• <tr id="yyy80"></tr>
  • <sup id="yyy80"></sup>
  • <tfoot id="yyy80"><noscript id="yyy80"></noscript></tfoot>
  • 99热精品在线国产_美女午夜性视频免费_国产精品国产高清国产av_av欧美777_自拍偷自拍亚洲精品老妇_亚洲熟女精品中文字幕_www日本黄色视频网_国产精品野战在线观看 ?

    The Change Features of the West Boundary Bifurcation Line of the North Equatorial Current in the Pacific

    2015-04-01 01:57:18GUOJunruLIUYulongSONGJunBAOXianwenLIYanCHENShaoyangandYANGJinkun
    Journal of Ocean University of China 2015年6期

    GUO Junru, LIU Yulong, SONG Jun, 5), *, BAO Xianwen, LI Yan, CHEN Shaoyang, and YANG Jinkun

    ?

    The Change Features of the West Boundary Bifurcation Line of the North Equatorial Current in the Pacific

    GUO Junru1), 2), 4), LIU Yulong3), SONG Jun3), 5), *, BAO Xianwen1), 5), LI Yan3), CHEN Shaoyang3), and YANG Jinkun3)

    1),,266100,2),100194,3),300171,4),,,, ACT2602,5),,266100,

    The equatorial Current in the North Pacific (NEC) is an upper layer westward ocean current, which flows to the west boundary of the ocean, east of the Philippines, and bifurcates into the northerly Kuroshio and the main body of the southerly Mindanao current. Thus, NEC is both the south branch of the Subtropical Circulation and the north branch of the Tropical Circulation. The junction of the two branches extends to the west boundary to connect the bifurcation points forming the bifurcation line. The position of the North Pacific Equatorial Current bifurcation line of the surface determines the exchange between and the distribution of subtropical and tropical circulations, thus affecting the local or global climate. A new identification method to track the line and the bifurcation channel was used in this study, focusing on the climatological characteristics of the western boundary of the North Equatorial Current bifurcation line. The long-term average NEC west boundary bifurcation line shifts northwards with depth. In terms of seasonal variation, the average position of the western boundary of the bifurcation line is southernmost in June and northernmost in December, while in terms of interannual variation, from spring to winter in the years when ENSO is developing, the position of the west boundary bifurcation line of NEC is relatively to the north (south) in EI Ni?o (La Ni?a) years as compared to normal years.

    North Equatorial Current; Pacific Ocean; bifurcation line; climate change; ENSO

    1 Introduction

    NEC system connects the subtropical and tropical cy- clones in the Pacific and makes important contributions to the heat budget in the western Pacific warm pool (Qu, 1997), while the warm pool is a key region that affects the circulation of ENSO (Webster and Lukas, 1992). The western boundary current systems of NEC directly enters the global thermohaline circulation through the Indone- sian throughflow (Gordon, 1986) and plays a decisive role in the meridional transport of heat, salt and mass in the world oceans (Qu, 1998). The western Pacific region is an intersection for the middle and high latitude water masses (Fine, 1994), from which the concept of subtropical cell is derived: The net heating from the low latitude ocean is transported northwards from the surface to the NEC and then via Kuroshio to the higher latitudes; while the cold subsurface/deep water water flows southwards in the thermocline and then to the trop- ics through different passageways after being bifurcated by the NEC (Lu, 1998; Johnson and Mcphaden, 1999); and lastly turns upwards at the equator, constitute- ing the sallow meridional overturning circulation (Mc- Creary and Lu, 1994; Liu, 1994). The NEC links the sub- tropical and tropical regions, and is the boundary between subtropical and tropical circulations. At the western bound- ary, NEC bifurcates into two branches: NEC north branch passageway (flowing to Kuroshio) and NEC south branch passageway (flowing to the Mindanao current) (Xu and M-Rizzoli, 2013). There are different bifurcation points of NEC at different depths, the line connecting these bi- furcation points is the bifurcation line which determines the distribution of mass, heat and salt between the sub- tropical and tropical circulations. The interannual and decadal changes of the NEC bifurcation line can affect the tropical and subtropical heat distribution and thermal structure change, thus affecting the local or global climate (Song, 2011). Therefore, the change of the NEC bifurcation line plays a very important role in our re- search on the global climate change. Previous studies mostly focus on the change of the western boundary bifurcation points and less research is made on the change pattern of the bifurcation points, but this charac- teristic of bifurcation line can more directly and accu- rately identify the change of circulation systems (Wang and Liu, 2000).

    The position of the bifurcation point of NEC plays an important role in the Climate Change, so the research on the latitude of the NEC bifurcation point began as early as in the 1970s. According to the hydrological observations in 1934–1968, Nitani (1972) held that the surface of the NEC bifurcation point is about between 11?N and 14.5?N and the position of the bifurcation point moves north- wards with the increase of depth. Through analysis of the distribution of water masses, Toole(1988) estimated that the latitude of bifurcation was about 12?N. From the hydrological data from the Sino-American Joint Survey between September, 1987 and April, 1988, Toole(1990) defined the latitude where the transport flow func- tion is zero and concluded that the bifurcation latitude was near 13?N. Employing the model results, Qiu and Lukas (1996) defined the latitude where the average me- ridional speed is zero within the zone of two degrees of latitude along the western boundary and concluded that the bifurcation latitude was close to 13?N. According to the results of model calculation, Metzger and Hurlburt (1996) concluded that the average position of NEC moved in 15.6?N±0.6?N, shifting northwards with depth and reaching 18?N at the depth of 700m. On the basis of the climatic data of temperature and salinity, Qu(1999) defined the place where the average meridional speed is zero within two degrees of longitude from the coast as the position of bifurcation and concluded that near the surface the bifurcation line was at 13.5?N, at 500m in 18?N and the vertical average position between 0–500m was in about 15?N. By using the WOA (1994) historical observations, Qu(1999) concluded that in the upper thermocline, the NEC bifurcation point was at 15?N, moved northwards with depth and on the 27.2kgm?3isopycnic surface (about 800m), reached 20?N. By analysing the historical observations (WOA98), Qu and Lukas (2002) defined the latitude where the merid- ional transport within 5 degrees of longitude from the western boundary is zero as the latitude of bifurcation point and concluded that near the surface within 100m it was at 14?N, shifted northwards with depth and reached 23?N at 800m. By using the data of world ocean tempera- ture, salinity and dissolved oxygen in 1998 of WOD, Qu and Lukas (2003) found that the average position of the bifurcation latitude near surface (within 100 m) is 14.2?N, and if the effect of Ekman transport is added, it moves to 13.3?N while the bifurcation latitude shifts northwards with depth and at the depth of 800m, it is located in 20?N. Based on the calculated results of the model, Yaremchuk and Qu (2004) defined the latitude of the mean merid- ional speed change symbol and it was derived from cal- culation that the NEC average position is 14.3?±0.7?N. By employing the computed results of the high resolution OGCM model, Kim(2004) defined the latitude where the average meridional speed is zero within two degrees of longitude away from the coast of the Philip- pines as the bifurcation latitude and obtained the annual average bifurcation latitude of 15.5?N, which shifts northwards with depth, and the bifurcation latitude moves from 14.3?N at the surface to 16.6?N at 500 m. By use of the WOCE drifting buoy data in 1987–1998, Li(2005) defined that the position of the bifurcation point is between the trajectories of the buoy west of 130?E turning southwards and northwards. And in the case of the trajec- tories of the buoy turning southwards and northwards that cross west of 130?E, the latitude of the bifurcation point is defined as the latitude where the buoy trajectories cross and the surface bifurcation latitude is estimated to be between 11?N and 14.7?N. Wang and Hu (2006) used the satellite altimeter data (October, 1992–December, 2004) and concluded that the bifurcation latitude at the NEC western boundary surface is located at 13.4?N. Zhang(2008) used the satellite altimeter data of high spatial and temporal resolution to calculate the geostrophic current and defined the average latitude where the velocity gradient quickly increases and the me- ridional velocity is zero when reaching the shore as the criterion by which to determine the latitude of bifurcation. And the annual average bifurcation latitude was estimated to be 13.4?N.

