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Advances in the treatment of street 
canyons and urban canopy flow in 
ADMS-Urban and ADMS-Roads 
Martin Seaton 
DMUG 
December 2014
DMUG 2014 
Contents 
• Background 
• Urban Canopy 
– Theory 
– Implementation in ADMS-Urban 
• Advanced Canyon 
– Theory 
– Implementation in ADMS-Urban 
• ADMS-Urban model set-up for London 
• Validation results 
• Conclusions
DMUG 2014 
Background 
In collaboration with the Hong Kong University of Science and Technology 
(HKUST), CERC have been contracted to develop an air dispersion modelling 
system appropriate for use in the Hong Kong Special Administrative Region 
• 3 500 km2 domain including: 
– Urban, rural and industrial regions 
– Complex topography 
– Marine environments
DMUG 2014 
Background 
• Two aspects to this work: 
– Improvement in modelling of urban areas – focus of this presentation 
– Develop a system to automatically nest ADMS-Urban in a regional 
model – ADMS-Urban Regional Model Link 
(www.cerc.co.ukRML)
Background: Urban Canopy 
• Urban architecture affects local air flow 
• Important to use urban flow characteristics for accurate calculation of 
DMUG 2014 
pollutant dispersion 
• Earliest historic studies (CFD, wind tunnel and field experiments) 
used regular arrays of cubic obstacles to represent urban buildings 
• Some later extensions to real 
urban areas with irregular 
arrays and non-cubic 
buildings 
• CERC parameterisation 
based on published 
experimental data, CFD 
modelling and theoretical 
considerations
DMUG 2014 
Background: Advanced Canyon 
• Many modern urban areas feature closely-packed tall buildings which form 
street canyons 
• Existing dispersion models for street canyons, eg. 
OSPM, were developed based on ‘European’ urban 
geometries 
– Canyon heights and widths of similar magnitude 
– Symmetric properties on each side of a canyon 
• Choice required between canyon and non-canyon 
modelling 
• A comprehensive model for street canyons 
should include: 
– Tall canyons (height/width > 1) 
– Asymmetric canyons: height, width, building density 
– Pavements and traffic lanes 
– Smooth transition between non-canyon and canyon 
modelling
DMUG 2014 
Urban Canopy 
Theory: Velocity 
• Upstream wind velocity profile is displaced above the buildings 
• Velocities are reduced below the average building height 
Uo 
Upstream flow 
UC 
z 
UH
DMUG 2014 
Urban Canopy 
Theory: Velocity 
• Upstream wind velocity profile is displaced above the buildings 
• Velocities are reduced below the average building height
• Turbulent velocities are reduced below the average building height 
DMUG 2014 
Urban Canopy 
Theory: Turbulence 
Uo 
Upstream flow 
σ 
z
DMUG 2014 
Urban Canopy 
Theory: Characterisation of urban area 
Figure from Evans CASA paper 
• Effective roughness z0b and displacement height d calculated 
relative to average building height H using plan and frontal 
area fractions λP and λF 
• λP = AP/AT • λF = AF/AT • d/H = 1 + (λP – 1)α-λP 
• z0b/H = (1-d/H)exp{-(0.5βCDλF(1-d/H)/κ2)-0.5} 
Macdonald et al. 1998 Atmos. Environ. 32:1857-1864
Transition region with 
linear smoothing 
DMUG 2014 
Urban Canopy 
Implementation in ADMS-Urban: Velocity 
Three-part velocity profile: above 2x displacement height, below 
displacement height and transition region. 
