Song-You Hong (shong@yonsei.ac.kr),
- Department of Atmospheric Sciences, College of Science, Yonsei University, Room 544, Seoul 120-749, Korea.
Jiwoo Lee (jiwoolee@yonsei.ac.kr),
- Department of Atmospheric Sciences, College of Science, Yonsei University, Room 532, Seoul 120-749, Korea.
1. Overall
We perform dynamical downscaling by utilizing a regional
climate model (RCM), namely the Regional Spectral Model (RSM),
which is also known as Regional Model Program (RMP) of the
Global/Regional Integrated Model System (GRIMs; Hong et al.,
2012). The dynamic frame of RMP is rooted in the National Center
for Environmental Prediction (NCEP) RSM (Juang and Kanamitsu,
1994; Juang et al., 1997), and most of physical parameterizations
are newly developed and adapted to the RMP. More detailed
information about the GRIMs-RMP is provided by Hong et al. (2012),
and evaluation and analyses of this dataset are provided by Lee et
al. (2012).
2. Domain and Resolution
The model domain includes East Asia, India, the Western
Pacific Ocean, and the northern part of Australia, as shown in
Fig. 1 and Table 1. This configuration of the model domain follows
a protocol of the Coordinated Regional climate Downscaling
Experiment (CORDEX) for Asia (Giorgi et al., 2009). The number of
grid points in Cartesian coordinates is 241 (west-east) by 198
(north-south), with a nominal horizontal resolution of 50 km. A
28-level terrain-following (sigma) vertical grid is used.
3. Dynamics
The dynamic frame of RMP is rooted in the NCEP regional
spectral model (RSM, Juang and Kanamitsu, 1994; Juang et al.,
1997). The RMP is a perturbation model, and the spectral
truncation to the perturbation tendency over the regional domain
provides a wave selection that avoids waves longer than the
regional domain. Thus, the large-scale wave longer than the
regional domain from the coarse-grid or global model cannot be
disturbed, during the entire period of integration (see Juang and
Hong, 2001). Together with this unique dynamic feature of this
model, the adaptation of the scale-selective bias correction
method (SSBC, Kamamaru and Kanamitsu, 2007) with subsequent
improvements (Kanamitsu et al., 2010; Hong and Chang, 2012)
provides major advantages in long-term integration without
significant synoptic-scale drift.
4. Physics
The physics package of the RMP in this study is version 3.0,
which employs the Simplified Arakawa?Schubert (SAS) convection
scheme (Hong and Pan, 1998) for convective parameterization, a
diagnostic microphysics scheme (Hong et al., 1998), the Yonsei
University planetary boundary layer (YSUPBL) scheme (Hong et al.,
2006), the National Centers for Environmental Prediction
(NCEP)?Oregon State University?US Air Force?National Weather
Service Office of Hydrologic Development (NOAH) land surface model
(Chen and Dudhia, 2001), and the shortwave (Chou, 1992) and
long?wave (Chou et al., 1999) radiation parameterizations.
5. Experimental Setup
The RMP experiments are conducted for 71 years; 26-year
simulation for the current (1980-2005, hereafter: CUR) climate and
two types of 45-year simulations for the future (2006-2050)
climate. The current climate simulation, or CUR experiment, is
driven from the historical run of the the Atmosphere-Ocean coupled
Hadley Center Global Environmental Model version 2 (HadGEM2-AO)
simulation of the National Institute of Meteorological Research
(NIMR) (Baek et al., 2012). For the future climate simulations,
two different boundary conditions are downscaled using the RMP
(hereafter: R45 and R85). They are driven by the HadGEM2-AO
following the Representative Concentration Pathways (RCP) 4.5 and
8.5 scenarios of the Intergovernmental Panel on Climate Change
(IPCC) Fifth Assessment Report (AR5; Moss et al., 2010),
respectively. The RCP 4.5 scenario is a stabilization scenario in
which total radiative forcing is stabilized before 2100 through
the employment of a range of technologies and strategies for
reducing greenhouse gas emissions (Thomson et al., 2011). The RCP
8.5 scenario is characterized by increasing greenhouse gas
emissions over time and is representative of scenarios in the
literature which result in high greenhouse gas concentration
levels (Riahi et al., 2011). The R45 and R85 experiments are
continuously simulated after the CUR experiment, thus the model
does not need to be spun-up multiple times.