    It can be seen that scientists (Zhai and Hu, 2012) have done a lot of researches on the flow field structure and bifurcation position of the western boundary current system, but most scholars located the bifurcation point in terms of the meridional velocity of the flow field, and as there are many factors affecting NEC and the change is complex, the difference in the results obtained from choosing to average over different width ranges is greater (Kim, 2004). Furthermore, even if the position of bifurcation point is determined, it is still impossible to reflect very well the bifurcation situation of the whole current system and obtain more detailed bifurcation fea- tures of the flow field. Hang and Wang (2001) and Wang and Huang (2005) proposed the method of quantitatively describing the barotrophic sea channel by wind stress, and that of quantitatively describing the baroclinic channel in recent years, by which to research into and analyse the property of the channel transport change with latitude. However, they did not make further research on the fea- tures of the bifurcation line.

    This paper compared the north Equatorial Current in the Pacific and tried to overcome the above mentioned shortcoming by using a new computational method,, identifying the position and change of bifurcation at each layer by calculating the isopycnal line, describing the NEC bifurcation line and making systematic analysis of its form and change pattern, analysing the plane distribu- tion of the bifurcation line on the two-dimensional plane, stratifying the data to obtain the vertical distribution of bifurcation lines and lastly deriving the climatic, seasonal and interannual changes of the bifurcation line though statistical analysis.

    2 Data and Methods

    2.1 Data Description

    This paper used the SODA (Simple Ocean Data As- similation) database version 2.0.2 (Carton and Giese, 2005), which is based on the GFDL (Geophysical Fluid Dynamics Laboratory) reanalysis data of the Parallel Ocean Program physics marine numerical model and data assimilation technology.

    This model includes the terrigenous freshwater flux with vertical resolution of 10m near the surface. The model’s wind stress forcing field is constructed by the COADS (Comprehensive Ocean-Atmosphere Data Set) and NECP (National Centers for Environmental Predic- tion) data (after 1992), of which the long-term trend of wind stress data not in harmony with the sea surface pressure trend observed has been eliminated. For the spe- cific description of these datasets involved in the research, refer to Carton and Giese (2008). The SODA data prod- ucts covers the 50 years from 1958 to 2007, with the global longitude range from 0.25? to 360.25? (from west to east) and the latitudinal range from ?75.25? to 89.25? (from south to north); the data have horizontal resolution 0.5?×0.5? and are vertically divided into 40 layers. The horizontal and vertical resolutions are high enough for studying the bifurcation of NEC.

    2.2 Method of Calculation and Data Processing

    The sea area selected in this study is in the North Pa- cific (100.25?E–120.25?W, 2.25?S–57.25?N). The paper used the data on the equipotential density surface layer by layer for analyzing the path. The specific method of cal- culation is as follows:

    The first step is to calculate the grid thermohaline data to get the potential temperature and density on thecoor- dinate (Except otherwise specified, the density or poten- tial density mentioned here after also represents the po- tential density). The layer-by-layer potential density av- eraged over the region is found and then the potential density layer is divided in equal intervals. In choosing the potential density layer, if it is too small, the low density water can only be reserved in the equatorial part of the west Pacific, which cannot display the path of water par- ticles; if it is too large, the bifurcation of western bound- ary trends to be blurred and disappears and so cannot be distinguished.

    The second step is to carry out the coordinate trans- formation, turning thecoordinate of raw data into the isopycnal surface coordinate for our analysis. First, the multiple density stratification is used to carry out the multi-layer division in the density stratification range and the algorithm of interpolation is employed to calculate this density range, and the meridional velocity, zonal ve- locity, temperature and salinity in isopycnal layer. Then, the isopycnal layer thickness is chosen according to the weight to represent the range. For the expanded and den- sified density layer, filter value taking is carried out ac- cording to the weight (the difference in the distance to the calculation point), and again the calculation is done to the required isopycnal surface, thus obtaining the variable required for the calculation under the density coordinate.

    The third step is to carry out the evaluation of integrals for the path with the nonlinear, high-order, one-step nu- merical algorithm of Runge-Kutta. The Runge-Kutta method is well-known as a multilevel algorithm, which is different from the integration method of ordinary differ- ential equations such as Adams-Bashorth, Adams-Monl- ton,(multiple methods) and it does not need to recal- culate the unknown function value of each order in the differential equation. It requires us to calculate the values offor a simple correction. The basic idea is to use the value of the intermediate step to replace the higher de- rivative.

    This paper uses for the first time the isopycnal surface stream line tracing and judging algorithm (Lagrangian particle tracking technique is used in this study), giving the accurate trace points of the NEC northern branch channel and southern branch channel and its bifurcation line on the calculated level by starting from the grid ve- locity field and tracking the stream lines within the chan- nels at different density layers. If the same calculation is done for the density layers, we can get the whole three-dimensional NEC western boundary current system. So this paper gives for the first time the precisely quanti- fied structure of the NEC western boundary channel and its bifurcation condition.

    3 Climatic Characteristics of the Pacific NEC Western Boundary Bifurcation Line

    This paper does not adopt the more limited method of bifurcation point, rather the integration path method to obtain the bifurcation line in the research. Fig.1 gives the long-term averaged stratified bifurcation line of the NEC western boundary. In the layer-by-layer change, with the increase of depth, the bifurcation line shifts northwards, which is consistent with the previous findings that in the sense of annual average the latitude of the western boundary bifurcation point moves northwards from the surface to deep layers. For the bifurcation line used in this paper, its distribution form of being high in the west and low in the east may be seen and the layer-by-layer bifur- cation lines tend to be parallel, do not overlap in the ver- tical direction and density changes little in the deeper layers, so the degree of separation between bifurcation lines increases on the deep-layer isopycnal surface. The latitudinal difference of a simple bifurcation line between the east and west ends of 130?E–170?E is about 1.5?.

    For the poleward shift of the NEC western boundary bifurcation line with depth, we approach this phenomenon from the oceanic circulation basis. In the vorticity equa- tion, the motion reaches a constant state and at the same time the exogenous process can be neglected (large-scale motion):

    Fig.1 Long-term averaged NEC western boundary stratification (23.4–26.4kgm?3) bifurcation lines.

    whereωis absolute vorticity;is horizontal flow veloc- ity;is density,is pressure.

    The relative vorticity of the large-scale motion is far smaller than the planetary vorticity:

    whereis the Coriolis parameter.

    The component form of baroclinic fluid may be ex- pressed as:

    hereis zonal coordinate with east positive;is merid- ional coordinate with north positive;is vertical coordi- nate with down positive.

