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Observations of Warm Water Volume Changes in the Equatorial Pacific and Their Relationship to El Niño and La Niña

C. S. Meinen1 and M. J. McPhaden2

1Joint Institute for the Study of the Atmosphere and Ocean, University of Washington, Seattle, Washington
2Pacific Marine Environmental Laboratory, National Oceanic and Atmospheric Administration, Seattle, Washington, 98115

Journal of Climate, 13(20), 3551–3559 (2000).
Copyright ©2000 by the American Meteorological Society. Further electronic distribution is not allowed.

Gallery of Figures

Figure 1

FIG. 1. Idealized schematic of the El Niño-La Niña oscillation (modified from Jin 1997a). All quantities shown are anomalies relative to the climatological mean. Depth anomaly is relative to the time mean structure along the equator. Dashed line indicates zero anomaly; shallow anomalies are above the dashed line and deep anomalies are below the dashed line. Thin arrows and symbol a represent the anomalous zonal wind stress; bold thick arrows represent the corresponding anomalous Sverdrup transports. SSTa is the sea surface temperature anomaly. Oscillation progresses clockwise around the panels following the roman numerals; panel I represents El Niño conditions, panel III indicates La Niña conditions.

Figure 2

FIG. 2. (a) Temporal mean and (b) standard deviation about the mean seasonal cycle of Z20 over the interval Jan 1980-May 1999. Contour values are in meters. Shaded areas represent land.

Figure 3

FIG. 3. First two empirical orthogonal functions (EOFs) fit to Z20. Upper panels denote spatial structure of the modes with contours (m); bold contour denotes zero. Shaded areas represent land. Lower panel shows mode amplitudes, which are nondimensional, as a function of time.

Figure 4

FIG. 4. Bold lines indicate, from top to bottom, Niño-3 SST in units of °C; the zonal wind stress averaged across the Pacific within 5°S-5°N in units of 10-2 N m-2; WWV determined from the Z20 anomaly about the zonal average Z20 integrated over the basin west of 155°W (VW), in units of 1014 m3; the warm water anomaly integrated over the basin east of 155°W (VE) (1014 m3), the total warm water volume west of 155°W (VW) (1014 m3), the total WWV basinwide within 5°S-5°N (1014 m3); and the observed rate of change of WWV [d(WWV)/dt] (Sv). Dashed lines are the Niño-3 SST repeated alongside each of the other time series to illustrate the phasing relationships between the different quantities.

Figure 5

FIG. 5. Lagged cross correlations between the Niño-3 SST anomaly and either the WWV (bold line) or the WWV "tilting" mode integrated west of 155°W ( VW, thin line). Correlations are for Niño-3 SST lagging both WWV quantities. Peak correlation with WWV occurs at 7 months with a peak value of r = 0.70, the correlation with VW peaks at 15 months with r = 0.57.

Figure 6

FIG. 6. Phase ellipses detailing the relationship between the Niño-3 SST and the main thermocline depth, and hence WWV, west of 155°W within 5°S-5°N: (a) relates Niño-3 SST to the total WWV west of 155°W (VW), (b) shows the relationship between SST and the WWV west of 155°W calculated after the zonal average Z20 is removed (VW), (c) shows the relationship between the SST and WWV. All quantities have been normalized by removing the mean seasonal cycle and dividing by the interannual standard deviation. Dots denote each monthly value, triangles denote the end of the time series.

Figure 7

FIG. 7. Comparison of Niño-3 SST and WWV anomalies. Both time series have been seasonally averaged (i.e., Jan-Mar, Apr-Jun, etc.) to reduce the scatter. SST time series has been shifted backward by 7 months to maximize the cross correlation between WWV and SST. Lines represent least square fits to the values, separated into seasons with a negative WWV anomaly and those with a positive WWV anomaly. Slopes of the fitted lines are 0.32°C (1014 m3)-1 and 1.29°C (1014 m3)-1 for the negative and positive sides, respectively.


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