6. References
Baek, H. J., and Coauthors, 2012 :
Climate change in the 21st Century simulated by HadGEM2-AO under representative concentration pathways. Asia-Pacific J. Atmos.
Sci. (to be submitted).
Chen, F. and J. Dudhia, 2001 :
Coupling and advanced land surface-hydrology model with the Penn State-NCAR MM5 modeling system. Part I: Model
implementation and sensitivity. Mon. Wea. Rev., 129, 569-585.
Chou, M.D., 1992 :
A solar radiation model for use in climate studies, J. Atmos. Sci., 49, 762?772.
Chou, M.D., K.?T. Lee, S.?C. Tsay, and Q. Fu, 1999 :
Parameterization for cloud longwave scattering for use in atmospheric models. J. Climate, 12, 159?169.
Giorgi, F., C. Jones, and G. R. Asrar,2009 :Addressing climate information needs at the regional
level: The CORDEX framework. World Meteorological Organization (WMO) Bulletin, 58, 175-183.
Hong, S.-Y. and H.-L. Pan, 1998 :
Convective Trigger Function for a Mass-Flux Cumulus Parameterization Scheme. Mon. Wea. Rev., 126, 2599?2620.
Hong, S.-Y., and E.-C., Chang, 2012 :
Spectral Nudging Sensitivity Experiments in a Regional Climate Model. Asia-Pacific J. Atmos. Sci. (accepted).
Hong, S.-Y., H.-M. H. Juang, and Q. Zhao, 1998 :
Implementation of Prognostic Cloud Scheme for a Regional Spectral Model. Mon. Wea. Rev., 126, 2621?2639.
Hong, S.-Y., Y. Noh, and J. Dudhia, 2006 :
A new vertical diffusion package with an explicit treatment of entrainment processes. Mon. Wea. Rev., 134, 2318-2341, doi:10.1175/MWR3199.1.
Hong, S.-Y., and Coauthors, 2012 :
A Multi-Scale Atmospheric/Oceanic Modeling System: The Global/Regional Integrated Model system (GRIMs). Asia-Pacific J. Atmos. Sci. (in review).
Juang, H.-M. H., and M. Kanamitsu, 1994 :
The NMC Nested Regional Spectral Model. Mon. Wea. Rev., 122, 3-26.
Juang, H.-M. H., and S.-Y. Hong, 2001 :
Sensitivity of the NCEP Regional Spectral Model to Domain Size and Nesting Strategy. Mon. Wea. Rev., 129, 2904-2922.
Juang, H.-M. H., S.-Y. Hong, and M. Kanamitsu, 1997 :
The NCEP Regional Spectral Model: An Update. Bull. Amer. Meteor. Soc., 78, 2125-2143.
Kanamaru, H., and M. Kanamitsu, 2007 :
Scale-Selective Bias Correction in a Downscaling of Global Analysis Using a Regional Model. Mon. Wea. Rev., 135, 334-350.
Kanamitsu, M., K. Yoshimura, Y.-B. Yhang, and S.-Y. Hong, 2010 :
Errors of Interannual Variability and Trend in Dynamical Downscaling of Reanalysis. J. Geophys. Res., 115, D17115.
Lee, J.-W., S.-Y., Hong, E.-C. Chang, M.-S. Suh, H.-S. Kang, 2012 :
Dynamically Downscaled Future Climate Change over East Asia. Climatic Change (to be submitted).
Moss, R. H., and Coauthors, 2010 :
The next generation of scenarios for climate change research and assessment. Nature, 463, 747-756.
Riahi K., S. Rao, V. Krey, C. Cho, V. Chirkov, G. Fischer, G. Kindermann, N. Nakicenovic, and P. Rafaj, 2011 :
RCP 8.5?A scenario of comparatively high greenhouse gas emissions. Climatic Change, 109, 33-57, doi:10.1007/s10584-011-0149-y.
Thomson, A., and Coauthors, 2011 :
RCP4.5: a pathway for stabilization of radiative forcing by 2100. Climatic Change, 109, 77-94. doi: 10.1007/s10584-011-0151-4.
Model domain and orography (m).
