Seasonal mixed layer heat budget of the tropical Atlantic Ocean



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Seasonal mixed layer heat budget of the tropical Atlantic Ocean


Gregory R. Foltz, Semyon A. Grodsky*, James A. Carton, and Michael J. McPhaden1




Revised for Journal of Geophysical Research - Oceans




January 15, 2003




Department of Meteorology


University of Maryland

College Park, MD 20742


1 NOAA/Pacific Marine Environmental Laboratory

7600 Sand Point Way NE

Seattle, WA 98115
* corresponding author

senya@atmos.umd.edu

Abstract


This paper addresses the atmospheric and oceanic causes of the seasonal cycle of sea surface temperature (SST) in the tropical Atlantic based on direct observations. Data sets include up to four years (September 1997 - February 2002) of measurements from moored buoys of the Pilot Research Array in the Tropical Atlantic (PIRATA), near-surface drifting buoys, and a blended satellite-in situ SST product. We analyze the mixed layer heat balance at eight PIRATA mooring locations and find that the seasonal cycles of latent heat loss and absorbed shortwave radiation are responsible for seasonal SST variability in the northwest basin (8 - 15ºN along 38ºW). Along the equator (10ºW - 35ºW) contributions from latent heat loss are diminished, while horizontal temperature advection and vertical entrainment contribute significantly. Zonal temperature advection is especially important during boreal summer near the western edge of the cold tongue, while horizontal eddy temperature advection, which most likely results from tropical instability waves, opposes temperature advection by the mean flow. The dominant balance in the southeast (6 - 10ºS along 10ºW) is similar to that in the northwest, with both latent heat loss and absorbed solar radiation playing important roles.

1. Introduction

The seasonal cycle of shortwave radiation at the top of the atmosphere is primarily semiannual in the tropics, with maxima in boreal spring and fall. On the other hand, variability in the tropical Atlantic ocean-atmosphere system is dominated by the annual harmonic. The difference reflects seasonal changes in the radiative properties of the atmosphere and the dynamics and thermodynamics of the ocean. In this study we use direct observations, primarily from recently deployed moorings of PIRATA (Pilot Research Array in the Tropical Atlantic) (Servain et al., 1998), to examine the causes of the seasonal cycle of SST in response to seasonally varying surface heating and winds.

Net surface heat flux is a combination of latent and sensible heat loss, shortwave radiation absorption, and net longwave emission. Sensible heat loss is insignificant (less than 10 W m-2) due to small air-sea temperature differences, while net emission of longwave radiation is a relatively constant ~ 50 W m-2 (da Silva et al., 1994). Seasonal variations in latent heat loss and downwelling surface shortwave radiation are more significant. Both are influenced by the latitudinal movement of the narrow band of clouds associated with the Intertropical Convergence Zone (ITCZ), and shortwave radiation is additionally influenced by changes in the solar zenith angle. In the northern tropics latent heat loss is lowest during boreal summer and fall, when winds are weak and relative humidity is high (> 85%). Latent heat loss rises during boreal winter and spring when the ITCZ is close to the equator, low-level humidity is lower, and the northeast trade winds are stronger. In the eastern equatorial zone latent heat loss has only weak seasonal variations, as low-level relative humidity and wind speed are fairly steady throughout the year (da Silva et al., 1994).

In contrast to the shortwave radiation at the top of the atmosphere, surface shortwave radiation has a significant annual harmonic at most locations. North of 5ºN surface solar radiation reaches a maximum in boreal spring, when the ITCZ is near its southernmost position and the solar zenith angle is high. Between the equator and 5ºN there is a strong semiannual component, with maxima in boreal spring and fall, while on the equator the annual harmonic is again significant with increasing amplitude toward the west reaching maximum in boreal fall. The reduced amplitude in the east is due to the appearance of reflective stratus clouds in boreal fall over the cool waters of the eastern basin (Klein and Hartmann, 1993; Philander et al., 1996).



Like the tropical atmosphere, the tropical ocean also has a strong annual harmonic. A westward shift of warm (> 27ºC) SST in the latitude band 5-15ºN occurs in boreal summer, along with the development of a tongue of cool 23C SST along and just south of the equator east of 30W. This shift occurs concurrently with the annual growth and eastward expansion of the Atlantic warm pool west of 50W (Wang and Enfield, 2001). In the west, seasonal changes in SST are weak in the equatorial zone, while north of 8N a strong annual harmonic appears with a maximum in boreal fall. South of the equator SST reaches its maximum in boreal spring with an annual harmonic that increases in amplitude eastward to up to 3C near the African coast (Reynolds and Smith, 1994).

The surface wind field is dominated by the northeast trade winds to the north of the ITCZ and the southeast trade winds to the south, with weakened winds between (da Silva et al., 1994). To the east a monsoonal circulation develops in boreal summer causing the northeast trades to reverse direction. Zonal currents develop in response to these changing winds and resulting Ekman divergence. On and south of the equator the westward South Equatorial Current is strongest in boreal summer, with speeds of 55 cm s-1 in the central basin (Richardson and Reverdin, 1987). Close to the latitude of the ITCZ (5-10N) the eastward North Equatorial Countercurrent is strong during boreal summer and fall with speeds of 35 cm s-1. Between these two major current systems, and on the northern edge of the cold tongue, lie the strong meridional fluctuations of tropical instability waves, which we anticipate are important in transporting heat into the cold tongue in the eastern and central basin (Weisberg and Weingartner, 1988).

