Large eddy simulation of ABL flow around a parabolic concave roof model
Numerical simulation by means of Large Eddy Simulation (LES) was carried out to study the effects of an Atmospheric Boundary Layer (ABL) flow around a parabolic concave roof model. The effects of inflow wind velocity and sag depth of the roof on time averaged drag coefficient, C_D , and pressure coe...
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2016
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sg-ntu-dr.10356-683372023-03-04T18:15:13Z Large eddy simulation of ABL flow around a parabolic concave roof model Zulfadli Bin Abdul Latiff Martin Skote School of Mechanical and Aerospace Engineering DRNTU::Engineering::Mechanical engineering::Fluid mechanics Numerical simulation by means of Large Eddy Simulation (LES) was carried out to study the effects of an Atmospheric Boundary Layer (ABL) flow around a parabolic concave roof model. The effects of inflow wind velocity and sag depth of the roof on time averaged drag coefficient, C_D , and pressure coefficient, C_P , was investigated. Reynolds number was kept above (2-3)*10^4 to allow for scalability. It was found that C_D increases as flow velocity increases, opposing the general trend for flow around a bluff body that C_D will decrease when Reynolds number increases. This is possibly due to the flow in the concaved region of the roof. C_P decreases on both the windward wall and leeward wall as flow velocity increases. As sag depth increases, C_D increases and the magnitude of C_P increases on both the windward wall and leeward wall. Bachelor of Engineering (Mechanical Engineering) 2016-05-25T06:53:16Z 2016-05-25T06:53:16Z 2016 Final Year Project (FYP) http://hdl.handle.net/10356/68337 en Nanyang Technological University 76 p. application/pdf |
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DRNTU::Engineering::Mechanical engineering::Fluid mechanics Zulfadli Bin Abdul Latiff Large eddy simulation of ABL flow around a parabolic concave roof model |
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Numerical simulation by means of Large Eddy Simulation (LES) was carried out to study the effects of an Atmospheric Boundary Layer (ABL) flow around a parabolic concave roof model. The effects of inflow wind velocity and sag depth of the roof on time averaged drag coefficient, C_D , and pressure coefficient, C_P , was investigated. Reynolds number was kept above (2-3)*10^4 to allow for scalability. It was found that C_D increases as flow velocity increases, opposing the general trend for flow around a bluff body that C_D will decrease when Reynolds number increases. This is possibly due to the flow in the concaved region of the roof. C_P decreases on both the windward wall and leeward wall as flow velocity increases. As sag depth
increases, C_D increases and the magnitude of C_P increases on both the windward wall and
leeward wall. |
author2 |
Martin Skote |
author_facet |
Martin Skote Zulfadli Bin Abdul Latiff |
format |
Final Year Project |
author |
Zulfadli Bin Abdul Latiff |
author_sort |
Zulfadli Bin Abdul Latiff |
title |
Large eddy simulation of ABL flow around a parabolic concave roof model |
title_short |
Large eddy simulation of ABL flow around a parabolic concave roof model |
title_full |
Large eddy simulation of ABL flow around a parabolic concave roof model |
title_fullStr |
Large eddy simulation of ABL flow around a parabolic concave roof model |
title_full_unstemmed |
Large eddy simulation of ABL flow around a parabolic concave roof model |
title_sort |
large eddy simulation of abl flow around a parabolic concave roof model |
publishDate |
2016 |
url |
http://hdl.handle.net/10356/68337 |
_version_ |
1759858164274036736 |