Influence of mechanical mixing on a low summertime SST in the western North Pacific ITCZ region

Similar documents
An ITCZ-like convergence zone over the Indian Ocean in boreal late autumn

The Air-Sea Interaction. Masanori Konda Kyoto University

Review for the second quarter. Mechanisms for cloud formation

ATMS 310 Tropical Dynamics

Lecture 14. Heat lows and the TCZ

Chapter 6: Atmospheric Pressure, Wind, and Global Circulation

Satellite observations of intense intraseasonal cooling events in the tropical south Indian Ocean

Variability in the tropical oceans - Monitoring and prediction of El Niño and La Niña -

RECTIFICATION OF THE MADDEN-JULIAN OSCILLATION INTO THE ENSO CYCLE

Causes of the Intraseasonal SST Variability in the Tropical Indian Ocean

Summer monsoon onset in the subtropical western North Pacific

Atmosphere Circulation

Effect of Orography on Land and Ocean Surface Temperature

Mesoscale air-sea interaction and feedback in the western Arabian Sea

Marine ecosystem simulation in the eastern tropical Pacific with a global eddy resolving coupled physical-biological model

CHANGE OF THE BRIGHTNESS TEMPERATURE IN THE MICROWAVE REGION DUE TO THE RELATIVE WIND DIRECTION

Scripps Institution of Oceanography, La Jolla, California. (Manuscript received 3 March 2009, in final form 15 June 2009) ABSTRACT

(20 points) 1. ENSO is a coupled climate phenomenon in the tropical Pacific that has both regional and global impacts.

ATOMOSPERIC PRESSURE, WIND & CIRCULATION

Data Analysis of the Seasonal Variation of the Java Upwelling System and Its Representation in CMIP5 Models

APPENDIX B NOAA DROUGHT ANALYSIS 29 OCTOBER 2007

Impacts of intraseasonal oscillation on the onset and interannual variation of the Indian summer monsoon

Lecture 13 El Niño/La Niña Ocean-Atmosphere Interaction. Idealized 3-Cell Model of Wind Patterns on a Rotating Earth. Previous Lecture!

Far Eastern Pacific Fresh Pool surface salinity variability observed by SMOS and Aquarius sensors over. the period

SUPPLEMENTARY INFORMATION

Hui Wang, Mike Young, and Liming Zhou School of Earth and Atmospheric Sciences Georgia Institute of Technology Atlanta, Georgia

ENSO Cycle: Recent Evolution, Current Status and Predictions. Update prepared by Climate Prediction Center / NCEP 8 March 2010

The Setting - Climatology of the Hawaiian Archipelago. Link to Video of Maui Waves

Lecture 24. El Nino Southern Oscillation (ENSO) Part 1


Abrupt seasonal variation of the ITCZ and the Hadley circulation

Investigation of Common Mode of Variability in Boreal Summer Intraseasonal Oscillation and Tropospheric Biennial Oscillation

9/25/2014. Scales of Atmospheric Motion. Scales of Atmospheric Motion. Chapter 7: Circulation of the Atmosphere

Geostrophic and Tidal Currents in the South China Sea, Area III: West Philippines

Wind Driven Circulation Indian Ocean and Southern Ocean

Biennial Oscillation of Tropical Ocean-Atmosphere System Associated with Indian Summer Monsoon

Winds and Ocean Circulations

Influence of enhanced convection over Southeast Asia on blocking ridge and associated surface high over Siberia in winter

3 The monsoon currents in an OGCM

Second peak in the far eastern Pacific sea surface temperature anomaly following strong El Niño events

Analysis of 2012 Indian Ocean Dipole Behavior

Local vs. Remote SST Forcing in Shaping the Asian-Australian Monsoon Variability

Asymmetry in zonal phase propagation of ENSO sea surface temperature anomalies

ATS150: Global Climate Change. Oceans and Climate. Icebergs. Scott Denning CSU 1

Section 1. Global Wind Patterns and Weather. What Do You See? Think About It. Investigate. Learning Outcomes

