Spatial Distribution Characteristics of Seasonal Thermocline in Korea 1, 2 Dong-Young Yoon1 and Hyun-Woo Choi2* Oceanographic Data & Information Center, Korea Institute of Ocean Science & Technology (KIOST) 787 Haean-ro(st) Sangnok-gu, Ansan-si, Gyunggi-do, Korea, [email protected], [email protected] *Corresponding author: [email protected] ABSTRACT In low-latitude waters such as the equatorial region, 20 °C isothermal line is defined as the permanent thermocline. However, mid-latitude waters have variable vertical profile of water temperature with respect to the season and region. Therefore, in this study we developed an algorithm for quantifying seasonal thermocline in order to extract parameters for vertical temperature profiles of Korean waters in summer. In addition, quantified parameters were used to identify spatial distribution characteristics of thermocline, and a model for relationship between thermocline parameters was established to help understand the structure of thermocline. Keyword: seasonal thermocline, thermocline parameters, spatial distribution, Korean waters INTRODUCTION Research of spatial characteristics of water temperature in the sea, which is a three-dimensional space, has been mostly limited to studies of horizontal distribution. In other words, research on vertical temperature characteristics, including the thermocline, is lacking. In the vertical temperature profile of the sea, the layer below the mixed layer in which the water temperature rapidly decreases with depth is referred to as the thermocline. This layer is important to understand marine physical and biological phenomenon. In order to study the thermocline, one must first determine if it has been existed and then extract the parameters of the thermocline structure. The most difficult step is determining at which depth the thermocline top and base points. For this purpose, one may visually inspect the vertical temperature profile. However, this method is impractical when analyzing vertical temperature profile dataset over a wide region and for an extended period of time. In research of the equatorial Pacific Ocean, Kessler (1990) has defined the depth of 20 °C isothermal line as the medium depth of the thermocline and this definition has since been used [1]. The NOAA (2012) has recently used this definition in discovering the relationship between El Niño/La Niña and thermocline [2]. In contrast to low-latitude waters, mid-latitude waters have seasonal thermocline and various vertical temperature profiles. Several studies have attempted to identify vertical temperature gradient (ΔT) conditions for different seasons and regions in order to extract depths of the thermocline top and base points [3, 4, 5]. Limitations of these studies are that there is no prior step for checking the formation of thermocline and that an absolute threshold ΔT has been used to extract thermocline. Such threshold will vary with season and region, which implies that an absolute value cannot be applied generally to mid-latitude waters. To solve this problem, we have developed an algorithm for detecting thermoclines and extracting relevant parameters in the various vertical temperature profiles in the southern Sea of Korea during summer [6]. In the study, ΔT threshold conditions were used to detect thermoclines, and structural characteristics of the hyperbolic tangent function were used to extract thermocline parameters. Although the developed algorithm is capable of extracting thermocline parameters, it is unable to achieve the fundamental goal of “detecting the thermocline and extracting its parameters regardless of the shape of the vertical temperature profile”. In this study, we aimed to develop an improved algorithm for detecting thermocline and extracting parameters, only using the structure of the hyperbolic tangent function. In addition, the algorithm was applied to the Korean waters having various vertical temperature profiles for establishing a model of relationship between thermocline parameters and understanding spatial distribution characteristics of thermocline. MATERIALS AND METHODS (1) Study area and data The Korean waters located at mid-latitude regions was selected as study area (Figure 1). These region is directly affected by the Kuroshio Warm Current and the North Korea Cold Current, and has various forms of seasonal thermocline during summer. The water temperature data used in this study was monitored by the NFRDI (National Fishers Research and Development Institute) at 205 sites during summer (August) for 30 years (from 1981 to 2010), as part of NSO (NFRDI Serial Oceanographic observation) project. The data contains water temperature at 14 standard depths (0, 10, 20, 30, 50, 75, 100, 125, 150, 200, 250, 300, 400, and 500 m). In order to obtain water temperature data with 1 m interval, monotone piecewise cubic interpolation was applied to the water temperature data of standard depths [7]. Figure 1. Study area with temperature observed stations by NFRDI (2) Thermocline detection The thermocline detection algorithm used in this study was based on the idea that the structure of the hyperbolic tangent function is similar to the thermocline structure, as shown in Figure 2. The concept of differential hyperbolic tangent function (DHTF) has been applied to the vertical structure of ΔT. The xcomponent of the DHTF is the depth and the y-component is the