. (116) Stathopoulos, T. (1997). Computational wind engineering: Past achievements and future challenges. Journal of Wind Engineering and Industrial Aerodynamics, 67-68, 509-532. (117) Stathopoulos, T. and Baniotopoulos, C.C. (2007). Wind Effects on Buildings and Design of Wind Sensitive Structures. New York: Springer Wien. (118) Teodosiu, C. and Rusaouen, G. (2000). Modelisation des corps de chauffe a l’aide des codes de champ. Proceedings of the Fourth Fluent Users Meetings – France. Paris, France. (119) Teodosiu, C., Hohota, R., Rusaouen, G. and Woloszyn, M. (2003). Numerical prediction of indoor air humidity and its effect on indoor environment. Building and Environment, 38(5), 655-664. 374 (120) Teunissen, H.W. (1982). Validation of Boundary Layer Simulation: Some Comparisons between Model and Full-Scale Flows. Proceedings of the International Workshop on Wind Tunnel Modeling Criteria and Techniques in Civil Engineering Applications, (April 1982, Gaithersburg, MD), T.A. Reinhold, Ed. Cambridge University Press, New York, 217235. (121) The Straits Times. (2012). Punggol likely to have more private homes than other areas. Newspaper article (Friday, October 19th, 2012). Singapore. (122) Theurer, W. (1999). Typical building arrangements for urban air pollution modeling. Atmospheric Environment, 33(24), 4057-4066. (123) Uehara, K., Murakami, S., Oikawa, S. and Wakamatsu, S. (2000). Wind tunnel experiments on how thermal stratification affects flow in and above urban street canyons. Atmospheric Environment, 34(10), 15531562. (124) Vardoulakis, S., Fisher, B.E.A., Pericleous, K. and Gonzalez-Flesca, N. (2003). Modeling air quality in street canyons: a review. Atmospheric Environment, 37(2), 155-182. (125) Versteeg, H.K. and Malalasekera, W. (1995). An Introduction to Computational Fluid Dynamics – The Finite Volume Method. Longman Scientific and Technical, New York. (126) Wedding, J.B., Lombardi, D.J. and Cermak, J.E. (1977). A Wind Tunnel Study of Gaseous Pollutants in City Street Canyons. Journal of the Air Pollution Control Association, 27(6), 557-566. (127) Wharton, S. and Lundquist J.K. (2012). Assessing atmospheric stability and its impacts on rotor-disk wind characteristics at an onshore wind farm. Wind Energy, 15, 525-546. (128) Wieringa, J. (1992). Updating the Davenport roughness classification. Journal of Wind Engineering and Industrial Aerodynamics, 41(1-3), 357-368. (129) Wolfstein, M. (1969). The velocity and temperature distribution of onedimensional flow with turbulence augmentation and pressure gradient. International Journal of Heat and Mass Transfer, 12, 301-318. (130) Wong, A.K. and Yeh, S.H.K. (1985). Housing a nation – 25 years of public housing in Singapore. Singapore: Housing and Development Board (HDB). (131) Xie, X., Huang, Z. and Wang, J.S. (2005c). Impact of building configuration on air quality in street canyon. Atmospheric Environment, 36, 3601-3613. 375 (132) Xu, W., Chen, Q. and Nieuwstadt F.T.M. (1998). A new turbulence model for near-wall natural convection. International Journal of Heat and Mass Transfer, 41(21), 3161-3176. (133) Yamartino, R.J. and Wiegand, G. (1986). Development and Evaluation of Simple Models for the Flow, Turbulence and Pollution Concentration Fields within an Urban Street Canyon. Atmospheric Environment, 20, 2137-2156. (134) Yang, T. (2004). CFD and Field Testing of a Naturally Ventilated FullScale Building. PhD Thesis. University of Nottingham. (135) Yoshida, H. and Omae, M. (2005). An approach for analysis of urban morphology: methods to derive morphological properties of city blocks by using an urban landscape model and their interpretations. Computers, Environment and Urban Systems, 29, 223-247. (136) Zhang, A., Gao, C-L. and Zhang, L. (2005). Numerical simulation of the wind field around different building arrangements. Journal of Wind Engineering and Industrial Aerodynamics, 93, 891-904. 