160 likes | 340 Views
The Vertical Structure of Eddy Heat Transport Simulated by an Eddy-Resolving OGCM. Bo Young et al. Outline. Introduction Model description Result Distribution of EKE and D-EHT Distribution of H e , H d and H K Seasonal variation of H e , H d and H K
E N D
The Vertical Structure of Eddy Heat Transport Simulated by an Eddy-Resolving OGCM Bo Young et al.
Outline • Introduction • Model description • Result • Distribution of EKE and D-EHT • Distribution of He, Hd and HK • Seasonal variation of He, Hd and HK • Vertical profiles of the zonally averaged T, EKE EHT • Effect of a seasonal thermocline on the structure of mesoscale eddy • Conclusion
Introduction • Heat transport by mesoscale eddy or eddy heat transport(EHT) constitutes an important part in meridional heat transport in the ocean (Wunsch 1999,and Roemmich and Gilson 2001) • Since the information below the sea surface is not available from Satellite, an assumption is introduced for the vertical, structure depth integrated value of EHT(D-EHT)(Stammer 1998).
Qiu and Chen assumed that the effective depth of EHT (He:=D-EHT/EHTsurface) is constant. • To resolve the mesoscale eddy and estimation of D-EHT require the resolution of 1/10 degree(Meijers et al. 2007) • The clarification of the vertical structure of EHT provides essential information for the parameterization of lateral mixing in coarse-resolution OGCMs (Killworth 1998)
Model • Research Institute for Applied Mechanics Ocean Model • Pacific ocean model covers 50S-65N, 95E-70W, 70 vertical level, 1/12 degree. • Advection momentum: the generalized Arakawa scheme (ishizaki and Motoi 1999). • Vertical mixings : Noh scheme • Input data: WOA94 climatological mean temperature and salinity. • Model integrated : 25 years
Effect of a seasonal thermocline on the structure of mesoscale eddy