2. Regional Context

a. Seasonal Evolution of SST and OLR fields

Outgoing longwave radiation (OLR) measured by satellites can be used as a proxy for deep convection in the tropics, and in the subtropics during summer, since this produces extensive cirrus anvil clouds which emit at relatively cold temperatures. Thus, the lowest OLR values over such regions generally indicate convective activity and cirrus anvil coverage (e.g. Zhang 1993). The OLR data used is available on a daily basis from twice daily NOAA AVHRR soundings (e.g. Gruber and Krueger 1984). The grid size is 2.5 x 2.5 degrees for the period 1974 to present. This data provides a reasonable indicator of the extent of convection. The SST data used are based upon an optimum interpolation analysis and adjusted for biases using the method of Reynolds (1988) and Reynolds and Marsico (1993). This analysis is produced weekly on a one-degree grid using in situ and satellite derived SSTs (hence blended data). However, this was not the SST data set used in the three year study, which has higher spatial resolution.

The evolution of SSTs and tropical convection inferred from OLR are shown in Fig. 1 and Fig. 2 for the monsoon and surrounding regions. Monthly averaged OLR and blended SST data, from 1974-1993, were used to generate the 20 year mean values. The SST isotherms are shown in color. Due to the 1 degree resolution of SST data, we do not have full confidence in the absolute SST magnitudes in the Gulf of California (especially its upper half), but the spatial and temporal behavior of the SST data should be realistic enough to recognize the general behavior of the system. We regard the 240 W m-2 OLR isoline as an estimate of the monsoon's extent, since OLR < 240 W m-2 generally appears associated with deep convection at these latitudes (Zhang 1993). Clear skies dominate the warm pool region in March and April, allowing solar insolation to expand the warm pool. By April, a 29°C isotherm extends off southern Mexico from 108°W to 92°W, and south to 7°N. In May, convection and cirrus build-up in the south may cool SSTs (Ramanathan and Collins 1991). In June, the 29°C water is closer to the coast, and is found further up the coast. This continues into July, with the 29°C isotherm extended deep into the gulf. Also in July, the 240 W m-2 OLR isoline makes a dramatic advance northwestward, indicating the onset of the monsoon. The question can be asked, "does the advance of the 29°C isotherm play a role in initiating the monsoon?". Although the monthly time resolution is crude, there is still the suggestion that the poleward advance of warmer SSTs into the Gulf of California corresponds with the poleward advance of OLR, or tropical convection, hence suggesting a possible link between SSTs and the monsoon onset. We have found that the poleward propagation of SSTs >29°C is as regular an event as the monsoon singularity, occurring to varying extents each year in July. As discussed below, this phenomena appears to be driven by both solar insolation and a coastal current.

b. Coastal current

Considerable evidence indicating a poleward transport of relatively warm water along the mainland coast of Mexico up into the Gulf of California, during late spring and early summer, has recently been reported by Collins et al. (1997), Castro et al. (1994), Ripa (1997) and Beier (1997). Collins et al. (1997) measured currents across the entrance to the Gulf of California in April, May and December of 1992, and January of 1993. On the mainland side, flow was into the gulf, while on the Baja Peninsula side, flow was out of the gulf, during all months studied. The inflow current was weakest in December and January, becoming stronger in April (average flows up to 25 cm s-1), and strongest in May (average flows up to 35 cm s-1), with highest velocities within 100 m of the surface. A current speed of 25 cm s-1 would transport water 670 km (416 miles) up the coast over one month, which, in combination with solar insolation, is plausible for explaining the observed northward advance of warmer water in May-June in Fig. 1. The gulf axis is about 1100 km long.


Fig. 1 and Fig. 2 - combined in one color-coded image. Fig. 1. Long-term mean (1974-93) seasonal evolution of SST fields (°C) in the eastern Pacific. Color coding: red = 29°C;   orange = 28°C   and each color change represents 1°C cooling.

Fig. 2. Long-term mean (1974-1993) seasonal evolution of OLR fields (W m-2) in the eastern Pacific and monsoon region (black lines).