376 GLOSSARY Buildings’ Height Variation (HV) Defined as the standard deviation of the height variation for all the high-rise buildings within the precinct or estate. N It is formulated as HV = ∑ ∑(Hi − Have) where Have is N i=1 the average height (metres) of all the buildings within the precinct, Hi is the height (metres) of each individual building and N is the number of buildings in the precinct. Building Shape (BS) An urban morphological variable that is quantified by the Capacity Factor (CF). Compacity Factor (CF) Defined mathematically as C F =∑ areaofbuil dingenvelo pe volumeofbu ilding . It is a summation of all the buildings’ surface areas (metres square) over their building volumes (metres cube). The surface area of the building envelope consists of all the vertical external wall area, the roof (top) and ground floor area (bottom). The building volume is simply the section area of the building multiplied by the building height. Geometry (GEO) An urban morphological variable that is quantified by the Maximum Hydraulic Diameter (HDMax). Maximum Hydraulic Diameter (HDMax) Defined as the summation of all the largest hydraulic diameter (HD) of individual outdoor grid space, that are each area-weighted over the whole given precinct. HDMax = ∑ [(Largest HD of Area i)*(% of Area i in Precinct)]  HD is the hydraulic diameter of the studied area HD = 2HW/ (H+W) found within the precinct, where H = average height (metres) of both the upwind and downwind buildings on both sides of an open space or canyon, W = horizontal distance (or canyon width) between the buildings (metres). The calculation of HD is performed along linear traverses at each grid area by selecting the largest value from the superimposed matrices from the two traversal directions. The HDMax is computed by using the summation of area-weighted average of the spatial distribution of the largest composite HD value from each grid area. Open areas and street intersections will be calculated by using H as the average height of all the buildings 377 within the estate and W as the largest dimension of the whole estate (e.g. 500m for base case) to work out the HD value. Gross Building Coverage Ratio (GBCR) The ratio between gross ground floor area of a building to a given site area (land to building footprint). It is defined mathematically as ∑ builtarea , which is simply λp = ∑ builtarea + ∑ unbuiltare a the ground area covered by buildings (metres square) over the area of the whole precinct (metres square). Orientation (ORIENT) An urban morphological variable that focuses on the orientation of all the spaces in-between (urban canyons) the buildings within a precinct, each at an angle to the prevailing wind direction. It is quantified by using the Relative Sinuosity Index (Sθ). Relative Sinuosity ( S θ ) Defined mathematically as S θ = ∑ Li cos (θ i ) , where ∑ Li Li is the length (metres) of the linear segment i, and θi is the angle (degrees) between the given azimuth (of flow) and the azimuth of linear segment i. It is the summation of all linear canyon segments e.g. Main streets or breezeways, relative to the wind direction and indicates the degree of wind penetration into the whole precinct. Permeability (PERM) Defined as the summation of continuous pore space i, perpendicular to or an angle to wind direction, describing the corridor for wind flow within the building itself. Li is the length (metres) of the linear segment i (within the building), and θi is the angle (degrees) between the given azimuth (of wind flow) and the azimuth of linear segment i. HD is the hydraulic diameter (metres) of the cross-section area of the opening of continuous pore space i (within the building), which can be described as HD = 2HW/ (H+W). H = average height (metres) of the opening, W = average width (metres) of the opening. PERM = ∑ [(cos θi)2 * (π/4 * HD2)i * Li]bldg / ∑ Vbldg i Porosity volume within all the buildings in the precinct (m3) Total volume of all the buildings within the precinct (m3) But in situations whereby porosity occurring on all the four walls of a building (e.g. HDB void decks or sky gardens) instead of a continuous pore space opening at the front and end only, the opening at the 378 longer side of the building is treated as the width (W) to work out the HD, together with the height (H) of the pore space. The shorter side of the building will be treated as the length of the linear pore space (L). In this case (cos θi)2 can be considered as one unit as the four sides of the wall are open for wind to flow in unrestricted. Staggering of Blocks It is quantified by the Frontal Area Ratio (Afront) Arrangement (STAG) Index A front = ∑ i =1 Ai , frontalarea / ATOTALwallarea . [( n )] Afront is defined as the summation of all buildings’ frontal areas (metres square) that face the wind direction normally, over the total vertical wall area (metres square) of all buildings within the given site or precinct area. Ai,frontal area is the frontal area of each building i that faces the wind direction normally, and ATOTALwallarea is the total wall area of all the buildings within the given site area. Urban canyon A relatively narrow street with buildings lined up continuously along both sides. 