Pattern correlation (PC) and root-mean-square error (RMSE) scores of the precipitation (mm d−1) and 2-m temperature (°C) simulated from the HG2 and RMP against the CRU observation for 1980-2005.
CORDEX Domain
Map Projection
Lambert Conformal
True latitude
55N, 15N
Domain center
118.96E, 22.04N
Horizontal resolution
50 km
Horizontal grid points
241 × 198
Δt
240s (180s for DJF)
Contact information
Myoung-Seok Suh (sms416@kongju.ac.kr),
- Department of Atmospheric Sciences, Kongju National University, 182 Shinkwan-dong, Gongju-city 314-701,ChungCheongnam-do, South Korea.
Seok-Geun Oh (poet1535@kongju.ac.kr),
- Department of Atmospheric Sciences, Kongju National University, 182 Shinkwan-dong, Gongju-city 314-701,ChungCheongnam-do, South Korea.
1. Overall
The Regional Climate Model version 4 (RegCM4) used in this
study, developed by the International Centre for Theoretical
Physics (ICTP), is the latest version with some noteworthy
improvements, such as the coupling of a sophisticated land surface
model, community land model 3
(http://www.ictp.it/research/esp/models/regcm4.aspx). Compared to
RegCM3, RegCM4 includes new land surface, planetary boundary
layer, and air-sea flux schemes, a mixed convection and tropical
band configuration, modifications to the pre-existing radiative
transfer and boundary layer schemes, and a full upgrade of the
model code aimed towards improved flexibility, portability, and
user friendliness. A detailed description of RegCM4 is given by
Giorgi et al. (2012).
2. Domain and Resolution
The model domain (Fig. 1), set based on the CORDEX-East Asia
domain, covers most of Asia, the western Pacific, the Bay of
Bengal, and the South China Sea. The number of grid points in
Lambert Conformal map projection is 243 (west-east) by 197
(north-south), with a horizontal resolution of 50 km. A 18-sigma
(74 hPa) vertical grid is used. A summary of simulation domain
including the central latitude/longitude information and true
latitudes is shown in Table 1.
3. Dynamics
The basic model dynamics have remained the same as in
RegCM3, which was essentially the same as that of the previous
version RegCM2 (Giorgi et al. 1993a, b). RegCM4 is thus a
hydrostatic, compressible, sigma-p vertical coordinate model run
on an Arakawa B-grid in which wind and thermodynamical variables
are horizontally staggered. A time-splitting explicit integration
scheme is used in which the 2 fastest gravity modes are first
separated from the model solution and then integrated with smaller
time steps. This allows the use of a longer time step for the rest
of the model. Essentially, the model dynamics are the same as that
of the hydrostatic version of MM5 (Grell et al. 1994).
4. Physics
In this study, the MIT-Emanuel (1991) cumulus
parameterization scheme, which showed relatively better simulation
in South Korea, is selected based on the one-year sensitivity
experiment by Oh et al. (2011). The Holtslag et al. (1990) scheme
and NCAR CCM3 (Kiehl et al., 1996) radiation scheme are used for
the planetary boundary layer, and the NCAR CLM3.5 is used for the
land surface model (Olseson et al., 2008). To minimize the
systematic errors that occur in long-term simulations over large
domains, spectral nudging is applied to RegCM4 (Von Storch et al.,
2000). The other physics used the default of RegCM4
5. Experimental Setup
In this study, two types of simulations using RegCM4 were
performed. One is a current climate simulation for the evaluation
of simulation skill of RegCM4 with a general circulation model
output. The other is future climate simulation for the projection
of future climate under the two emission scenarios, representative
concentration pathways (RCP) 4.5 and 8.5. The simulation periods
for the current and future climate simulations are 27-year (from
1979 to 2005) and 45-year (from 2006 to 2050), respectively. And
the model output of HadGEM2-AO produced by the National Institute
of Meteorological Research (NIMR)/Korea Meteorological
Administration (KMA) under two IPCC (Intergovernmental Panel on
Climate Change) RCP4.5/8.5 scenarios were used as an initial and
boundary conditions. RCP scenarios are the latest emission
scenarios recommended to use for the Fifth Assessment Report (AR5)
of IPCC. To participate in CMIP5 (phase five of the Coupled Model
Intercomparison Project) with new global climate change scenarios
based on RCP, the NIMR/ KMA simulated the several experiments such
as preindustrial control run, historical run, and RCP scenarios
(2.6, 4.5, 6.0, 8.5) run for long term projection recommended by
CMIP5 using the coupled global atmosphere-ocean model, HadGEM2-AO.
