TY - JOUR
T1 - The GFDL-CM4X Climate Model Hierarchy, Part I
T2 - Model Description and Thermal Properties
AU - Griffies, Stephen M.
AU - Adcroft, Alistair
AU - Beadling, Rebecca L.
AU - Bushuk, Mitchell
AU - Chang, Chiung Yin
AU - Drake, Henri F.
AU - Dussin, Raphael
AU - Hallberg, Robert W.
AU - Hurlin, William J.
AU - Khatri, Hemant
AU - Krasting, John P.
AU - Lobo, Matthew
AU - MacGilchrist, Graeme A.
AU - Reichl, Brandon G.
AU - Sane, Aakash
AU - Sergienko, Olga
AU - Sonnewald, Maike
AU - Steinberg, Jacob M.
AU - Tesdal, Jan Erik
AU - Thomas, Matthew
AU - Turner, Katherine E.
AU - Ward, Marshall L.
AU - Winton, Michael
AU - Zadeh, Niki
AU - Zanna, Laure
AU - Zhang, Rong
AU - Zhang, Wenda
AU - Zhao, Ming
N1 - Publisher Copyright:
© 2025 Crown copyright and The Author(s). Journal of Advances in Modeling Earth Systems published by Wiley Periodicals LLC on behalf of American Geophysical Union. This article is published with the permission of the Controller of HMSO and the King’s Printer for Scotland. This article has been contributed to by U.S. Government employees and their work is in the public domain in the USA.
PY - 2025/10
Y1 - 2025/10
N2 - We present the GFDL-CM4X (Geophysical Fluid Dynamics Laboratory Climate Model version 4X) coupled climate model hierarchy. The primary application for CM4X is to investigate ocean and sea ice physics as part of a realistic coupled Earth climate model. CM4X utilizes an updated MOM6 (Modular Ocean Model version 6) ocean physics package relative to CM4.0, and there are two members of the hierarchy: one that uses a horizontal grid spacing of (Formula presented.) (referred to as CM4X-p25) and the other that uses a (Formula presented.) grid (CM4X-p125). CM4X also refines its atmospheric grid from the nominally 100 km (cubed sphere C96) of CM4.0–50 km (C192). Finally, CM4X simplifies the land model to allow for a more focused study of the role of ocean changes to global mean climate. CM4X-p125 reaches a global ocean area mean heat flux imbalance of (Formula presented.) within (Formula presented.) years in a pre-industrial simulation, and retains that thermally equilibrated state over the subsequent centuries. This 1850 thermal equilibrium is characterized by roughly (Formula presented.) less ocean heat than present-day, which corresponds to estimates for anthropogenic ocean heat uptake between 1870 and present-day. CM4X-p25 approaches its thermal equilibrium only after more than 1000 years, at which time its ocean has roughly (Formula presented.) more heat than its early 21st century ocean initial state. Furthermore, the root-mean-square sea surface temperature bias for historical simulations is roughly 20% smaller in CM4X-p125 relative to CM4X-p25 (and CM4.0). We offer the mesoscale dominance hypothesis for why CM4X-p125 shows such favorable thermal equilibration properties.
AB - We present the GFDL-CM4X (Geophysical Fluid Dynamics Laboratory Climate Model version 4X) coupled climate model hierarchy. The primary application for CM4X is to investigate ocean and sea ice physics as part of a realistic coupled Earth climate model. CM4X utilizes an updated MOM6 (Modular Ocean Model version 6) ocean physics package relative to CM4.0, and there are two members of the hierarchy: one that uses a horizontal grid spacing of (Formula presented.) (referred to as CM4X-p25) and the other that uses a (Formula presented.) grid (CM4X-p125). CM4X also refines its atmospheric grid from the nominally 100 km (cubed sphere C96) of CM4.0–50 km (C192). Finally, CM4X simplifies the land model to allow for a more focused study of the role of ocean changes to global mean climate. CM4X-p125 reaches a global ocean area mean heat flux imbalance of (Formula presented.) within (Formula presented.) years in a pre-industrial simulation, and retains that thermally equilibrated state over the subsequent centuries. This 1850 thermal equilibrium is characterized by roughly (Formula presented.) less ocean heat than present-day, which corresponds to estimates for anthropogenic ocean heat uptake between 1870 and present-day. CM4X-p25 approaches its thermal equilibrium only after more than 1000 years, at which time its ocean has roughly (Formula presented.) more heat than its early 21st century ocean initial state. Furthermore, the root-mean-square sea surface temperature bias for historical simulations is roughly 20% smaller in CM4X-p125 relative to CM4X-p25 (and CM4.0). We offer the mesoscale dominance hypothesis for why CM4X-p125 shows such favorable thermal equilibration properties.
UR - https://www.scopus.com/pages/publications/105019402612
U2 - 10.1029/2024MS004861
DO - 10.1029/2024MS004861
M3 - Article
AN - SCOPUS:105019402612
SN - 1942-2466
VL - 17
JO - Journal of Advances in Modeling Earth Systems
JF - Journal of Advances in Modeling Earth Systems
IS - 10
M1 - e2024MS004861
ER -