    This is the thermogenic wind relationship, which con- structs the relationship between the variation of vertical flow velocity and the horizontal density (temperature), which is a very important relationship between flow ve- locity and density (temperature) in the ocean. Further- more, it is derived from the magnitude relation:

    In the meantime, for the vertical flow velocity shear and horizontal density gradients, we have:

    . (3-5)

    As the gradient of salinity is smaller, when the density (temperature) increases polewards, the increase of the current with depth quickly produces the flow westwards, as a result of which, the centre of the subtropical gyre (anticyclonic) moves polewards with the increase of depth (Liu, 2011). Therefore, we get the image of the shift polewards of the western boundary bifurcation line with depth due to the effect of the subtropical gyre.

    Figs.2 and 3 give the long-term averaged distribution of the NEC western boundary bifurcation lines in the sec- tion of 130?E under thecoordinate and potential density coordinate. Under the depth coordinate it may be seen that the depth of the first layer density 23.4kgm?3 in the whole section of 130?E over a span of 8?N–25?N between south and north is between 75m and 125m; on the depth coordinate are contained the information on the equal potential density line, isotherm and zonal velocity field. On the section of 130?E near the western boundary, the isotherm and the isopycnal line are basically parallel. At the same time, the upper temperature gradient in the low latitude area is greater than that in the high latitude area and the isopycnal line is far shallower. For instance, the isopycnal line of 26.4kgm?3is 210m at about 8?N, while at about 25?N it amounts to 555m. It can be seen from the figure that the western boundary bifurcation latitude in this section is not at the extremum centre of zonal veloc- ity, but is to the north a little. On the section of depth co- ordinate, the depth from the first layer to the last layer totals 500m in depth; the bifurcation line latitude varies for about 4?, with each 100m deepening the bifurcation latitude moves northwards for about 1 degree and the northward distance in the upper layer is slightly larger than that in the lower layer. In the density coordinates of Fig.3, the bifurcation line points shift in the density layer. As the upper layer is relatively thinner, the variation of bifurcation line points in the density coordinates is not obvious, while in the lower layer there is a distinct northward shift. This has been verified in Fig.2 in which in area of bifurcation line points, it may be clear that it is located at the largest bended location,, near the low-lying (deeper) place of the isopycnal surface.

    Fig.2 Long-term averaged 130?E sectional (depth coordinated) drawing, in which there are the NEC western boundary bifurcation lines (grey squares), isopycnal lines (solid lines) and equal zonal velocity lines (dotted lines).

    Fig.3 Long-term averaged 130?E sectional (depth coordinates) drawing, in which there are the NEC western boundary bifurcation lines (grey squares), isobaths lines (solid lines) and equal zonal transport lines (dotted lines).

    4 Seasonal Variation Features of the NEC Western Boundary Bifurcation Line

    Fig.4 gives the seasonal variations of the fine verti- cally-averaged NEC western boundary bifurcation line (23.4kgm?3–26.4kgm?3), derived on the basis of the channel algorithm. In winter (November, December and January), the bifurcation line is relatively straight and the difference in the latitude of bifurcation is not obvious in the east and west directions, which is related to the dis- tribution of NEC flow pattern in the winter, being about 15.7?N on the average. The bifurcation line is located at the higher latitudes throughout the year, being northern- most in November. Starting from February it obviously begins to move southwards gradually, showing inclining state of being high in the east and lower in the west. In June the westernmost end of the bifurcation line moves to the southernmost position in the year, in about 14.3?N on the average. This coincides with the findings of Qu and Lukas (2002) by use of the data on the west Pacific tem- perature, salinity, DO concentration,The research makes an integral calculation of the dynamic height and its corresponding circulation from surface to 1000 m, and in the light of the Ekman transport, concludes that the NEC bifurcation point begins to move southwards in January, reaches the southernmost end and then moves northwards, reaching the northernmost end in December. The time difference is mainly due to the different integra- tion methods used. This paper carries out the vertical in- tegration according to the density coordinate. And the calculated density layers are mostly within 100–600m, not including all the intervals of integration in 0–1000m. After June, the bifurcation line begins to shift northwards, the east-to-west dip is more obvious and the difference in latitude between the east and west ends of the line in au- tumn reaches the highest throughout the year, up to 2.8?, while such difference in winter when the bifurcation line is relatively straight is only 0.9?, and with the lapse of time, the bifurcation line moves northwards and the dip angle decreases gradually.

    Fig.4 Seasonal variations of the vertically averaged NEC western boundary bifurcation line (23.4–26.4kgm?3).

    Fig.5 is the seasonal variations of the NEC western boundary bifurcation lines layer by layer. In each sheet, there are 16 curves, representing the bifurcation lines in the 16 density layers. The distribution of the bifurcation lines on all the isopycnal surfaces in the whole area is relatively regular, and seasonally the latitude of bifurcation line moves northwards with depth and basically is parallel with the bifurcation line of the upper density layer. In winter, the bifurcation line is relatively higher in latitude and straight in shape while in summer and autumn it in- clines and at the west end of the line the wind direction changes and the wind stress magnitude is lower as com- pared with that in spring and winter. The location repre- sented by the first layer bifurcation line is not different from that indicated by the vertically averaged seasonal change,, it is moving northwards in winter and southwards in summer, being straight in winter and in- clining in autumn. The change in shape is displayed more obviously in the layer-by-layer bifurcation line. Among others, there exists a bifurcation line ridge layer by layer (the line bulges northwards), and the deviation of the ridge from the main axis of the bifurcation line may reach about 1.2?; it belongs to an obvious abnormal fluctuation. Such phenomenon begins to appear and develops in March and April; it speeds up in July, the intensity being lower at about 168?E, and in August propagates west- wards to 166?E, with a tendency to increase. In Septem- ber, the ridge moves to 163?E, further strengthening. By October, the ridge with the largest intensity has reached the location of 158?E; in November the follow-up fluc- tuation of October forms another ridge, which propagates westwards; and the former ridge moves westwards to about 155?E to form a double ridge with its intensity also dropping significantly. In December, the ridge propagates to the western boundary, which results in the up dip of the western boundary bifurcation point; and then it basically weakens and disappears. Figs.3–9 show the seasonal change in the NEC western boundary bifurcation line’s vertical dipping. A simple point-to-point method of inter- polation is used to treat the degree of diffusion of the layer-to-layer bifurcation line from bottom to surface along the longitudinal direction. The phenomenon with the maximum diffusion magnitude of the ridge in the whole calculated layer exceeding 4.4? appears in the spring and summer months of May and June, while the minimum magnitude of diffusion smaller than 2.1? occurs in the autumn months of September and October. It can be seen from the time evolution figure that the diffusion amplitude of the bifurcation line as a whole in January and February is smaller, the degree of diffusion is smaller, and the degree of diffusion in the western part of the line is even weaker than that in the eastern part. In March, the degree of diffusion of the bifurcation line in the vertical direction begins to increase and the amplitude fluctuation grows. By June, the vertical amplitude reaches the maxi- mum, generally exceeding 3.6? from west to east, which is the largest throughout the year. In July, the diffusion amplitude begins to drop and upon entering the autumn months of August, September and October, it contracts to the minimum level and part of the variation amplitude is as low as below 2.4?, which is the smallest throughout the year. Starting from November, the vertical variation am- plitude of the NEC western boundary bifurcation line again grows gradually, so we can say that the diffusion amplitude of the bifurcation line varies regularly with season.

    Fig.5 Seasonal variations of the layer-by-layer NEC western boundary bifurcation lines.