Details of HadGEM2-AO are given by Collins et al. (2011), and the
results of the HadGEM2-AO CMIP5 experiment by NIMR/KMA are shown
in Baek et al. (2012).
6. References
Baek, H.-J., and co-authors, 2012 :
Climate change in the 21st 12 Century simulated by HadGEM2-AO under representative concentration pathways, submitted to APJAS.
Collins, W. J., Coauthors, 2011 :
Development and evaluation of an Earth-system model – HadGEM2, Geosci. Model Dev. Discuss., 4, 997–1062, doi:10.5194/gmdd-4-997-2011.
Emanuel, K. A., 1991 :
A scheme for representing cumulus convection in large-scale models. J. Climate, 48, 2313-2335.
Giorgi, F., MR. Marinucci, and G. Bates, 1993a :
Development of a second generation regional climate model (RegCM2). I. Boundary layer and radiative transfer processes. Mon. Wea. Rev. 121, 2794-2813.
Giorgi, F., MR. Marinucci, G. Bates, and G. DeCanio, 1993b :
Development of a second generation regional climate model (RegCM2). II. Convective processes and assimilation of lateral boundary conditions. Mon. Wea. Rev. 121, 2814-2832.
Giorgi, F., E. Coppola, F. Solmon, L. mariotti, and others, 2012 :
RegCM4: model description and preliminary test over multi CORDEX domain, Clim. Res., 52, 7-29.
Grell, G. J. Dudhia, and DR. Stauffer, 1994 :
A description of the fifth generation Penn State/NCAR Mesoscale Model (MM5). National Center for Atmospheric Research Tech Note NCAR/TN-298 + STR, NCAR, Boulder, CO.
Oh, S. G., M. S. Suh, J. S. Myoung, and D. H. Cha, 2011 :
Impact of boundary conditions and cumulus parameterization schemes on regional climate simulation over South-Korea in the CORDEX-East Asia domain using the RegCM4 model. J. Korean Ear. Sci. Soc., 32, 373-387.
Oh, S. G., M. S. Suh, D. H. Cha, and S. J. Choi, 2011 :
Simulation skills of RegCM4 for regional climate over CORDEX East Asia driven by HadGEM2-AO. Jour. Korean Earth Sci. Soc., 32(7),732-749.
Holtslag, A. A. M., E. I. F. De Bruijin, and H. L. Pan, 1990 :
A high resolution air mass transformation model for short-range weather forecasting. Mon. Wea. Rev., 118, 1561- 1575.
Kiehl, J. T., J. J. Hack, G. B. Bonan, B. A. Boville, B. P. Briegleb, D. L. Williamson, and P. J. Rasch, 1996 :
Description of NCAR Community Climate Model(CCM3). NCAR Tech. Note NCAR/TN-420+STR, 152 pp.
Oleson, K. W., G. Y. Niu, Z. L. Yang, D. M. Lawrence, P. E. Thornton, P. J. Lawrence, R. Stöckli, R. E. Dickinson, G. B. Bonan, S. Levis, A. Dai, and T. Qian, 2008 :
Improvements to the community land model and their impact on the hydrological cycle. J. Geophys. Res., 113, G01021, doi:10.1029/2007JG000563.
Von Storch, H., H. Langerberg, and F. Feser, 2000:
A spectral nudging technique for dynamical downscaling purposes. Mon. Wea. Rev., 128, 3664-3673, doi: 1175/1520- 0493.
Model domain and topography (m) for the 50km gird spacing.
Model configuration used in this study.
Contents
Description
Domain
CORDEX framework - 50-km horizontal resolution
- Central Lat. and Lon. : 22.04°N, 118.96°E - 197 (Lat.)
× 243 (Lon.)
Dong-kyu Lee (dklee@snu.ac.kr),
- Department of Earth and Enviromental Sciences, Seoul National University, 1 Gwanak-ro, Gwanak-gu, Seoul 151-742, South Korea.