d 
d 
U 
z 
Details of standard ADMS velocity profiles can be found at 
http://www.cerc.co.uk/environmental-software/technical-specifications.html 
Standard ADMS-Urban 
profile displaced 
upwards by d with local 
roughness z0b 
Logarithmic velocity 
profile near surface
DMUG 2014 
Urban Canopy 
Implementation in ADMS-Urban: Turbulence 
Two part profile: above and below displacement height 
z 
Details of standard ADMS turbulent velocity profiles can be found at 
http://www.cerc.co.uk/environmental-software/technical-specifications.html 
d 
σ 
Standard ADMS 
profile, displaced 
upwards by d, with 
local roughness z0b 
Turbulence decays 
towards the ground
Urban Canopy 
Implementation in ADMS-Urban: Flow regimes 
• Full urban canopy if displacement height d > max(2 m, H/2) 
DMUG 2014 
– Full urban canopy flow profiles 
– Effective roughness length due to buildings z0b < d/2 
• Low displacement if displacement height d < max(2 m, H/2) 
– Interpolation between full urban canopy and no displacement 
• No displacement if displacement height d < max(1 m, H/10) 
– Standard ADMS-Urban flow profiles with local roughness z0b 
• No urban canopy if displacement height d < 1 mm 
– Standard ADMS-Urban flow profiles used
DMUG 2014 
Advanced Canyon 
Theory: Canyon properties 
Each side of the canyon has properties 
• Whether there is a canyon wall: minimum height and building length 
• Height: average, minimum and maximum 
• Width: from road centreline to canyon wall 
• Porosity: proportion of canyon wall without buildings ie. 
1-(building length/total length) 
These are combined to find total canyon width (wall to wall) g, 
average height H and overall porosity α 
Upstream wind 
U 
H 
g
DMUG 2014 
Advanced Canyon 
Theory: Canyon effects 
5 principal effects of street canyons on dispersion 
1. Pollutants are channelled along street canyons 
2. Pollutants are dispersed across street canyons by circulating 
flow at road height 
3. Pollutants are trapped in recirculation regions 
4. Pollutants leave the canyon through gaps between buildings as if 
there was no canyon 
5. Pollutants leave the canyon from the canyon top 
1 
Upstream wind 
U 
2 
3 
5 
4
DMUG 2014 
Advanced Canyon 
Theory: Component sources 
Each effect is modelled using a component source, with differing 
• Source geometry 
• Source dispersion type 
• Wind direction 
• Region of influence 
• Source strength 
The final concentration is the weighted sum of contributions from 
the component sources 
1 
Upstream wind 
U 
2 
3 
5 
4
DMUG 2014 
Advanced Canyon 
ADMS-Urban Implementation: Canyon flow 
• Upstream wind is split into components parallel and 
perpendicular to the canyon axis 
• Perpendicular component is further reduced in magnitude due 
to recirculation ĥ(z) and obstacles (user-editable factor η) 
Ux(z) = U(z) cos Δφ 
Uy(z) = U(z) η ĥ(z) sin Δφ 
Upstream 
wind U 
Ux 
Uy 
Δφ
Advanced Canyon 
ADMS-Urban Implementation: S1 Along canyon 
• Pollution is advected and dispersed by flow channelled along 
DMUG 2014 
the canyon 
– Geometry: standard road 
– Dispersion: 
• standard ADMS-Urban road with width limit due to canyon walls and 
simplified calculation of mean plume height 
• well-mixed across canyon after a reflection reaches the opposite wall 
• option to set a constant segment length to obtain constant along-canyon 
concentration (continuous road network assumption) 
– Wind direction: along canyon 
– Region of influence: within canyon 
1 
Upstream 
wind U 
3 
2 
5 
4 Ux
Advanced Canyon 
ADMS-Urban Implementation: S2 Across canyon 
DMUG 2014 
• Pollution is dispersed across the canyon by circulating flow 
• Deeper canyons have more complex flow structures 
– Geometry: standard road 
– Dispersion: well-mixed along road, analytical integration across 
road to output point 
– Wind direction: across canyon, opposite direction to upstream if 
a shallow canyon, both opposite and in line with upstream if deep 