    Fig.7 gives the latitudes of the Pacific NEC western boundary bifurcation line and the depth values corre- sponding to it. In terms of the movement of the western boundary bifurcation line, as far as the 140m and 160m depth lines are concerned, the 160m depth line is located near the surface in June, which shows the depth of the bifurcation line is the largest in June. And in December, the 140m depth line is located far away from the surface, showing that the bifurcation line in December is the shal- lowest. Fluctuations are constantly seen on the bifurcation line to propagate from west to east. Starting from May there are two obvious wave crests located at the longi- tudes of 145?E and 170?E from top to bottom, constantly propagating westwards. By October the wave crest propa- gating from 170?E has developed most strongly while the 145?E wave crest has propagated up to the western boundary, thus causing the bifurcation line within 10 de- grees of longitude of the western boundary to swing from the southwest-northeast direction in May to the north- west-southeast direction in December and lowest latitu- dinal position to shift from the western boundary to about 140?E with a longitudinal difference of over 10 degrees.

    From the layer-by-layer angle with time as the variation axis, it may be clearly seen that the latitudinal change propagates from west to east and that the depth is the largest at the lowest latitude. Another phenomenon is that the lowest latitude of the western boundary bifurcation occurs around June while the latitude at 145?E which is the inflection point of the high value latitude propagation occurs around October, but at the bottom,, 26kgm?3, the lowest signal of the western boundary latitude occurs around July, the highest latitude is postponed to occur around November and possibly the signal that first changes propagates from the upper layer to the lower layer.

    5 Response of the Location of the NEC Western Boundary Bifurcation Line to the ENSO Event

    El Ni?o and La Ni?a years are chosen according to the Ni?o 3.4 exponent. The Ni?o 3.4 abnormal temperature maximum occurs in winter. The spring in the year when ENSO develops is usually chosen as the initial developing season and a multi-seasonal bifurcation line comparison is made with season as unit. Analysis is made according to four seasons of spring (March–May), summer (June–August), autumn (September–November) and winter (De- cember–February), which may be further divided into several time periods of the initial spring (March–May), developing summer (June–August), developing summer (June–August), developing autumn (September–Novem- ber), peak winter (December–February) and weakening spring (March–May) on the basis of the process of de- velopment-peak-weakening of ENSO and the variations of the bifurcation line are obtained from calculation as follows:

    Figs.8–15 give separately the NEC western boundary bifurcation lines in the spring (initial), summer (develop- ing), autumn (developing), and winter (peak) in the year when ENSO occurs and those in the next year’s spring (weakening), summer (weakening), autumn (weakening), and in the figures, the three lines indicate the El Ni?o year (Red Line), La Ni?a year (Blue Line), Long-Term Average (Black Line). It is usually believed that the spring of the year when ENSO occurs is the period when ENSO begins to develop, and in the spring of developing period, the upper bifurcation line first appears in the east to north in the form that it is higher (lower) of latitude in the El Ni?o (La Ni?a) year relative to normal years. With the change of seasons, up to the summer of the year when ENSO occurs, the three bifurcation line are completely separated from each other, the highest (lowest) latitude in the El Ni?o (La Ni?a) year. The bottom flow pattern is confused in the La Ni?a year and the situation in autumn is similar to that in summer, which will not be discussed in detail. The winter bifurcation lines in the year when ENSO occurs come back to the average state, the separa- tion degree at the east ends of the three bifurcation lines is reduced, the bifurcation lines begin to draw near, but their west ends still have a higher degree of separation, which is in consistent with the developing period.

    Fig.7 NEC western boundary bifurcating line and the variations at its corresponding depths (the shadow part is the latitude values at the two ends of the line).

    Fig.8 NEC western boundary bifurcation line in the initial spring: El Ni?o year (red line), La Ni?a year (blue line), long-term average (black line).

    In the spring of the second year when ENSO occurs, the signed of the bifurcation line in the east by south (by north) further increases, propagating westwards to around 150?N, higher (lower) in the west in the El Ni?o year (La Ni?a year),which the bifurcation line in average years is located in the middle. The main intersection point of the summer bifurcation lines in the second year propagates up to the western boundary. In other parts except the western boundary, the El Ni?o (La Ni?a) year’s lower (higher) average lines are in the middle, and in the El Ni?o year there appear obvious fluctuation ridges of bi- furcation lines, the distribution patterns being basically constant in the upper and lower layers. In the second year’s autumn following the year when ENSO occurs, the bifurcation line transforms into the state where the El Ni?o (La Ni?a) year’s lower (higher) average line is in the middle, and in the meanwhile, the fluctuating peak formed in summer continues to propagate west wards, and the fluctuation in the El Ni?o year is stronger than that in the La Ni?a year. In the second year’s winter fol- lowing the year when ENSO occurs, the relative average value of the ENSO occurs, the relative average value of the NEC western boundary bifurcation line falls as a whole and in the following season returns to normal. By then, this ENSO event has ended.

    Fig.9 NEC western boundary bifurcation line in the developing summer: El Ni?o year (red line), La Ni?a year (blue line), long-term average (black line).

    Fig.10 NEC western boundary bifurcation line in the developing autumn: El Ni?o year (red line), La Ni?a year (blue line), long-term average (black line).

    Fig.11 NEC western boundary bifurcation line in the peak winter: El Ni?o year (red line), La Ni?a year (blue line), long-term average (black line).

    Fig.12 NEC western boundary bifurcation line in the weakening spring: El Ni?o year (red line), La Ni?a year (blue line), long-term average (black line).

    Fig.13 NEC western boundary bifurcation line in the weakening summer: El Ni?o year (red line), La Ni?a year (blue line), long-term average (black line).

    Fig.14 NEC western boundary bifurcation line in the weakening autumn: El Ni?o year (red line), La Ni?a year (blue line), long-term average (black line).

    Fig.15 NEC western boundary bifurcation line in the weakening winter: El Ni?o year (red line), La Ni?a year (blue line), long-term average (black line).

    6 Conclusions

    By use of the SODA data, this paper studies the cli- matic, interannual and seasonal variations of the NEC western boundary bifurcation line. It gives a visual dis- play of the channel bifurcation line proposed by this paper, makes an analysis of the position and its physical quantity change and obtains the following results with regularity:

    1) The long-term averaged NEC western boundary bi- furcation line shifts northwards with depth, and its main mechanism could be explained by the thermal wind rela- tionship in the ocean. The western boundary point of the bifurcation line is from 13.8?N of the 23.4kgm?3isopy- cnal surface to 17.7?N of the 26.4kgm?3isopycnal sur- face. It may be seen from the sections in different longi- tudes: with each 100 meters deepening, the latitudinal bifurcation moves northwards for about 1 degree and the northward shifting distance in the upper layer is slightly larger than that in the lower layer. The bifurcation line is located north of the centre with the maximum meridional velocity and near the low-lying (deeper) place of the isopycnal surface.

    2) The seasonal variation of the vertically averaged NEC western boundary bifurcation line is characterized by south-north moving and east-west dipping on the whole and the western boundary bifurcation point is a part of the whole movement of the bifurcation line. In terms of the zonal position of bifurcation line, it is north- ernmost in December with an average latitude of 15.7?N; In June, it is southernmost with an average latitude of about 14.3?N. The difference in the winter bifurcation latitude in the east and west directions is not obvious and the bifurcation line is relatively straight; The spring bi- furcation line begins to show a dipping state of being high in the east and low in the west, and the autumn latitudinal difference in the east and west directions is as large as over 2.8?.

