Transcript Slide 1

Progress on an urban surface energy balance
model comparison study
Sue Grimmond, Martin Best, Janet Barlow
King's College London, UK Met Office, University of Reading
With (people participating so far):
J-J Baik (Korea), M Best (UK), M Bruse (Germany), I Calmet (France), A Dandou (Greece),
K Fortuniak (Poland), R Hamdi (Belgium), M Kanda (Japan), H Kondo (Japan),
S Krayenhoff (Canada), S-B Limor (Israel), A Martilli (Spain), V Masson (France),
K Oleson (USA), A Porson (UK), U Sievers (Germany), H Thompson (UK)
Acknowledge:
 UK Met Office, Vasilis Pappas (KCL), Rob Mullen (KCL)
COST-728 Exeter meeting, 3-4 May 2007
Variety of Applications for Urban Energy Balance Models
 For example:
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Meso-scale modelling
Global climate modelling
Air quality
View factor determinations
Heat island studies
Upper boundary conditions for other models
Weather forecasting
Energy assessments
Emergency response
Meso-scale
 This Study
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Suite of different models
Range of complexity
Range of applications
Range of data needs
Range of computer needs
Common: all run offline
Urban
Vegetation
Water
Computational Requirements
Available models
Too expensive to run?
Globally more
applicable?
Parameters difficult to
get?
Number of Parameters
Past Model Evaluations
TEB
Vancouver: Masson et al. 2002
Mexico City: Masson et al. 2002
Marseille: Lemonsu et al. 2004
MOSES
Vancouver: Best et al. 2006
Mexico City: Best et al. 2006
Lodz: Offerle 2003
LUMPS
Lodz: Offerle 2003
CLMU
Vancouver: Oleson et al. 2007
Mexico City: Oleson et al. 2007
Distinct Features of Comparison
Models run offline
Following the
methodology
used by PILPS
Project for
Intercomparison of
Land-Surface
Parameterization
Schemes
Henderson-Sellers et al.
(1993)
Common Forcing Data Set
All fluxes evaluated
Canyon variables: Temperature, Wind speed
Increasing levels of information
provided
Forcing data
only
Easily
obtained
urban
morphology
Urban fabric
properties
Evaluation
data
(back
calculate
parameters)
Key Questions
What are the main physical processes
controlling the urban energy balance which
need to be resolved?
How complex does a model need to be in
order to produce a realistic simulation of
urban surface fluxes and temperatures?
Which input parameter information is
required by an urban model to perform
realistically?
Are we measuring the correct variables at
the correct scales for model evaluation?
Current Status
Determine level of interest and
identify participants
Inventory of models
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Collect details of all participating models
Set up project infrastructure
How to distribute data
Website / Email
www.kcl.ac.uk/ip/suegrimmond/model_comparison.htm
Staged distribution of data
Data formats
Sample forcing dataset preparation
Sent out to people
Waiting for data runs to come back
Obtain suitable observational datasets
• Comprehensive set of observations
• Ideally dataset unused previously for model testing
Immediate Next steps
Analysis for
suitability of
observational
dataset
• Ensure quality of observational datasets
• Ensure dataset fulfils requirements of
comparison
• Identify limitations of experiment from
observational dataset
Funding
• Waiting to hear from NERC
• Other alternatives
• Met Office has funded the initial stages
Multi-step model
runs
• Different levels of input data are released to
the modellers
• At each stage more information is released
about the morphology and physical
properties of the site
• enables determination of model parameters
with more accuracy
Multi-step model runs
 Simulation of the components of the surface energy
balance (net radiation, storage, sensible and latent heat fluxes) for
the location(s) of the evaluation dataset
 Four stages
 Different levels of input data are released to the modellers
 At each stage more information is released about the
morphology and physical properties of the site
 enables determination of model parameters with more
accuracy
 Staged approach to establish the required accuracy for each
model parameter by comparing the quality of the simulation
at each stage.
Multi-step model runs
Forcing data
only:
Add urban
morphology:
•Models run with no prior knowledge of the urban surface
•i.e. model default values for all parameters
•only the main forcing data supplied, e.g. winds, temperature,
solar radiation.
