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开展多波束水深测量应同步进行声速剖面探测。因海上作业条件恶劣、作业时间受限及设备性能局限等影响,在深远海海域常获取不到全深度的实测声速剖面。尽管利用温盐场模型可将声速剖面直接延拓至实地水深的最大深度,但这种气候态平均声速剖面与实际的声速剖面间存在不可控的系统性偏差,会给声速改正及水深测量成果带来质量隐患。给出了一种提高深远海全深度声速剖面重构精度的方法,即利用有效探测深度附近的实测温度盐度值,对大于有效探测深度的各水层的模型温度盐度值施加程度不一的约束控制。结果表明,经优化后全深度声速剖面的重构精度得到明显提高,其中2个XCTD站点声速剖面的互差SSPD分别由-2.5~1.0 m/s优化为0.0~1.0 m/s、0.0~2.6 m/s优化为-1.5~0.0 m/s; 2个CTD站点声速剖面的互差SSPD分别由-0.5~1.7 m/s优化为-0.4~0.3 m/s、-2.15~0.8 m/s优化为-1.4~0.8 m/s。 相似文献
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为准确获取深远海海洋声速资料,充分了解深水声速规律,选取了西太地区两个水深超过5000m的S1和S2站位的声速资料为研究对象,以SVP(声速剖面仪)实测资料为参考标准,通过对CTD资料利用Chen-Millero、Del-Grosso以及Wilson的3种经验公式计算的声速与SVP资料进行对比分析,得出Del-Grosso经验公式计算的声速误差最小。为进一步提高声速资料精度,对Del-Grosso公式进行修正,并利用另外3个站位数据进行验证,发现利用校正后的公式计算的声速资料精度明显提升,这为其他深远海区利用CTD或其他温盐深资料获取高精度声速资料提供参考。 相似文献
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声速误差是多波束水深地形测量主要误差源之一,通常采用现场声速剖面测量的方式加以改正,但在深远海多波束水深地形测量时,现场获取全深度的声速剖面并非易事。针对这一问题,利用东南印度洋海洋调查工作中采集到的17个站位的CTD数据,将所有站位声速剖面拓展到全深度,采用经验正交函数分析法(Empirical Orthogonal Functions,EOF)构建调查区声速剖面场,可获得声速剖面场内任意一点的声速值。然后通过EOF重构声速剖面场获得的声速值对测区内多波束水深地形数据进行改正,并与实测声速剖面对多波束水深地形数据的改正结果进行对比,结果表明,5000 m水深范围内2种声速改正结果相差很小,EOF重构法对深水多波束的声速改正满足水深测量的要求。 相似文献
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声速是影响多波束勘测精度的重要的外部因素,它决定着声线跟踪的精度,并最终影响到测深精度。由于停船投放CTD时间成本比较高,探索经济高效的远海走航式多波束水深测量,特别是航渡测量期间的声速剖面获取方法成为现场测量人员急需解决的问题。在对HYCOM/WOA13数据与现场CTD数据进行了数据偏差分布、相关性等比对,验证HYCOM/WOA13数据适用性的基础上,提出了基于HYCOM模式数据、WOA13同化数据及单点历史CTD数据与现场XCTD/XBT多源组合的远海走航式多波束水深测量声速剖面获取方法。对比表明,该多源组合的声速剖面能较好反映施测位置的声速剖面情况,该方法对提高远海水深测量的精度和经济效益具有一定的借鉴意义。 相似文献
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浅地层剖面测量是海洋工程勘察、灾害地质调查和大陆架海洋地质科学研究的重要手段,资料解译的准确程度将对地质调查和研究成果的可靠性造成直接影响。由于发收分置型浅地层剖面仪的激发装置与接收装置是分开的,当调查区域的水深过浅时,将其近似为自激自收的单道地震系统会导致地层的畸变,水深越浅地层畸变率越大。根据浅地层剖面仪的基本原理,推导出了浅部地层厚度畸变校正公式,为用C-View软件更准确地解译此类浅地层剖面资料提供了参考。海底沉积物的声速直接影响浅地层剖面地层厚度解译的准确性,利用卢博等建立的适用于中国东南近海的声速经验公式,在某人工岛构造调查中,根据地质钻孔获取的孔隙度参数计算各沉积层的平均声速,建立相应的声速结构剖面,对地层厚度进行校正,取得较好的效果,用孔隙度预测声速的方法参数容易获取,能够提高浅地层剖面资料的解译精度,使地层的厚度更接近于实际,具有一定的实用意义。 相似文献
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We applied the maximum offset of sound velocity algorithm to sound velocity profile streamlining and optimization to overcome multibeam survey and data-processing efficiency problems. The impact of sound velocity profile streamlining on sounding data accuracy is evaluated. By automatically optimizing the threshold, the reduction rate of sound velocity profile data can reach over 90% and the standard deviation percentage error of sounding data can be controlled to within 0.1%. The optimized sound velocity profile data improved the operational efficiency of the multi-beam survey and data postprocessing by 3.4 times, indicating that this algorithm has practical value for engineering applications. 相似文献
