共查询到17条相似文献,搜索用时 78 毫秒
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针对海洋中尺度涡对水声传播的影响,利用中尺度涡区的历史水文实测数据提取涡旋强度,空间尺度等中尺度涡特征参数,建立了海洋中尺度涡理论计算模型。运用MMPE水下声场模型仿真试验研究了涡旋性质、强度和位置、声源频率和置放深度对声传播特性的影响。结果表明:暖涡使得会聚区的位置“后退”,会聚区宽度增加;冷涡使得会聚区的位置“前移”,会聚区宽度减小。涡旋的强度越大,“前移”或“回退”的效应越显著。 相似文献
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海洋中声速起伏导致水声信道发生变化,进而引起声线到达结构的变化,对水声传播及定位精度产生一定影响。为讨论这一效应,基于TDOA体制建立了考虑声线弯曲的水下目标无源定位模型,分析了声速起伏对水下声传播路径及传播时间的影响,进而研究了声速起伏对水下无源定位测量精度影响程度。结果表明:当水平传播距离较大时,声速剖面起伏对声传播路径及传播时间的影响更为显著;以典型四元阵为例,若基线长度为20 km,接收阵位于水下5 km处,在不考虑其它随机误差影响下,海洋声速起伏造成的声源定位误差量级在0.5 m以内。分析结果有助于更好地利用环境特征优化无源定位测量方案,可为高精度水下无源定位系统设计及精度评估提供依据。 相似文献
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海洋中的低频(<1000Hz)声吸收主要决定于海洋的pH值.虽然测得的远程(1000km量级)声传播的绝对幅度相当复杂地依赖于海洋的介质和环境参数,但对不同频率间的相对吸收差的测量能给出有用的信息.此外,沿海面反射声线(RSR)的传播衰减还应附加上海面散射引起的损失.原则上通过比较发射和接收到的声信号的频谱能估算海洋的pH值和表面粗糙度.我们分析了北太平洋750km声传播实验的部分数据.实验结果与理论估算定性地相符,但其测量精度还不足以进行定量的比较(该实验并不是为测量相对吸收差而设计的).估算表明,为了获得0.05的pH测量精度,当信号频率为550±100Hz,传播距离为750km时,对北太平洋(pH≈7.7)和大西洋(pH≈8.0)海域分别需要对100和60个独立测量样本进行平均以消除内波及噪声引起的幅度谱畸变. 相似文献
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为厘清海底沉积层声学特性信息的水声环境保障需求,构建浅海两层海底环境参数模型,并参考Hamilton海底底质9种分类设置沉积层声速、密度、衰减系数及厚度的参考值及计算采样区间,利用Kraken简振波模型,采用控制变量的方法,研究了浅海沉积层声学特性参数对声传播损失的影响;开展了建模理论推导及数值技术分析,研究了海底沉积层声学特性参数在模型计算过程中调用过程,并从建模计算的角度对仿真计算的结果进行解释,对海底沉积层声学特性调查装备发展及调查重点参数具有一定的参考价值。 相似文献
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运用海洋声传播二维 PE算法对不规则海底边界条件的处理 ,作者提出 1种改进方法 ,即利用抛物方程和界面边界条件 ,对界面附近的抛物方程的差分形式进行修正 ,以考虑复杂海底边界的影响。通过实际的数值计算表明 ,运用该方法计算声场 ,在提高计算精度方面起到有益的作用。 相似文献
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Shigehisa Nakamura 《Marine Geodesy》2013,36(4):305-312
A note is presented on tsunami bore front. This tsunami bore front is an old dynamical problem but also a new problem to be understood. The tsunami event on 2004 December 26 has raised this is an urgent problem. The author introduces here a model in order to see a hydrodynamical specific property of the tsunami bore front. This modeling gives us a new understanding about what mechanics is for the interested tsunami bore front, especially, around a coastal zone. This work adds a new understanding about mechanics of water motions as the tsunamis generated by the earthquake undersea at a distant area from the coast. The model in this work points out a specific transitional pattern as a function of time and space of tsunami bore front. This modeling gives what is essential at considering tsunami bore front. 相似文献
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Shigehisa Nakamura 《Marine Geodesy》2005,28(4):305-312
A note is presented on tsunami bore front. This tsunami bore front is an old dynamical problem but also a new problem to be understood. The tsunami event on 2004 December 26 has raised this is an urgent problem. The author introduces here a model in order to see a hydrodynamical specific property of the tsunami bore front. This modeling gives us a new understanding about what mechanics is for the interested tsunami bore front, especially, around a coastal zone. This work adds a new understanding about mechanics of water motions as the tsunamis generated by the earthquake undersea at a distant area from the coast. The model in this work points out a specific transitional pattern as a function of time and space of tsunami bore front. This modeling gives what is essential at considering tsunami bore front. 相似文献
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Fei Chai Mingshun Jiang Richard T. Barber Richard C. Dugdale Yi Chao 《Journal of Oceanography》2003,59(4):461-475
The interdecadal climate variability affects marine ecosystems in both the subtropical and subarctic gyres, consequently the
position of the Transition Zone Chlorophyll Front (TZCF). A three-dimensional physical-biological model has been used to study
interdecadal variation of the TZCF using a retrospective analysis of a 30-year (1960–1990) model simulation. The physical-biological
model is forced with the monthly mean heat flux and surface wind stress from the COADS. The modeled winter mixed layer depth
(MLD) shows the largest increase between 30°N and 40°N in the central North Pacific, with a value of 40–60% higher during
1979–90 relative to 1964–75 values. The winter Ekman pumping velocity difference between 1979–90 and 1964–75 shows the largest
increase located between 30°N and 45°N in the central and eastern North Pacific. The modeled winter surface nitrate difference
between 1979–90 and 1964–75 shows increase in the latitudinal band between 30°N and 45°N from the west to the east (135°E–135°W),
the modeled nitrate concentration is about 10 to 50% higher during the period of 1979–90 relative to 1964–75 values depending
upon locations. The increase in the winter surface nitrate concentration during 1979-90 is caused by a combination of the
winter MLD increase and the winter Ekman pumping enhancement. The modeled nitrate concentration increase after 1976–77 enhances
primary productivity in the central North Pacific. Enhanced primary productivity after the 1976–77 climatic shift contributes
higher phytoplankton biomass and therefore elevates chlorophyll level in the central North Pacific. Increase in the modeled
chlorophyll expand the chlorophyll transitional zone and push the TZCF equatorward.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
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