•Morphological information provided, e.g. building density, mean
building height, vegetation fraction.
•More easily obtained data sets
Add urban
fabric
properties:
•Urban building materials information would be given
•e.g. thermal properties, albedo
•information specific to each city/site not known in general on a
global basis.
•Reliance on these types of data makes a scheme difficult to use for
global applications
Add
evaluation
data:
•Evaluation dataset released
• optimisation of model parameters for best fit to observations
•Optimised parameters returned as well as the standard outputs.
•requested limit parameter values between observational limits
•encouraged to undertake analysis of their results if the optimal
solution required unrealistic parameter values.
Process-oriented statistical analysis
Statistical analysis of
the model
performance relative
to the observations
Analysis to assess
urban climatological
phenomena explicitly
Many of the models
also predict variables
beyond the SEB terms
•flux by flux
•hour by hour evaluation as well as central tendency of the
mean
•assessment will be done at a series of time-scales (hourly,
daily, monthly, annual etc.) to determine any biases within
the model performance.
•statistics will consist of a range of metrics
• mean, standard deviation, probability distribution function, linear
regression, root mean square error (systematic, unsystematic),
index of agreement, mean absolute error, mean bias error,
correlation coefficient, coefficient of determination, etc.
•e.g.
•positive sensible heat flux at night
•storage heat flux magnitude and timing
•latent heat flux - often neglected term
• e.g. air temperature, surface temperature
• Evaluate performance
Urban Energy Balance Models
participating so far
CODE
BEP02
BEP0X
CLMU
CTTC
ENVI
LUMPS
MCBM
Authors
Martilli
Martilli
Oleson et al
Limor & Hoffman
Bruse
Grimmond & Oke
Kondo, Hiroaki
Contact Person
Alberto Martilli
Heather Thompson
Keith Oleson
S-B Limor
Michael Bruse
Sue Grimmond
Hiroaki Kondo
Version used
older version
Linked to METRAS
v.1.0
Country
Spain
UK
USA
Israel
Germany
UK/USA
Japan
MM5u
Dandou & Tombrou
Aggeliki Dandou, Maria Tombrou
MM5V3-6-1
Greece
MOSES1T
MOSES2T
MUKLIMO
SM2U
SRUM
M. Best
M. Best
Siewers, Uwe
Dupont & Mestayer
Porson, Harman,
M. Best
M. Best
U. Sievers
Isabelle Calmet
A. Porson
One tile version
Two tile version
Thermodynamic
UK
UK
Germany
France
UK
SUMM
Kanda, T.Kawai, R
Moriwaki
Masson, Valery
Masson, Valery
Clark, Best, Belcher
Manabu Kanda, Toru
Kawai, Ryo Moriwaki
TEB
Valery Masson
TEB07
Rafiq Hamdi
Krayenhoff & Voogt
TUF2d
Scott Krayenhoff
Krayenhoff & Voogt
TUF3d
Scott Krayenhoff
Krayenhoff & Voogt
TUFopt
Scott Krayenhoff
TVM_BEP05 Martilli, Alberto
Rafiq Hamdi
ULEB
Fortuniak, Krzysztof K. Fortuniak
VUCM
Lee, S-H & Park, S-U Jong-Jin Baik
Green CTTC model
Under development
Coupled with 1D-vegetation
model
Japan
Single-layer
last version
2-d version
3-d version
Optimized 3-d ver
last version
France
Belgium
Canada
Canada
Canada
Belgium
Poland
Korea
Multiple versions
CODE
BEP02
BEP0X
CLMU
CTTC
ENVI
LUMPS
MCBM
Authors
Martilli
Martilli
Oleson et al
Limor & Hoffman
Bruse
Grimmond & Oke
Kondo, Hiroaki