– Region of influence: within canyon 
1 
Upstream 
wind U 
3 
2 
5 
U 
4 Shallow canyon: 
single circulation 
U 
Deep canyon: 
multiple circulation 
Uy
Advanced Canyon 
ADMS-Urban Implementation: S3 Recirculation 
• Pollution can be trapped within the canyon by the recirculating 
DMUG 2014 
flow 
– Geometry: full width of canyon, height depends on H and g 
– Dispersion: well mixed, analytical solution 
– Wind direction: n/a 
– Region of influence: within canyon 
1 
Upstream 
wind U 
3 
2 
5 
4 
U 
Shallow symmetric 
canyon 
U 
Deep symmetric canyon 
U 
U 
Shallow asymmetric 
canyons
Advanced Canyon 
ADMS-Urban Implementation: S4 Non-canyon 
• Some of the pollution from the road disperses through gaps 
DMUG 2014 
between buildings in the canyon walls 
• Allows for transition from open to full canyon roads 
– Geometry: standard road 
– Dispersion: standard ADMS-Urban road 
– Wind direction: upstream 
– Region of influence: inside and outside canyon 
1 
Upstream 
wind U 
3 
2 
5 
4 
U 
Details of standard ADMS source definitions and dispersion calculations can be found at 
http://www.cerc.co.uk/environmental-software/technical-specifications.html
Advanced Canyon 
ADMS-Urban Implementation: S5 Canyon top 
DMUG 2014 
• Pollution leaves the canyon from the top 
– Geometry: volume source with canyon width, depth depends on 
canyon height 
– Dispersion: standard ADMS-Urban volume source 
– Wind direction: upstream 
– Region of influence: outside canyon 
1 
Upstream 
wind U 
3 
2 
5 
4 
U
Advanced Canyon 
ADMS-Urban Implementation: Source weightings 
DMUG 2014 
• Balance between in-canyon (S1,S2) and non-canyon (S4) 
weighting based on porosity squared 
• Non-canyon increased if the canyon is shallow 
• In-canyon divided between along-canyon (S1) and across-canyon 
(S2) based on wind direction relative to canyon axis 
• In-canyon (S1, S2) may be reduced due to canyon asymmetry 
• Canyon-top (S5) equal to in-canyon (1-S4) 
• Recirculation (S3) equal to across-canyon (S2) 
1 
Upstream 
wind U 
3 
2 
4 
5
road centreline vertical profile 
DMUG 2014 
Example concentration profiles 
• Shallow symmetric canyon, perpendicular wind 
1.5 m output height across-canyon 
100 
90 
80 
70 
60 
50 
40 
30 
20 
10 
0 
profile 
-10 0 10 20 30 40 50 
Concentration (ug/m3) 
Distance from road centreline (m) 
Road 
Pavements 
45 
40 
35 
30 
25 
20 
15 
10 
5 
0 
0 20 40 60 80 100 
Z (m) 
Concentration (ug/m3) 
C1Q1 
C2Q2 
C3Q3 
C4Q4 
C5Q5 
Total AC 
No Canyon 
Old Canyon+NB 
1 
2 
3 
4 
5 
U
DMUG 2014 
ADMS-Urban model set-up for London 
Input data 
• Standard ADMS-Urban modelling approach for London 
– Measured meteorological data from Heathrow airport 
– Measured upwind rural background concentrations 
– London Atmospheric Emissions Inventory (LAEI) emissions data 
– Modelling year 2012 
– Modelling domain 10x15 km central London 
• Model configurations tested 
– No canyon: no street canyon modelling 
– Basic canyon: existing ADMS-Urban street canyon model 
– Advanced canyon & Urban Canopy: Urban Canopy flow field 
with new street canyon modelling
DMUG 2014 
ADMS-Urban model set-up for London 
Monitoring network 
• 29 monitors located within the ‘buildings data’ area 
• Monitor information (values, locations, heights) available from web 
• Data for NOx, NO2, PM10, PM2.5, O3 
• 21 kerbside/roadside, 8 urban background 
– Some of the urban background sites are within canyons 
• Monitor heights generally less than or equal to 3 m 
Monitors 
16 km
DMUG 2014 
Validation Results 
Tools used for analysis 
• MyAir Toolkit for Model Evaluation 
http://www.cerc.co.uk/environmental-software/myair-toolkit.html 
• openair 
http://www.openair-project.org/Downloads/Default.aspx 
Wind speed in m/s 
shown radially 
Polar plots 
Example shows observed NOx 
concentrations at a single 
receptor 
Hourly data binned according to 
wind speed and direction 
Colour indicates average 
