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ENSO ENSO - - Related Related Interannual Interannual Variability of Temperature and Salinity in the Upper Tropical P Variability of Temperature and Salinity in the Upper Tropical P acific Ocean during 2005 acific Ocean during 2005 - - 2006 2006 Qiuxia Qiuxia Wu Wu @ @ and and Yonghong Yonghong Yin Yin @ @ Corresponding author address: Dr. Corresponding author address: Dr. Qiuxia Qiuxia Wu, State Key Laboratory of Severe Weather, Chinese Academy of Wu, State Key Laboratory of Severe Weather, Chinese Academy of Meteorological Sciences, No.46 South Avenue, Meteorological Sciences, No.46 South Avenue, Zhongguancun Zhongguancun , , Haidian Haidian District, Beijing 100081, District, Beijing 100081, China. Email address: China. Email address: [email protected] [email protected] MOTIVATION: MOTIVATION: 1) 1) Spatial distributions of temperature and salinity determine th Spatial distributions of temperature and salinity determine th e upper ocean thermodynamic states, which shows a corresponding e upper ocean thermodynamic states, which shows a corresponding variation associated with ENSO cycle. variation associated with ENSO cycle. 2) 2) The previous ocean observations, such as the TAO/TRITON moored The previous ocean observations, such as the TAO/TRITON moored buoy, drifting buoy, ship buoy, drifting buoy, ship - - of of - - opportunity XBT and satellites, can not provide a satisfactory c opportunity XBT and satellites, can not provide a satisfactory c overage in terms of time and space. For the first time, the Argo overage in terms of time and space. For the first time, the Argo profiling float project allows continuous profiling float project allows continuous monitoring of temperature and salinity in the upper 2000 m of th monitoring of temperature and salinity in the upper 2000 m of th e ocean in near e ocean in near - - real time (Gould et al., 2004). real time (Gould et al., 2004). 3) 3) Aims: To investigate the observed details of the 2005/2006 ENS Aims: To investigate the observed details of the 2005/2006 ENS O O - - related variation of temperature and salinity in the entire trop related variation of temperature and salinity in the entire trop ical Pacific Ocean to improve the understanding of ENSO formatio ical Pacific Ocean to improve the understanding of ENSO formatio n mechanism, with the available Argo profile datasets. n mechanism, with the available Argo profile datasets. DATA and METHOD DATA and METHOD The real The real - - time quality controlled and delayed mode temperature and salinit time quality controlled and delayed mode temperature and salinit y of Argo profiling floats. y of Argo profiling floats. ( ( ftp:// ftp:// ftp.ifremer.fr/ifremer/argo/geo/pacific_ocean ftp.ifremer.fr/ifremer/argo/geo/pacific_ocean ) ) Cubic Cubic - - spline spline functions functions (201 standard pressure levels extending from 5 to 2000 db, with (201 standard pressure levels extending from 5 to 2000 db, with vertical interval of 10 db at 10 to 2000 db and 5 db at depths s vertical interval of 10 db at 10 to 2000 db and 5 db at depths s hallower than 10 hallower than 10 db) db) Potential temperature for the estimates of ILD Potential temperature for the estimates of ILD (UNESCO1983 empirical formula ( (UNESCO1983 empirical formula ( Fofonoff Fofonoff and Millard, 1983); the equation of state for seawater of Gill and Millard, 1983); the equation of state for seawater of Gill (1982) and (1982) and Bryden Bryden (1973) ). (1973) ). The isothermal layer depth ( The isothermal layer depth ( ILD ILD ) :The depth where the potential temperature ( ) :The depth where the potential temperature ( PT PT ) is equal to the sea surface potential temperature ( ) is equal to the sea surface potential temperature ( SSPT SSPT ) ) minus 0.5 minus 0.5 ( ( Monterey and Monterey and Levitus Levitus 1997). 1997). , Where Z means the depth. , Where Z means the depth. (De Boyer Montegut et al.,2007) (De Boyer Montegut et al.,2007) Indicating the vertical motions in the Indicating the vertical motions in the thermocline thermocline . (Upward: , Dow . (Upward: , Dow nward: nward: The dynamic height ( The dynamic height ( DH DH ) refers to the pressure associated with a column of sea water, ) refers to the pressure associated with a column of sea water, defined as follows: defined as follows: Where Where p p 1 1 and and p p 2 2 are two reference pressure levels, are two reference pressure levels, δ δ is the specific volume anomaly from a standard specific volume is the specific volume anomaly from a standard specific volume determined at a salinity of determined at a salinity of 35 35 psu psu , a temperature of 0 , a temperature of 0 , , T T is the temperate, is the temperate, S S is the salinity, and is the salinity, and p p is the pressure. is the pressure. Indicating cumulative effects of the Temperature/Salinity variat Indicating cumulative effects of the Temperature/Salinity variat ions in the vertical direction. ions in the vertical direction. ) 5 . 0 ( = = SSPT PT Z ILD 0 < t ILD 0 > t ILD ILD ILD = 2 1 ) , , ( ) , ( 2 1 p p dp p S T p p DH δ Referring to vertical displacements of sea level: Referring to vertical displacements of sea level: Ascend Ascend Descend Descend 0 , 0 < > t S t T 0 , 0 > < t S t T SSTA and Argo profiles’ spatial distribution La Ni La Ni ñ ñ a a El Ni El Ni ñ ñ o o Figure 1. Figure 1. The temporal The temporal - - longitudinal section longitudinal section of SSTA along the EQ during Jan 2005 to of SSTA along the EQ during Jan 2005 to Feb 2007. (A moderate La Ni Feb 2007. (A moderate La Ni ñ ñ a reaches its a reaches its mature phase in December 2005 and then a mature phase in December 2005 and then a moderate El Ni moderate El Ni ñ ñ o develops and reaches its o develops and reaches its mature phase in December 2006 ( mature phase in December 2006 ( McPhaden McPhaden , , 2008) ) 2008) ) Figure 2. Figure 2. The spatial distribution of Argo The spatial distribution of Argo profiles in December 2005, illustrating a profiles in December 2005, illustrating a horizontal resolution of roughly 3 degree. horizontal resolution of roughly 3 degree. TEMPERATURE The major variation of temperature is trapped in the sharp The major variation of temperature is trapped in the sharp thermocline thermocline , and the greatest subsurface temperature variation is found at , and the greatest subsurface temperature variation is found at 5 5 º º S S - - 15 