Contact Person
Alberto Martilli
Heather Thompson
Keith Oleson
S-B Limor
Michael Bruse
Sue Grimmond
Hiroaki Kondo
Version used
older version
Linked to METRAS
v.1.0
Country
Spain
UK
USA
Israel
Germany
UK/USA
Japan
MM5u
Dandou & Tombrou
Aggeliki Dandou, Maria Tombrou
MM5V3-6-1
Greece
MOSES1T
MOSES2T
MUKLIMO
SM2U
SRUM
M. Best
M. Best
Siewers, Uwe
Dupont & Mestayer
Porson, Harman,
M. Best
M. Best
U. Sievers
Isabelle Calmet
A. Porson
One tile version
Two tile version
Thermodynamic
UK
UK
Germany
France
UK
SUMM
Kanda, T.Kawai, R
Moriwaki
Masson, Valery
Masson, Valery
Clark, Best, Belcher
Manabu Kanda, Toru
Kawai, Ryo Moriwaki
TEB
Valery Masson
TEB07
Rafiq Hamdi
Krayenhoff & Voogt
TUF2d
Scott Krayenhoff
Krayenhoff & Voogt
TUF3d
Scott Krayenhoff
Krayenhoff & Voogt
TUFopt
Scott Krayenhoff
TVM_BEP05 Martilli, Alberto
Rafiq Hamdi
ULEB
Fortuniak, Krzysztof K. Fortuniak
VUCM
Lee, S-H & Park, S-U Jong-Jin Baik
Green CTTC model
Under development
Coupled with 1D-vegetation
model
Japan
Single-layer
last version
2-d version
3-d version
Optimized 3-d ver
last version
France
Belgium
Canada
Canada
Canada
Belgium
Poland
Korea
Methods used to model outgoing
shortwave radiation
CODE
# reflections
MUKLIMO
TEB
TEB07
BEP02
SRUM
CLMU
TVM_BEP05
infinite
infinite
multiple
multiple
multiple
multiple
BEP0X
TUF3d
TUF2d
TUFopt
VUCM
MCBM
MOSES2T
MOSES1T
SM2U
MM5u
ENVI
CTTC
ULEB
multiple
multiple (min 2)
multiple (min 2)
multiple (min 2)
three
two
one
one
one
one
one
one
one
albedo
canyon, roof
canyon, roof
canyon
bulk/effective
by facet
canyon
patches /facet
patches /facet
patches /facet
by facet
canyon, roof
bulk
bulk/effective
bulk/town
by facet
by facet
bulk/town
CODE
Methods
used to heat
determine
Anthropogenic Heat Flux
Anthropogenic
flux Methods
BEP0X
MUKLIMO
heat fluxes from the interior of the buildings
TEB
domestic heating computed
TEB07
domestic heating computed
BEP02
Partially accounted for by imposing a fixed temp at the building interior
BEP05
Partially accounted for by imposing a fixed temp at the building interior
TUF3d
Prescribed bulk value
TUF2d
Prescribed bulk value
TUFopt
Prescribed bulk value
VUCM
Prescribed bulk value
SM2U
Prescribed
CTTC
Prescribed per vehicle (for vehicles only)
CLMU
prescribed traffic fluxes, parameterized waste heat fluxes from heating/ air conditioning
MOSES2T
not modelled itself but possible to be included for calculation of turbulent fluxes
MOSES1T
not modelled itself but possible to be included for calculation of turbulent fluxes
SRUM
not modelled itself but possible to be included for calculation of turbulent fluxes
ULEB
not modelled itself but possible to be included for calculation of turbulent fluxes
MM5u
calculated (offline) as a temporal & spatial function of the anthropogenic emissions
ENVI
from heat transfer ew through walls, no storage term
MCBM
Modelled by Kikegawa et al. offline
CODE
Methods to calculate turbulent sensible heat flux
CTTC
TEB07
calculated by the model
From each surface
BEP02
From each surface
BEP05
From each surface
SRUM
Resistance network based on Harman et al. (2004)
CLMU
BEP0X
TUF3d
TUF2d
TUFopt
SM2U
TEB
resistances between canyon surfaces and canyon air based on Rowley (1930),