Ocean dynamic processes responsible for the interannual. variability of the tropical Indian Ocean SST. associated with ENSO

Chapter 10: Global Wind Systems

Lecture 15 General Circulation of the Atmosphere and Ocean

Determination of Coastal Current System Between Mindanao and New Guinea

ENSO Cycle: Recent Evolution, Current Status and Predictions. Update prepared by Climate Prediction Center / NCEP 4 September 2012

Modification of the Stratification and Velocity Profile within the Straits and Seas of the Indonesian Archipelago

Interannual variation of northeast monsoon rainfall over southern peninsular India

Air Pressure and Wind

Climatology of the 10-m wind along the west coast of South American from 30 years of high-resolution reanalysis

Monsoon Systems Valsavarenche Val d Aosta, Italy

OCN 201 Lab Fall 2009 OCN 201. Lab 9 - El Niño

Lecture 33. Indian Ocean Dipole: part 2

Intraseasonal Variability in Sea Level Height in the Bay of Bengal: Remote vs. local wind forcing & Comparison with the NE Pacific Warm Pool

Atlantic warm pool, Caribbean low-level jet, and their potential impact on Atlantic hurricanes

Chapter. Air Pressure and Wind

Agronomy 406 World Climates

SEA SURFACE TEMPERATURE RETRIEVAL USING TRMM MICROWAVE IMAGER SATELLITE DATA IN THE SOUTH CHINA SEA

Oceans and the Global Environment: Lec 2 taking physics and chemistry outdoors. the flowing, waving ocean

IX. Upper Ocean Circulation

Effects of the Tibetan Plateau on the onset of the summer monsoon in South Asia: The role of the air-sea interaction

The Ocean is a Geophysical Fluid Like the Atmosphere. The Physical Ocean. Yet Not Like the Atmosphere. ATS 760 Global Carbon Cycle The Physical Ocean

Remote influence of Interdecadal Pacific Oscillation on the South Atlantic Meridional Overturning Circulation variability

Observed Intraseasonal Oceanic Variations in the Eastern Equatorial Indian Ocean and in the Outflow Straits of the Indonesian Throughflow

Subsurface Ocean Indices for Central-Pacific and Eastern-Pacific Types of ENSO

CHAPTER 6 Air-Sea Interaction

Increasing intensity of El Niño in the central equatorial Pacific

J4.2 AUTOMATED DETECTION OF GAP WIND AND OCEAN UPWELLING EVENTS IN CENTRAL AMERICAN GULF REGIONS

Haibo Hu Jie He Qigang Wu Yuan Zhang

3. Climatic Variability. El Niño and the Southern Oscillation Madden-Julian Oscillation Equatorial waves

Outline. 1 Background Introduction. 3 SST Amphidrome 4 Niño Pipe 5. SST in China Seas. Seasonality Spiral. Eddy Tracking. Concluding Remarks

Section 6. The Surface Circulation of the Ocean. What Do You See? Think About It. Investigate. Learning Outcomes

Lecture 5: Climate Tapestry. Sea/Land Breeze. Thermal Energy to Kinetic Energy

Dynamics and variability of surface wind speed and divergence over mid-latitude ocean fronts

The atmospheric circulation system

Monsoon IntraSeasonal Oscillation (MISO) in the Bay of Bengal: Effect of mixed layer and barrier layer on SST and convection

Are Hurricanes Becoming More Furious Under Global Warming?

CHAPTER 7 Ocean Circulation

18.1 Understanding Air Pressure 18.1 Understanding Air Pressure Air Pressure Defined Measuring Air Pressure Air pressure barometer

- terminology. Further Reading: Chapter 07 of the text book. Outline. - characteristics of ENSO. -impacts

ESCI 485 Air/sea Interaction Lesson 9 Equatorial Adjustment and El Nino Dr. DeCaria

Impact of Typhoons on the Western Pacific: Temporal and horizontal variability of SST cooling Annual Report, 2011 James F. Price