15 º º N, N, associated with the shoaling and sharpening of the associated with the shoaling and sharpening of the thermocline thermocline . . The vertical motions in the The vertical motions in the thermocline thermocline due to Kelvin/ due to Kelvin/ Rossby Rossby waves plays a key role in the waves plays a key role in the thermocline thermocline - - trapped temperature variation trapped temperature variation Worthwhile noting, the greatest cooling on the equatorial Paci Worthwhile noting, the greatest cooling on the equatorial Paci fic western boundary might be due to a strong upwelling (maybe fic western boundary might be due to a strong upwelling (maybe the strongest the strongest upwelling in the tropical Pacific Ocean), which need to be check upwelling in the tropical Pacific Ocean), which need to be check ed by the future works. ed by the future works. When the greatest warming occurs along the equatorial central an When the greatest warming occurs along the equatorial central an d eastern Pacific, the greatest cooling is found along the major d eastern Pacific, the greatest cooling is found along the major thermocline thermocline ridge at about 5 ridge at about 5 º º N N - - 15 15 º º N and the secondary N and the secondary thermocline thermocline ridge on the equatorial Pacific western boundary, associated wi ridge on the equatorial Pacific western boundary, associated wi th the greatest shoaling and th the greatest shoaling and sharpening of the sharpening of the thermocline thermocline . . The asymmetric distribution of the subsurface cooling with res The asymmetric distribution of the subsurface cooling with res pect to the equator could be thought to be associated with the a pect to the equator could be thought to be associated with the a symmetric shape symmetric shape of the of the thermocline thermocline ; that is, there exist the major ; that is, there exist the major thermocline thermocline ridge at about 5 ridge at about 5 º º N N - - 15 15 º º N and the secondary N and the secondary thermocline thermocline ridge on the equatorial Pacific ridge on the equatorial Pacific western boundary. western boundary. Along the Along the thermocline thermocline ridge, the greatest shoaling of the ridge, the greatest shoaling of the thermocline thermocline causes the nearest subsurface cold water to the sea surface and causes the nearest subsurface cold water to the sea surface and acts acts together with the greatest sharpening (Corresponding to the stro together with the greatest sharpening (Corresponding to the stro ngest static stability: ) to permit the ngest static stability: ) to permit the greatest response of the greatest response of the subsurface ocean to the atmospheric forcing. subsurface ocean to the atmospheric forcing. According to the subsurface ocean memory mechanisms (Wang, 200 According to the subsurface ocean memory mechanisms (Wang, 200 1; Wang and 1; Wang and Picaut Picaut , 2004), the , 2004), the thermocline thermocline ridges at about 5 ridges at about 5 º º N N - - 15 15 º º N and N and on the equatorial Pacific western boundary could be crucial regi on the equatorial Pacific western boundary could be crucial regi ons for ENSO phase transition. ons for ENSO phase transition. Figure 3. Figure 3. The zonal sections above 500db The zonal sections above 500db pressure level along 10 pressure level along 10 ° ° N (upper panel), the N (upper panel), the equator (middle panel) and 5 equator (middle panel) and 5 ° ° S (lower panel). S (lower panel). The contour represents the temperature in The contour represents the temperature in December 2006 with interval of 2 December 2006 with interval of 2 ° ° C; the C; the difference in temperature is defined by difference in temperature is defined by subtracting the temperature value in December subtracting the temperature value in December 2005 from that in December 2006, and the areas 2005 from that in December 2006, and the areas with magnitude larger than 1 with magnitude larger than 1 ° ° C are filled in C are filled in with color. Superimposed thick lines with with color. Superimposed thick lines with closed and open circle represent the isothermal closed and open circle represent the isothermal layer depth (ILD) in December 2005 and layer depth (ILD) in December 2005 and December 2006, respectively. December 2006, respectively. Figure 4. Figure 4. As in Fig. 3, except for the As in Fig. 3, except for the meridional meridional sections along 140 sections along 140 ° ° E, E, 180 180 ° ° E, 140 E, 140 ° ° W and 100 W and 100 ° ° W (From the left to the right panels). W (From the left to the right panels). Major Major Thermocline Thermocline Ridge Ridge 5 S-15 N Greatest Sharpening Greatest Sharpening Greatest Shoaling Greatest Shoaling Secondary Secondary Thermocline Thermocline Ridge Ridge Figure 5. Figure 5. The map for the variation of surface dynamic height (DH) refer The map for the variation of surface dynamic height (DH) refer red to red to 500dbar due to the temperature variation, isothermal layer depth 500dbar due to the temperature variation, isothermal layer depth (ILD) , defined by (ILD) , defined by subtracting the value in December 2005 from that in December 200 subtracting the value in December 2005 from that in December 200 6. The area with the 6. The area with the magnitude of the DH variation larger than 5 magnitude of the DH variation larger than 5 dyn dyn cm is filled in with color, and the cm is filled in with color, and the superimposed contour represents the ILD variation with the inter superimposed contour represents the ILD variation with the inter val of 10 m and the val of 10 m and the contour with magnitude smaller than 10 m is not shown. contour with magnitude smaller than 10 m is not shown. Major Major Thermocline Thermocline Ridge Ridge Secondary Secondary Thermocline Thermocline Ridge Ridge p T SALINITY SALINITY In the tropical Pacific Ocean, the salinity variation is also as In the tropical Pacific Ocean, the salinity variation is also as sociated with ENSO cycle on sociated with ENSO cycle on interannual interannual time scales. time scales. SPTW SPTW Figure 6. Figure 6. The map for the variation of the sea surface salinity (SSS), The map for the variation of the sea surface salinity (SSS), (Evaporation (Evaporation Precipitation) and the surface dynamic height (DH) Precipitation) and the surface dynamic height (DH) referred to 500 referred to 500 dbar dbar due to the salinity variation. Left: The SSS variation due to the salinity variation. Left: The SSS variation is defined by subtracting the Argo salinity value in December 20 is defined by subtracting the Argo salinity value in December 20 05 from 05 from that in December 2006, and the area with magnitude lager than 0. that in December 2006, and the area with magnitude lager than 0. 