between canyon air and atmosphere depend on stability as in CLM3
Resistances based on Clarke (1985)
Resistances based on flat-plate heat transfer coeffs (vertical patches) and based on
MO similarity (horiz. patches)
Resistance (Guilloteau, 1998 + Zilitinkevich, 1995)
Resistance
MOSES2T
Standard resistance
MOSES1T
Standard resistance
ENVI
from turbulence model (wall function) and surface energy balance
MM5u
Parametric formulation
VUCM
Parametric formulation
MCBM
MUKLIMO
MO or Jurges
ULEB
M-O similarity: Louis (1979) modified by Mascart at al. (1995)
MO-laws
CODE
Methods used to calculate Heat Storage Flux
CTTC
calculated by the model
BEP02
BEP0X
TEB
Diffusion
TEB07
diffusion
CLMU
Diffusion
BEP05
Diffusion
TUF3d
Diffusion
TUF2d
Diffusion
TUFopt
Diffusion
MOSES2T
Diffusion
MOSES1T
Diffusion
VUCM
Diffusion
SM2U
Difference + Diffusion + Force restore
MM5u
OHM scheme (Grimmond et al., 1991)
ENVI
soil: 1D model, fully resolved, walls/building system: no storage term
ULEB
As QG in urban slab (solution of multi layer thermal diffusion equation)
MCBM
Finite difference
MUKLIMO
Walls and roofs have a heat capacity
What is resolved in the model?
CODE
Resolved:
CANYONS
Resolved:
Roof
Resolved:
walls
Walls with
orientation
Walls
sunlit/
shaded
Road
sunlit/
shaded
Turbulence
within
canyon
resolved
BEP02
Yes
Yes
Yes
Yes
Yes
No
Yes
BEP05
Yes
Yes
Yes
Yes
Yes
No
Yes
BEP0X
No
No
No
No
No
No
No
CLMU
No
Yes
Yes
No
Yes
No
No
CTTC
Yes
Yes
Yes
No
No
No
Yes
ENVI
No
Yes
Yes
No
No
No
Yes
MCBM
No
Yes
Yes
No
Yes
Yes
Yes
MM5u
No
No
No
No
No
No
No
MOSES1T
No
No
No
No
No
No
No
MOSES2T
Yes
Yes
No
No
No
No
No
MUKLIMO
No
No
No
No
No
No
Yes
SM2U
No
No
No
No
No
No
No
SRUM
Yes
Yes
No
No
No
No
No
TEB
No
Yes
Yes
No
No
No
No
TEB07
No
No
No
No
No
No
No
TUF
Yes
Yes
Yes
Yes
Yes
Yes
No
ULEB
No
No
No
No
No
No
No
VUCM
Yes
Yes
Yes
No
Yes
Yes
No
Final Comments
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Models that are already participating show a wide range of approaches
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Need to follow up on some details
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Multiple versions of some individual models are participating
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Initial trial dataset now available
 Data back from three groups
 This is allowing us to iron out issues at both ends

People can still participate
 Encouraged to do so! Contact me: [email protected]
 Participants will be co-authors in manuscripts etc

Waiting to hear if NERC will fund the next parts of this project
Within Canyon
processes
modelled
Canyons are
resolved
Above canyon
modelled
Canyon top
modelled
CODE
Type of Model
BEP02
Multiple layer
No
No
No
No
BEP05
Multiple layer
No
No
No
No
BEP0X
Multiple layer
No
No
No
No
CLMU
Single layer
Yes
No
Yes
Yes
CTTC
Single layer
No
No
No
No
Yes
Yes
Yes
Yes
ENVI
MCBM
Multiple layer
No
No
No
No
MM5u
Single layer
No
No
No
No
MOSES1T
Single Layer
No
No
No
No
MOSES2T
Single Layer
No
No
No
No
Yes
Yes
No
No
MUKLIMO
SM2U
Single Layer
No
No
No
No
SRUM
Single Layer
No
No
No
No
TEB
No
No
No
No
TEB07
No
No
No
No
TUF
No
Yes
No
No
BEP05
No
No
No
No
ULEB
Multiple layer
No
No
No
No
VUCM
Single layer
Yes
No
Yes
Yes