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1.
为了研究频率域2.5维非线性共轭梯度反演在海洋天然气水合物探测中的实际应用效果,利用美国Scripps研究所在South Hydrate海域采集的可控源电磁探测数据进行2.5维非线性共轭梯度反演计算,结合其他地球物理方法在同一海区的研究结果,综合分析2.5维反演计算的准确性和有效性。结果表明,非线性共轭梯度反演能够清晰地反映出该区域海底面以下1~2 km地层的电导率结构分布,其局部反演结果与地震反射、地震层序、测井分析结果基本一致,且对小尺寸异常、浅层高阻体分辨力较强,尤其在海洋天然气水合物探测方面具有较大潜力。  相似文献   

2.
二维有耗色散介质的时域逆散射方法   总被引:2,自引:0,他引:2  
刘广东  张业荣 《海洋学报》2010,32(10):6969-6979
为了重建二维有耗色散介质的电参数分布,基于Debye模型,应用泛函分析和变分法,提出一种时域逆散射新方法.该方法首先以最小二乘准则构造目标函数,将逆问题表示为约束最小化问题;接着应用罚函数法转化为无约束最小化问题;然后基于变分计算导出闭式的Lagrange函数关于特征参数的Fréchet导数;最后借助梯度算法和时域有限差分法迭代反演Debye模型参数.为了对抗噪声污染和逆问题的病态特性,采用了一阶Tikhonov正则化方法.数值应用中,利用Polak-Ribière-Polyak非线性共轭梯度法,对二维乳  相似文献   

3.
杨怿  余建星 《海洋通报》2008,27(3):67-74
依据波浪力成因和作用效果的不同,将波浪力分为两部分(Morisson 波浪力和 Inundation波浪力)讨论.对于两种波浪力中的非线性拖曳力项,采用高次多项式逼近,结合高斯型统计量高阶矩计算原理、相关函数、变换法和单输入多输出系统的互谱关系,预测海流海浪联合作用下的海洋平台响应谱的理论形式,求得总波浪力谱以及平台响应谱.在Inundation模态力的相关函数推导过程中,考虑海流影响时,惯性力项与拖曳力项的相关函数总和为0,这一结果与不考虑海流影响时的结果相同.  相似文献   

4.
由于大范围同步连续观测海流流速很困难,这才产生建立一定的理论及方法认真计算海流流速的要求.可是,过去沿用至今的动力计算[1],方法虽简便,但只能计算因密度分布所生的梯度流(或地转流),且存在着既不考虑风力,又不顾及湍流摩擦力,再加无运动面难以确定,即令设法作出浅海订正,其结果又往往与事实不符等根本性缺陷;而如籍Ekman漂流理论计算海流,又仅能计算因风所生的漂流,且还存在着既不考虑海水密度分布,又视海面无倾斜,再加湍流动力粘滞系量难以确定等与实际相差较远的理论依据.近代兴起的一些海流数值计算,又往往都局限于全流或深度平均流速的计算.因此,建立一种既考虑到海洋内部海水分布,又考虑到海面风力外加海面大气压力作用,顾及到海洋中湍流摩擦力,又体现流速随深度变化,而更重要的是应用起来简易的计算海流流速的理论及方法,便成为很需要解决的问题了.  相似文献   

5.
本文在仅考虑铅直湍流的情况下,提出一种计算海流流速及予报海流流速的理论及方法。是在海流基本上是由海洋内部密度分布及海面风力和气压作用下形成的认识下,依据一定的事实,先行确定水平压强梯度力及铅直湍流动力粘滞系量,而后计算定常恒速海流及予报海流流速的。在建立海流流速予报方程解时,除了要求得流速随时间变化的解,尚需求得海水密度随时间变化的解。在海水密度随时间的变化予知的情况下,即可依据予知的风速及降水、蒸发差等随时间的变化,予报海流。曾对东中国海黑潮流系进行了定常恒速水平流速的计算。  相似文献   

