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15 MAY 2007 S T E P HENS ET AL. 2191 Differences in Atmospheric Circulation between the Development of Weak and Strong Warm Events in the Southern Oscillation DAVID J. STEPHENS AND MICHAEL J. MEULENERS Department of Agriculture and Food WA, South Perth, Western Australia, Australia HARRY VAN LOON Colorado Research Associates/Northwest Research Associates, Boulder, Colorado MALCOLM H. LAMOND Lamond Weather Services, Karrinyup, Western Australia, Australia NICOLA P. TELCIK Yarra Valley Water, Mitcham, Victoria, Australia (Manuscript received 5 October 2005, in final form 7 September 2006) ABSTRACT In this study temporal and spatial aspects of El Niño (warm event) development are explored by com- paring composite sequences of sea level pressure (SLP), surface wind, and sea surface temperature (SST) anomalies leading into strong and weak events. El Niño strength is found to be related to the magnitude and spatial extent of large-scale SLP anomalies that move in a low-frequency mode. In association with this, it is also intricately linked to the amplitude and wavelength of the Rossby waves in the southern midlatitudes. The primary signature of the Southern Oscillation is a more pronounced standing wave of pressure anoma- lies between southeastern Australia and the central South Pacific leading into stronger events. A strong reversal in the strength of the annual cycle between these two regions causes a stronger (weaker) SLP gradient that drives southwesterly (northwesterly) wind stress forcing toward (away from) the western equatorial Pacific in austral winter–spring of year 0 (Ϫ1). Thus, pressure variations in the southwest Pacific preconditions the equatorial environment to a particular phase of ENSO and establishes the setting for greater tropical–extratropical interactions to occur in stronger events. Maximum warming in the Niño-3 region occurs between April and July (0) when a strong South Pacific trough most influences the trade winds at both ends of the Pacific. Cool SST anomalies that form to the east of high pressure anomalies over Indo–Australia assist an eastward propogation of high pressure into the Pacific midlatitudes and the demise of El Niño. Strong events have a more pronounced eastward propo- gation of SST and SLP anomalies and a much more noticeable enhancement of winter hemisphere Rossby waves from May–July (Ϫ1) to November–January (ϩ1). Weak events require an enhanced South Pacific trough to develop but have much less support from the North Pacific. They also appear more variable in their development and more difficult to predict with lead time. 1. Introduction ability (Latif et al. 1998; Fedorov and Philander 2000). However, the failure of operational forecasting models Recent theories and models of ENSO development to predict the rapid development, intensity, and abrupt have centered on equatorial ocean–atmosphere cou- termination of the intense 1997/98 El Niño (Ander- pling as sole explanators of Southern Oscillation vari- son and Davey 1998; Trenberth 1998; Barnston et al. 1999; Landsea and Knaff 2000) challenged this as- sumption. Subsequent analysis of the event provided Corresponding author address: Dr. David Stephens, Climate Risks and Opportunities Project, Dept. of Agriculture and Food support for the two main theories of the Southern Os- WA, Locked Bag No. 4, Bentley DC WA 6983, Australia. cillation. E-mail: [email protected] First, the Southern Osillation can be explained as a DOI: 10.1175/JCLI4131.1 © 2007 American Meteorological Society Unauthenticated | Downloaded 10/07/21 04:00 PM UTC JCLI4131 2192 JOURNAL OF CLIMATE VOLUME 20 weakly damped oscillator that needs to be triggered by Of critical importance to ENSO dynamics is the in- a random disturbance. Westerly wind bursts in the ference by van Loon (1984) that the quasi-permanent western equatorial Pacific appear necessary at the onset South Pacific trough in the surface westerlies weakens of El Niño as they are associated with 1) an eastward both the South Pacific high and associated trades dur- shift of warm water and convection, and 2) the genera- ing the important months between May, June, and July tion of oceanic Kelvin waves that warm the central and (MJJ, hereafter 3-month periods are denoted by the eastern Pacific through zonal advection and displace- first letter of each respective month). At this time, the ment of the thermocline. The timing and amplitude of trough and subtropical jet stream reach their farthest 1997 warming was attributed to exceptionally strong northward extent as part of the semiannual oscillation westerly wind events/Madden–Julian oscillation (MJO) (SAO) in trough positioning and intensity (van Loon activity, strong downwelling kelvin waves (McPhaden 1967; van Loon 1972; Hurrell et al. 1998). Over the year and Yu 1999; Picaut et al. 2002; Lengaigne et al. 2003), leading into El Niño, the South Pacific trough changes and a buildup of upper-ocean heat early in the