A number of observational (e.g., Wyrtki, 1981; Enfield, 1986; Hayes et al., 1991; Wang and McPhaden, 1999; Swenson and Hansen, 1999) and modeling (e.g., Koberle and Philander, 1994; Kessler et al., 1998) studies have addressed the causes of the seasonal cycle of SST in the eastern equatorial Pacific. Observational studies in particular have had difficulty closing the heat budget. Hayes et al. (1991) used mooring observations in the eastern equatorial Pacific, together with surface meteorology, to calculate contributions to the mixed layer heat budget during 1986-1988. They found discrepancies between their forcing and actual heat storage that in some cases exceeded 100 W m-2 and attributed these discrepancies to errors in parameterizations of mixed layer depth, entrainment, and meridional eddy heat divergence.

Wang and McPhaden (1999) used a combination of 15 years of daily mooring observations and climatological surface meteorology to estimate terms in the equatorial Pacific mixed layer heat budget. They estimated a mean seasonal cycle and found significant contributions from net surface heat flux and horizontal advection. They found discrepancies of up to 120 W m-2 in the east and attributed these differences to a combination of two missing terms: vertical entrainment and vertical diffusion. Consistent with these results, Swenson and Hansen (1999) used a combination of drifting buoys and vertical temperature profiles to investigate the heat budget of the cold tongue. They found that strong seasonal cycles of entrainment and horizontal advection account for a large fraction of seasonal SST variability.

In the equatorial Atlantic, Hastenrath (1977) and Merle (1980) used climatologies of surface heat flux and heat storage to deduce that horizontal and vertical temperature advection are necessary to balance the annual mean net surface heat flux. Molinari et al. (1985) used atmospheric and oceanic measurements from the First Global Atmospheric Research Program’s (GARP) Global Experiment (FGGE) in 1979 to explicitly evaluate the effects of surface energy fluxes and zonal temperature advection on the seasonal cycle of mixed layer temperature. Their results revealed important contributions from zonal advection between 3 - 9ºN. They calculated the sum of vertical and meridional advection/diffusion as a residual and found this term to be important within 3º of the equator. Unfortunately, none of the above studies was able to explicitly calculate the effects of meridional advection or vertical entrainment/diffusion on the mixed layer heat balance.

Weingartner and Weisberg (1991a,b) examined the seasonal heat budget based on one year of observations from an equatorial mooring at 28ºW (midbasin). They concluded that upwelling creates the cold SST tongue in boreal spring, while SST increases in boreal summer as the result of tropical instability waves. In late summer and fall advection terms are small and compensating and diffusion at the base of the mixed layer balances net surface heat gain. In boreal winter SST increases in response to a net surface heat flux concentrated by the shallower mixed layer.

Modeling studies have also stressed the importance of ocean dynamics in the equatorial Atlantic heat budget. Carton and Zhou (1997) concluded that zonal mass divergence causes cooling in the equatorial region east of 20ºW, while meridional Ekman divergence plays an important role in the west. Their results indicate that solar heating is most important south of 5ºS and north of 10ºN, while latent heat loss is dominant in the western basin between 8 - 12ºN. DeWitt and Schneider (1999) also found that advection plays a crucial role in the equatorial region, while the importance of latent heat loss increases toward the subtropics.



The studies mentioned above reveal that surface fluxes as well as horizontal and vertical temperature advection play a major role in shaping the seasonal cycle of SST in the equatorial Atlantic. However, the limited duration (~ 1 year) and spatial coverage of previous in situ observational programs has hindered efforts to quantify these contributions. In this study we use a variety of in situ and satellite measurements, with extended duration and spatial coverage, to explicitly calculate all contributions (with the exception of vertical turbulent diffusion) to the mixed layer heat balance to obtain a quantitative picture of the tropical Atlantic seasonal mixed layer heat balance.

2. Data and Methods


The mixed layer heat budget represents a balance of several terms (Stevenson and Niiler, 1983; Moisan and Niiler, 1998):

. (1)

The terms represent, from left to right, local storage, horizontal advection (separated into mean and eddy terms), entrainment, vertical temperature/velocity covariance, and the combination of net atmospheric heating and vertical turbulent diffusion at the base of the mixed layer. Here h is the depth of the mixed layer, T and are temperature and velocity vertically averaged from the surface to a depth of -h, T’ and are deviations from the time means (the overbar represents a time mean), and represent deviations from the vertical average, q0 is net surface heat flux, while q-h represents the sum of heat flux due to penetrative shortwave radiation and turbulent mixing at the base of the mixed layer. Swenson and Hansen (1999) estimate that the vertical temperature/velocity covariance term in (1) is less than 10% as large as other terms, and we therefore proceed to neglect this term. Entrainment velocity may be rewritten as , following Stevenson and Niiler (1983) (see their Eqs.(2) and (3)), and is associated with a mass flux that crosses an isopycnal surface.

Estimation of the terms in (1) requires knowledge of vertically averaged mixed layer horizontal velocity. Unfortunately, vertical profiles of velocity are not available at the PIRATA mooring locations. We therefore use alternative methods (described later in this section) to estimate mean and eddy advection terms in (1).



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