concentration for each bin 
Observations at this site 
indicate high concentrations 
for a range of wind speeds 
and restricted wind directions 
Concentration bins with 
<8 entries shown in grey
DMUG 2014 
Validation Results 
Mean NO2 concentrations scatter plot 
• All sites shown 
• When canyons are 
modelled, means 
usually increase, 
giving a better 
estimate 
• Modelling canyons 
does not affect the 
lower concentration 
sites
DMUG 2014 
Validation Results 
NO2 concentration statistics 
• Data for all sites for whole year 
• Best statistics highlighted 
Data Mean NMSE R Fac2 Fb 
Observed 70.8 0.00 1.00 1.00 0.00 
No Canyon 53.8 0.76 0.36 0.73 -0.27 
Basic Canyon 61.5 0.53 0.49 0.79 -0.14 
Advanced Canyon & 
Urban Canopy 
63.1 0.39 0.62 0.81 -0.11
DMUG 2014 
Validation Results 
Polar plots: Full canyon 
• Consider a receptor ‘CD9’ within a standard canyon (H/g = 0.96, porosity = 0.26) 
• Wind from North West gives 
low concentrations and from 
the South East gives high 
concentrations due to 
presence of canyon 
• ‘No canyon’ and ‘Basic 
canyon’ runs predict similar 
concentrations in all 
directions 
Observations No canyon 
Basic canyon Advanced canyon & UC 
NO2 
concentrations
DMUG 2014 
Validation Results 
Polar plots: Asymmetric canyon 
• Consider a receptor ‘HF4’ within an asymmetric canyon (H = 15 m) 
• Wind from West gives high 
concentrations and from the 
East gives lower 
concentrations due to 
presence of asymmetric 
canyon 
• ‘No canyon’ and ‘Basic 
canyon’ runs predict wind 
from East giving higher 
values 
Observations No canyon 
Basic canyon Advanced canyon & UC 
NO2 
concentrations
DMUG 2014 
Conclusions 
• New methodologies for modelling an urban canopy flow field 
and advanced street canyon effects have been developed. 
• Modules based on these developments have been added to 
ADMS-Urban 
• Validation ongoing in London and Hong Kong in order to 
finalise the advanced canyon model 
• Combined with nesting within a regional model these 
developments allow for a multi-scale of modelling from regional 
down to street scale
DMUG 2014 
Acknowledgements 
The urban canopy and advanced street canyon modules have 
been developed in collaboration with researchers from the 
Hong Kong University of Science and Technology, supported 
by the Hong Kong Environmental Protection Department.

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Martin Seaton - DMUG 2014

  • 1. Advances in the treatment of street canyons and urban canopy flow in ADMS-Urban and ADMS-Roads Martin Seaton DMUG December 2014
  • 2. DMUG 2014 Contents • Background • Urban Canopy – Theory – Implementation in ADMS-Urban • Advanced Canyon – Theory – Implementation in ADMS-Urban • ADMS-Urban model set-up for London • Validation results • Conclusions
  • 3. DMUG 2014 Background In collaboration with the Hong Kong University of Science and Technology (HKUST), CERC have been contracted to develop an air dispersion modelling system appropriate for use in the Hong Kong Special Administrative Region • 3 500 km2 domain including: – Urban, rural and industrial regions – Complex topography – Marine environments
  • 4. DMUG 2014 Background • Two aspects to this work: – Improvement in modelling of urban areas – focus of this presentation – Develop a system to automatically nest ADMS-Urban in a regional model – ADMS-Urban Regional Model Link (www.cerc.co.ukRML)
  • 5. Background: Urban Canopy • Urban architecture affects local air flow • Important to use urban flow characteristics for accurate calculation of DMUG 2014 pollutant dispersion • Earliest historic studies (CFD, wind tunnel and field experiments) used regular arrays of cubic obstacles to represent urban buildings • Some later extensions to real urban areas with irregular arrays and non-cubic buildings • CERC parameterisation based on published experimental data, CFD modelling and theoretical considerations