    3) The seasonal variation of the NEC western boundary bifurcation line has a significant feature of the fluctuation propagating westwards, indicating that the bifurcation point is obviously modulated by the westward propagate- ing fluctuation (Rossby wave). Starting from July, the ridge occurring at 168?E (The bifurcation line bulges northwards) propagates westwards and is strengthened; it moves westwards in October to the place west of 158?E, with the amplitude reaching the maximum; In November it continues to propagate westwards but its intensity is obviously weakened; in December it propagates to the western boundary where it is basically weakened and disappears. The bifurcation lines of deeper layers in No- vember and December have a shape of three ridges and two troughs, but at the surface this distribution of forms is not distinct. In terms of the south-north movement of the NEC western boundary bifurcation line, the signal of latitude change in the lower layer lags behind that in the upper layer and the westward propagation of the bifurca- tion line ridge may cause the western boundary bifurca- tion point to swing between south and north. The bifurca- tion line in each layer has a northward jump by a large margin (The average latitude of bifurcation line in each layer has a northward jump of over 1.6?), which in time is in agreement with the first northward jump of the atmos- pheric subtropic high pressure system. In March the bi- furcation lines in all layers all withdraw to the south. Therefore the bifurcation lines may be divided into two clusters: being concentrated in the south in March–June and in the north in July–February. Corresponding to this, the average layer thickness of layers along the bifurcation line is also relatively small in March–June and larger in other months, which should be the result of vorticity conservation.

    4) The interannual variation of the NEC western boundary bifurcation line shows that in the developing and strengthening period of El Ni?o (La Ni?a), the bifur- cation line is to the north (to the south). Base on the proc- ess of development-peak-weakening of ENSO, several time periods are divided,, initial spring (March–May), developing summer (June–August), developing summer (June–August), developing autumn (September–Novem- ber), peak winter (December–February) and weakening spring (March–May). In the initial spring of El Ni?o, the bifurcation line is first in the east by north; in the devel- oping summer and autumn, the whole bifurcation line is to the north and reaches the maximum. In the peak winter, the bifurcation line restores the average state and the east part begins to go by south; in the weakening spring, the signal in the east by south further increases and propa- gates westwards. During the La Ni?a, the development of the bifurcation line is similar, but in opposite phase. Dur- ing the ENSO, there is an obvious feature of propagating westwards. The phenomenon that the maximum south-north shift of the western boundary bifurcation line oc- curs before the prime period of ENSO deserves further study in the future.

    Acknowledgements

    This work was supported by the National Natural Sci- ence Foundation of China (41206013, 41106004, 41376014, 41430963); Key Marine Science Foundation of the State Oceanic Administration of China for Young Scholar (2013203, 2012202, 2012223); POL Visiting Fellowship Program (Jun Song); the Public Science and Technology ResearchFundsProjectsofOcean(201205018,201005019); China Scholarship Council ([2008]3019, [2012]3013).

    Carton, J. A., and Giese, B. S., 2005. SODA: A reanalysis of ocean climate., 1: 1-30.

    Carton, J. A., and Giese, B. S., 2008. A reanalysis of ocean climate using simple ocean data assimilation (SODA)., 136: 2999-3017.

    Fine, R., Lukas, R., Bingham, F. M., Warner, M. J., and Gammon, R. H., 1994. The western equatorial Pacific is a water mass crossroads., 99: 25063-25080.

    Gordon, A. L., 1986. Interocean exchange of thermocline water., 91: 5037-5046.

    Huang, R. X., and Wang, Q., 2001. Interior communication from the subtropical to the tropical oceans., 31: 3538-3550.

    Johnson, G. C., and McPhaden, M. J., 1999. Interiod pycnocline flow from the subtropical to the equatorial Pacific Ocean., 29: 3073-3089.

    Kim, Y. Y., Qu, T., and Jensen, T, 2004. Seasonal and interannual variations of the North Equatorial Current bifurcation in a high-resolution OGCM., 109, C03040.

    Li, L. J., Liu, Q. Y., and Liu, W., 2005. Surface current speed andbifurcation of the North Equatorial Current in the Pacific Ocean., 35 (3): 370-374.

    Liu, Y. L., Wang, Q., Song, J., Zhu, X. D., Gong, X. Q., and Wu, F., 2011. Numerical study on the bifurcation of the North Equatorial Current., 10 (4): 305-313.

    Liu, Z., 1994. A simple model of the mass exchange between the subtropical and tropical ocean., 24: 1153-1165.

    Lu, P., McCreary, J. P., and Klinger, B. A., 1998. Meridional circulation cell and the source water of the Pacific equatorial undercurrent., 28:62-84.

    McCreary, J. P., and Lu, P., 1994. On the interaction between the subtropical and equatorial ocean circulation: The subtropical cell., 24: 466-497.

    Metzger, E. J., and Hurlburt, H. E., 1996. Coupled dynamics of the South China Sea, the Sulu Sea, and the Pacific Ocean., 101: 12331-12352.

    Nitani, H., 1972.. University of Washington Press, Washington, 129-163.

    Qiu, B., and Lukas, R., 1996. Seasonal and interannual variability of the North Equatorial Current, the Mindanao Current, and the Kuroshio along the Pacific western boundary., 101: 12315-12330.

    Qu, T. D., Meyers, J. G., and Godfrey, S., 1997. Upper ocean dynamics and its role in maintaining the annual mean western Pacific warm pool in a global GCM., 17: 711-724.

    Qu, T. D., Mitsudera, H., and Yamagata, T., 1998. On the western boundary currents in the Philippine Sea., 103 (4): 7537-7548.

    Qu, T. D., Mitsudera, H., and Yamagata, T., 1999. A climatology of the circulation and water mass distribution near the Phi- lippine coast., 29: 1488-1505.

    Qu, T., and Lukas, R., 2002. Depth distribution of the subtropical Gyre in the North Pacific., 58 (3): 525-529.

    Qu, T., and Lukas, R., 2003. The bifurcation of the North Equatorial Current in the Pacific., 33: 5-18.

    Song, J., Xue, H. J., Bao, X. W., and Wu, D. X., 2011. A spectral mixture model analysis of the Kuroshio variability and the water exchange between the Kuroshio and the East China Sea., 29 (2): 446-459.

    Toole, J. M., Zou, E., and Millard, R. C., 1988. On the circulation of the upper waters in the western equatorial Pacific Ocean., 35: 1451-1482.

    Toole, J., Millard, C., Wang, Z., and Pu, S., 1990. Observations of the Pacific North Equatorial Current bifurcation at the Philippine coast., 20: 307-318.

    Wang, Q., and Huang, R. X., 2005. Decadal variability of pycnocline flows from the subtropical to the equatorial Pacific., 35 (10): 1861-1875.

    Wang, Q., and Liu, Q. Y., 2000. The study on the Pacific Subtropical Cell., 1: 1-5.

    Wang, Q. Y., and Hu, D. X., 2006. Bifurcation of the North Equatorial Current derived from altimetry in the Pacific Ocean., 18 (5): 620-626.

    Webster, P. J., and Lukas, R., 1992. TOGA/COARE: The coupledocean-atmosphere response experiment., 73: 1377-1416

    Xu, D., and M-Rizzoli, P., 2013. Seasonal variation of the upper layer of the South China Sea and the Indonesian Seas: An ocean model study., 63: 103-130.