year from a weakened to an enhanced state, that is, takes on (Meinen and McPhaden 2000; Sun 2003). MJO activity a more permanent feature (van Loon 1984). Associated was also proposed as a “triggering mechanism” that with this is a west-to-east pressure anomaly reversal or accelerated the ending of the event (Takayabu et al. “seesaw” in the southern midlatitudes (Berlage 1966; 1999; Straub et al. 2006). van Loon and Shea 1985, 1987) and other important However, the influence of the MJO on ENSO re- wind and SST anomalies (Trenberth 1976; Rasmusson mains a controversial topic (McPhaden 2004) as periods and Carpenter 1982; Harrison 1984; Harrison and Lar- of enhanced westerlies and MJO activity do not always kin 1996, 1998). Figure 1 sumarizes this process, which lead to El Niño (Chen and Wu 2000; Bergman et al. we shall call the “van Loon hypothesis.” 2001; Zhang and Gottschalck 2002; Jones et al. 2004; In austral winter/spring in the year before El Niño Levinson 2005). Of the 13 strongest MJO events since (year Ϫ1), the annual cycle is weak in the southern 1979, only the two events late in 1996 and early 1997 midlatitudes, with a strong trough pattern over the re- actually preceded an El Niño (Jones et al. 2004). Slingo gion of the Australian subtropical high, and a weak et al. (1999) found that the statistical relationship be- trough in the South Pacific (Fig. 1a). Northerly wind tween ENSO and MJO indices do not show that they anomalies between these two regions warm the Coral are causally related, and Bergman et al. (2001) specu- Sea and the southwest edge of the South Pacific con- lated that the MJO might be relevant to the timing and vergence zone (SPCZ) as it expands south in austral initial growth of El Niño rather than be responsible for spring (Ϫ1). Increased convection and lower pressures the event. over this warm water then coincide with anomalous Second, the Southern Oscillation can be viewed as a westerlies on the equatorward side of the northern lower-frequency self-sustaining mode of oscillation in SPCZ (Rasmusson and Carpenter 1982; Von Storch et the the tropical Pacific (Chen et al. 2004). Wang and al. 1988). At the southern end of the SPCZ, negative Weisberg (2000) found that off-equatorial SST and as- pressure anomalies continue to form over warm water sociated pressure anomalies in the subtropics played an and this is associated with an equatorward reposition- important role in the development and decay of the ing of the surface trough into the South Pacific (van 1997/98 El Niño. However, what went unnoticed was a Loon and Shea 1985; Fig. 1b). This whole process is major seesaw in pressure in the southern midlatitudes linked to the convective maximum in the annual cycle (van Loon and Shea 1985, 1987), and a large-scale gradually moving from southeast Asia into the Austra- propagating SLP signal noted in previous El Niño lian monsoon region (austral summer), and onto the events (Barnett 1985; Krishnamurti et al. 1986). southern end of the SPCZ (austral autumn; Meehl When Bjerknes (1966, 1969) linked maximum oce- 1987). anic warming in the eastern equatorial Pacific (El Niño) By austral winter in the El Niño year (year 0) the to the “Southern Oscillation” in pressure, the primary annual cycle is enhanced in the southern midlatitudes. cause for these events was attributed to an anomalous Stronger highs occur over Australia, and negative SLP weakening of the trade winds of the Southern Hemi- and upper-level height anomalies become established sphere and associated oceanic upwelling (Bjerknes in the central South Pacific along with an equatorward 1969). Since the South Pacific high dominates the equa- movement in the subtropical jet (Karoly 1989; Kiladis torial flow in the central and eastern Pacific to 10°N, and Mo 1998). The first result of this pattern is strong Bjerknes (1966) speculated that reasons for this warm- southerly wind anomalies to the east of an enhanced ing must be sought south of the equator. Australian high pressure. These southerlies converge Unauthenticated | Downloaded 10/07/21 04:00 PM UTC 15 MAY 2007 S T E P HENS ET AL. 2193 FIG. 1. Schematic diagram showing major weather systems and anomalies in the Southern Hemisphere in winter–spring in (a) the year before El Niño [year (Ϫ1)] and (b) during El Niño [year (0)]. The Walker Circulation (white) and westerly surface troughs (red curve) sit above surface anomalies measured at key stations represented by crosses [Alice Springs (A), Darwin (D), Easter Island (E), Mildura (M), Noumea (N), Rapa Island (R), Tahiti (T), Willis Island (W)]. The SPCZ is represented by parallel gray lines. Warm (red) and cold (green) SST anomalies are indicated, as are wind anomalies (black arrows). High and low SLP are indi- cated by “H” and “L” and anomalous pressures in the midlatitudes are dashed. with and intensify westerly wind anomalies in the equa- 2004; Thompson and Lorenz 2004; Anderson and Ma- torial western Pacific and appear to play a determining loney 2006).