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The GFDL-CM4X climate model hierarchy, Part I: model description and thermal properties
  • +25
  • Stephen M Griffies,
  • Alistair Adcroft,
  • Rebecca Lynn Beadling,
  • Mitchell Bushuk,
  • Chiung-Yin Chang,
  • Henri Francois Drake,
  • Raphael Dussin,
  • Robert W. Hallberg,
  • William Hurlin,
  • Hemant Khatri,
  • John P Krasting,
  • Matthew Lobo,
  • Graeme MacGilchrist,
  • Brandon G Reichl,
  • Aakash Sane,
  • Olga V. Sergienko,
  • Maike Sonnewald,
  • Jacob M. Steinberg,
  • Jan-Erik Tesdal,
  • Matthew D Thomas,
  • Katherine Elise Turner,
  • Marshall L Ward,
  • Michael Winton,
  • Niki Zadeh,
  • Laure Zanna,
  • Rong Zhang,
  • Wenda Zhang,
  • Ming Zhao
Stephen M Griffies
NOAA Geophysical Fluid Dynamics Laboratory

Corresponding Author:[email protected]

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Alistair Adcroft
Princeton University
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Rebecca Lynn Beadling
Temple University
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Mitchell Bushuk
GFDL/NOAA
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Chiung-Yin Chang
Princeton University
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Henri Francois Drake
University of California Irvine
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Raphael Dussin
National Oceanic and Atmospheric Administration
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Robert W. Hallberg
NOAA/Geophysical Fluid Dynamics Laboratory
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William Hurlin
NOAA/GFDL
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Hemant Khatri
University of Liverpool
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John P Krasting
Geophysical Fluid Dynamics Laboratory
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Matthew Lobo
Princeton University
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Graeme MacGilchrist
University of St Andrews
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Brandon G Reichl
NOAA Geophysical Fluid Dynamics Laboratory
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Aakash Sane
Princeton University
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Olga V. Sergienko
AOS, Princeton University/GFDL
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Maike Sonnewald
University of California, Davis
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Jacob M. Steinberg
Geophysical Fluid Dynamics Laboratory
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Jan-Erik Tesdal
Princeton University
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Matthew D Thomas
Centre for Environment, Fisheries and Aquaculture Science
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Katherine Elise Turner
University of Arizona
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Marshall L Ward
Australian National University
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Michael Winton
GFDL/NOAA
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Niki Zadeh
NOAA/GFDL
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Laure Zanna
New York University
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Rong Zhang
GFDL/NOAA
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Wenda Zhang
Princeton University
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Ming Zhao
GFDL/NOAA
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Abstract

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 $0.25^{\circ}$ (referred to as CM4X-p25) and the other that uses a $0.125^{\circ}$ grid (CM4X-p125). CM4X also refines its atmospheric grid from the nominally 100~km (cubed sphere C96) of CM4.0 to 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 $-0.02~\mbox{W}~\mbox{m}^{-2}$ within $\mathcal{O}(150)$ years in a pre-industrial simulation, and retains that thermally equilibrated state over the subsequent centuries. This 1850 thermal equilibrium is characterized by roughly $400~\mbox{ZJ}$ less ocean heat than present-day, which corresponds to estimates for anthropogenic ocean heat uptake between 1850 and present-day. CM4X-p25 approaches its thermal equilibrium only after more than 1000 years, at which time its ocean has roughly $1100~\mbox{ZJ}$ {\it 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 {\it mesoscale dominance hypothesis} for why CM4X-p125 shows such favorable thermal equilibration properties.
26 Nov 2024Submitted to ESS Open Archive
28 Nov 2024Published in ESS Open Archive