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声速剖面仪水下探头软硬件设计 总被引:4,自引:1,他引:3
简要阐述了直接测量式声速剖面仪的测量原理及水下机探头的体系结构;并进一步介绍了自容式和拖缆式两种结构的声速剖面仪的控制单元、模数转换、数据存储、数据提取、控制命令的响应和执行、系统状态的检查及设备的可靠性处理等模块的软硬件实现方法。 相似文献
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水深测量中的声速改正问题研究 总被引:7,自引:0,他引:7
海域水文资料的不断丰富和声速仪的广泛使用,推动了水深声速改正精度的提高。结合黄骅港水深测量数据,针对声速剖面测量与声速改正以及声速、器差、指标差等要素间的内在联系及相互影响予以系统阐述。 相似文献
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关于表层声速对多波束测深影响及改正的探讨 总被引:1,自引:0,他引:1
通过分析波束形成的原理与实测数据处理得出结论:表层声速误差将对多波束测量产生不可挽回的错误;而当表层声速正确、声速剖面误差时,在后处理可以通过适当的声速剖面加以改正。 相似文献
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Correction method for full-depth current velocity with lowered acoustic Doppler current profiler (LADCP) 总被引:1,自引:0,他引:1
A new method is presented to process and correct full-depth current velocity data obtained from a lowered acoustic Doppler
current profiler (LADCP). The analysis shows that, except near the surface, the echo intensity of a reflected sound pulse
is closely correlated with the magnitude of the difference in vertical shear of velocity between downcast and upcast, indicating
an error in velocity shear. The present method features the use of echo intensity for the correction of velocity shear. The
correction values are determined as to fit LADCP velocity to shipboard ADCP (SADCP) and LADCP bottom-tracked velocities. The
method is as follows. Initially, a profile of velocity relative to the sea surface is obtained by integrating vertical shears
of velocity after low-quality data are rejected. Second, the relative velocity is fitted to the velocity at 100–800 dbar measured
by SADCP to obtain an “absolute” velocity profile. Third, the velocity shear is corrected using the relationship between the
errors in velocity shears and echo intensity, in order to adjust the velocity at sea bottom to the bottom-tracked velocity
measured by LADCP. Finally, the velocity profile is obtained from the SADCP-fitted velocity at depths less than 800 dbar and
the corrected velocity shear at depths greater than 800 dbar. This method is valid for a full-depth LADCP cast throughout
which the echo intensity is relatively high (greater than 75 dB in the present analysis). Although the processed velocity
may include errors of 1–2 cm s−1, this method produced qualitatively good current structures in the Northeast Pacific Basin that were consistent with the
deep current structures inferred from silicate distribution, and the averaged velocities were significantly different from
those calculated by the Visbeck (2002) method. 相似文献