1. Overall
SNU-MM5(Seoul National University Meso-scale Model version
5)(Lee et al. 2004) is based on version 5 of the Penn State
University/National Center for Atmospheric Research Meso-scale
Model (MM5) (Grell 1994) and the community land model version 3
(CLM3) is an advanced and comprehensive land surface model. The
spectral nudging technique (von Storch et al. 2000) was performed
an alternative to the modified relaxation method (Liang et al.
2001) reducing systematic bias. Planetary boundary layer scheme of
the Yonsei University (YSU) was added to the SNU-MM5 for better
simulation of precipitation over the ocean (Cha et al.
2008).SNU-MM5 and SNURCM(Seoul National University Regional
Climate Model) are the same model.
2. Domain and Resolution
The model domain(Fig. 1) follows a protocol of the
Coordinated Regional climate Downscaling Experiment (CORDEX) for
Asia, includes north-south direction from Australia in the north
to Russia and east-west direction from west of the Tibetan Plateau
to western Pacific. The number of grid points is 233 (west-east)
by 197 (north-south) horizontal grids centering at 22.04°N and
118.96°E with a nominal horizontal resolution of 50 km. A 24-level
terrain-following (sigma) vertical grid frome the surface to the
model top of 70 hPa is used.
3. Dynamics
SNU-MM5 dynamics is based on the MM5. The MM5 uses a
nonhydrostaric primitive equation system with a terrain-following
sigma vertical coordinate, which is a well-studied mesoscale model
that has been applied widely in atmospheric study. A spectral
nudging technique of Von Storch et al. (2000) was implemented for
lateral boundary handling. The technique is applied to the entire
model domain, while the relaxation method is applied only to the
lateral buffer zone.
4. Physics
The physical parameterization schemes used in this study are
the Kain-Fritsch cumulus convective parameterization scheme (Kain
and Fritsch 1990), the Reisner Ⅱ explicit moisture scheme (Reisner
et al. 1998), the CCM2 radiative transfer scheme (Briegleb 1992),
the CLM3 land surface model (Bonan et al. 2002), and the YSU
planetary boundary layer scheme (Hong et al. 2006). (table 1)
5. Experimental Setup
This experiments produced the present 26-yesrs regional
climate (1980-2005) and assessed the systematic bias caused by
HadGEM2-AO. Also 45-years future climate simulations (2006-2049)
were produced using SNU-MM5 with the HadGEM2-AO following the
lateral boundary forcing of two AR5 representative concentration
pathways (RCP) 4.5 and 8.5 scenarios. This scenarios are the
latest emission scenarios recommended to use for the Fifth
Assessment Report (AR5) of IPCC. To participate in the phase five
of the Coupled Model Intercomparison Project (CMIP5) with new
global climate change scenarios based on RCP, the NIMR/ KMA
simulated the several experiments such as preindustrial control
run, historical run, and RCP scenarios (2.6, 4.5, 6.0, 8.5) run
for long term projection recommended by CMIP5 using the coupled
HadGEM2-AO.
Model domain
SNU-MM5 configurations for the present
climate simulation using the HadGEM2-AO data.
Contents
Description
SNU-MM5
Vertical layers (top)
24 sigma (70 hPa)
Cumulus parameterization scheme(CPS)
Kain-Fritch
Explicit moisture scheme(EMS)
Reisner2
Radiation
CCM2 package
Planetary boundary layer (PBL)
YSU
Land surface model(LSM)
NCAR CLM3
Spectral nudging
Yes
Contact information
Dong-kyu Lee (dklee@snu.ac.kr),
- Department of Earth and Enviromental Sciences, Seoul National University, 1 Gwanak-ro, Gwanak-gu, Seoul 151-742, South Korea.
1. Overall
The Weather Research and Forecasting (WRF) Model is a
mesoscale numerical weather prediction system designed to serve
both operational forecasting and atmospheric research needs. It
features multiple dynamical cores a 3-dimensional variational
(3DVAR) data assimilation system, a software architecture allowing
for computational parallelism and system
extensibility(www.wrf-model.org). In this study, we utilized
WRF3.2 by applying the spectral nudging technique (von Storch et
al. 2000) suitable for long-term climate simulations(Choi 2010).
