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1.
作者采用浊度计和声学多普勒流速剖面仪(ADCP)在近海区域连续、定点观测的应用中,利用浊度与悬沙浓度之间良好的线性关系,对潮汐半月周期内的浊度和ADCP后向散射声强数据进行相关性分析,讨论了小、中、大潮期间利用ADCP后向散射声强反演悬沙浓度的可靠性,反演过程中综合考虑了声学近场非球面扩散和本底噪声的影响。结果表明,在实验海域中,小潮情况下,各水层内悬浮泥沙成分较为稳定,ADCP后向散射声强与浊度变化相关性较高,达到0.91;而在大潮情况下,ADCP后向散射声强与浊度变化的相关性降低,悬沙浓度及成分容易在海流的影响下发生变化。 相似文献
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夏季加拿大海盆海冰边缘区声体积后向散射强度研究 总被引：1，自引：1，他引：0
声信号的体积后向散射强度是声传播过程中一个关键的参数。海冰边缘区的声体积后向散射强度研究对深入认识北极声场环境有着十分重要的意义。本文利用中国第六次北极科学考察获取的数据资料研究了海冰边缘区声体积后向散射强度特性。结果表明:加拿大海盆海冰边缘区是声体积后向散射强度的明显过渡区。无冰海面(海冰密集度小于15%)海洋深层水的声体积后向散射强度明显大于密集海冰区域的海水(海冰密集度大于50%)。讨论了声体积后向散射强度与海冰融化之间的关系,造成融冰区声体积后向散射强度增大的原因是水下悬浮泥沙、浮游生物等悬浮物质增加。根据海冰密集海域的海水后向散射强度弱的特点,对北极下放式声学多普勒测流仪(LADCP)观测的设置提出建议。 相似文献
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本文研究了泥沙悬浮液浊度对叶绿素荧光计测定水样中活体叶绿素荧光的影响。结果表明,浊度产生的荧光效应和遮蔽效应对活体叶绿素荧光测定具有显著影响。在100 NTU浊度范围内,浊度会导致荧光效应使活体叶绿素荧光值测量结果随着浊度的增大而增大,并构成良好的线性关系;实际测定水体中硅藻的活体叶绿素荧光值时,泥沙悬浮液的浊度会导致遮蔽效应使活体叶绿素荧光值测量结果随着浊度的增大而减小,水体中硅藻质量浓度越高遮蔽效应越显著,在1 000 mV(约10 μg/L)硅藻质量浓度,100 NTU浊度条件下,浊度遮蔽效应可导致活体叶绿素荧光值偏低20%。根据近海泥沙实验数据,本文提出了一种活体叶绿素荧光检测的浊度影响修正方法,在100 NTU浊度内,修正后叶绿素荧光值偏差率都下降到±10%以内,校准后的荧光值与真实叶绿素荧光值较为接近。 相似文献
4.
依据2012年ROSE航次船载ADCP和LADCP的观测数据,对南海秋季声散射层的垂向分布特征和日变化进行了分析;根据估算出的散射层中散射体的垂向迁移速度,对散射体类型进行了分析。观测结果表明,南海存在着2个声散射层,一个声散射层位于0~200m,散射强度具有显著的日变化特征,即白天弱,夜晚强;另一声散射层则处于300~500m的深度,其散射强度的日变化与另一个相反,白天较强,夜晚变弱。通过计算可得,散射体的垂向迁移,在傍晚时分运动方向向上,速度约为1.74cm/s;而凌晨左右运动方向向下,速度约为1.39cm/s。观测结果还表明,ADCP和LADCP的观测结果能够互相补充,更有利于对声散射层的细致研究。 相似文献
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为了研究西太平洋声散射层的垂向分布特征和日变化规律,分析了多波束测深系统的水体影像数据。观测结果表明,西太平洋存在着两个声散射层,一个声散射层位于0～200 m,另一个声散射层位于500～700 m,两个声散射层散射强度具有明显的日变化特征,上层散射层的散射强度呈现白天弱,夜晚强的特征,而下层散射层的散射强度日变化规律与上层相反,并且发现深散射层的厚度也存在日变化特征;分析了此种方法的优缺点,对以后声散射层的观测分析提供了新的思路。此外,利用同时下放的声速仪(SVP)的温度和深度数据对下放式声学多普勒流速剖面仪(LADCP)的观测结果进行了修正,得到了更为精确的声散射层垂向位置分布。 相似文献