  • 6. DMUG 2014 Background: Advanced Canyon • Many modern urban areas feature closely-packed tall buildings which form street canyons • Existing dispersion models for street canyons, eg. OSPM, were developed based on ‘European’ urban geometries – Canyon heights and widths of similar magnitude – Symmetric properties on each side of a canyon • Choice required between canyon and non-canyon modelling • A comprehensive model for street canyons should include: – Tall canyons (height/width > 1) – Asymmetric canyons: height, width, building density – Pavements and traffic lanes – Smooth transition between non-canyon and canyon modelling
  • 7. DMUG 2014 Urban Canopy Theory: Velocity • Upstream wind velocity profile is displaced above the buildings • Velocities are reduced below the average building height Uo Upstream flow UC z UH
  • 8. DMUG 2014 Urban Canopy Theory: Velocity • Upstream wind velocity profile is displaced above the buildings • Velocities are reduced below the average building height
  • 9. • Turbulent velocities are reduced below the average building height DMUG 2014 Urban Canopy Theory: Turbulence Uo Upstream flow σ z
  • 10. DMUG 2014 Urban Canopy Theory: Characterisation of urban area Figure from Evans CASA paper • Effective roughness z0b and displacement height d calculated relative to average building height H using plan and frontal area fractions λP and λF • λP = AP/AT • λF = AF/AT • d/H = 1 + (λP – 1)α-λP • z0b/H = (1-d/H)exp{-(0.5βCDλF(1-d/H)/κ2)-0.5} Macdonald et al. 1998 Atmos. Environ. 32:1857-1864
  • 11. Transition region with linear smoothing DMUG 2014 Urban Canopy Implementation in ADMS-Urban: Velocity Three-part velocity profile: above 2x displacement height, below displacement height and transition region. d d U z Details of standard ADMS velocity profiles can be found at http://www.cerc.co.uk/environmental-software/technical-specifications.html Standard ADMS-Urban profile displaced upwards by d with local roughness z0b Logarithmic velocity profile near surface
  • 12. DMUG 2014 Urban Canopy Implementation in ADMS-Urban: Turbulence Two part profile: above and below displacement height z Details of standard ADMS turbulent velocity profiles can be found at http://www.cerc.co.uk/environmental-software/technical-specifications.html d σ Standard ADMS profile, displaced upwards by d, with local roughness z0b Turbulence decays towards the ground
  • 13. Urban Canopy Implementation in ADMS-Urban: Flow regimes • Full urban canopy if displacement height d > max(2 m, H/2) DMUG 2014 – Full urban canopy flow profiles – Effective roughness length due to buildings z0b < d/2 • Low displacement if displacement height d < max(2 m, H/2) – Interpolation between full urban canopy and no displacement • No displacement if displacement height d < max(1 m, H/10) – Standard ADMS-Urban flow profiles with local roughness z0b • No urban canopy if displacement height d < 1 mm – Standard ADMS-Urban flow profiles used
  • 14. DMUG 2014 Advanced Canyon Theory: Canyon properties Each side of the canyon has properties • Whether there is a canyon wall: minimum height and building length • Height: average, minimum and maximum • Width: from road centreline to canyon wall • Porosity: proportion of canyon wall without buildings ie. 1-(building length/total length) These are combined to find total canyon width (wall to wall) g, average height H and overall porosity α Upstream wind U H g
  • 15. DMUG 2014 Advanced Canyon Theory: Canyon effects 5 principal effects of street canyons on dispersion 1. Pollutants are channelled along street canyons 2. Pollutants are dispersed across street canyons by circulating flow at road height 3. Pollutants are trapped in recirculation regions 4. Pollutants leave the canyon through gaps between buildings as if there was no canyon 5. Pollutants leave the canyon from the canyon top 1 Upstream wind U 2 3 5 4
