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   <subfield code="a">10.1007/s10652-010-9202-z</subfield>
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   <subfield code="a">(NATIONALLICENCE)springer-10.1007/s10652-010-9202-z</subfield>
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  <datafield tag="245" ind1="0" ind2="0">
   <subfield code="a">On the heating environment in street canyon</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[Rizwan Memon, D. Leung]</subfield>
  </datafield>
  <datafield tag="520" ind1="3" ind2=" ">
   <subfield code="a">This study investigates the impact of building aspect ratio (building-height-to-street-canyon-width-ratio), wind speed and surface and air-temperature difference (Δθs−a) on the heating environment within street canyon. The Reynolds-averaged Navier-Stokes (RANS) and energy transport equations were solved with Renormalization group (RNG) theory version of k-$${\varepsilon}$$ turbulence model. The validation process demonstrated that the model could be trusted for simulating air-temperature and velocity trends. The temperature and velocity patterns were discussed in idealized street canyons of different aspect ratios (0.5-2.0) with varying ambient wind speeds (0.5-1.5m/s) and Δθs−a (2-8K). Results show that air-temperatures are directly proportional to bulk Richardson number (R b) for all but ground heating situation. Conversely, air-temperatures increase significantly across the street canyon with a decrease in ambient wind speed; however, the impact of Δθs−a was negligible. Clearly, ambient wind speed decreases significantly as it passes over higher AR street canyons. Notably, air-temperatures were the highest when the windward wall was heated and the least during ground heating. Conversely, air-temperatures were lower along the windward side but higher within the street canyon when the windward wall was heated.</subfield>
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   <subfield code="a">The Author(s), 2010</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Heating</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Surface-temperature</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">CFD</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Turbulence</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Street-canyon</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">AR : Aspect ratio</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">H : Street canyon height (m)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">W : Street canyon width (m)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">X/W : Spatial co-ordinate in X-direction non-dimensionalised by street canyon width</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">$${\overline{{u}}_i }$$ : Mean streamwise (u) and vertical (υ) velocity components (ms−1)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">u a : Horizontal inflow wind speed (ms−1)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">$${\varepsilon}$$ : Dissipation rate of turbulent kinetic energy (m2s−3)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">θ g : Ground level temperature (K)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">μ eff : Effective turbulent viscosity</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">G b : Turbulence kinetic energy production due to buoyancy (kgm−1s−3)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Pr t : Turbulent Prandtl number</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">υ : Kinematic viscosity (μ eff/ρ) (m2s−1)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">$${\overline{{u}'_i {u}'_j}}$$ : Reynolds stresses (m2s−2)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Re y : Wall distance based Reynolds number</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">g : Acceleration due to gravity (ms−2)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">p : Pressure (Pascal)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">u i : Velocity components (u,v) in the x and z directions (ms−1)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Z/H : Spatial coordinate in Z direction non-dimensionalized by street canyon height</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Re H : Reynolds number (based on street canyon height) = uaH/ ν</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">R b : $${{\rm Bulk \, Richardson \, number} = \frac{gH(\theta_a -\theta_g )}{\theta_a u_a ^{2}}}$$</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">k : Turbulent kinetic energy (m2s−2)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">θ a : Ambient air-temperature (K)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">μ t : Turbulent viscosity</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">G k : Turbulence kinetic energy production due to mean velocity gradient (kgm−1 s −3)</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">β : Thermal expansion coefficient (K)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">S ij : Mean rate of strain tensor (1/s)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">$${\alpha_{k}, \alpha_{\varepsilon}}$$ : Inverse Prandtl number for k and $${\varepsilon}$$</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Δ θ s−a : Difference between the surface and ambient air-temperature (K)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Memon</subfield>
   <subfield code="D">Rizwan</subfield>
   <subfield code="u">Department of Mechanical Engineering, Mehran University of Engineering &amp; Technology, Jamshoro, Sindh, Pakistan</subfield>
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   <subfield code="a">Leung</subfield>
   <subfield code="D">D.</subfield>
   <subfield code="u">Department of Mechanical Engineering, University of Hong Kong, Pokfulam Road, Pokfulam, Hong Kong</subfield>
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   <subfield code="t">Environmental Fluid Mechanics</subfield>
   <subfield code="d">Springer Netherlands</subfield>
   <subfield code="g">11/5(2011-10-01), 465-480</subfield>
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   <subfield code="a">research-article</subfield>
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   <subfield code="a">Metadata rights reserved</subfield>
   <subfield code="b">Springer special CC-BY-NC licence</subfield>
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