1 |
heimbach |
1.1 |
Interannual Variation of Mixed-layer Heat Balance: |
2 |
|
|
contrasting different climate phenemena and the roles of linear |
3 |
|
|
versus nonlinear effects |
4 |
|
|
|
5 |
|
|
Tong Lee, Ichiro Fukumori, Benyang Tang, and Dimitris Menemenlis |
6 |
|
|
|
7 |
|
|
Variation of mixed-layer heat balance are studied using an ECCO |
8 |
|
|
assimilation product (http://www.ecco-group.org). The analysis |
9 |
|
|
focuses on the similarity and difference associated with El |
10 |
|
|
Nino-Southern Oscillation (ENSO), Indian-Ocean Dipole (OID), and |
11 |
|
|
Pacific Decadal Oscillation (PDO), and the relative importance of |
12 |
|
|
linear versus nonlinear advective tendencies. In the eastern and central |
13 |
|
|
equatorial Pacific, the warming and cooling are caused by the combined |
14 |
|
|
effect of oceanic advection and diffusion. Surface heat flux opposes |
15 |
|
|
the change. The opposite is true for the western equatorial Pacific. |
16 |
|
|
The relative contribution of different components of oceanic advection |
17 |
|
|
is spatially dependent. Zonal advection is dominant in the central |
18 |
|
|
equatorial Pacific where zonal temperature gradient associated with |
19 |
|
|
the warm-pool edge is large. Vertical advection is more important in |
20 |
|
|
the eastern equatorial Pacific where upwelling and vertical |
21 |
|
|
temperature gradient are large. Diffusion has a smaller magnitude |
22 |
|
|
than advection, but is comparable to the temporal change of |
23 |
|
|
mixed-layer temperature (MLT). Advection of anomalous temperature |
24 |
|
|
gradient by mean flow and advection of mean temperature gradient by |
25 |
|
|
anomalous flow have comparable magnitude, both being in-phase with the |
26 |
|
|
change of MLT. Nonlinear tendency (advection of anomalous temperature |
27 |
|
|
gradient by anomalous flow) is sizable and counteracts the two linear |
28 |
|
|
tendencies above. Different from the tropical Pacific, nonlinear effect |
29 |
|
|
in mid-latitude Pacific is very small; the advection of mean temperature |
30 |
|
|
gradient by anomalous flow has the largest contribution to the total |
31 |
|
|
advection of heat. The role of total oceanic advection in MLT balance is |
32 |
|
|
similar for ENSO, IOD, and PDO. However, that of surface heat flux is |
33 |
|
|
different. |
34 |
|
|
|