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The general features of the seasonal suuface heat budget in the tropical western Pacific Ocean,20°S-20°N, western boundary-160°E, were documented by Qu (1995) using a high-resolution generalcirculation model (GCM, Semtner & Chervin,1992) ard existing observations.Close inspection of thesmaller areas, with the whole region further partitioned into six parts, showed different mechanisms balancethe seasonal surface heat budget in different parts of the region The results of study on five subregionsare detailed in this article. In the equatorial (3°S - 3°N) aed North Equatorial Countercurrent(3°N-9°N) region, the surface the flux the does not change significantly throughout the year, so the surface heat content is determined largely by vertical motion near the equator and roughly helf due to horizontal and halfdue to vertical circulation in the region of the North Equatorial Countercurrent(NECC). In the othersubregions (9°N-20°N, 20°S -11°S aed 11°S -3°S ), however, in addition to ocean dynamics
The general features of the seasonal suuface heat budget in the tropical western Pacific Ocean, 20 ° S-20 ° N, western boundary-160 ° E, were documented by Qu (1995) using a high-resolution general circulation model (GCM, Semtner & Chervin, 1992) ard existing observations. Close inspection of thesmaller areas, with the whole region further partitioned into six parts, showed different mechanisms balance the seasonal surface heat budget in different parts of the region The results of study on five subregions detailed in this article. In the equatorial (3 ° S - 3 ° N) aed North Equatorial Countercurrent (3 ° N-9 ° N) region, the surface the flux the does not change significantly throughout the year, so the surface heat content is determined substantially by vertical motion near the equator and roughly helf due to horizontal and halfdue to vertical circulation in the region of the North Equatorial Countercurrent (NECC). In the others (9 ° N - 20 ° N, 20 ° S - 11 ° S aed 11 ° S -3 ° S), however, in additio n to ocean dynamics