    Yaremchuk, M., and Qu, T. D., 2004. Seasonal variability of the large-scale currents near the coast of the Philippines., 34 (4): 844-855.

    Zhai, F. G., and Hu, D. X., 2012. Interannual variability of transport and bifurcation of the North Equatorial Current in the tropical North Pacific Ocean., 30 (1): 177-185.

    Zhang, X. D., Xiu, Y. R., Liu, J. F., Su, G., and Wang, Q. Y., 2008. The determination about the bifurcation latitude of the NEC and its variations., 25 (2): 33-41.

    (Edited by Xie Jun)

    DOI 10.1007/s11802-015-2594-0

    ISSN 1672-5182, 2015 14 (6): 957-968

    ? Ocean University of China, Science Press and Springer-Verlag Berlin Heidelberg 2015

    (February 6, 2014; revised March 12, 2014; accepted September 2, 2015)

    * Corresponding author. E-mail: thunder098@hotmail.com

    考比视频在线观看| 中文字幕另类日韩欧美亚洲嫩草| 国产精品一区www在线观看| 亚洲 欧美一区二区三区| 黑人高潮一二区| 99热国产这里只有精品6| 国产在线免费精品| 亚洲,欧美精品.| 在线观看免费视频网站a站| 亚洲图色成人| 美女国产高潮福利片在线看| 中国三级夫妇交换| 欧美xxⅹ黑人| 久久久国产精品麻豆| 久久久国产精品麻豆| 黄色一级大片看看| 热re99久久精品国产66热6| 久久久精品94久久精品| 五月伊人婷婷丁香| 制服丝袜香蕉在线| 国产高清不卡午夜福利| 亚洲,欧美,日韩| 熟女av电影| 久久婷婷青草| 老女人水多毛片| 99热全是精品| 热99国产精品久久久久久7| 在线观看免费高清a一片| 精品一区在线观看国产| 爱豆传媒免费全集在线观看| 另类亚洲欧美激情| 国产在线一区二区三区精| 亚洲精品456在线播放app| 999精品在线视频| 午夜久久久在线观看| 国产精品国产三级专区第一集| 日韩熟女老妇一区二区性免费视频| 久久毛片免费看一区二区三区| videos熟女内射| 久热久热在线精品观看| 性色avwww在线观看| 亚洲精品av麻豆狂野| 欧美精品国产亚洲| 亚洲av中文av极速乱| 人人妻人人澡人人爽人人夜夜| 亚洲精品久久成人aⅴ小说| 女人被躁到高潮嗷嗷叫费观| 女性被躁到高潮视频| 久久久久人妻精品一区果冻| 国产一区二区在线观看av| 亚洲一区二区三区欧美精品| 国产男女超爽视频在线观看| 考比视频在线观看| 日日啪夜夜爽| 久久人人爽人人片av| 国产精品久久久久久av不卡| 男女高潮啪啪啪动态图| av片东京热男人的天堂| 美女大奶头黄色视频| 国产av精品麻豆| 波野结衣二区三区在线| 久久国产精品大桥未久av| 精品人妻在线不人妻| 亚洲国产成人一精品久久久| 午夜激情av网站| 日韩一区二区三区影片| 热re99久久精品国产66热6| 麻豆精品久久久久久蜜桃| 下体分泌物呈黄色| 亚洲精品成人av观看孕妇| 国产精品久久久久久精品电影小说| 97人妻天天添夜夜摸| 夜夜骑夜夜射夜夜干| 91久久精品国产一区二区三区| 免费在线观看黄色视频的| 这个男人来自地球电影免费观看 | 最黄视频免费看| 插逼视频在线观看| 岛国毛片在线播放| 久久久久久久久久成人| 男女午夜视频在线观看 | 国产精品成人在线| 亚洲天堂av无毛| 黄片无遮挡物在线观看| 久久99蜜桃精品久久| 国产黄频视频在线观看| 欧美xxⅹ黑人| 91午夜精品亚洲一区二区三区| 婷婷色麻豆天堂久久| 黄片无遮挡物在线观看| 日韩一本色道免费dvd| 尾随美女入室| 精品一区二区三卡| 考比视频在线观看| 国产在线免费精品| 亚洲精品一二三| 一区二区日韩欧美中文字幕 | 亚洲国产精品国产精品| 欧美日韩亚洲高清精品| 妹子高潮喷水视频| 欧美3d第一页| 成人二区视频| 在线观看www视频免费| 蜜桃国产av成人99| 黄色 视频免费看| 久久久a久久爽久久v久久| 伊人久久国产一区二区| 国产成人aa在线观看| 老司机影院成人| 美女内射精品一级片tv| 黄色怎么调成土黄色| 国产亚洲最大av| 桃花免费在线播放| 99热国产这里只有精品6| 如日韩欧美国产精品一区二区三区| av网站免费在线观看视频| 午夜福利在线观看免费完整高清在| 免费av不卡在线播放| 久久久久精品人妻al黑| 蜜桃在线观看..| 两个人免费观看高清视频| 日韩视频在线欧美| 新久久久久国产一级毛片| 久久久久久人人人人人| 国产精品国产三级国产专区5o| 久久久久精品性色| 亚洲欧美日韩另类电影网站| 丝袜在线中文字幕| 亚洲国产成人一精品久久久| 国产精品99久久99久久久不卡 | 亚洲在久久综合| 99国产综合亚洲精品| 国产极品天堂在线| 欧美亚洲 丝袜 人妻 在线| 国产熟女午夜一区二区三区| 99热网站在线观看| 亚洲av电影在线观看一区二区三区| 美女福利国产在线| 国产在视频线精品| 咕卡用的链子| 一边亲一边摸免费视频| 九色成人免费人妻av| 国产精品一区二区在线不卡| 亚洲成人手机| 少妇人妻精品综合一区二区| 在线亚洲精品国产二区图片欧美| 大片免费播放器 马上看| av卡一久久| 91精品伊人久久大香线蕉| 夜夜骑夜夜射夜夜干| 春色校园在线视频观看| 狂野欧美激情性bbbbbb| 天天躁夜夜躁狠狠躁躁| 久久精品国产鲁丝片午夜精品| 亚洲国产毛片av蜜桃av| 国产av一区二区精品久久| 久久久欧美国产精品| 国产一区二区激情短视频 | 欧美日韩av久久| 国产成人aa在线观看| 曰老女人黄片| 美女视频免费永久观看网站| 久久精品国产a三级三级三级| 老女人水多毛片| 久久精品熟女亚洲av麻豆精品| 成年女人在线观看亚洲视频| 国产av一区二区精品久久| 亚洲欧美成人精品一区二区| 亚洲久久久国产精品| 深夜精品福利| 免费女性裸体啪啪无遮挡网站| 亚洲欧美一区二区三区黑人 | 赤兔流量卡办理| 久久久欧美国产精品| 热99久久久久精品小说推荐| 18+在线观看网站| 午夜免费男女啪啪视频观看| 欧美激情 高清一区二区三区| 伦精品一区二区三区| 亚洲精品美女久久久久99蜜臀 | 国产伦理片在线播放av一区| 成人午夜精彩视频在线观看| 国产一区二区三区综合在线观看 | 亚洲精品av麻豆狂野| 欧美精品av麻豆av| 精品久久国产蜜桃| 欧美少妇被猛烈插入视频| 久久免费观看电影| 日本午夜av视频| 国产亚洲午夜精品一区二区久久| 久久青草综合色| 人妻人人澡人人爽人人| 99热全是精品| 午夜影院在线不卡| 久久鲁丝午夜福利片| 中文字幕另类日韩欧美亚洲嫩草| 国产精品.