Climate & Earth System Science. Introduction to Meteorology & Climate. Chapter 07. Lecture 14. Global Scale Winds. Simple Introductory Examples:

Goal: Describe the principal features and characteristics of monsoons

Indian Ocean Dipole - ENSO - monsoon connections and Overcoming coupled model systematic errors

Trade winds How do they affect the tropical oceans? 10/9/13. Take away concepts and ideas. El Niño - Southern Oscillation (ENSO)

Mechanism of the Asymmetric Monsoon Transition as. Simulated in an AGCM

An Evolution of the Asian Summer Monsoon Associated with Mountain Uplift Simulation with the MRI Atmosphere-Ocean Coupled GCM

Lecture Outlines PowerPoint. Chapter 18 Earth Science 11e Tarbuck/Lutgens

Equatorial upwelling. Example of regional winds of small scale

THE ATMOSPHERE. WEATHER and CLIMATE. The Atmosphere 10/12/2018 R E M I N D E R S. PART II: People and their. weather. climate?

PROC. ITB Eng. Science Vol. 36 B, No. 2, 2004,

The General Circulation and El Niño. Dr. Christopher M. Godfrey University of North Carolina at Asheville

Summary of Lecture 10, 04 March 2008 Introduce the Hadley circulation and examine global weather patterns. Discuss jet stream dynamics jet streams

McKnight's Physical Geography 11e

ESCI 107 The Atmosphere Lesson 11 Global Circulation

Transcription:

GEOPHYSICAL RESEARCH LETTERS, VOL. 33,, doi:10.1029/2006gl025997, 2006 Influence of mechanical mixing on a low summertime SST in the western North Pacific ITCZ region N. Sato, 1 H. Tokinaga, 1 R. Shirooka, 1 and N. Suginohara 1 Received 8 February 2006; revised 1 June 2006; accepted 9 June 2006; published 22 July 2006. [1] A region with a low sea-surface temperature (SST) was identified in the western North Pacific (WNP) Intertropical Convergence Zone (ITCZ) or warm water pool region in boreal summer. The SST decreases by up to 0.5 C from May to the June July August (JJA) season just east of Mindanao Island. Analyses of the observed data indicated that a northeastward surface current constantly exists throughout the year, supplying cold subsurface water through the Molucca Strait. As a result, the subsurface water is colder by several degrees compared with that in the surrounding regions. The sea-surface wind is strong over this region in the JJA season. Examination of Argo float data demonstrated that the mixed layer becomes deeper from May to the JJA season. It is suggested that the strong wind causes vertical mixing between the surface and subsurface layers, resulting in the low summertime SST. Citation: Sato, N., H. Tokinaga, R. Shirooka, and N. Suginohara (2006), Influence of mechanical mixing on a low summertime SST in the western North Pacific ITCZ region, Geophys. Res. Lett., 33,, doi:10.1029/2006gl025997. 1. Introduction [2] Large-scale convective activity over the ocean east of the Philippines is sometimes referred to as the WNP summer monsoon (WNPSM) [Wang and LinHo, 2002]. This convective activity is most active corresponding to high SST over the WNPSM or the WNP ITCZ region. The seasonal cycle of atmospheric convective activity on large spatial scales has been examined by Wang and LinHo [2002]. Furthermore, Kubota et al. [2005] revealed a seasonal cycle of convective activity over the WNP ITCZ region in more detail, by using in-situ observation data from Palau. In general, large-scale convection systems are more active in the JJA season than in other seasons, associated with the low-level westerly wind. [3] However, the seasonal changes in the air-sea coupling system in the WNPSM and WNP ITCZ region have not been well examined, partly because we have not had sufficient observed data. Although the Philippine Sea is often recognized as a warm-water pool with a high SST, oceanic conditions may differ over relatively small spatial scales, since the deformation radius in the ocean is much smaller than that in the atmosphere. Moreover, the topography is complicated near the maritime continent. Localized eddies actually exist in the climatological field corresponding to such complicated geographical conditions. For example, the 1 Institute of Observational Research for Global Change, Japan Agency for Marine-Earth Science and Technology, Yokosuka, Japan. Copyright 2006 by the American Geophysical Union. 0094-8276/06/2006GL025997 Mindanao and Halmahera eddies are already well known to oceanographers [Arruda and Nof, 2003]. However, the airsea interaction associated with such localized oceanic eddies has not yet been studied in detail. [4] In the present study, we examine the air-sea interaction over the WNP ITCZ region by using satellite observation data and in-situ measurement data provided by Argo floats [Argo Science Team, 2001]. In particular, we focus on the airsea interaction related to the Mindanao and Halmahera eddies. 2. Methods [5] Tropical Rainfall Measuring Mission Microwave Imager (TMI) SST data were used to examine the seasonal changes in SST with a resolution of 0.25 0.25 averaged from 1998 to 2005 over the WNP ITCZ region. For simplicity, the daily data sets were edited first. Missing values caused by the lack of a path width were replaced with temporally interpolated values at each grid point. We focused on the difference between the SST distribution in May and the JJA season, and confirmed that the SST is lower in the JJA season over the WNP ITCZ region. [6] The Special Sensor Microwave/Imager (SSM/I) precipitation rate data, with a resolution of 0.25 0.25, were also examined for the same periods in order to confirm that convection is relatively weak over the low SST region. [7] Sea-surface wind fields were investigated using QuikScat sea-surface wind data. We replaced the missing values with interpolated values as we did for TMI SST data. Note that we analyzed data from 2000 to 2005 for the seasurface wind, since QuikScat data was available back to July 1999. [8] The Aviso absolute dynamic topography (ADT) data obtained by satellite observation were used to infer nearsurface currents in the WNP ITCZ region. The data set was a merged satellite observation that was taken only one or two times a week. Thus, we made a daily data set, with a resolution of 2.5 2.5, using temporal interpolation, and then calculated the climatological means for May and for the JJA season. We analyzed data from 2002 to 2005 here. [9] Real-time quality-controlled data from Argo profiling floats deployed in the Pacific Ocean were examined. The data indicated the sea-water temperature and salinity at 10- day intervals [Argo Science Team, 2001]. The vertical interval is about 10 db, and the shallowest level is approximately 5 db in most cases. First, the data were used to examine the horizontal temperature distribution of near- or sub-surface water. The temperature at the 80 db level was calculated by vertical interpolation for each observed temperature profile. The 80 db temperatures were plotted for the March April May (MAM) and JJA seasons. Note that we 1of5