2 2 psu psu is is filled in with the shade of color. The superimposed contour repr filled in with the shade of color. The superimposed contour repr esents esents the surface DH variation with magnitude larger than 1.25 the surface DH variation with magnitude larger than 1.25 dyn dyn cm, cm, defined by subtracting the difference in the DH between December defined by subtracting the difference in the DH between December 2006 2006 and December 2005 estimated using the WOA2005 annual mean salini and December 2005 estimated using the WOA2005 annual mean salini ty ty data from that estimated using the observed Argo salinity data. data from that estimated using the observed Argo salinity data. The The superimposed thick solid (red) and dashed (green) contours respe superimposed thick solid (red) and dashed (green) contours respe ctively ctively represent 34.6 represent 34.6 psu psu in December 2005 and December 2006. Right: E in December 2005 and December 2006. Right: E - - P P field in kg/s/m field in kg/s/m 2 is obtained from the Comprehensive Ocean Atmosphere is obtained from the Comprehensive Ocean Atmosphere Data Set (COADS), and the variation of E Data Set (COADS), and the variation of E - - P is defined by subtracting the P is defined by subtracting the value in December 2005 from that in December 2006 (Positive valu value in December 2005 from that in December 2006 (Positive valu e: e: E>P; Negative value: E<P). The thick solid lines with mark 1, 2 E>P; Negative value: E<P). The thick solid lines with mark 1, 2 and 3 and 3 represent the cross sections of Figure 7, respectively. represent the cross sections of Figure 7, respectively. 2 2 1 1 N PT W N PT W 3 3 2 2 1 1 3 3 The overall distribution pattern of the surface DH variation The overall distribution pattern of the surface DH variation is similar to that of the SSS variation, indicating that the is similar to that of the SSS variation, indicating that the major variation of salinity is confined in the surface major variation of salinity is confined in the surface isothermal layer. Moreover, the greatest freshening is found in isothermal layer. Moreover, the greatest freshening is found in the surface isothermal layer over the major and secondary the surface isothermal layer over the major and secondary thermocline thermocline ridges. ridges. The SSS variation is due to the advection and the external The SSS variation is due to the advection and the external forcing terms (Evaporation forcing terms (Evaporation - - Precipitation). Precipitation). P E S V t S + = v Forcing Forcing Advection Advection On the southern flank of the high On the southern flank of the high - - salinity North Pacific salinity North Pacific Tropical Water (NPTW), the increased SSS occurs due to the Tropical Water (NPTW), the increased SSS occurs due to the southward movement of the NPTW (Shown by the southward southward movement of the NPTW (Shown by the southward displacement of the contour of 34.6 displacement of the contour of 34.6 psu psu ), and the increased ), and the increased dryness (E dryness (E - - P>0). P>0). Along the ITCZ, including the eastern edge of the western Along the ITCZ, including the eastern edge of the western Pacific warm pool (WPWP), the strong freshening, due to Pacific warm pool (WPWP), the strong freshening, due to severe rainfall (E severe rainfall (E - - P<0), is found there and causes SSS to P<0), is found there and causes SSS to decline. (Johnson et al. 2002; decline. (Johnson et al. 2002; McPhaden McPhaden , 2008) , 2008) In the southeastern part of the SPCZ, the increased SSS In the southeastern part of the SPCZ, the increased SSS occurs, due to the increased dryness (E occurs, due to the increased dryness (E - - P>0). P>0). Figure 7. Figure 7. The vertical sections of the salinity variation The vertical sections of the salinity variation above 500 db pressure level along the southern margin of above 500 db pressure level along the southern margin of the North Pacific Tropical Water (solid line 1 in Fig. 6, the North Pacific Tropical Water (solid line 1 in Fig. 6, upper left panel), the northern margin of the South Pacific upper left panel), the northern margin of the South Pacific Tropical Water (solid line 2 in Fig. 6, upper right panel), the Tropical Water (solid line 2 in Fig. 6, upper right panel), the SPCZ (solid line 3 in Fig. 6, lower left panel) and the SPCZ (solid line 3 in Fig. 6, lower left panel) and the equator (lower right panel). The area with the magnitude of equator (lower right panel). The area with the magnitude of the salinity variation larger than 0.2 the salinity variation larger than 0.2 psu psu is filled in with the is filled in with the shade of color. The superimposed contour with the interval shade of color. The superimposed contour with the interval of 1 of 1 represents the temperature variation, and the contour represents the temperature variation, and the contour with magnitude smaller than 1 with magnitude smaller than 1 is not shown. is not shown. The The temperature and salinity variations are defined by temperature and salinity variations are defined by subtracting the value in December 2005 from that in subtracting the value in December 2005 from that in December 2006, respectively. December 2006, respectively. Contrary to temperature, the major variation of Contrary to temperature, the major variation of salinity is indeed confined in the surface isothermal salinity is indeed confined in the surface isothermal layer, with the greatest freshening occurring in the layer, with the greatest freshening occurring in the surface isothermal layer over the major and surface isothermal layer over the major and secondary secondary thermocline thermocline ridge ridge The variation of subsurface salinity is trapped in The variation of subsurface salinity is trapped in the the thermocline thermocline and is synchronized with the major and is synchronized with the major variation of subsurface temperature, due to the variation of subsurface temperature, due to the vertical motions associated with the subsurface vertical motions associated