379 APPENDICES 380 APPENDIX Derivation of Roughness Length (Z0) and Power-law Coefficient (α) Figure A1-1 shows the published field roughness determinations that were gathered for over thirty years from hundreds of field investigators who measured the roughness in all possible landscapes. Care was taken to make sure that the data were checked for quality in terms of their correct documentation of the investigated terrain, adequacy of the observation and evaluation methods, proper use of measurement arrays and making sure the described roughness came from a long enough fetch (Wieringa, 1992). Figure A1-1: Range of homogeneous surface roughness (Z0) from good experiments (Wieringa, 1992) Power-law Coefficient (α) The ABL is created by aerodynamic friction resulting from the motion of the air relative to the earth’s surface and thermal gradients between the upper atmosphere and the surface. The resultant is a vertical wind shear that varies not only in magnitude but also in structure. The variation in mean wind speeds with height above ground is often defined using the power-law relationship (Cochran, 2002). The magnitude of the power law coefficient (α) may vary between 0.1 in exceptionally smooth terrain to approximately 0.35 in very rough terrain such as built-up urban areas (Snyder, 1981). An estimate for the value of the powerlaw coefficient can be obtained from the surface roughness length (Z0), using the relationship from Counihan (Counihan, 1975): α = 0.24 + 0.096 log10 Z0 + 0.016(log10 Z0)2 = 0.24 + 0.096 log10 (0.50) + 0.016(log10 0.50)2 = 0.21 381 Figure A1-2 shows typical values for n (α in this case) and Z0 for various terrains ranging from seas to highly built-up urban areas, along with plots of the associated vertical velocity profiles. Figure A1-2: Longitudinal velocity profiles over uniform terrain in neutral flow (n here is actually α which is the power-law coefficient) (Cochran, 2002) Turbulence Intensity (TI) In addition to producing velocity deficit near the surface, the presence of aerodynamic friction and thermal gradients are also responsible for the creation of atmospheric turbulence (Cochran, 2002). The variation in the longitudinal turbulence intensity, TI, within the lower portion of the atmospheric boundary layer from to 100m above ground, can be defined from the following relationship from Snyder (Snyder, 1981): TI = α ln (30/Z0) ÷ ln (Z/Z0) ←valid for Z from 0.0~100.0m above ground = 0.21 ln (30/0.50) ÷ ln (100/0.50) = 0.16228 ≈ 0.16 (at 100m above ground) At heights above 100m, Snyder suggests that the turbulence intensity can be estimated by assuming a TI value of 0.01 at 600m and assuming a linear relationship between 100m and 600m. From Z > 100m onwards, assume a linear relationship between 100m~600m, where at 600m → TI = 0.01 Figure A1-3 shows the corresponding variation in longitudinal turbulence as a function of height above ground for the same terrain features shown in vertical velocity profiles indicated in Figure A1-2. 382 Figure A1-3: Turbulent intensity profiles over uniform terrain in neutral flow (n here is actually α which is the power-law coefficient) (Cochran, 2002) A reasonable estimate of 0.05 for TI will be suitable for strongly stable wind (TI < 0.08) for free-stream air (Wharton and Lundquist, 2012). Slope = (0.01-0.16) / (600 – 100) = -0.0003 At TI = 0.05, the height above ground (H) is equal to: -0.0003 = (0.05 – 0.16) / (H – 100) H = 466.67m ≈ 467m (above ground) The free stream velocity at 467m is around 5.56m/s (power-law plot from BCA’s average wind velocity of 2.7m/s at 15m) (BCA, 2012). Figure A1-4 shows the wind velocity profile worked out from BCA’s specifications using α=0.21. 383 Figure A1-4: Power-law wind velocity plot of worked out from BCA’s specifications (α=0.21) Turbulence Kinetic Energy (TKE) and Dissipation Rate (ε) TKE = 3/2 (U*TI)2 = 3/2 (5.56 * 0.05)2 = 0.115926 J/kg ≈ 0.11593 J/kg ε = [Cμ3/4 TKE3/2]/L , where L = 0.07*characteristic length. = [(0.09)3/4 (0.11593)3/2] / (0.07*500) = 1.8530414E-4 J/kg-s = 1.85304E-4 J/kg-s The characteristic length = 500m (longest dimension of the precinct). 384 [...]