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Equatorward jets and poleward undercurrents along the eastern boundary of the mid-latitude North Pacific.

机译:沿中纬度北太平洋东部边界的赤道急流和极地逆流。

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摘要

We sharpen our view of an eastern boundary current region during the upwelling season through the analysis of several data sets. We focus on the mesoscale flow field off of northern California, observed during the Coastal Transition Zone (CTZ) experiment of 1988. First, we estimate tidal currents in the region by least-squares harmonic analysis of both shipboard acoustic Doppler current profiler (ADCP) and moored data. The tide is predominantly M{dollar}sb2{dollar} and varies from 1-4 cm/s across the region, consistent with previous tidal studies. Next, we use detided ADCP together with conductivity-temperature-depth data to infer absolute geostrophic velocities during each of the five surveys in July-August 1988. Referencing geostrophy with the ADCP reveals a stronger equatorward jet than previously reported; southward volume transport from 0-500 m through a 200 km onshore-offshore line is as high as {dollar}rm8.0times10sp6msp3ssp{lcub}-1{rcub},{dollar} with a mean over the five surveys of {dollar}rm6.3pm1.3times10sp6msp3ssp{lcub}-1{rcub}.{dollar} The jet was about 50 km wide, with core velocities {dollar}>{dollar}0.6 m/s. During a two-week period in July 1988, horizontal velocity shears were sufficient to shift the effective local inertial frequency 10% higher on the cold (inshore) side and 5% lower on the warm (offshore) side of the jet. Observed near-inertial currents have amplified energy in the region with lower effective inertial frequency, consistent with theoretical predictions. Next, the basic instability mechanism leading to a meandering CTZ jet is analyzed using a linear quasi-geostrophic model applied to observed basic state velocity profiles. The jet is subject to both barotropic and baroclinic instability processes, and meander wavelengths of 260-265 km are the fastest growing. Growth periods of 7-11 days and along-jet phase speeds of 4-8 km/d are predicted. Finally, the poleward undercurrent which was observed during the 1988 CTZ experiment is also investigated with a series of shipboard ADCP sections collected from 33-51{dollar}spcirc{dollar}N during July-August 1995. Subsurface poleward flow occurred in 91% of the sections, with a mean undercurrent core velocity of 17 {dollar}pm{dollar} 1 cm/s and transport in a 140-325 m layer of {dollar}rm0.9pm0.1times10sp6msp3ssp{lcub}-1{rcub}.{dollar} One portion of the undercurrent is continuous over a 440 km length.
机译:通过对几个数据集的分析,我们对上升流季节东部边界当前区域的观点更加清晰。我们集中研究1988年沿海过渡带(CTZ)实验期间观察到的北加州中尺度流场。首先,我们通过对两船舰载声多普勒电流剖面仪(ADCP)的最小二乘谐波分析来估计该地区的潮流和停泊的数据。潮汐主要为M {dollar} sb2 {dollar},整个区域的潮汐变化为1-4 cm / s,与之前的潮汐研究一致。接下来,我们在1988年7月至8月的五次测量中的每一个中,都使用经过测量的ADCP以及电导率-温度-深度数据来推断绝对的地转速度。从0-500 m到200公里的陆上-近海线的向南运输量高达{dol} rm8.0times10sp6msp3ssp {lcub} -1 {rcub},{dollar},在{dollar} rm6的五次调查中的平均值.3pm1.3times10sp6msp3ssp {lcub} -1 {rcub}。{dollar}喷气机宽约50 km,核心速度{dollar}> {dollar} 0.6 m / s。在1988年7月的两周时间内,水平速度剪切足以使有效局部惯性频率在射流的冷(近海)侧高出10%,而温暖(近海)侧低出5%。观察到的近惯性电流在有效惯性频率较低的区域放大了能量,与理论预测一致。接下来,使用应用于观测到的基本状态速度剖面的线性拟地转模型分析导致曲折CTZ射流的基本不稳定性机理。射流同时经历正压和斜压不稳定过程,并且260-265 km的曲折波长增长最快。预计生长期为7-11天,沿射流阶段速度为4-8 km / d。最后,还利用1995年7月至8月期间从33-51 {sp} {dol} N收集的一系列舰载ADCP剖面对在1988 CTZ实验期间观察到的极向性暗流进行了研究。这些部分的平均潜流核心速度为17 {pm} pm {dollar} 1 cm / s,并在140-325 m {rm} pm0.9pm0.1times10sp6msp3ssp {lcub} -1 {rcub}层中传输。{一美元的暗流在440公里的长度上是连续的。

著录项

  • 作者

    Pierce, Stephen Davis.;

  • 作者单位

    Oregon State University.;

  • 授予单位 Oregon State University.;
  • 学科 Physical Oceanography.; Physical Geography.
  • 学位 Ph.D.
  • 年度 1998
  • 页码 147 p.
  • 总页数 147
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 海洋物理学;自然地理学;
  • 关键词

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