SATO ET AL.: WARM WATER POOL Figure 2. Precipitation rate averaged for JJA season. Figure 1. SST averaged for (top) May and (bottom) JJA season. The low-sst region is marked by a circle. analyzed data for the MAM season instead of May because we could not obtain enough data for the one-month period. Data for the years from 2003 to 2005 were used here. [10] We also investigated the vertical profiles of temperature and salinity in the surface layer using the Argo data. The vertical profiles of JJA temperature, averaged over 0 to 5 N, 5 to 10 N, and 10 to 15 N for 125 to 135 E, were compared. Next, the seasonal changes of the temperature profiles averaged over 5 to 10 N, 125 to 135 E, were also examined. Here, the changes from May to the JJA season were analyzed. T-S diagrams were also drawn for both periods, in order to confirm the effects of vertical mixing. May. However, to the south or east of Mindanao Island, the convection does not change significantly or becomes less intense from May to JJA (not shown). [13] Figure 3 depicts the QuikScat sea-surface wind during JJA. The arrows indicate the mean wind vector, and the contours and tones indicate the averaged scalar wind speed. The southwesterly wind speed is high over the lowsst region or the suppressed convection region. High wind speed is not observed in May (not shown). [14] The Aviso ADT averaged for JJA is depicted in the top plot of Figure 4. A cyclonic eddy associated with a low ADT is identified just to the east of Mindanao Island. This corresponds to the Mindanao eddy [Arruda and Nof, 2003]. Although the Halmahera eddy is not as clear as the Mindanao eddy, relatively high ADT is observed near Halmahera Island. The gradient of ADT is extremely large southeast of Mindanao Island as illustrated in Figure 4 (top). The estimated geostrophic current is 1 m/s at maximum. It is inferred that a strong northeastward current exists in this region. We can identify the large ADT gradient and the strong geostrophic current in the other seasons of the year (not shown). [15] The features related to the low-sst region depicted in Figures 1 4 can be seen in the JJA season of each year, for all or most of the years. [16] The 80 db sea-water temperatures observed by Argo floats in the JJA season are depicted in the bottom plot of 3. Results [11] The TMI SSTs averaged for May (top) and the JJA season (bottom) are shown in Figure 1. In May (top), the SST is above 29.6 C between the equator and 10 N in the WNP. The warm SST region expands northward in the JJA season (bottom). However, the SST decreases east of Mindanao Island. As a result, a low-sst region is formed in the southern part of the WNP warm pool. It is identified every year except 1998, a post-el Nin o year. [12] Figure 2 depicts the averaged precipitation rate for JJA. Convective activity is strong over the subtropical WNP in the JJA season, corresponding to the WNPSM. However, the precipitation rate is relatively lower south and east of Mindanao Island. The suppressed convection region corresponds to the low-sst region illustrated in Figure 1 (bottom). In general, convective activity over the warm pool intensifies in the JJA season compared with that in Figure 3. Sea-surface wind vector (arrows) and scalar wind speed (tones) averaged for JJA season. 2 of 5

