Key papers that chart the development of MITgcm
are:
Marshall, J., C. Hill, L. Perelman, and A. Adcroft, (1997)
Hydrostatic, quasi-hydrostatic, and nonhydrostatic ocean
modeling
J. Geophysical Res., 102(C3), 5733-5752.
Marshall, J., A. Adcroft, C. Hill, L. Perelman, and C. Heisey,
(1997)
A finite-volume, incompressible Navier Stokes model for studies
of the ocean on parallel computers.
J. Geophysical Res., 102(C3), 5753-5766.
Adcroft, A.J., Hill, C.N. and J. Marshall, (1997)
Representation of topography by shaved cells in a height
coordinate ocean model
Mon Wea Rev, vol 125, 2293-2315
Marshall, J., Jones, H. and C. Hill, (1998)
Efficient ocean modeling using non-hydrostatic algorithms.
Journal of Marine Systems, 18, 115-134
Adcroft, A., Hill C. and J. Marshall: (1999)
A new treatment of the Coriolis terms in C-grid models at both
high and low resolutions.
Mon. Wea. Rev. Vol 127, pages 1928-1936
Marotzke, J, Giering,R., Zhang, K.Q., Stammer,D., Hill,C.,
and T.Lee, (1999)
Construction of the adjoint MIT ocean general circulation model
and application to Atlantic heat transport variability
J. Geophysical Res., 104(C12), 29,529-29,547.
Adcroft, A. and J-M. Campin, (2004)
Rescaled height coordinates for accurate representation of
free-surface flows in ocean circulation models. Ocean Modeling,
Vol. 7 (3-4): 269-284
Adcroft,
A., J-M Campin, C. Hill and J. Marshall (2004) Implementation of
an atmosphere-ocean general circulation model on the expanded
spherical cube. Mon. Wea. Rev., 132 (12), 2845-2863
Marshall, J. A. Adcroft,
J-M Campin and C. Hill (2004)
Atmosphere-ocean modeling exploiting fluid isomorphisms.
Mon. Wea. Rev., 132 (12), 2882-2894
Campin,
J-M., A Adcroft, C. Hill and J. Marshall (2004) Conservation of
properties in a free surface model. Ocean Modelling, Vol 6,
221-244.
Hill,
C., C. DeLuca, V. Balaji, M. Suarez, and A. da Silva, 2004:
Architecture of the Earth System Modeling Framework. Computing
in Science and Engineering, Volume 6, Number 1.
A list of published papers that make use of MITgcm can be
found here.
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