The offline Lagrangian particle model FLEXPART-NorESM/CAM (v1): model description and comparisons with the online NorESM transport scheme and with the reference FLEXPART model

被引:17
作者
Cassiani, Massimo [1 ]
Stohl, Andreas [1 ]
Olivie, Dirk [2 ]
Seland, Oyvind [2 ]
Bethke, Ingo [3 ]
Pisso, Ignacio [1 ]
Iversen, Trond [2 ]
机构
[1] NILU Norwegian Inst Air Res, POB 100, N-2027 Kjeller, Norway
[2] Norwegian Meteorol Inst, POB 43, N-0313 Oslo, Norway
[3] Bjerknes Ctr Climate Res, Uni Res Climate, POB 7810, N-5020 Bergen, Norway
关键词
AEROSOL-CLIMATE INTERACTIONS; ATMOSPHERIC OBSERVATIONS; BOUNDARY-LAYER; CONVECTION; DISPERSION; CIRCULATION; PARAMETERIZATION; FRAMEWORK; POLLUTION; IMPACTS;
D O I
10.5194/gmd-9-4029-2016
中图分类号
P [天文学、地球科学];
学科分类号
07 ;
摘要
The offline FLEXible PARTicle (FLEXPART) stochastic dispersion model is currently a community model used by many scientists. Here, an alternative FLEXPART model version has been developed and tailored to use with the meteorological output data generated by the CMIP5-version of the Norwegian Earth System Model (NorESM1-M). The atmospheric component of the NorESM1-M is based on the Community Atmosphere Model (CAM4); hence, this FLEXPART version could be widely applicable and it provides a new advanced tool to directly analyse and diagnose atmospheric transport properties of the state-of-the-art climate model NorESM in a reliable way. The adaptation of FLEXPART to NorESM required new routines to read meteorological fields, new post-processing routines to obtain the vertical velocity in the FLEXPART coordinate system, and other changes. These are described in detail in this paper. To validate the model, several tests were performed that offered the possibility to investigate some aspects of offline global dispersion modelling. First, a comprehensive comparison was made between the tracer transport from several point sources around the globe calculated online by the transport scheme embedded in CAM4 and the FLEXPART model applied offline on output data. The comparison allowed investigating several aspects of the transport schemes including the approximation introduced by using an offline dispersion model with the need to transform the vertical coordinate system, the influence on the model results of the sub-grid-scale parameterisations of convection and boundary layer height and the possible advantage entailed in using a numerically non-diffusive Lagrangian particle solver. Subsequently, a comparison between the reference FLEXPART model and the FLEXPART-NorESM/CAM version was performed to compare the well-mixed state of the atmosphere in a 1-year global simulation. The two model versions use different methods to obtain the vertical velocity but no significant difference in the results was found. However, for both model versions there was some degradation in the well-mixed state after 1 year of simulation with the buildup of a bias and an increased scatter. Finally, the capability of the new combined modelling system in producing realistic, backward-in-time transport statistics was evaluated calculating the average footprint over a 5-year period for several measurement locations and by comparing the results with those obtained with the reference FLEXPART model driven by re-analysis fields. This comparison confirmed the effectiveness of the combined modelling system FLEXPART with NorESM in producing realistic transport statistics.
引用
收藏
页码:4029 / 4048
页数:20
相关论文
共 79 条
[1]   Toward a Fully Lagrangian Atmospheric Modeling System [J].
Alam, Jahrul M. ;
Lin, John C. .
MONTHLY WEATHER REVIEW, 2008, 136 (12) :4653-4667
[2]  
[Anonymous], 1989, The kinematics of mixing: stretching, chaos, and transport
[3]  
[Anonymous], 2010, CCSM4.0 user's guide
[4]   An isopycnic ocean carbon cycle model [J].
Assmann, K. M. ;
Bentsen, M. ;
Segschneider, J. ;
Heinze, C. .
GEOSCIENTIFIC MODEL DEVELOPMENT, 2010, 3 (01) :143-167
[5]   The Norwegian Earth System Model, NorESM1-M - Part 1: Description and basic evaluation of the physical climate [J].
Bentsen, M. ;
Bethke, I. ;
Debernard, J. B. ;
Iversen, T. ;
Kirkevag, A. ;
Seland, O. ;
Drange, H. ;
Roelandt, C. ;
Seierstad, I. A. ;
Hoose, C. ;
Kristjansson, J. E. .
GEOSCIENTIFIC MODEL DEVELOPMENT, 2013, 6 (03) :687-720
[6]  
BLECK R, 1992, J PHYS OCEANOGR, V22, P1486, DOI 10.1175/1520-0485(1992)022<1486:SDTTIA>2.0.CO
[7]  
2
[8]   The Lagrangian particle dispersion model FLEXPART-WRF version 3.1 [J].
Brioude, J. ;
Arnold, D. ;
Stohl, A. ;
Cassiani, M. ;
Morton, D. ;
Seibert, P. ;
Angevine, W. ;
Evan, S. ;
Dingwell, A. ;
Fast, J. D. ;
Easter, R. C. ;
Pisso, I. ;
Burkhart, J. ;
Wotawa, G. .
GEOSCIENTIFIC MODEL DEVELOPMENT, 2013, 6 (06) :1889-1904
[9]  
Brown S. A., 1993, Computers in Physics, V7, P304
[10]  
Byun DW, 1999, J ATMOS SCI, V56, P3808, DOI 10.1175/1520-0469(1999)056<3808:DCFIMA>2.0.CO