SATO ET AL.: WARM WATER POOL Figure 5. Averaged vertical profiles of JJA sea-water temperature in 0 to 5 N (thin solid line), 5 to 10 N (thick solid line) and 10 to 15 N (dotted line), 125 to 135 E. Figure 4. (top) Absolute dynamic height averaged for JJA season and (bottom) sea-water temperature observed by Argo floats at 80 db. For the top plot, the contour interval is 10 cm. Values greater than 250 cm are shaded, and those less than 200 cm are hatched. Figure 4. Roughly speaking, the sea-water temperature is high (28 C) in the WNP warm pool. However, we detected lower temperatures, below 22 C in some locations, between 5 N and 10 N. Low near- or sub-surface water temperatures are also found in the MAM season (not shown). The cold region in the bottom plot corresponds well to the northeastward or eastward geostrophic current in the top plot. [17] Figure 5 illustrates vertical profiles of the temperatures obtained by Argo floats averaged over 0 to 5 N (thin solid line), 5 to 10 N (thick solid line), and 10 to 15 N (dotted line) for 125 to 135 E in the JJA season. The mixed layer is shallower and the subsurface water is colder for 5 to 10 N (thick solid line) compared with those in the other regions (thin solid line and dotted line). Figure 6 presents the seasonal changes in the temperature profiles averaged over 5 to 10 N, 125 to 135 E in May (thin line) and JJA (thick line). The mixed layer becomes deeper with statistical significance and becomes cold in JJA. The T-S diagram is smoothed and shifted to the low-salinity side in the JJA season (not shown). 4. Discussion [18] In Figure 1, the SST decreases east of Mindanao Island from May to the JJA season. Conversely, in the other areas of the low-latitude WNP, the SST rises in boreal summer. The seasonal change in SST in the WNP ITCZ region located east of Mindanao Island is quite different from that in the surrounding regions. The spatial distribution of precipitation suggests that convective activity is suppressed by the low SST. [19] The large gradient of ADT between the cyclonic Mindanao eddy and the anticyclonic Halmahera eddy depicted in Figure 4 (top) indicates a strong northeastward or eastward geostrophic current from the Molucca Strait. Although only the surface current is estimated here, we can infer similar currents in the surface and subsurface layers, since the baroclinicity caused by the horizontal gradient of density is not so large here. The sea water at the near- or sub-surface level is colder in the current than that in the surrounding regions (the bottom plot of Figure 4). Furthermore, cold subsurface water is most clearly observed near the Molucca Strait. The vertical temperature profiles shown in Figure 5 also confirm the clear difference in the subsurface temperature. These results demonstrate that the cold subsurface water is supplied from the Molucca Strait. A Figure 6. Averaged vertical profiles of sea-water temperature in 5 to 10 N, 125 to 135 E in May (thin solid line) and JJA (thick solid line). 3of5