6.
垂直梯度法与最优分割法确定温跃层边界的比较分析   总被引:2,自引:2,他引:0  
垂直梯度法是跃层示性特征计算中普遍使用的方法,但在某些情况下并不能很好地描述海洋要素的跃变特征.针对垂直梯度法的不足,引入水团分析中的最优分割法,对典型剖面,以及边界型、逆变型、多层型等几类特殊剖面的跃层边界分别进行了计算,并对垂直梯度法与垂直梯度法的计算结果进行了比较分析,结果表明最优分割法确定的跃层边界更为合理.通过对两种方法确定的中国近海温跃层的整体分布进行比较分析,证明了最优分割法能够弥补垂直梯度法在计算深海与浅海过渡区中的跃层时遇到的标准不匹配问题,较好地保持跃层的连续性.  相似文献   

7.
海洋钻井隔水管的动力分析   总被引:1,自引:0,他引:1       下载免费PDF全文
本文对规则波浪与随机波浪以及海流作用下的海洋钻井隔水管进行了动力分析,建立力学模型,推导有限元动力方程,计算非线性时间域历程响应与线性化频率域最大响应,并对这两种方法的结果进行比较,此外还讨论了若干影响因素,数值计算结果表明本文理论分析正确,计算精度足够,本文所提供的动力分析方法以及计算机程序可供海洋有关部门参考使用.  相似文献   

8.
本文采甲1958—1972年南海船舶天气观测报告和多年的海流调查资料,以及1907—1973年的海洋调查资料,对南海东北部冬季海流进行初步探讨。其中最具特色是逆NE风而流动的从SW往NE流去的海流。由表层水温水平梯度算得的梯度流表明,116°E以东的海流均往NE向流去,其强度与南海东北部风况有关,NE风强盛时海流也强盛,在弱的SE风时,流速相应地较弱,在NE风场向SE风场过渡或SE风场向NE风场过渡的时期内,流速最小。计算流和实测流均有着上述共同的规律性。  相似文献   

9.
夏季台湾海峡海流的计算Ⅰ.三维诊断计算   总被引:1,自引:0,他引:1  
在σ坐标下建立了一个三维非线性诊断模式,并用于台湾海峡夏季海流的计算.计算结果表明,夏季通过台湾海峡北上的流量为0.83×106m3/s,其中在海峡南边界上,通过东西两半边界的流量分别为0.58×106m3/s与0.25×106m3/s;海峡内水平速度分布东侧最大,西次侧之;上升流普遍发生在福建沿岸;夏季台湾海峡的海流特性,主要是密度流,风海流是其次的.  相似文献   

10.
广西沿海年极值波高分析   总被引:2,自引:0,他引:2  
经分析发现广西沿海极值波高不符合用的P-Ⅲ型分布,并分析了其符合的分布函数,结果表明对Weibull分布符合最好,为解决Weibull分布参数难于确定的问题,引入了共轭梯度法计算其参数,最终计算了多年一遇极值波高。  相似文献   

11.
由于卫星高度计数据分辨率高、观测范围广的特点,我们使用该数据开展了黑潮流的研究。在之前的研究中,卫星绝对地转流都被用于对黑潮流域的表层流场的时空变化特征进行研究,并采用了一些探测方法提取了黑潮流轴和流路。然而,海面绝对地转流是由绝对动力地形估计得到,应该被当做实际流场的地转分量,在实际应用中并不能代表真实流场。在本研究中,建立了气候态绝对地转流与网格平均的漂流浮标流场间的数学校验关系,以此对卫星绝对地转流场进行修正,即便这两种数据的性质存在些许偏差。因此,基于主成分探测法,修正后的卫星绝对地转流被用于探测黑潮流轴和流路。对比结果表明,由修正后的卫星地转流场探测得到的黑潮流轴和流路均要好于地转流和表层流估计结果。修正后的地转流有助于开展更加准确的黑潮流轴和流路的逐日探测。  相似文献   

12.
A method to extract geostrophic current in the daily mean HF radar data in the Kuroshio upstream region is established by comparison with geostrophic velocity determined from the along-track altimetry data. The estimated Ekman current in the HF velocity is 1.2% (1.5%) and 48° (38°)-clockwise rotated with respect to the daily mean wind in (outside) the Kuroshio. Furthermore, additional temporal smoothing is found necessary to remove residual ageostrophic currents such as the inertial oscillation. After removal of the ageostrophic components, the HF geostrophic velocity agrees well with that from the altimetry data with rms difference 0.14 (0.12) m/s in (outside) the Kuroshio.  相似文献   