with the subsurface Kelvin/ Kelvin/ Rossby Rossby waves in the waves in the thermocline thermocline . . Worthwhile noting, like a greatest Worthwhile noting, like a greatest thermocline thermocline - - trapped cooling on the equatorial Pacific western trapped cooling on the equatorial Pacific western boundary, a great boundary, a great thermocline thermocline - - trapped freshening is trapped freshening is also found there, due to a strong upwelling, maybe also found there, due to a strong upwelling, maybe the strongest upwelling in the tropical Pacific Ocean. the strongest upwelling in the tropical Pacific Ocean. CONCLUSION CONCLUSION The greatest sharpening and shoaling of The greatest sharpening and shoaling of thermocline thermocline exists in the major exists in the major thermocline thermocline ridge at 5 ridge at 5 N N - - 15 15 N and the N and the secondary secondary thermocline thermocline ridge on the equatorial Pacific western boundary. ridge on the equatorial Pacific western boundary. Due to the greatest sharpening and shoaling of Due to the greatest sharpening and shoaling of thermocline thermocline , the major and secondary , the major and secondary thermocline thermocline ridges is favorable ridges is favorable for the strong air for the strong air - - sea interaction (Hermes and Reason,2009; sea interaction (Hermes and Reason,2009; Vialard Vialard et al., 2009), indicated by the greatest et al., 2009), indicated by the greatest thermocline thermocline - - trapped cooling and the greatest surface trapped cooling and the greatest surface - - isotermal isotermal - - layer layer - - confined freshening, and could play a key role in ENSO phase confined freshening, and could play a key role in ENSO phase transition. transition. Worthwhile noting, on the equatorial Pacific western boundary, Worthwhile noting, on the equatorial Pacific western boundary, there maybe exist a strongest upwelling in the tropical there maybe exist a strongest upwelling in the tropical Pacific Ocean, which might be a deciding factor in the ENSO phas Pacific Ocean, which might be a deciding factor in the ENSO phas e transition. e transition. The future works is focused to check if the major and secondar The future works is focused to check if the major and secondar y y thermocline thermocline ridges is crucial regions for ENSO phase ridges is crucial regions for ENSO phase transition. transition. REFERENCES REFERENCES Bryden, H. L., 1973: New polynomials for thermal expansion, adia Bryden, H. L., 1973: New polynomials for thermal expansion, adia batic temperature gradient, and potential temperature batic temperature gradient, and potential temperature of sea water, of sea water, Deep Deep - - Sea Res. Sea Res. , 20, , 20, 401 401 408. 408. De Boyer De Boyer Mont Mont é é gut gut , C., J. , C., J. Mignot Mignot , A. Lazar, and S. , A. Lazar, and S. Cravatte Cravatte (2007), Control of salinity on the mixed layer depth in the (2007), Control of salinity on the mixed layer depth in the world ocean: 1. General description, world ocean: 1. General description, J. J. Geophys Geophys . Res. . Res. , , 112 112 , C06011, doi:10.1029/2006JC003953. , C06011, doi:10.1029/2006JC003953. Fofonoff, N. P., and R. C. Millard Jr., 1983: Algorithms for com Fofonoff, N. P., and R. C. Millard Jr., 1983: Algorithms for com putation of fundamental properties of seawater, putation of fundamental properties of seawater, UNESCO Tech Papers in Marine Sci. UNESCO Tech Papers in Marine Sci. , No. 44, 53 pp. , No. 44, 53 pp. Gill, A. E., 1982: Gill, A. E., 1982: Atmosphere Atmosphere - - Ocean Dynamics Ocean Dynamics , Academic Press, 662 pp. , Academic Press, 662 pp. Gould, J., et al., 2004: Argo profiling floats bring new era of Gould, J., et al., 2004: Argo profiling floats bring new era of in situ ocean observations, in situ ocean observations, Eos Trans Eos Trans , , AGU AGU , 85(19), , 85(19), doi:10.1029/2004EO190002. doi:10.1029/2004EO190002. Hermes, J. C., and Reason, C. J. C. 2009. The sensitivity of the Hermes, J. C., and Reason, C. J. C. 2009. The sensitivity of the Seychelles Seychelles Chagos Chagos thermocline thermocline ridge to large ridge to large - - scale wind scale wind anomalies. anomalies. ICES Journal of Marine Science, 66: 000 ICES Journal of Marine Science, 66: 000 000 000 . . Johnson G. C., B. M. Sloyan, W. S. Kessler, and K. E. McTaggart, Johnson G. C., B. M. Sloyan, W. S. Kessler, and K. E. McTaggart, 2002: Direct measurements of upper ocean currents 2002: Direct measurements of upper ocean currents and water properties across the tropical Pacific Ocean during th and water properties across the tropical Pacific Ocean during th e 1990's, e 1990's, Progress in Oceanography Progress in Oceanography , 52(1), 31 , 52(1), 31 61. 61. McPhaden McPhaden , M. J., 2008: Evolution of 2006 , M. J., 2008: Evolution of 2006 - - 2007 El Ni 2007 El Ni ñ ñ o: the role of o: the role of introseasonal introseasonal to to interannual interannual time scale dynamics, time scale dynamics, Adv. Adv. Geosci Geosci . . , 14, 219 , 14, 219 - - 230. 230. Monterey, G., and S. Monterey, G., and S. Levitus Levitus , 1997: , 1997: Seasonal Variability of Mixed Layer Depth for the World Ocean Seasonal Variability of Mixed Layer Depth for the World Ocean , NOAA Atlas , NOAA Atlas NESDIS 14, U.S. Gov. Printing Office, Wash., D.C., 96 pp. 87 fig NESDIS 14, U.S. Gov. Printing Office, Wash., D.C., 96 pp. 87 fig s. s. Vialard Vialard , J., and Coauthors, 2009: , J., and Coauthors, 2009: Cirene Cirene : Air : Air Sea Interactions in the Seychelles Sea Interactions in the Seychelles Chagos Chagos Thermocline Thermocline Ridge Region. Ridge Region. Bull. Amer. Meteor. Soc. Bull. Amer. Meteor. Soc. , 90, 45 , 90, 45 61. 61. Wang, C., 2001: A unified oscillator model for the El Ni Wang, C., 2001: A unified oscillator model for the El Ni ñ ñ o o - - Southern Oscillation, Southern Oscillation, J. Climate J. Climate , , 14, 98 14, 98 - - 115. 115. Wang, C., and J. Picaut, 2004: Understanding ENSO physics Wang, C., and J. Picaut, 2004: Understanding ENSO physics A review, in A review, in Earth Earth s Climate: The Ocean s Climate: The Ocean - - Atmosphere Atmosphere Interaction Interaction , Geophysical Monograph Series, Volume 147, edited by C. Wang, S , Geophysical Monograph Series, Volume 147, edited by C. Wang, S . . - - P. Xie, and J. A. Carton, pp. 21 P. Xie, and J. A. Carton, pp. 21 - - 48, 48, AGU, Washington, D.C. AGU, Washington, D.C.