SATO ET AL.: WARM WATER POOL comparison of Figure 1 (bottom) and Figure 4 (bottom) suggests that the subsurface cold water corresponds to the low SST. Although some in-situ measurements of the currents near the Philippines have been done, focusing on the bifurcation of the North Equatorial Current [e.g., Toole et al., 1990], we cannot yet obtain enough observed data in the Molucca Strait. However, the existence of the northeastward current through the Molucca Strait is confirmed in the result of the simulation using an ocean general circulation model [Masumoto et al., 2001]. [20] The strong northeastward or eastward subsurface current and the resulting cold subsurface water also exist in the other seasons (not shown). Thus, the cold subsurface water alone cannot explain why a low SST appears only in the JJA season. According to the results shown in Figure 2, the sea-surface wind is strong east of Mindanao Island in the JJA season. The strong wind can be regarded as a part of the Asian-Australian monsoon system [e.g., Matsumoto, 1992], and it appears to be localized by the complicated topography over the maritime continent. Such a strong wind is not detected in the other seasons (not shown). Moreover, the mixed layer becomes deeper and colder from May to JJA, as indicated in Figure 6. These results suggest that the strong surface wind that appears in the JJA season mixes up the cold subsurface water, resulting in the low SST. The T-S diagram is smoothed from May to JJA, which is consistent with the inference that the vertical mixing is strengthened in the JJA season (not shown). The curl of the surface wind is almost zero or anticyclonic near the center of the low-sst region (Figure 4). Therefore, it is inferred that the Ekman upwelling does not contribute to the SST decrease. Since the low-sst region is not in contact with the coast of the Philippines, it is suggested that the contribution of coastal upwelling is also small. [21] The region of subsurface cold water extends eastward from the center of the low-sst region (Figure 4). On the other hand, the strong-wind region does northeastward (Figure 3). The low SST is observed only where both of them are observed. In more detail, the low-sst region in Figure 1 (bottom) is slightly shifted southeastward compared with the surface wind maximum and the 80-db temperature minimum. This may be caused by the Ekman transport associated with the southwesterly wind. [22] In boreal summer, the SST is lower in the Arafra Sea than in the Philippine Sea. The strong surface current may transport the cold surface water from the Arafra Sea into the warm pool. However, a minimum of SST is observed off Mindanao Island, especially in June. The low-sst region then expands over the southern part of the Philippine Sea (not shown). Therefore, the formation of a low-sst region cannot be explained by only the advection of cold surface water from the Arafra Sea through the Molucca Strait. [23] Sato [2005] demonstrated that sudden SST coolings over a 10-day interval occur when the oceanic mixed layer is shallow in the WNP ITCZ region. The locations of such cooling events roughly correspond to the cold subsurface water examined in the present study. Although Sato [2005] did not discuss the formation mechanism of the shallow mixed layer which is favored by the cooling events, the shallow mixed layer related to the sudden cooling appears to also be related to the cold subsurface water supplied through the Molucca Strait. [24] Xie et al. [2003] demonstrated that the low summertime SST over the South China Sea is formed by adiabatic surface cooling related to strong surface wind and by an Ekman upwelling associated with the positive wind-stress curl. In the WNP ITCZ region, the low SST does not correspond to the cyclonic curl of the surface wind in Figure 3. Furthermore, the sea water in and near the mixed layer is not lifted up in the vertical temperature profiles shown in Figure 6. The Ekman upwelling is not a predominant process in the formation of the low-sst region. Since the latent heat flux from the sea surface is generally important to the surface heat budget in a tropical ocean, adiabatic cooling caused by strong surface wind may contribute to the low SST. However, from the authors examination of the vertical profile of sea-water temperature and the T-S diagram, adiabatic cooling does not seem to be a predominant process for the low SST. It appears that the formation mechanisms of a cold water pool are different in different regions. 5. Conclusions [25] The SST over the WNP ITCZ region just to the east of Mindanao Island is lower in boreal summer compared with the SST in May or that in the surrounding region. Convective activity is weak over this cold-sst region. Cold subsurface water is supplied almost constantly from the Molucca Sea throughout the year by the northeastward current related to the Mindanao and Halmahera eddies. The temperature of the subsurface water is lower by several degrees at maximum than that near the equator or in the central Philippine Sea at the same longitude. A strong sea-surface wind is observed in boreal summer. The mixingup of the subsurface water due to the strong wind stress causes the summertime cold SST to the east of Mindanao Island. [26] Acknowledgments. The authors would like to thank the many people who kindly assisted in this work. N. Shikama and E. Oka of the Institute of Observational Research for Global Change, Japan Agency for Marine-Earth Science and Technology (IORGC/JAMSTEC) kindly helped us obtain and utilize the Argo data. The authors would like to thank all the members of the Argo group in IORGC/JAMSTEC for their efforts in acquiring data with such high quality. They also thank the two anonymous reviewers for their comments. The TMI, SSM/I and QuikScat data were provided by Remote Sensing Systems (RSS) (http://www.ssmi.com/). It was produced by RSS under the sponsorship of the Ocean Vector Winds Science Team at the National Aeronautics and Space Administration (NASA). The ADT data were provided by Aviso, from their Web site at http://www.jason.oceanobs.com/. The Argo data were provided by IORGC/ JAMSTEC (ftp://ftp.jamstec.go.jp/pub/argo/). The GFD-DENNOU Library was utilized for drawing the figures. References Argo Science Team (2001), Argo: The global array of profiling floats, in Observing the Oceans in the 21st Century, edited by C. J. Koblinsky and N. P. Smith, pp. 248 258, GODAE Proj. Off., Melbourne, Victoria, Australia. Arruda, W. Z., and D. Nof (2003), The Mindanao and Halmahera eddies Twin eddies induced by nonlinearities, J. Phys. Oceanogr., 33, 2815 2830. Kubota, H., R. Shirooka, T. Ushiyama, T. Chuda, S. Iwasaki, and K. Takeuchi (2005), Seasonal variations of precipitation properties associated with the monsoon over Palau in the western Pacific, J. Hydrol., 6, 518 531. Masumoto, Y., T. Kagimoto, M. Yoshida, M. Fukuda, N. Hirose, and T. Yamagata (2001), Intraseasonal eddies in the Sulawesi Sea simulated in an ocean general circulation model, Geophys. Res. Lett., 28, 1631 1634. 4of5