  • 16. DMUG 2014 Advanced Canyon Theory: Component sources Each effect is modelled using a component source, with differing • Source geometry • Source dispersion type • Wind direction • Region of influence • Source strength The final concentration is the weighted sum of contributions from the component sources 1 Upstream wind U 2 3 5 4
  • 17. DMUG 2014 Advanced Canyon ADMS-Urban Implementation: Canyon flow • Upstream wind is split into components parallel and perpendicular to the canyon axis • Perpendicular component is further reduced in magnitude due to recirculation ĥ(z) and obstacles (user-editable factor η) Ux(z) = U(z) cos Δφ Uy(z) = U(z) η ĥ(z) sin Δφ Upstream wind U Ux Uy Δφ
  • 18. Advanced Canyon ADMS-Urban Implementation: S1 Along canyon • Pollution is advected and dispersed by flow channelled along DMUG 2014 the canyon – Geometry: standard road – Dispersion: • standard ADMS-Urban road with width limit due to canyon walls and simplified calculation of mean plume height • well-mixed across canyon after a reflection reaches the opposite wall • option to set a constant segment length to obtain constant along-canyon concentration (continuous road network assumption) – Wind direction: along canyon – Region of influence: within canyon 1 Upstream wind U 3 2 5 4 Ux
  • 19. Advanced Canyon ADMS-Urban Implementation: S2 Across canyon DMUG 2014 • Pollution is dispersed across the canyon by circulating flow • Deeper canyons have more complex flow structures – Geometry: standard road – Dispersion: well-mixed along road, analytical integration across road to output point – Wind direction: across canyon, opposite direction to upstream if a shallow canyon, both opposite and in line with upstream if deep – Region of influence: within canyon 1 Upstream wind U 3 2 5 U 4 Shallow canyon: single circulation U Deep canyon: multiple circulation Uy
  • 20. Advanced Canyon ADMS-Urban Implementation: S3 Recirculation • Pollution can be trapped within the canyon by the recirculating DMUG 2014 flow – Geometry: full width of canyon, height depends on H and g – Dispersion: well mixed, analytical solution – Wind direction: n/a – Region of influence: within canyon 1 Upstream wind U 3 2 5 4 U Shallow symmetric canyon U Deep symmetric canyon U U Shallow asymmetric canyons
  • 21. Advanced Canyon ADMS-Urban Implementation: S4 Non-canyon • Some of the pollution from the road disperses through gaps DMUG 2014 between buildings in the canyon walls • Allows for transition from open to full canyon roads – Geometry: standard road – Dispersion: standard ADMS-Urban road – Wind direction: upstream – Region of influence: inside and outside canyon 1 Upstream wind U 3 2 5 4 U Details of standard ADMS source definitions and dispersion calculations can be found at http://www.cerc.co.uk/environmental-software/technical-specifications.html
  • 22. Advanced Canyon ADMS-Urban Implementation: S5 Canyon top DMUG 2014 • Pollution leaves the canyon from the top – Geometry: volume source with canyon width, depth depends on canyon height – Dispersion: standard ADMS-Urban volume source – Wind direction: upstream – Region of influence: outside canyon 1 Upstream wind U 3 2 5 4 U
  • 23. Advanced Canyon ADMS-Urban Implementation: Source weightings DMUG 2014 • Balance between in-canyon (S1,S2) and non-canyon (S4) weighting based on porosity squared • Non-canyon increased if the canyon is shallow • In-canyon divided between along-canyon (S1) and across-canyon (S2) based on wind direction relative to canyon axis • In-canyon (S1, S2) may be reduced due to canyon asymmetry • Canyon-top (S5) equal to in-canyon (1-S4) • Recirculation (S3) equal to across-canyon (S2) 1 Upstream wind U 3 2 4 5