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Page 1: ENSO-Related Interannual Variability of Temperature and ...Feb 2007. (A moderate La NiFeb 2007. (A moderate La Niñña reaches its a reaches its mature phase in December 2005 and then

ENSOENSO--Related Related InterannualInterannual Variability of Temperature and Salinity in the Upper Tropical PVariability of Temperature and Salinity in the Upper Tropical Pacific Ocean during 2005acific Ocean during 2005--20062006QiuxiaQiuxia WuWu@@ and and YonghongYonghong Yin Yin

@@Corresponding author address: Dr. Corresponding author address: Dr. QiuxiaQiuxia Wu, State Key Laboratory of Severe Weather, Chinese Academy of Wu, State Key Laboratory of Severe Weather, Chinese Academy of Meteorological Sciences, No.46 South Avenue, Meteorological Sciences, No.46 South Avenue, ZhongguancunZhongguancun, , HaidianHaidian District, Beijing 100081, District, Beijing 100081, China. Email address: China. Email address: [email protected]@gmail.comMOTIVATION:MOTIVATION:

1)1) Spatial distributions of temperature and salinity determine thSpatial distributions of temperature and salinity determine the upper ocean thermodynamic states, which shows a corresponding e upper ocean thermodynamic states, which shows a corresponding variation associated with ENSO cycle. variation associated with ENSO cycle. 2)2) The previous ocean observations, such as the TAO/TRITON mooredThe previous ocean observations, such as the TAO/TRITON moored buoy, drifting buoy, shipbuoy, drifting buoy, ship--ofof--opportunity XBT and satellites, can not provide a satisfactory copportunity XBT and satellites, can not provide a satisfactory coverage in terms of time and space. For the first time, the Argooverage in terms of time and space. For the first time, the Argo profiling float project allows continuous profiling float project allows continuous

monitoring of temperature and salinity in the upper 2000 m of thmonitoring of temperature and salinity in the upper 2000 m of the ocean in neare ocean in near--real time (Gould et al., 2004).real time (Gould et al., 2004).3)3) Aims: To investigate the observed details of the 2005/2006 ENSAims: To investigate the observed details of the 2005/2006 ENSOO--related variation of temperature and salinity in the entire troprelated variation of temperature and salinity in the entire tropical Pacific Ocean to improve the understanding of ENSO formatioical Pacific Ocean to improve the understanding of ENSO formation mechanism, with the available Argo profile datasets. n mechanism, with the available Argo profile datasets.

DATA and METHODDATA and METHODThe realThe real--time quality controlled and delayed mode temperature and salinittime quality controlled and delayed mode temperature and salinity of Argo profiling floats.y of Argo profiling floats.((ftp://ftp://ftp.ifremer.fr/ifremer/argo/geo/pacific_oceanftp.ifremer.fr/ifremer/argo/geo/pacific_ocean))CubicCubic--splinespline functionsfunctions(201 standard pressure levels extending from 5 to 2000 db, with (201 standard pressure levels extending from 5 to 2000 db, with vertical interval of 10 db at 10 to 2000 db and 5 db at depths svertical interval of 10 db at 10 to 2000 db and 5 db at depths shallower than 10 hallower than 10 db)db)Potential temperature for the estimates of ILDPotential temperature for the estimates of ILD(UNESCO1983 empirical formula ((UNESCO1983 empirical formula (FofonoffFofonoff and Millard, 1983); the equation of state for seawater of Gill and Millard, 1983); the equation of state for seawater of Gill (1982) and (1982) and BrydenBryden (1973) ).(1973) ).The isothermal layer depth (The isothermal layer depth (ILDILD) :The depth where the potential temperature () :The depth where the potential temperature (PTPT) is equal to the sea surface potential temperature () is equal to the sea surface potential temperature (SSPTSSPT) )

minus 0.5minus 0.5℃℃ ((Monterey and Monterey and LevitusLevitus 1997).1997).