久久久| 久久女婷五月综合色啪小说| 亚洲av欧美aⅴ国产| 亚洲伊人久久精品综合| 久久热在线av| www日本在线高清视频| 国产精品蜜桃在线观看| 国产精品国产三级国产专区5o| 国产一级毛片在线| 丝袜喷水一区| 国产成人一区二区在线| 国产成人精品福利久久| 91午夜精品亚洲一区二区三区| 亚洲国产av新网站| 亚洲情色 制服丝袜| 婷婷色综合www| 韩国高清视频一区二区三区| 久久精品国产亚洲av天美| 久久国产精品男人的天堂亚洲 | 亚洲国产av新网站| 国产高清国产精品国产三级| 丝袜美足系列| 51国产日韩欧美| 2021少妇久久久久久久久久久| 99九九在线精品视频| 亚洲欧美日韩另类电影网站| 国产高清三级在线| 欧美最新免费一区二区三区| 欧美日韩综合久久久久久| 久久人妻熟女aⅴ| 欧美精品一区二区免费开放| 少妇的丰满在线观看| 午夜免费鲁丝| www日本在线高清视频| 美女视频免费永久观看网站| av黄色大香蕉| 精品视频人人做人人爽| 波野结衣二区三区在线| 欧美日韩视频精品一区| 亚洲国产精品专区欧美| 自拍欧美九色日韩亚洲蝌蚪91| 久久午夜综合久久蜜桃| 丝袜美足系列| 九色亚洲精品在线播放| 国产精品蜜桃在线观看| 巨乳人妻的诱惑在线观看| 国产伦理片在线播放av一区| 国产精品一区二区在线观看99| av网站免费在线观看视频| 日日撸夜夜添| 日本猛色少妇xxxxx猛交久久| 日本猛色少妇xxxxx猛交久久| 国产男女内射视频| 国产免费视频播放在线视频| 丰满饥渴人妻一区二区三| 成年女人在线观看亚洲视频| 夫妻性生交免费视频一级片| 一本一本久久a久久精品综合妖精 国产伦在线观看视频一区 | 人人妻人人澡人人看| av国产精品久久久久影院| 久久国内精品自在自线图片| 在线免费观看不下载黄p国产| 在线观看www视频免费| 精品人妻在线不人妻| 国产男女超爽视频在线观看| 亚洲色图 男人天堂 中文字幕 | 亚洲国产精品成人久久小说| 成年人午夜在线观看视频| 妹子高潮喷水视频| 精品人妻在线不人妻| 久久久久精品人妻al黑| 汤姆久久久久久久影院中文字幕| 男女高潮啪啪啪动态图| 国产成人aa在线观看| 久久精品aⅴ一区二区三区四区 | 久久精品国产亚洲av天美| 亚洲精品美女久久久久99蜜臀 | 亚洲精品自拍成人| av免费在线看不卡| 亚洲国产最新在线播放| 亚洲图色成人| videosex国产| 亚洲美女黄色视频免费看| 国产国语露脸激情在线看| 男女边吃奶边做爰视频| 少妇猛男粗大的猛烈进出视频| 蜜桃国产av成人99| 看免费成人av毛片| 免费观看av网站的网址| 国产黄色免费在线视频| 日韩三级伦理在线观看| 国产免费视频播放在线视频| 韩国高清视频一区二区三区| 国产成人精品一,二区| 国产成人精品福利久久| 这个男人来自地球电影免费观看 | 成人影院久久| 春色校园在线视频观看| 啦啦啦啦在线视频资源| 另类亚洲欧美激情| 1024视频免费在线观看| 少妇被粗大猛烈的视频| 国产视频首页在线观看| 国产在视频线精品| 久久久久久久大尺度免费视频| 少妇被粗大的猛进出69影院 | 国产熟女午夜一区二区三区| 男女高潮啪啪啪动态图| 亚洲欧美清纯卡通| 女的被弄到高潮叫床怎么办| 国产成人午夜福利电影在线观看| 欧美xxⅹ黑人| 亚洲综合色惰| 日日摸夜夜添夜夜爱| 免费黄色在线免费观看| 国产又爽黄色视频| 波野结衣二区三区在线| 哪个播放器可以免费观看大片| √禁漫天堂资源中文www| 性色avwww在线观看| 国产欧美日韩一区二区三区在线| 久久毛片免费看一区二区三区| 日本-黄色视频高清免费观看| 又大又黄又爽视频免费| 国精品久久久久久国模美| 欧美日韩亚洲高清精品| 欧美变态另类bdsm刘玥| a级毛片在线看网站| 多毛熟女@视频| 少妇人妻精品综合一区二区| 高清视频免费观看一区二区| 精品国产一区二区三区久久久樱花| 国产极品粉嫩免费观看在线| 免费观看性生交大片5| 热re99久久精品国产66热6| 深夜精品福利| 日韩伦理黄色片| 毛片一级片免费看久久久久| 精品99又大又爽又粗少妇毛片| 亚洲在久久综合| 久久精品久久久久久噜噜老黄| 好男人视频免费观看在线| 丝袜喷水一区| 国产精品 国内视频| 黑人猛操日本美女一级片| 亚洲欧美一区二区三区国产| 男女无遮挡免费网站观看| 天堂中文最新版在线下载| av又黄又爽大尺度在线免费看| 国产精品嫩草影院av在线观看| 午夜免费观看性视频| 91国产中文字幕| 91精品伊人久久大香线蕉| 涩涩av久久男人的天堂| 看十八女毛片水多多多| 国产极品天堂在线| 久久综合国产亚洲精品| 另类精品久久| www.av在线官网国产| 99香蕉大伊视频| 精品国产国语对白av| 午夜影院在线不卡| 欧美精品人与动牲交sv欧美| 久久综合国产亚洲精品| 亚洲伊人色综图| 精品国产一区二区三区久久久樱花| 99久久中文字幕三级久久日本| 99久国产av精品国产电影| 一级爰片在线观看| 欧美精品人与动牲交sv欧美| 高清av免费在线| 另类精品久久| 亚洲成人av在线免费| 少妇的逼好多水| 免费看av在线观看网站| 久久鲁丝午夜福利片| 国产精品无大码| 精品久久久久久电影网| 午夜福利视频精品| 国产精品一区www在线观看| 国产色婷婷99| 亚洲美女黄色视频免费看| av国产久精品久网站免费入址| 国产亚洲av片在线观看秒播厂| 99视频精品全部免费 在线| 日韩大片免费观看网站| 中文乱码字字幕精品一区二区三区| 精品一区二区三卡| 91午夜精品亚洲一区二区三区| 成人影院久久| 如何舔出高潮| 国产成人精品在线电影| av免费在线看不卡| 9热在线视频观看99| 