SATO ET AL.: WARM WATER POOL Matsumoto, J. (1992), The seasonal changes in Asian and Australian monsoon regions, J. Meteorol. Soc. Jpn., 70, 257 273. Sato, N. (2005), Influences of intraseasonal disturbances on the oceanic mixed layer in the western North Pacific ITCZ region, Geophys. Res. Lett., 32, L17601, doi:10.1029/2005gl023577. Toole, J. M., R. C. Millard, Z. Wang, and S. Pu (1990), Observations of the Pacific North Equatorial Current bifurcation at the Philippine coast, J. Phys. Oceanogr., 20, 307 318. Wang, B., and LinHo (2002), Rainy season of the Asian-Pacific summer monsoon, J. Clim., 15, 386 398. Xie, S., Q. Xie, D. Wang, and W. T. Liu (2003), Summer upwelling in the South China Sea and its role in regional climate variations, J. Geophys. Res., 108(C8), 3261, doi:10.1029/2003jc001867. N. Sato, R. Shirooka, N. Suginohara, and H. Tokinaga, Institute of Observational Research for Global Change, Japan Agency for Marine-Earth Science and Technology, 2-15 Natsushima-cho, Yokosuka, Kanagawa, 237-0061, Japan. (naoki@jamstec.go.jp) 5of5