, Where Z means the depth. , Where Z means the depth. (De Boyer Montegut et al.,2007) (De Boyer Montegut et al.,2007)

Indicating the vertical motions in the Indicating the vertical motions in the thermoclinethermocline. (Upward: , Dow. (Upward: , Downward: )nward: )

The dynamic height (The dynamic height (DHDH) refers to the pressure associated with a column of sea water, ) refers to the pressure associated with a column of sea water, defined as follows:defined as follows:

Where Where pp11 and and pp22 are two reference pressure levels, are two reference pressure levels, δδ is the specific volume anomaly from a standard specific volume is the specific volume anomaly from a standard specific volume determined at a salinity of determined at a salinity of 35 35 psupsu, a temperature of 0, a temperature of 0℃℃, , TT is the temperate, is the temperate, SS is the salinity, and is the salinity, and pp is the pressure.is the pressure.

Indicating cumulative effects of the Temperature/Salinity variatIndicating cumulative effects of the Temperature/Salinity variations in the vertical direction.ions in the vertical direction.

)5.0( −== SSPTPTZILD

0<∂∂

tILD 0>

∂∂

tILD

ILDILD

∫=2

1

),,(),( 21

p

pdppSTppDH δ

Referring to vertical displacements of sea level:Referring to vertical displacements of sea level:AscendAscend

DescendDescend

0,0 <∂∂>

∂∂

tS

tT

0,0 >∂∂<

∂∂

tS

tT

SSTA and Argo profiles’ spatial distribution

La NiLa Niññaa

El NiEl Niññoo

Figure 1.Figure 1. The temporalThe temporal--longitudinal section longitudinal section of SSTA along the EQ during Jan 2005 to of SSTA along the EQ during Jan 2005 to Feb 2007. (A moderate La NiFeb 2007. (A moderate La Niñña reaches its a reaches its mature phase in December 2005 and then a mature phase in December 2005 and then a moderate El Nimoderate El Niñño develops and reaches its o develops and reaches its mature phase in December 2006 (mature phase in December 2006 (McPhadenMcPhaden, , 2008) )2008) )

Figure 2.Figure 2. The spatial distribution of Argo The spatial distribution of Argo profiles in December 2005, illustrating a profiles in December 2005, illustrating a horizontal resolution of roughly 3 degree.horizontal resolution of roughly 3 degree.

TEMPERATURE

The major variation of temperature is trapped in the sharp The major variation of temperature is trapped in the sharp thermoclinethermocline, and the greatest subsurface temperature variation is found at , and the greatest subsurface temperature variation is found at 55ººSS--1515ººN, N, associated with the shoaling and sharpening of the associated with the shoaling and sharpening of the thermoclinethermocline. .

The vertical motions in the The vertical motions in the thermoclinethermocline due to Kelvin/due to Kelvin/RossbyRossby waves plays a key role in the waves plays a key role in the thermoclinethermocline--trapped temperature variationtrapped temperature variationWorthwhile noting, the greatest cooling on the equatorial PaciWorthwhile noting, the greatest cooling on the equatorial Pacific western boundary might be due to a strong upwelling (maybe fic western boundary might be due to a strong upwelling (maybe the strongest the strongest

upwelling in the tropical Pacific Ocean), which need to be checkupwelling in the tropical Pacific Ocean), which need to be checked by the future works.ed by the future works.

When the greatest warming occurs along the equatorial central anWhen the greatest warming occurs along the equatorial central and eastern Pacific, the greatest cooling is found along the majord eastern Pacific, the greatest cooling is found along the major thermoclinethermoclineridge at about 5ridge at about 5ººNN--1515ººN and the secondary N and the secondary thermoclinethermocline ridge on the equatorial Pacific western boundary, associated wiridge on the equatorial Pacific western boundary, associated with the greatest shoaling and th the greatest shoaling and sharpening of the sharpening of the thermoclinethermocline..

The asymmetric distribution of the subsurface cooling with resThe asymmetric distribution of the subsurface cooling with respect to the equator could be thought to be associated with the apect to the equator could be thought to be associated with the asymmetric shape symmetric shape of the of the thermoclinethermocline; that is, there exist the major ; that is, there exist the major thermoclinethermocline ridge at about 5ridge at about 5ººNN--1515ººN and the secondary N and the secondary thermoclinethermocline ridge on the equatorial Pacific ridge on the equatorial Pacific western boundary.western boundary.

Along the Along the thermoclinethermocline ridge, the greatest shoaling of the ridge, the greatest shoaling of the thermoclinethermocline causes the nearest subsurface cold water to the sea surface andcauses the nearest subsurface cold water to the sea surface and acts acts together with the greatest sharpening (Corresponding to the strotogether with the greatest sharpening (Corresponding to the strongest static stability: ) to permit the ngest static stability: ) to permit the greatest response of the greatest response of the subsurface ocean to the atmospheric forcing.subsurface ocean to the atmospheric forcing.