... blocks, mid -level of GBCR - courtyard configuration 14 9 Table 5 .15 : Tabulated values of HV for the parametric study for point and slab blocks 15 1 Table 5 .16 : Parametric study findings and their explanations for point blocks, pedestrian level of HV - random configuration 15 3 Table 5 .17 : Parametric study findings and their explanations for point blocks, pedestrian level of HV -... positions for point blocks (top) and slab blocks (bottom) 11 4  Figure 4.5: Comparison of wind tunnel and CFD readings for point blocks, 0˚ north wind orientation, at both the pedestrian and mid -level 11 6  Figure 4.6: Comparison of wind tunnel and CFD readings for point blocks, 22.5˚ north wind orientation, at both the pedestrian and mid -level 11 7  Figure 4.7: Comparison of wind tunnel... readings for point blocks, 45˚ north wind orientation, at both the pedestrian and mid -level 11 7  Figure 4.8: Comparison of wind tunnel and CFD readings for slab blocks, 0˚ north wind orientation, at both the pedestrian and mid -level 11 8  Figure 4.9: Comparison of wind tunnel and CFD readings for slab blocks, 45˚ north wind orientation, at both the pedestrian and mid -level 11 8  Figure 4 .10 :... Figure 4 .10 : Comparison of wind tunnel and CFD readings for slab blocks, 90˚ north wind orientation, at both the pedestrian and mid -level 11 9  xxvi Figure 4 .11 : Box-plot for the difference between CFD and wind tunnel readings (CFD minus wind tunnel readings in m/s) for (a) point blocks and (b) slab blocks 12 0  Figure 5 .1: Pedestrian level area-averaged VR against GBCR for (a) random, (b)... perimeter outline of the enclosed precinct area 327  Figure 8.9: Plan view of proposed HDB precinct base design indicating the perimeter outline of the enclosed precinct area and individual outdoor grid space 329  xxxi Figure 8 .10 : Plan view of proposed HDB precinct base design indicating the building perimeter that faces the wind direction normally without being blocked (red) for wind orientation... findings and their explanations for point blocks, pedestrian level of GBCR - courtyard configuration 13 1 xv Table 5.6: Parametric study findings and their explanations for point blocks, mid -level of GBCR - random configuration 13 4 Table 5.7: Parametric study findings and their explanations for point blocks, mid -level of GBCR - group configuration 13 5 Table 5.8: Parametric study findings... explanations for point blocks, mid -level of GBCR - courtyard configuration 13 6 Table 5.9: Parametric study findings and their explanations for slab blocks, pedestrian level of GBCR - random configuration 14 1 Table 5 .10 : Parametric study findings and their explanations for slab blocks, pedestrian level of GBCR - group configuration 14 2 Table 5 .11 : Parametric study findings and their... patterns of behavior have important implications for building and urban planning development of residential estates in future and support the possibility of using all these variables in the form of morphological indices (independent variables) – to build an overall Wind Velocity Ratio model using the area-averaged Wind Velocity Ratio (VR) as the dependent variable The development of the models (one for. .. 15 5 Table 5 .18 : Parametric study findings and their explanations for point blocks, mid -level of HV - random configuration 15 8 xvi Table 5 .19 : Parametric study findings and their explanations for point blocks, mid -level of HV - stratified configuration 15 9 Table 5.20: Parametric study findings and their explanations for slab blocks, pedestrian level of HV - random configuration 16 2... explanations for slab blocks, pedestrian level of GBCR - courtyard configuration 14 4 Table 5 .12 : Parametric study findings and their explanations for slab blocks, mid -level of GBCR - random configuration 14 7 Table 5 .13 : Parametric study findings and their explanations for slab blocks, mid -level of GBCR - group configuration 14 8 Table 5 .14 : Parametric study findings and their explanations for . Motivation 1 1. 1 .1 Reduction of Wind Speed 2 1. 1.2 Research Motivation 2 1. 1.3 Developments in this Research Area 4 1. 1.4 Design Standards for Optimal Ventilation 5 1. 1.4 .1 Singapore – HDB. 5.3 .1. 1 .1 Point Blocks, Pedestrian Level 12 5 5.3 .1. 1 .1. 1 Point Blocks, Pedestrian Level - Random Configuration 12 7 5.3 .1. 1 .1. 2 Point Blocks, Pedestrian Level - Group Configuration 12 8 . LEVEL VENTILATION 12 1 5 .1 Introduction 12 1 5.2 Parametric Approach 12 2 5.3 Findings from Parametric Study 12 2 5.3 .1 Gross Building Coverage Ratio (GBCR) 12 2 5.3 .1. 1 Point Blocks 12 5

Ngày đăng: 10/09/2015, 09:05

TỪ KHÓA LIÊN QUAN