On the Wind-Driven Circulation of the Uncoupled and Coupled NCAR Climate System Ocean Model

Gokhan Danabasoglu National Center for Atmospheric Research, Boulder, Colorado

Search for other papers by Gokhan Danabasoglu in
Current site
Google Scholar
PubMed
Close
Restricted access

Abstract

The time-mean wind-driven circulation of the uncoupled and coupled National Center for Atmospheric Research Climate System Model ocean model is investigated. Although the coupled surface wind stress and wind stress curl magnitudes are, in general, larger than the uncoupled distributions, the coupled wind stresses are realistic, given the substantial uncertainties in the observational estimates. The Sverdrup balance, which represents a simple dynamical relation, can indeed describe the model depth-integrated transports to a large degree and shows that the increase in the coupled ocean barotropic transports is mainly due to the larger wind stress curl of the coupled system. Another simple dynamical tool, the Ekman transport analysis, shows that the coupled ocean upwelling and downwelling velocities are, in general, larger than in uncoupled ocean, consistent with the larger wind stress curl. Both models have similar upper-ocean upwelling magnitudes in the equatorial Atlantic. In the equatorial Pacific, the coupled ocean upwelling is much larger. The coupled ocean surface currents, similarly stronger than in uncoupled ocean, differ from the uncoupled currents especially in the Nordic Seas. The Ekman transport contribution to the northward heat transport is significant in the tropical regions and in the Southern Hemisphere midlatitudes, and this transport is larger in coupled ocean than in uncoupled ocean.

Corresponding author address: Dr. Gokhan Danabasoglu, NCAR/CGD, P.O. Box 3000, Boulder, CO 80307-3000.

Abstract

The time-mean wind-driven circulation of the uncoupled and coupled National Center for Atmospheric Research Climate System Model ocean model is investigated. Although the coupled surface wind stress and wind stress curl magnitudes are, in general, larger than the uncoupled distributions, the coupled wind stresses are realistic, given the substantial uncertainties in the observational estimates. The Sverdrup balance, which represents a simple dynamical relation, can indeed describe the model depth-integrated transports to a large degree and shows that the increase in the coupled ocean barotropic transports is mainly due to the larger wind stress curl of the coupled system. Another simple dynamical tool, the Ekman transport analysis, shows that the coupled ocean upwelling and downwelling velocities are, in general, larger than in uncoupled ocean, consistent with the larger wind stress curl. Both models have similar upper-ocean upwelling magnitudes in the equatorial Atlantic. In the equatorial Pacific, the coupled ocean upwelling is much larger. The coupled ocean surface currents, similarly stronger than in uncoupled ocean, differ from the uncoupled currents especially in the Nordic Seas. The Ekman transport contribution to the northward heat transport is significant in the tropical regions and in the Southern Hemisphere midlatitudes, and this transport is larger in coupled ocean than in uncoupled ocean.

Corresponding author address: Dr. Gokhan Danabasoglu, NCAR/CGD, P.O. Box 3000, Boulder, CO 80307-3000.

Save
  • Bonan, G. B., 1998: The land surface climatology of the NCAR Land Surface Model coupled to the NCAR Community Climate Model. J. Climate,11, 1307–1326.

  • Böning, C. W., and F. O. Bryan, 1996: Large-scale transport processes in high-resolution circulation models. The Warmwatersphere of the North Atlantic Ocean, W. Krauss, Ed., Gebrüder Borntraeger, 91–128.

  • Boville, B. A., and P. R. Gent, 1998: The NCAR Climate System Model, version one. J. Climate,11, 1115–1130.

  • ——, and J. W. Hurrell, 1998: A comparison of the atmospheric circulations simulated by the CCM3 and CSM1. J. Climate,11, 1327–1341.

  • Bryan, F. O., 1998: Climate drift in a multicentury integration of the NCAR Climate System Model. J. Climate,11, 1455–1471.

  • ——, C. W. Böning, and W. R. Holland, 1995: On the midlatitude circulation in a high-resolution model of the North Atlantic. J. Phys. Oceanogr.,25, 289–305.

  • Bryan, K., 1969: A numerical method for the study of the circulation of the World Ocean. J. Comput. Phys.,4, 347–376.

  • ——, 1984: Accelerating the convergence to equilibrium of ocean climate models. J. Phys. Oceanogr.,14, 666–673.

  • Cox, M. D., 1984: A primitive equation, 3-dimensional model of the ocean. GFDL Ocean Group Tech. Rep. 1, 143 pp. [Available from GFDL/Princeton University, Princeton, NJ 08542.].

  • Danabasoglu, G., and J. C. McWilliams, 1995: Sensitivity of the global ocean circulation to parameterizations of mesoscale tracer transports. J. Climate,8, 2967–2987.

  • ——, ——, and W. G. Large, 1996: Approach to equilibrium in accelerated global oceanic models. J. Climate,9, 1092–1110.

  • Doney, S. C., F. O. Bryan, and W. G. Large, 1998: Surface ocean fluxes and water-mass transformation rates in the coupled NCAR Climate System Model. J. Climate,11, 1420–1441.