  • 24. road centreline vertical profile DMUG 2014 Example concentration profiles • Shallow symmetric canyon, perpendicular wind 1.5 m output height across-canyon 100 90 80 70 60 50 40 30 20 10 0 profile -10 0 10 20 30 40 50 Concentration (ug/m3) Distance from road centreline (m) Road Pavements 45 40 35 30 25 20 15 10 5 0 0 20 40 60 80 100 Z (m) Concentration (ug/m3) C1Q1 C2Q2 C3Q3 C4Q4 C5Q5 Total AC No Canyon Old Canyon+NB 1 2 3 4 5 U
  • 25. DMUG 2014 ADMS-Urban model set-up for London Input data • Standard ADMS-Urban modelling approach for London – Measured meteorological data from Heathrow airport – Measured upwind rural background concentrations – London Atmospheric Emissions Inventory (LAEI) emissions data – Modelling year 2012 – Modelling domain 10x15 km central London • Model configurations tested – No canyon: no street canyon modelling – Basic canyon: existing ADMS-Urban street canyon model – Advanced canyon & Urban Canopy: Urban Canopy flow field with new street canyon modelling
  • 26. DMUG 2014 ADMS-Urban model set-up for London Monitoring network • 29 monitors located within the ‘buildings data’ area • Monitor information (values, locations, heights) available from web • Data for NOx, NO2, PM10, PM2.5, O3 • 21 kerbside/roadside, 8 urban background – Some of the urban background sites are within canyons • Monitor heights generally less than or equal to 3 m Monitors 16 km
  • 27. DMUG 2014 Validation Results Tools used for analysis • MyAir Toolkit for Model Evaluation http://www.cerc.co.uk/environmental-software/myair-toolkit.html • openair http://www.openair-project.org/Downloads/Default.aspx Wind speed in m/s shown radially Polar plots Example shows observed NOx concentrations at a single receptor Hourly data binned according to wind speed and direction Colour indicates average concentration for each bin Observations at this site indicate high concentrations for a range of wind speeds and restricted wind directions Concentration bins with <8 entries shown in grey
  • 28. DMUG 2014 Validation Results Mean NO2 concentrations scatter plot • All sites shown • When canyons are modelled, means usually increase, giving a better estimate • Modelling canyons does not affect the lower concentration sites
  • 29. DMUG 2014 Validation Results NO2 concentration statistics • Data for all sites for whole year • Best statistics highlighted Data Mean NMSE R Fac2 Fb Observed 70.8 0.00 1.00 1.00 0.00 No Canyon 53.8 0.76 0.36 0.73 -0.27 Basic Canyon 61.5 0.53 0.49 0.79 -0.14 Advanced Canyon & Urban Canopy 63.1 0.39 0.62 0.81 -0.11
  • 30. DMUG 2014 Validation Results Polar plots: Full canyon • Consider a receptor ‘CD9’ within a standard canyon (H/g = 0.96, porosity = 0.26) • Wind from North West gives low concentrations and from the South East gives high concentrations due to presence of canyon • ‘No canyon’ and ‘Basic canyon’ runs predict similar concentrations in all directions Observations No canyon Basic canyon Advanced canyon & UC NO2 concentrations
  • 31. DMUG 2014 Validation Results Polar plots: Asymmetric canyon • Consider a receptor ‘HF4’ within an asymmetric canyon (H = 15 m) • Wind from West gives high concentrations and from the East gives lower concentrations due to presence of asymmetric canyon • ‘No canyon’ and ‘Basic canyon’ runs predict wind from East giving higher values Observations No canyon Basic canyon Advanced canyon & UC NO2 concentrations
  • 32. DMUG 2014 Conclusions • New methodologies for modelling an urban canopy flow field and advanced street canyon effects have been developed. • Modules based on these developments have been added to ADMS-Urban • Validation ongoing in London and Hong Kong in order to finalise the advanced canyon model • Combined with nesting within a regional model these developments allow for a multi-scale of modelling from regional down to street scale
  • 33. DMUG 2014 Acknowledgements The urban canopy and advanced street canyon modules have been developed in collaboration with researchers from the Hong Kong University of Science and Technology, supported by the Hong Kong Environmental Protection Department.