ΔT, and the depths at which ΔT is 42% of the maximum ΔT were defined as the top and base point depths of thermocline [6]. Occurrence of thermocline was determined by the existence of depths that have gradients that are 42% of maximum ΔT. The following 10 parameters were extracted from the datasets in which thermocline exists: 1) sea surface temperature (SST), 2, 3) thermocline top point depth & temperature, 4, 5) maximum ΔT point depth & temperature, 6, 7) thermocline base point depth & temperature, 8) maximum ΔT, 9) thickness of thermocline, and 10) difference of temperature between thermocline top and base point. Figure 2. The vertical temperature and ΔT profile using a) hyperbolic tangent function and b) differential hyperbolic tangent function to understand the structure RESULT (1) Thermocline occurrence frequency Of total 5,329 datasets, 3,231 were found to have thermocline. Thermocline occurrence frequency for each station is shown in Figure 3. There are 15 stations with frequency below 25%, 33 stations with frequency between 25% and 50%, 89 stations with frequency between 50% and 75%, and 68 stations with frequency above 75%. Regions close to the land with shallow depth had relatively lower thermocline occurrence frequency compared to the outer sea. To investigate the spatial distribution characteristics of thermocline, average value for ten parameters was calculated at each station with occurrence frequency above 50%. Figure 3. Map of thermocline occurrence frequency (2) Distribution of thermocline parameters The spatial distribution maps were created for the four parameters representing the thermocline, which are SST, thermocline top point depth, maximum ΔT, and thickness of thermocline (Figure 4). The range of SST of the Korean waters during summer was from 22 °C to 30 °C, with southeastern area of the Jeju Island being the highest and the East Sea being the lowest. This is most likely because the southeastern area of the Jeju Island is affected by the Kuroshio Warm Current and the East Sea is affected by the North Korea Cold Current. The top point depth of thermocline had a range of 9 m to 27 m, with it being the deepest near Tsushima Island. Maximum ΔT was higher in the west of Jeju Island compared to east, while the thickness of thermocline showed an opposite trend. From the results, it was concluded that thermoclines in the Korean waters are formed more strongly in the western region compared to the eastern region of Jeju Island. Figure 4. Spatial distribution pattern of thermocline parameters a) SST, b) top point depth, c) maximum ΔT, d) thickness of thermocline (3) Correlation analysis Correlation analysis was performed to identify the relationship between the four parameters, which had various spatial distribution pattern (Table 1). SST was positively correlated with maximum ΔT, and SST was negatively correlated with thickness of thermocline. This implies that higher the SST, maximum ΔT becomes larger and thickness of thermocline becomes smaller. Therefore, SST was found to influence the strength of thermocline. In contrast to SST, top point depth of thermocline was negatively correlated with maximum ΔT and positively correlated with thickness of thermocline. Also, maximum ΔT and the thickness were negatively correlated. Therefore, relational model of thermocline parameters can be used to deduce the relationship of SST with other parameters. Table 1. Pearson’s correlation coefficients between thermocline parameters SST (A) Thermocline top point depth (B) Maximum ΔT (C) B C D 0.129 0.189* -0.407** -0.362* 0.497** -0.645** Thickness of thermocline (D) p-value (**<0.01, *<0.05), total number of data is 157 CONCLUSION We developed an algorithm for detecting and quantifying thermoclines in various vertical temperature profiles, and used it to extract parameters for seasonal thermocline in the mid-latitude waters. By quantifying parameters related to thermocline, spatial distribution characteristics of thermocline in the Korean waters during summer has been identified for the first time. Also, we established a model of thermocline structure through correlation analysis of the parameters. It is anticipated that the algorithm developed in this study can be used for the analysis of relationship between thermocline with climate change index and marine organisms in the mid-latitude waters. ACKNOWLEDGMENT This study was supported by KIOST project (PE98971) “Development of Algorithm for Detecting and Extracting Thermocline”. REFERENCES [1] Kessler W.S., 1990, Observations of Long Rossby Waves in the Northern Tropical Pacific, Journal of Geophysical Research, 95(C4) 5183-5217. [2] NOAA, 2012, ENSO Cycle: Recent evolution, current status and predictions, Climate Prediction Center/NCEP, http://www.cpc.ncep.noaa.gov (accessed on 1st December 2013). [3] Hastenrath S., Merle J., 1987, Annual cycle of subsurface thermal structure in the tropical Atlantic Ocean, Journal of Physical Oceanography, (17) 1518-1538. [4] Prasad T.G., Bahulayan N., 1996, Mixed layer depth and thermocline climatology of the Arabian Sea and western equatorial Indian Ocean, Indian Journal of Marine Sciences, (25) 189-194. [5] Park S., Chu P.C., 2007, Synoptic distributions of thermocline surface mixed layer and thermocline in the Southern Yellow and East China Seas, Journal of Oceanography, (63) 1021-1028. 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