North Atlantic thermohaline circulation predictability in a coupled ocean-atmosphere model

Predictability of the North Atlantic thermohaline circulation (THC) variability as simulated in the Geophysical Fluid Dynamics Laboratory’s coupled ocean-atmosphere general circulation model is established for a set of ensemble experiments. There is a large separation of time scales between the slow...

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Bibliographic Details
Main Authors: Stephen M. Griffies, Kirk Bryan
Other Authors: The Pennsylvania State University CiteSeerX Archives
Format: Text
Language:English
Published: 1995
Subjects:
Online Access:http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.342.886
http://arxiv.org/pdf/ao-sci/9502001v4.pdf
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Summary:Predictability of the North Atlantic thermohaline circulation (THC) variability as simulated in the Geophysical Fluid Dynamics Laboratory’s coupled ocean-atmosphere general circulation model is established for a set of ensemble experiments. There is a large separation of time scales between the slower oceanic processes, whose predictability is of interest here, and the much more rapid atmospheric processes to which the ocean is coupled. The ensembles consist of identical oceanic initial conditions underneath a model atmosphere chosen randomly from the model climatology. This experimental design is based on the separation in time scales present in the model which motivates the assumption that the predictability deduced from these ensembles provides an upper limit to the model’s THC predictability. The climatology, against which the ensemble statistics are compared, is taken from a multi-century model integration whose THC variability has power concentrated at the 40-60 year time scale. A linear stochastic perspective, motivated from Brownian motion and THC box model case studies, is shown to be generally consistent with the ensemble statistics. The linear theory suggests a natural measure of ensemble predictability as the time at which the ensemble variance becomes a subjectively defined fraction (50 % used here) of the climatological variance. It is furthermore of