According to the subsurface ocean memory mechanisms (Wang, 200According to the subsurface ocean memory mechanisms (Wang, 2001; Wang and 1; Wang and PicautPicaut, 2004), the , 2004), the thermoclinethermocline ridges at about 5ridges at about 5ººNN--1515ººN and N and on the equatorial Pacific western boundary could be crucial region the equatorial Pacific western boundary could be crucial regions for ENSO phase transition.ons for ENSO phase transition.

Figure 3. Figure 3. The zonal sections above 500db The zonal sections above 500db pressure level along 10pressure level along 10°°N (upper panel), the N (upper panel), the equator (middle panel) and 5equator (middle panel) and 5°°S (lower panel). S (lower panel). The contour represents the temperature in The contour represents the temperature in December 2006 with interval of 2December 2006 with interval of 2°°C; the C; the difference in temperature is defined by difference in temperature is defined by subtracting the temperature value in December subtracting the temperature value in December 2005 from that in December 2006, and the areas 2005 from that in December 2006, and the areas with magnitude larger than 1with magnitude larger than 1°°C are filled in C are filled in with color. Superimposed thick lines with with color. Superimposed thick lines with closed and open circle represent the isothermal closed and open circle represent the isothermal layer depth (ILD) in December 2005 and layer depth (ILD) in December 2005 and December 2006, respectively. December 2006, respectively. Figure 4.Figure 4. As in Fig. 3, except for the As in Fig. 3, except for the meridionalmeridional sections along 140sections along 140°°E, E,

180180°°E, 140E, 140°°W and 100W and 100°°W (From the left to the right panels). W (From the left to the right panels).

Major Major ThermoclineThermoclineRidgeRidge

5◦S-15◦N

Greatest SharpeningGreatest Sharpening

Greatest ShoalingGreatest ShoalingSecondary Secondary ThermoclineThermocline RidgeRidge

Figure 5.Figure 5. The map for the variation of surface dynamic height (DH) referThe map for the variation of surface dynamic height (DH) referred to red to 500dbar due to the temperature variation, isothermal layer depth500dbar due to the temperature variation, isothermal layer depth (ILD) , defined by (ILD) , defined by subtracting the value in December 2005 from that in December 200subtracting the value in December 2005 from that in December 2006. The area with the 6. The area with the magnitude of the DH variation larger than 5 magnitude of the DH variation larger than 5 dyndyn cm is filled in with color, and the cm is filled in with color, and the superimposed contour represents the ILD variation with the intersuperimposed contour represents the ILD variation with the interval of 10 m and the val of 10 m and the contour with magnitude smaller than 10 m is not shown.contour with magnitude smaller than 10 m is not shown.

Major Major ThermoclineThermocline RidgeRidgeSecondary Secondary

ThermoclineThermocline RidgeRidge

pT ∂∂−

SALINITYSALINITYIn the tropical Pacific Ocean, the salinity variation is also asIn the tropical Pacific Ocean, the salinity variation is also associated with ENSO cycle on sociated with ENSO cycle on interannualinterannual time scales.time scales.

SPTWSPTW

Figure 6.Figure 6. The map for the variation of the sea surface salinity (SSS), The map for the variation of the sea surface salinity (SSS), (Evaporation (Evaporation –– Precipitation) and the surface dynamic height (DH) Precipitation) and the surface dynamic height (DH) referred to 500 referred to 500 dbardbar due to the salinity variation. Left: The SSS variation due to the salinity variation. Left: The SSS variation is defined by subtracting the Argo salinity value in December 20is defined by subtracting the Argo salinity value in December 2005 from 05 from that in December 2006, and the area with magnitude lager than 0.that in December 2006, and the area with magnitude lager than 0.2 2 psupsu is is filled in with the shade of color. The superimposed contour reprfilled in with the shade of color. The superimposed contour represents esents the surface DH variation with magnitude larger than 1.25 the surface DH variation with magnitude larger than 1.25 dyndyn cm, cm, defined by subtracting the difference in the DH between Decemberdefined by subtracting the difference in the DH between December 2006 2006 and December 2005 estimated using the WOA2005 annual mean saliniand December 2005 estimated using the WOA2005 annual mean salinity ty data from that estimated using the observed Argo salinity data. data from that estimated using the observed Argo salinity data. The The superimposed thick solid (red) and dashed (green) contours respesuperimposed thick solid (red) and dashed (green) contours respectively ctively represent 34.6 represent 34.6 psupsu in December 2005 and December 2006. Right: Ein December 2005 and December 2006. Right: E--P P field in kg/s/mfield in kg/s/m22 is obtained from the Comprehensive Ocean Atmosphere is obtained from the Comprehensive Ocean Atmosphere Data Set (COADS), and the variation of EData Set (COADS), and the variation of E--P is defined by subtracting the P is defined by subtracting the value in December 2005 from that in December 2006 (Positive valuvalue in December 2005 from that in December 2006 (Positive value: e: E>P; Negative value: E<P). The thick solid lines with mark 1, 2 E>P; Negative value: E<P). The thick solid lines with mark 1, 2 and 3 and 3 represent the cross sections of Figure 7, respectively.represent the cross sections of Figure 7, respectively.

2211NPTWNPTW

33

2211

33

The overall distribution pattern of the surface DH variation The overall distribution pattern of the surface DH variation is similar to that of the SSS variation, indicating that the is similar to that of the SSS variation, indicating that the major variation of salinity is confined in the surface major variation of salinity is confined in the surface isothermal layer. Moreover, the greatest freshening is found in isothermal layer. Moreover, the greatest freshening is found in the surface isothermal layer over the major and secondary the surface isothermal layer over the major and secondary thermoclinethermocline ridges.ridges.

