Impact of an improved longwave radiation model, RRTM, on the energy budget and thermodynamic properties of the NCAR community climate model, CCM3

The effect of introducing a new longwave radiation parameterization, RRTM, on the energy budget and thermodynamic properties of the National Center for Atmospheric Research (NCAR) community climate model (CCM3) is described. RRTM is a rapid and accurate, correlated k, radiative transfer model that has been developed for the Atmospheric Radiation Measurement (ARM) program to address the ARM objective of improving radiation models in GCMs. Among the important features of RRTM are its connection to radiation measurements through comparison to the extensively validated line-by-line radiative transfer model (LBLRTM) and its use of an improved and validated water vapor continuum model. Comparisons between RRTM and the CCM3 longwave (LW) parameterization have been performed for single atmospheric profiles using the CCM3 column radiation model and for two 5-year simulations using the full CCM3 climate model. RRTM produces a significant enhancement of LW absorption largely due to its more physical and spectrally extensive water vapor continuum model relative to the current CCM3 water continuum treatment. This reduces the clear sky, outgoing longwave radiation over the tropics by 6–9 W m−2. Downward LW surface fluxes are increased by 8–15 W m−2 at high latitudes and other dry regions. These changes considerably improve known flux biases in CCM3 and other GCMs. At low and midlatitudes, RRTM enhances LW radiative cooling in the upper troposphere by 0.2–0.4 K d−1 and reduces cooling in the lower troposphere by 0.2–0.5 K d−1. The enhancement of downward surface flux contributes to increasing lower tropospheric and surface temperatures by 1–4 K, especially at high latitudes, which partly compensates documented, CCM3 cold temperature biases in these regions. Experiments were performed with the weather prediction model of the European Center for Medium Range Weather Forecasts (ECMWF), which show that RRTM also impacts temperature on timescales relevant to forecasting applications. RRTM is competitive with the CCM3 LW model in computational expense at 30 layers and with the ECMWF LW model at 60 layers, and it would be relatively faster at higher vertical resolution.

[1]  A. Lacis,et al.  A description of the correlated k distribution method for modeling nongray gaseous absorption, thermal emission, and multiple scattering in vertically inhomogeneous atmospheres , 1991 .

[2]  J. Curry,et al.  Radiative characteristics of the Arctic atmosphere during spring as inferred from ground-based measurements , 1997 .

[3]  S. Bony,et al.  Clear-sky greenhouse effect sensitivity to sea surface temperature changes : an evaluation of AMIP simulations , 1997 .

[4]  Yongxiang Hu,et al.  An Accurate Parameterization of the Radiative Properties of Water Clouds Suitable for Use in Climate Models , 1993 .

[5]  Xin-Zhong Liang,et al.  Cloud overlap effects on general circulation model climate simulations , 1997 .

[6]  Y. Fouquart Radiative Transfer in Climate Models , 1988 .

[7]  James J. Hack,et al.  Description of the NCAR Community Climate Model (CCM3). Technical note , 1996 .

[8]  Edwin F. Harrison,et al.  Earth Radiation Budget Experiment (ERBE) archival and April 1985 results , 1989 .

[9]  R E Roberts,et al.  Infrared continuum absorption by atmospheric water vapor in the 8-12-microm window. , 1976, Applied optics.

[10]  J. R. Garratt,et al.  The Surface Radiation Budget over Oceans and Continents , 1998 .

[11]  M. Webb,et al.  A 15-year Simulation of the Clear-Sky Greenhouse Effect Using the ECMWF Reanalyses: Fluxes and Comparisons with ERBE , 1998 .

[12]  Stephen A. Klein,et al.  The role of vertically varying cloud fraction in the parametrization of microphysical processes in the ECMWF model , 1999 .

[13]  E. Mlawer,et al.  Radiative transfer for inhomogeneous atmospheres: RRTM, a validated correlated-k model for the longwave , 1997 .

[14]  W. J. Lafferty,et al.  Experimental Investigation of the Self{ and N 2 {broadened Continuum within the 2 Band of Water Vapor , 2022 .

[15]  Frank J. Murcray,et al.  Measurements of the downward longwave radiation spectrum over the Antarctic Plateau and comparisons with a line-by-line , 1998 .

[16]  K. Lau,et al.  Comparison of model-calculated and ERBE-retrieved clear-sky outgoing longwave radiation , 1998 .

[17]  B. Bonnel,et al.  Intercomparing shortwave radiation codes for climate studies , 1991 .

[18]  M. Iacono,et al.  Line-by-Line Calculations of Atmospheric Fluxes and Cooling Rates: Application to Water Vapor , 1992 .

[19]  T. Phillips,et al.  A summary documentation of the AMIP models , 1994 .

[20]  M. Iacono,et al.  Line‐by‐line calculation of atmospheric fluxes and cooling rates: 2. Application to carbon dioxide, ozone, methane, nitrous oxide and the halocarbons , 1995 .

[21]  W. Gates AMIP: The Atmospheric Model Intercomparison Project. , 1992 .

[22]  G. Bonan The Land Surface Climatology of the NCAR Land Surface Model Coupled to the NCAR Community Climate Model , 1998 .

[23]  Robert G. Ellingson,et al.  The intercomparison of radiation codes used in climate models: Long wave results , 1991 .

[24]  J. Curry,et al.  A parameterization of ice cloud optical properties for climate models , 1992 .

[25]  James J. Hack,et al.  The Hydrologic and Thermodynamic Characteristics of the NCAR CCM3 , 1998 .

[26]  James J. Hack,et al.  Response of Climate Simulation to a New Convective Parameterization in the National Center for Atmospheric Research Community Climate Model (CCM3) , 1998 .

[27]  H. Barker,et al.  Comparison of the seasonal change in cloud-radiative forcing from atmospheric general circulation models , 1997 .

[28]  F. X. Kneizys,et al.  Line shape and the water vapor continuum , 1989 .

[29]  James J. Hack,et al.  The Energy Budget of the NCAR Community Climate Model: CCM3* , 1998 .

[30]  V. Ramaswamy,et al.  Intercomparing shortwave radiation codes for climate studies. J. Geophys. Res., 96, 8955-8968 , 1991 .

[31]  W. Collins,et al.  Validation of Clear-Sky Fluxes for Tropical Oceans from the Earth Radiation Budget Experiment. , 1995 .

[32]  David H. Bromwich,et al.  Polar Radiation Budgets of the NCAR CCM3 , 1998 .

[33]  D. Bromwich,et al.  Polar Climate Simulation of the NCAR CCM3 , 1998 .

[34]  Raymond K. Garcia,et al.  Downwelling spectral radiance observations at the SHEBA ice station: Water vapor continuum measurements from 17 to 26μm , 1999 .

[35]  B. Briegleb Delta‐Eddington approximation for solar radiation in the NCAR community climate model , 1992 .

[36]  S. Schwartz,et al.  The Atmospheric Radiation Measurement (ARM) Program: Programmatic Background and Design of the Cloud and Radiation Test Bed , 1994 .

[37]  V. Ramaswamy,et al.  Radiative effects of CH4, N2O, halocarbons and the foreign‐broadened H2O continuum: A GCM experiment , 1999 .

[38]  R. West,et al.  THE CORRELATED-k METHOD FOR RADIATION CALCULATIONS IN NONHOMOGENEOUS ATMOSPHERES , 1989 .

[39]  M. Webb,et al.  The spectral signature of global warming , 1997 .