13.
为了探究海表温度和海面高度之间的瞬时相关性,介绍了一种卫星测高数据的拉格朗日分析指数--有限尺度李雅普诺夫指数(Finite Size Lyapunov Exponent,FSLE),以黑潮延伸体区域的涡旋和南大西洋的亚南极锋为例,通过对观测、模式结果和融合产品结果的分析,探讨了该指数与海表温度梯度(Sea Surface Temperature Gradient,SSTG)之间的相关性。比较FSLE图像和SSTG图像发现,FSLE与SSTG均呈丝状结构,对海洋表层水体结构描述具有一致性,尤其在温度梯度大和地转流强的区域更为一致。二者的一致性要远好于其他常用方式,比如全流速、OW参数涡旋识别方法和Winding-Angle涡旋识别方法。不同区域FSLE与SSTG之间的相关性表现不同,黑潮延伸体区域相关系数存在显著的季节变化,而南大西洋亚南极锋区域季节内变化突出。  相似文献   

14.
高度计资料监测日本以南黑潮主轴特性的变化   总被引:3,自引:0,他引:3  
应用1993年至2001年TOPEX/Poseidon(以下简写为T/P)卫星高度计3条下行轨道的沿轨资料,计算分析了日本以南黑潮主轴的摆动特性,发现在1993年和2000—2001年010轨道上有2次空间尺度较大、持续时间较长的弯曲。黑潮处于平直路径时流速比较大;呈稳定弯曲状态时流速与多年平均值相差不大;而黑潮在两种稳态之间转换时,伴随着流速负距平的出现。  相似文献   

15.
A time series of surface geostrophic velocity is developed using satellite altimetry data during 1992–2010 for a track across the Kuroshio southeast of Kyushu, Japan. The temporal mean geostrophic velocity is estimated by combining the along-track sea level anomaly and shipboard ADCP data. This approximately 6-km resolution dataset is successful in representing the Kuroshio cross-current structure and temporal variation of the Kuroshio current-axis position during 2000–2010. The authors use this dataset to examine the winter Kuroshio path destabilization phenomenon. Its seasonal features are characterized as follows: the velocity shear on the inshore side of the Kuroshio becomes stronger and the Kuroshio path state becomes unstable from the summer to winter. This evidence is consistent with the hypothetical mechanism governing the destabilization phenomenon discussed in a previous study. Furthermore, the interannual amplitude modulation of the seasonality is examined in relation to interannual variations in the winter northerly wind over the northern Okinawa Trough and the Pacific Decadal Oscillation (PDO) index. The destabilization phenomenon appears 15 times in the period 2000–2010. Ten cases are related to local wind effects, and 7 of these are also connected with the PDO index. This is probably because the winter northerly wind over the northern Okinawa Trough is regulated by the PDO signal in interannual time-scales. Only 4 cases are related to the PDO index, but their driving mechanism remains uncertain.  相似文献   

16.
张志春  袁东亮  李博 《海洋科学》2015,39(7):93-102
基于2004 年1 月~2009 年12 月月平均Argo(Array for Real-time Geostrophic Oceanography)温盐格点资料, 结合P-vector 方法重构了西北太平洋绝对地转流, 重点分析了西北太平洋环流时空变化特征。结果表明, 基于Argo 资料西北太平洋三维结构特征与以前的研究结果是一致的。与WOA09(World Ocean Atlas 2009)计算的纬向流相比, Argo 资料计算的纬向流要偏大。北赤道逆流(NECC)、北赤道流(NEC)、黑潮再生流(KCC)和黑潮延伸体(KE)都有明显的季节和年际变化。NECC 和NEC 基本上呈现春强秋弱的季节变化特征, KCC 和KE 的季节特征与NECC 和NEC 存在反相关系。NECC 和NEC 表现出周期为1~2 a 的年际信号, KCC 和KE 为非周期性的年际信号。表层NEC 流核所在位置以及NEC南边界位置都有南移的趋势。另外, NEC、KCC 和KE 的流量也呈逐渐增大的趋势。  相似文献   