  • Fieux, M., C. Andrié, P. Delecluse, A. G. Ilahude, A. Kartavtseff, F. Mantisi, R. Molcard, and J. C. Swallow, 1994: Measurements within the Pacific–Indian Oceans throughflow region. Deep-Sea Res.,41, 1091–1130.

  • ——, R. Molcard, and A. G. Ilahude, 1996: Geostrophic transport of the Pacific–Indian Oceans throughflow. J. Geophys. Res.,101, 12 421–12 432.

  • Gent, P. R., and J. C. McWilliams, 1990: Isopycnal mixing in ocean circulation models. J. Phys. Oceanogr.,20, 150–155.

  • ——, F. O. Bryan, G. Danabasoglu, S. C. Doney, W. R. Holland, W. G. Large, and J. C. McWilliams, 1998: The NCAR climate system model global ocean component. J. Climate,11, 1287–1306.

  • Godfrey, J. S., 1989: A Sverdrup model of the depth-integrated flow for the World Ocean allowing for island circulations. Geophys. Astrophys. Fluid Dyn.,45, 89–112.

  • ——, 1996: The effect of the Indonesian Throughflow on ocean circulation and heat exchange with the atmosphere: A review. J. Geophys. Res.,101, 12 217–12 237.

  • Gould, W. J., J. Loynes, and J. Backhaus, 1985: Seasonality in slope current transports northwest of Shetland. ICES, Hydrography Committee C. M. 1985/C, Vol. 7, 13 pp. [Available from ICES, Palægade 2-4, OK-1261 Copenhagen K, Denmark.].

  • Harrison, D. E., 1989: On climatological monthly mean wind stress and wind stress curl fields over the World Ocean. J. Climate,2, 57–70.

  • Hellerman, S., and M. Rosenstein, 1983: Normal monthly wind stress over the World Ocean with error estimates. J. Phys. Oceanogr.,13, 1093–1104.

  • Hogg, N. G., 1992: On the transport of the Gulf Stream between Cape Hatteras and the Grand Banks. Deep-Sea Res.,39, 1231–1246.

  • Holland, W. R., J. C. Chow, and F. O. Bryan, 1998: Application of a third-order upwind scheme in the NCAR ocean model. J. Climate,11, 1487–1493.

  • Kiehl, J. T., J. J. Hack, G. B. Bonan, B. A. Boville, D. L. Williamson, and P. J. Rasch, 1998: The National Center for Atmospheric Research Community Climate Model: CCM3. J. Climate,11, 1131–1149.

  • Large, W. G., J. C. McWilliams, and S. C. Doney, 1994: Oceanic vertical mixing: A review and a model with a nonlocal boundary layer parameterization. Rev. Geophys.,32, 363–403.

  • ——, G. Danabasoglu, S. C. Doney, and J. C. McWilliams, 1997: Sensitivity to surface forcing and boundary layer mixing in a global ocean model: Annual-mean climatology. J. Phys. Oceanogr.,27, 2418–2447.

  • Larsen, J. C., 1992: Transport and heat flux of the Florida Current at 27°N derived from cross-stream voltages and profiling data: Theory and observations. Phil. Trans. Roy. Soc. London,338A, 169–236.

  • NCAR Oceanography Section, 1996: The NCAR CSM Ocean Model. NCAR Tech. Note NCAR/TN-423+STR, 84 pp. [Available from NCAR, P.O. Box 3000, Boulder, CO 80307.].

  • Pacanowski, R. C., K. Dixon, and A. Rosati, 1991/93: The GFDL modular ocean model users guide. GFDL Ocean Group Tech. Rep. 2. [Available from GFDL, Princeton University, Princeton, NJ 08542.].

  • Peterson, R. G., and L. Stramma, 1991: Upper-level circulation in the South Atlantic Ocean. Progress in Oceanography, Vol. 26, Pergamon, 1–73.

  • Qiu, B., and T. M. Joyce, 1992: Interannual variability in the mid- and low-latitude western North Pacific. J. Phys. Oceanogr.,22, 1062–1079.

  • Stramma, L., and J. R. E. Lutjeharms, 1997: The flow field of the subtropical gyre of the South Indian Ocean. J. Geophys. Res.,102, 5513–5530.

  • Trenberth, K. E., W. G. Large, and J. G. Olson, 1990: The mean annual cycle in global ocean wind stress. J. Phys. Oceanogr.,20, 1742–1760.

  • Wajsowicz, R. C., 1993: The circulation of the depth-integrated flow around an island with application to the Indonesian Throughflow. J. Phys. Oceanogr.,23, 1470–1484.

  • Weatherly, J. W., B. P. Briegleb, W. G. Large, and J. A, Maslanik, 1998: Sea ice and polar climate in the NCAR CSM. J. Climate,11, 1472–1486.

  • Whitworth, T., III, 1983: Monitoring the transport of the Antarctic Circumpolar Current at Drake Passage. J. Phys. Oceanogr.,13, 2045–2057.

  • Wunsch, C., and D. Roemmich, 1985: Is the North Atlantic in Sverdrup balance? J. Phys. Oceanogr.,15, 1876–1880.

All Time Past Year Past 30 Days
Abstract Views 0 0 0
Full Text Views 869 695 199
PDF Downloads 71 23 3