久久精品aⅴ一区二区三区四区 | 一级黄片播放器| 午夜福利,免费看| 婷婷色综合大香蕉| 亚洲成人手机| 久久久a久久爽久久v久久| 午夜福利在线观看免费完整高清在| 日韩中文字幕视频在线看片| 亚洲精品第二区| 亚洲,欧美,日韩| 亚洲国产av影院在线观看| 2021少妇久久久久久久久久久| 18禁国产床啪视频网站| 日韩伦理黄色片| 性色avwww在线观看| 亚洲欧美色中文字幕在线| 男女下面插进去视频免费观看 | 久久久久久久国产电影| 日本黄大片高清| 视频中文字幕在线观看| 亚洲少妇的诱惑av| 国产精品 国内视频| 97在线视频观看| 欧美 日韩 精品 国产| 国产免费一级a男人的天堂| 最近中文字幕高清免费大全6| 日本91视频免费播放| 黄片无遮挡物在线观看| 午夜91福利影院| 亚洲丝袜综合中文字幕| 婷婷色麻豆天堂久久| 国产精品一区二区在线不卡| 亚洲国产成人一精品久久久| 欧美日韩成人在线一区二区| 两个人看的免费小视频| 九九爱精品视频在线观看| 男女下面插进去视频免费观看 | 国产亚洲精品第一综合不卡 | 国产乱来视频区| 精品酒店卫生间| 免费不卡的大黄色大毛片视频在线观看| 欧美日韩av久久| 九草在线视频观看| xxx大片免费视频| 日韩一区二区三区影片| 久久久久久久久久人人人人人人| 国产成人精品婷婷| 三上悠亚av全集在线观看| 91午夜精品亚洲一区二区三区| 嫩草影院入口| 国产不卡av网站在线观看| 日韩制服骚丝袜av| 水蜜桃什么品种好| 成人免费观看视频高清| 国产国拍精品亚洲av在线观看| 中文字幕亚洲精品专区| 边亲边吃奶的免费视频| 青青草视频在线视频观看| 精品亚洲乱码少妇综合久久| 日产精品乱码卡一卡2卡三| 波野结衣二区三区在线| 人人妻人人澡人人爽人人夜夜| 国产亚洲欧美精品永久| 欧美3d第一页| 免费女性裸体啪啪无遮挡网站| 美女xxoo啪啪120秒动态图| 新久久久久国产一级毛片| 亚洲精品自拍成人| 亚洲国产最新在线播放| 深夜精品福利| 亚洲内射少妇av| 日日啪夜夜爽| 亚洲熟女精品中文字幕| 2021少妇久久久久久久久久久| 一本一本久久a久久精品综合妖精 国产伦在线观看视频一区 | 天天躁夜夜躁狠狠躁躁| 国产女主播在线喷水免费视频网站| 两个人看的免费小视频| 97在线人人人人妻| 18在线观看网站| 18禁在线无遮挡免费观看视频| 日韩欧美一区视频在线观看| 成人黄色视频免费在线看| 2021少妇久久久久久久久久久| 免费在线观看完整版高清| 久久久久久伊人网av| 麻豆乱淫一区二区| 欧美日韩综合久久久久久| 久久ye,这里只有精品| 精品亚洲乱码少妇综合久久| 男女边摸边吃奶| 精品少妇内射三级| 国产精品国产av在线观看| 亚洲国产av新网站| 99热全是精品| 国产av码专区亚洲av| 黄片播放在线免费| 国产成人精品一,二区| 亚洲色图 男人天堂 中文字幕 | 99久久人妻综合| 黄片无遮挡物在线观看| 国产精品一区www在线观看| 99视频精品全部免费 在线| 久久精品久久精品一区二区三区| 赤兔流量卡办理| 桃花免费在线播放| 99热这里只有是精品在线观看| 亚洲成色77777| 国产精品一区二区在线不卡| tube8黄色片| 少妇人妻 视频| 亚洲国产欧美日韩在线播放| 这个男人来自地球电影免费观看 | 大话2 男鬼变身卡| 啦啦啦中文免费视频观看日本| 97超碰精品成人国产| 日韩av免费高清视频| 日本91视频免费播放| 久久久久精品久久久久真实原创| 99热这里只有是精品在线观看| 最近最新中文字幕大全免费视频 | 在线观看国产h片| 国产色婷婷99| 99久久中文字幕三级久久日本| 午夜精品国产一区二区电影| 两性夫妻黄色片 | 国产xxxxx性猛交| 亚洲伊人久久精品综合| 成人二区视频| 亚洲精品日韩在线中文字幕| 欧美国产精品va在线观看不卡| 国产高清不卡午夜福利| av在线播放精品| 国产精品国产av在线观看| 日韩av免费高清视频| av在线老鸭窝| 日韩精品有码人妻一区| 亚洲成人一二三区av| 街头女战士在线观看网站| 韩国av在线不卡| 亚洲激情五月婷婷啪啪| 在线 av 中文字幕| 精品国产一区二区三区久久久樱花| 久久精品久久精品一区二区三区| 国产精品国产av在线观看| 国产亚洲午夜精品一区二区久久| 国产免费又黄又爽又色| 亚洲伊人久久精品综合| 纯流量卡能插随身wifi吗| 91aial.com中文字幕在线观看| 侵犯人妻中文字幕一二三四区| 久久久久久久久久久久大奶| www日本在线高清视频| 免费观看av网站的网址| 高清欧美精品videossex| 全区人妻精品视频| 午夜福利视频精品| 久久鲁丝午夜福利片| 国产综合精华液| 少妇被粗大的猛进出69影院 | 在线观看免费高清a一片| 欧美激情极品国产一区二区三区 | 18+在线观看网站| 伦理电影免费视频| 日韩一区二区视频免费看| 国产一区亚洲一区在线观看| 十八禁高潮呻吟视频| 国产麻豆69| 国产深夜福利视频在线观看| 午夜免费男女啪啪视频观看| 久久这里只有精品19| 久久久久久久国产电影| 中文字幕人妻熟女乱码| 国产精品蜜桃在线观看| 日本色播在线视频| 美女视频免费永久观看网站| 国产一区二区三区av在线| 丰满饥渴人妻一区二区三| 亚洲精品久久久久久婷婷小说| 最近的中文字幕免费完整| 日韩一本色道免费dvd| 一二三四在线观看免费中文在 | 自拍欧美九色日韩亚洲蝌蚪91| 日本欧美视频一区| 国产国拍精品亚洲av在线观看| 欧美精品高潮呻吟av久久| av免费在线看不卡| 十八禁高潮呻吟视频| 亚洲伊人久久精品综合| 丝瓜视频免费看黄片| 搡女人真爽免费视频火全软件| 久久久久久久国产电影| 久久精品国产自在天天线| 晚上一个人看的免费电影| 哪个播放器可以免费观看大片| 成人二区视频| 哪个播放器可以免费观看大片| 婷婷色av中文字幕| 成人黄色视频免费在线看| 丝袜在线中文字幕| 欧美日韩精品成人综合77777| 香蕉精品网在线| av福利片在线| 欧美成人午夜免费资源| 亚洲国产av影院在线观看| 精品亚洲乱码少妇综合久久| 日本vs欧美在线观看视频| av在线app专区| 亚洲成国产人片在线观看| 欧美精品高潮呻吟av久久| 五月玫瑰六月丁香| 日韩视频在线欧美| 国产激情久久老熟女| 午夜视频国产福利| 久久久久人妻精品一区果冻| 欧美激情 高清一区二区三区| 免费大片18禁| 久久久久精品人妻al黑| 日日摸夜夜添夜夜爱| videosex国产| 日韩欧美精品免费久久| 免费女性裸体啪啪无遮挡网站| 免费日韩欧美在线观看| 在线看a的网站| 丝袜脚勾引网站|