17.
A P - vector method is optimized using the variational data assimilation technique(VDAT). The absolute geostrophic velocity fields in the vicinity of the Luzon Strait (LS) are calculated, the spatial structures and seasonal variations of the absolute geostrophic velocity field are investigated. Our results show that the Kuroshio enters the South China Sea (SCS) in the south and middle of the Luzon Strait and flows out in the north, so the Kuroshio makes a slight clockwise curve in the Luzon Strait, and the curve is strong in winter and weak in summer. During the winter, a westward current appears in the surface, and locates at the west of the Luzon Strait. It is the north part of a cyclonic gyre which exits in the northeast of the SCS; an anti-cyclonic gyre occurs on the intermediate level, and it exits in the northeast of the SCS, and an eastward current exits in the southeast of the anti-cyclonic gyre.  相似文献   

18.
The sea level difference between Naze and Nishinoomote and sea level anomalies (the residuals after removal of seasonal variations) around the Nansei Islands were examined in relation to the large meander in the Kuroshio south of central Japan. They are indices of surface velocity and geostrophic transport of the Kuroshio in the Tokara Strait and in the East China Sea, respectively. All of them were large during the meandering period, and each of them reached a maximum before or after the generation of the large meander in 1975. Thus the surface velocity and the geostrophic transport of the Kuroshio in the Tokara Strait and the East China Sea were large during the meandering period. The sea level difference between Naze and Nishinoomote (or Makurazaki) shows that the surface velocity and geostrophic transport in the Tokara Strait were significantly larger during the extinction stage in 1963 and during the generation stage in 1975 and were correlated with the position of the Kuroshio east of Kyûshû in 1974 and 1975 before the generation of the large meander.The surface velocity of the Kuroshio southeast of Yakushima (E-line) based on dynamic calculation referred to 1,000 db was weak during the meandering period, and was out of phase with the variation of surface velocity in the Tokara Strait monitored by tide gauge data. The analysis of GEK and hydrographic data shows that southwestward flow existed below 600 m in the slope region on the E-line and weakened during the meandering period. Thus, the out-of-phase variation in surface velocity mentioned above seems to be partly explained by the variation in velocity on the reference level at the E-line.  相似文献   

19.
Sea surface dynamic topography (SSDT) can be divided into temporal mean SSDT and fluctuation SSDT. The former is approximated with a climatological mean SSDT and the latter is derived from satellite altimetry data, to give an approximated total SSDT (called a composite SSDT). The method is applied to detecting fluctuations of the Kuroshio axis south of Japan using TOPEX/POSEIDON altimeter data from the first year mission in 1992–1993. The fluctuation SSDT averaged over a wide area south of Japan clearly shows an annual cycle with an amplitude of about 15 cm. Temporal changes of SSDT along a subsatellite track crossing the Kuroshio compare moderately well with those estimated from repeated hydrographic observations, although there is a discrepancy of unknown origin. The composite SSDT also compares well with SSDT estimated from the same hydrographic data. Horizontal distribution of the surface geostrophic velocity component normal to subsatellite tracks is derived every ten days from the composite SSDT. Most locations of estimated strong eastward geostrophic velocities coincide well with locations of the Kuroshio axis determined every 15 days fromin situ surface velocity measurements on various vessels; for example, a fairly large meander of the Kuroshio south of Honshu is clearly detected. It is concluded that the composite SSDT can be used reliably to detect fluctuations of the Kuroshio axis south of Japan.  相似文献   

20.
Theoretically, the geostrophic approximation holds for the low-frequency flow field, but no detailed examination has been done on how well the estimated geostrophic velocity corresponds with the observed velocity. Intensive surveys were carried out during 1993–1995 in the Kuroshio and its recirculation regions south of Shikoku, Japan, including repeated hydrographic surveys and direct current measurements at nominal depths of 700, 1500 and 3000 m. For these depth intervals, vertical differences of estimated geostrophic velocity are compared with those of observed velocity. For the intermediate layer (between 700 and 1500 m depths), the slope of the regression line is 0.99, correlation coefficient is 0.98, and the root-mean-square of difference from geostrophic balance is 2.8 cm/s which is close to the estimated error of 2.1 cm/s. For the deep layer (between 1500 and 3000 m depths), the corresponding values are 0.82, 0.93, 1.2 cm/s and 2.0 cm/s, respectively. The results indicate that the estimated geostrophic velocity compares well with the observed velocity in these regions. This revised version was published online in August 2006 with corrections to the Cover Date.  相似文献   

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