The SSS variation is due to the advection and the external The SSS variation is due to the advection and the external forcing terms (Evaporation forcing terms (Evaporation -- Precipitation).Precipitation).

PESVtS

−+∇•−=∂∂ v

ForcingForcingAdvectionAdvectionOn the southern flank of the highOn the southern flank of the high--salinity North Pacific salinity North Pacific

Tropical Water (NPTW), the increased SSS occurs due to the Tropical Water (NPTW), the increased SSS occurs due to the southward movement of the NPTW (Shown by the southward southward movement of the NPTW (Shown by the southward displacement of the contour of 34.6 displacement of the contour of 34.6 psupsu), and the increased ), and the increased dryness (Edryness (E--P>0).P>0).

Along the ITCZ, including the eastern edge of the western Along the ITCZ, including the eastern edge of the western Pacific warm pool (WPWP), the strong freshening, due to Pacific warm pool (WPWP), the strong freshening, due to severe rainfall (Esevere rainfall (E--P<0), is found there and causes SSS to P<0), is found there and causes SSS to decline. (Johnson et al. 2002; decline. (Johnson et al. 2002; McPhadenMcPhaden, 2008), 2008)

In the southeastern part of the SPCZ, the increased SSS In the southeastern part of the SPCZ, the increased SSS occurs, due to the increased dryness (Eoccurs, due to the increased dryness (E--P>0).P>0).

Figure 7. Figure 7. The vertical sections of the salinity variation The vertical sections of the salinity variation above 500 db pressure level along the southern margin of above 500 db pressure level along the southern margin of the North Pacific Tropical Water (solid line 1 in Fig. 6, the North Pacific Tropical Water (solid line 1 in Fig. 6, upper left panel), the northern margin of the South Pacific upper left panel), the northern margin of the South Pacific Tropical Water (solid line 2 in Fig. 6, upper right panel), the Tropical Water (solid line 2 in Fig. 6, upper right panel), the SPCZ (solid line 3 in Fig. 6, lower left panel) and the SPCZ (solid line 3 in Fig. 6, lower left panel) and the equator (lower right panel). The area with the magnitude of equator (lower right panel). The area with the magnitude of the salinity variation larger than 0.2 the salinity variation larger than 0.2 psupsu is filled in with the is filled in with the shade of color. The superimposed contour with the interval shade of color. The superimposed contour with the interval of 1 of 1 ℃℃ represents the temperature variation, and the contour represents the temperature variation, and the contour with magnitude smaller than 1 with magnitude smaller than 1 ℃℃ is not shown.is not shown. The The temperature and salinity variations are defined by temperature and salinity variations are defined by subtracting the value in December 2005 from that in subtracting the value in December 2005 from that in December 2006, respectively.December 2006, respectively.

Contrary to temperature, the major variation of Contrary to temperature, the major variation of salinity is indeed confined in the surface isothermal salinity is indeed confined in the surface isothermal layer, with the greatest freshening occurring in the layer, with the greatest freshening occurring in the surface isothermal layer over the major and surface isothermal layer over the major and secondary secondary thermoclinethermocline ridgeridge

The variation of subsurface salinity is trapped in The variation of subsurface salinity is trapped in the the thermoclinethermocline and is synchronized with the major and is synchronized with the major variation of subsurface temperature, due to the variation of subsurface temperature, due to the vertical motions associated with the subsurface vertical motions associated with the subsurface Kelvin/Kelvin/RossbyRossby waves in the waves in the thermoclinethermocline..

Worthwhile noting, like a greatest Worthwhile noting, like a greatest thermoclinethermocline--trapped cooling on the equatorial Pacific western trapped cooling on the equatorial Pacific western boundary, a great boundary, a great thermoclinethermocline--trapped freshening is trapped freshening is also found there, due to a strong upwelling, maybe also found there, due to a strong upwelling, maybe the strongest upwelling in the tropical Pacific Ocean.the strongest upwelling in the tropical Pacific Ocean.

CONCLUSIONCONCLUSIONThe greatest sharpening and shoaling of The greatest sharpening and shoaling of thermoclinethermocline exists in the major exists in the major thermoclinethermocline ridge at 5ridge at 5◦◦NN--1515◦◦N and the N and the

secondary secondary thermoclinethermocline ridge on the equatorial Pacific western boundary.ridge on the equatorial Pacific western boundary.Due to the greatest sharpening and shoaling of Due to the greatest sharpening and shoaling of thermoclinethermocline, the major and secondary , the major and secondary thermoclinethermocline ridges is favorable ridges is favorable

for the strong airfor the strong air--sea interaction (Hermes and Reason,2009; sea interaction (Hermes and Reason,2009; VialardVialard et al., 2009), indicated by the greatest et al., 2009), indicated by the greatest thermoclinethermocline--trapped cooling and the greatest surfacetrapped cooling and the greatest surface--isotermalisotermal--layerlayer--confined freshening, and could play a key role in ENSO phase confined freshening, and could play a key role in ENSO phase transition. transition.

Worthwhile noting, on the equatorial Pacific western boundary,Worthwhile noting, on the equatorial Pacific western boundary, there maybe exist a strongest upwelling in the tropical there maybe exist a strongest upwelling in the tropical Pacific Ocean, which might be a deciding factor in the ENSO phasPacific Ocean, which might be a deciding factor in the ENSO phase transition.e transition.

The future works is focused to check if the major and secondarThe future works is focused to check if the major and secondary y thermoclinethermocline ridges is crucial regions for ENSO phase ridges is crucial regions for ENSO phase transition.transition.

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