2. Domain and Resolution
The model domain(Fig. 1) follows a protocol of the
Coordinated Regional climate Downscaling Experiment (CORDEX) for
Asia, includes north-south direction from Australia in the north
to Russia and east-west direction from west of the Tibetan Plateau
to western Pacific. The number of grid points is 233 (west-east)
by 197 (north-south) horizontal grids centering at 22.04°N and
118.96°E with a nominal horizontal resolution of 50 km. A 27-level
terrain-following (sigma) vertical grid from the surface to the
model top of 70 hPa is used.
3. Dynamics
The Advanced Research WRF (ARW) and Nonhydrostatic Mesoscale
Model (NMM) are dynamical cores which include mostly advection
pressure-gradients, coriolis, buoyancy, filters, diffusion and
time-stepping. Both are nonhydrostatic Eulerian dynamical cores
with terrain-following pressuer-based vertical coordinates. ARW
dynamical core designed for research as well as NWP. NMM dynamical
core used in NCEP operational regional models.
4. Physics
The physical parameterization schemes used in this study are
the Kain-Fritsch cumulus convective parameterization scheme (Kain
and Fritsch 1990), the Reisner Ⅱ explicit moisture scheme (Reisner
et al. 1998), the Unified Noah land surface model and the YSU
planetary boundary layer scheme (Hong et al. 2006). Longwave
radiative transfer scheme is RRTM and shortwave radiative transfer
scheme is Dudhia.
5. Experimental Setup
This experiments produced the present 26-yesrs regional
climate (1980-2005) and assessed the systematic bias caused by
HadGEM2-AO. Also 45-years future climate simulations (2006-2049)
were produced using SNU-MM5 with the HadGEM2-AO following the
lateral boundary forcing of two AR5 representative concentration
pathways (RCP) 4.5 and 8.5 scenarios. This scenarios are the
latest emission scenarios recommended to use for the Fifth
Assessment Report (AR5) of IPCC. To participate in the phase five
of the Coupled Model Intercomparison Project (CMIP5) with new
global climate change scenarios based on RCP, the NIMR/ KMA
simulated the several experiments such as preindustrial control
run, historical run, and RCP scenarios (2.6, 4.5, 6.0, 8.5) run
for long term projection recommended by CMIP5 using the coupled
HadGEM2-AO.
Model domain
SNU-WRF configurations for the present
climate simulation.
Hyun-Suk Kang (hyunskang@korea.kr; hyunsuk306.kang@gmail.com),
- Climate Research Laboratory, National Institute of Meteorological Research, 33 Seohobuk-ro, Seogwipo-si, Jeju-do, Korea.
Yu-Kyung Hyun (ykhyun@korea.kr),
- Climate Research Laboratory, National Institute of Meteorological Research, 33 Seohobuk-ro, Seogwipo-si, Jeju-do, Korea.
1. Overall
National Institute of Meteorological Research (NIMR) is
participating in the CORDEX with a regional climate model,
HadGEM3-RA which is based on the global atmospheric HadGEM3 of the
Met Office Hadley Centre (MOHC). Configuration of HadGEM3-RA is
almost same as the HadGEM3-A (See sections 3 and 4), except that
the dynamic settings are taken from the operational limited area
model. Detailed descriptions for dynamics core and physical
packages are described in Davies et al. (2005) and Martin et al.
(2006).
2. Domain and Resolution
The configuration of the model domain follows a protocol of
the Coordinated Regional climate Downscaling Experiment (CORDEX)
for Asia (Giorgi et al., 2009). The model domain includes East
Asia, India, the Western Pacific Ocean, and the northern part of
Australia, as shown in Fig. 1. The number of grid points is 220
(west-east) by 183 (north-south), with a horizontal resolution
0.44 degree (approximately 50km). The buffer zone for lateral
boundary conditions is 8 grids at each direction, where is located
between outer solid line and blue dotted line in Fig. 1. For
high-resolution experiments, the number of grid points is 184
(west-east) by 164 (north-south) without 8-grids lateral boundary
zone and the horizontal resolution is selected to 0.11°, about
12.5 km (red dotted line in Fig. 1).