Perhaps the best evidence for a spring-summer warm current altering SSTs to the north is given in Castro et al. (1994), who used most of the available hydrographic data (extending to 400 m depth) and meteorological data to carry out a seasonal heat balance for the gulf. In simple terms, the gulf may gain heat at the surface from solar radiation and sensible heat flux, and gain heat horizontally through import of warmer water from the Pacific (i.e. advection). It may lose heat at the surface through evaporation, radiation, sensible heat flux, and horizontally lose heat via advection. Through constructing a heat budget for the surface and horizontal fluxes, the advection terms (longitudinal heat fluxes, or LHF) were solved for, implicating the role of currents in heat transport. From late March to early July, the surface heat flux (solar and sensible) was not nearly enough to account for the observed heating rate of the gulf waters, giving negative LHFs. A net gain of heat had to be supplied through horizontal processes (advection) to account for the observed heat contents in the gulf during that period. From August to February, LHFs were larger but opposite in sign, indicating the water columns were losing heat by horizontal transport. These larger values reflect the fact that the net "vertical" energy exchange at the surface was positive, and that this net heat gain must be exported out of the gulf through horizontal advection (along with heat advected during March-July) to explain the observed heat contents during this period.

The Castro et al. results indicate an intrusion of warmer water from the eastern Pacific warm pool occurs from mid-March through mid-July on average, heating the upper waters over the entire gulf length, over and above that which would result from solar and sensible heating. This is consistent with the recent finding (Torres-Orozco, 1993) that the amount of Tropical Surface Water (TSW) at the entrance to the gulf increases from winter to summer. Broadly in phase with this accumulation of TSW is the annual cycle of the along-gulf surface tilt, with sea levels highest in the upper gulf during summer (Roden and Groves 1959; Ripa 1997). The annual changes in sea level throughout the gulf, and the annual changes in surface-layer velocity and mean heat content through the gulf's mouth, appear primarily due to forcing by the Pacific Ocean which excites a baroclinic Kelvin wave at the mouth of the gulf (Ripa 1997; Beier 1997).

c. Wind field climatology

As noted by Hales (1972) and Douglas (1995), a low level pressure difference exists between the region near Mazatlan and the desert southwest (i.e. Tucson, Arizona) below 3 km (700 mb) during summer, the tropical air being cooler and denser. Douglas (1995) shows this pressure difference appears to support a persistent low-level jet flowing parallel to the Gulf's axis, with maximum winds up to 15 m/s about 300 m above the surface. This may facilitate the "gulf surges" of southerly wind and associated heavy summer rains in southern Arizona (Hales 1972; Brenner 1974; Stensrud 1997). Low level winds from the northwest are generally redirected out of the south or southeast as they blow over the Gulf during summer. Based on 11 years of data for July, Douglas et al. (1993) demonstrate that low level flow at 900 mb is southeasterly, emerging from south of 16°N latitude, out of the eastern Pacific warm pool, with streamlines approximately parallel to the coast of mainland Mexico. Collectively, these data show that low level monsoon moisture transport is from the southeast, with the Gulf of California and tropical eastern Pacific as potential moisture sources. However, a strong "sea-breeze" effect is superimposed on this mean flow during afternoons (e.g. Douglas 1995; Douglas and Li 1996), drawing moisture inland over the deserts and the western slopes of the Sierra Madre Occidental. This results in a strong diurnal cycle of vigorous convection and rainfall, most active during late afternoon/early evening (Gourley et al. 1998; Douglas and Li 1996).

d. Diabatic heating

As described in Barlow et al. (1999) and Higgins et al. (1998), diabatic heating over northwestern Mexico and the U.S. southwest appears responsible for the establishment of an upper-level (i.e. 200 mb) high pressure dome over this region, characterizing the N.A. monsoon. While the source contributions to this heating were not delineated in these studies, the sources themselves include solar insolation and deep convection over land. Since solar insolation is very intense during June, with deep convection generally commencing somewhat later (especially further north), solar heating to mid-levels is likely to develop first. This will set up a temperature gradient between the cool Pacific associated with the California current, and the mainland of N.W. Mexico. Moreover, the transport of tropical warm water into the gulf during Spring may facilitate this temperature gradient at low-levels (i.e. within the boundary layer), especially during nighttime when the land cools. This temperature gradient, running parallel to the gulf, should establish a thermal wind circulation at low- to mid-levels, and may account for the mean circulation described in the previous subsection. This circulation should set up in June, establishing southerly winds traveling over the warmest water, providing a moisture conduit for subsequent convection. Such behavior was observed in Douglas et al. (1993) regarding the evolution of wind fields over the central gulf. Carleton et al. (1990) noted strong monsoon years were well correlated with cooler SSTs off the southern California and northern Baja coasts, and also suggested a SST gradient/thermal wind explanation. Once deep convection begins, this temperature gradient may be intensified through latent heating, and extended to higher levels. The above rationale may explain the abrupt change in low-level winds over the gulf from N.W. to S.E. during July, as described in Douglas (1995).

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