3. Dynamics
The dynamic core of HadGEM3-RA is a nonhydrostatic, fully
compressible, deep atmosphere formulation using a
terrain-following, height-based vertical coordinate. It includes
semi-Lagrangian advection of all prognostic variables except
density, permitting relatively long time steps to be used at high
resolution. The model uses the Arakawa-C grid in which the zonal
and meridional wind components are staggered as well as the
momentum and thermodynamic variables. HadGEM3-RA runs on a
Charney-Phillips vertical grid in which the momentum and
thermodynamic variables are staggered (Davies et al., 2005; Martin
et al., 2006).
4. Physics
Model physics are summarized in Table 1. Detailed
descriptions for dynamics core and physical packages are described
in Davies et al. (2005) and Martin et al. (2006).
5. Experimental Setup
The experiments are conducted for 151 years; 56-year simulation
for the current (1950-2005) climate and two types of 95-year
simulations for the future (2006-2100) climate. The current
climate simulation is driven from the historical run of the
Atmosphere-Ocean coupled Hadley Center Global Environmental Model
version 2 (HadGEM2-AO) simulation of the National Institute of
Meteorological Research (NIMR) (Baek et al., 2012).
For the future climate simulations, two different boundary
conditions from the Representative Concentration Pathways (RCP)
4.5 and 8.5 scenarios of HadGEM2-AO. The RCP 4.5 scenario is a
stabilization scenario in which total radiative forcing is
stabilized before 2100 through the employment of a range of
technologies and strategies for reducing greenhouse gas emissions
(Thomson et al., 2011). The RCP 8.5 scenario is characterized by
increasing greenhouse gas emissions over time and is
representative of scenarios in the literature which result in high
greenhouse gas concentration levels (Riahi et al., 2011).
6. References
Baek, H. J., and Coauthors, 2012 :
Climate change in the 21st Century simulated by HadGEM2-AO under representative concentration pathways. Asia-Pacific J. Atmos. Sci. (to be submitted).
Davies, T., M. J. P. Cullen, A. J. Malcolm, M. H. Mawson, A. Staniforth, A. A. White, and N. Wood, 2005 :
A new dynamical core for the Met Office’s global and regional modeling of the atmosphere. Quart. J. Roy. Meteor. Soc., 131,1759- 1782.
Giorgi, F., C. Jones, and G. R. Asrar, 2009 :
Addressing climate information needs at the regional level: The CORDEX framework. World Meteorological Organization (WMO) Bulletin, 58, 175-183.
Martin, G. M., M. A. Ringer, V. D. Pope, A. Jones, C. Dearden, and T. J. Hinton, 2006 :
The physical properties of the atmosphere in the new Hadley Centre Global Environmental Model (HadGEM1). Part I: Model description and global climatology. J. Clim 19, 1274-1302.
Riahi K., S. Rao, V. Krey, C. Cho, V. Chirkov, G. Fischer, G. Kindermann, N. Nakicenovic, and P. Rafaj, 2011 :
RCP 8.5—A scenario of comparatively high greenhouse gas emissions. Climatic Change, 109, 33-57, doi:10.1007/s10584-011-0149- y.
Thomson, A., and Coauthors, 2011 :
RCP4.5: a pathway for stabilization of radiative forcing by 2100. Climatic Change, 109, 77-94. doi: 10.1007/s10584-011-0151-4.
Model domain and orography (m).
Summary of configuration of the HadGEM3-RA
Description
Radiation
General 2-stream radiation (Edwards and Slingo 1996;
Cusack et al. 1999a)
Boundary layer
Nonlocal mixing scheme for unstable layers (Lock et al.
2000). Local Richardson number scheme for stable layers (Smith
1990)
Microphysics
Mixed phase scheme including prognostic ice content;
solves physical equations for microphysical processes using
particle size information (Wilson and Ballard 1999)
Convection
Revised mass flux scheme from Gregory and Rowntree
(1990) including triggering of deep and shallow cumulus
convection based on the boundary layer scheme, parameterized
entrainment/detrainment rates for shallow convection (Grant and
Brown 1999), and the treatment of momentum transports by deep
and shallow convection based on an eddy viscosity model.
Gravity wave drag
Orographic scheme including flow blocking (Webster et
al. 2003)
Land surface
MOSES-II (Essery et al. 2003); nine surface tile types
plus coastal tiling
Clouds
Smith (1990) scheme using parameterized RH-crit (Cusack
et al. 1999b)