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采用2007年5月大亚湾浮标定点航次采集的生物-光学数据, 分析了大亚湾水体后向散射比率的光谱变化及其影响因素。分析结果表明, 660nm处后向散射比率变化范围在0.0040—0.0245之间, 均值为0.0082±0.0032, 实测后向散射比率光谱波段间的相对变化不超过15%; 颗粒后向散射比率随着叶绿素a浓度增加呈减小的趋势, 高叶绿素浓度显著对应较低的后向散射比率; 粒径是影响大亚湾水体后向散射比率的重要因素之一, 随着水体中Junge粒级斜率的增大, 颗粒后向散射比率显著增大; 折射率的变化也对后向散射比率产生一定影响, 类似的水体粒径分布情况下, 浮游植物与非藻类物质相对贡献的变化将导致折射率的明显变化, 并将主导水体后向散射比率的变化。 相似文献
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2004年7～8月在台湾浅滩周边水域进行了两个断面的水体悬浮物浊度、叶绿素a荧光调查，通过对该区域悬浮物质浊度、叶绿素a荧光的夏季分布变化特征研究，结合水文相关要素分析，初步揭示了区域海洋沉积和再悬浮过程对悬浮体浊度、叶绿素a荧光分布的影响。指出悬浮物质浊度在近岸与陆架外缘主要受再悬浮作用影响，而浅滩区再悬浮作用不明显：在陆架外缘区浮游植物的聚集作用对浊度有一定的贡献作用，而近岸区则不明显。 相似文献
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北半球夏季中高纬海洋声散射层分布研究 总被引：1，自引：0，他引：1
利用第八次北极调查走航ADCP后向散射强度数据，结合太阳高度、海冰密集度和实测水体环境参数数据，统计分析了中高纬海洋声散射层的时空变化特征。结果表明，纬度越高，声散射层在海表滞留时间越短，即使在极昼期间及全海冰覆盖海域，虽然其迁移幅度和后向散射强度减弱，但仍受太阳高度变化影响，且二者具有较强的时序相关性；在北极中央海域，不仅声散射层迁移活动较弱，且出现无明显散射层的情况，可能是因为该海域浮游动物和鱼类聚集度相对较低且迁移活动微弱，超出了本文所用ADCP的探测精度范围；从鄂霍次克海至白令海西南海域，往返ADCP数据均显示有两个后向散射强度上高下低，但垂直迁移时间同步的声散射层，且二者间距随纬度增加而逐渐减小并合为一体，这可能是由不同生活习性的海洋生物造成的。 相似文献
9.
海洋微波散射模型相比于以经验统计建立的地球物理模式函数具有不受特定微波频率限制的优势。组合布拉格散射模型和几何光学模型形成了复合雷达后向散射模型。利用南海北部气象浮标2014年海面风速风向实测值作为散射模型输入，分别比较了复合雷达后向散射模型与RADARSAT-2卫星C波段SAR、HY-2A卫星Ku波段微波散射计的海面后向散射系数，偏差分别为(?0.22±1.88) dB (SAR)、(0.33±2.71) dB (散射计VV极化）和(?1.35±2.88) dB (散射计HH极化)；以美国浮标数据中心(NDBC)浮标2011年10月1日至2014年9月30日共3年的海面风速、风向实测值作为散射模型输入，分别比较了复合雷达后向散射模型与Jason-2、HY-2A卫星Ku波段高度计海面后向散射系数，偏差分别为(1.01±1.15) dB和(1.12±1.29) dB。中等入射角和垂直入射下的卫星传感器后向散射系数观测值与复合雷达后向散射模型模拟值比较，具有不同的偏差，但具有相同的海面风速检验精度，均方根误差小于1.71 m/s。结果表明，复合雷达后向散射模型可模拟计算星载SAR、散射计和高度计观测条件下的海面雷达后向散射系数，且与CMOD5、NSCAT-2、高度计业务化海面风速反演的地球物理模式函数的计算结果具有一致性；复合雷达后向散射模型可用于微波遥感器的定标与检验、海面雷达后向散射的模拟。 相似文献
10.
浮游藻类是海水中的重要组成成分,对其固有光学特性的研究有助于深入了解水体光学的辐射传输。在过去的30年中,大量的研究都集中在藻类吸收特性上,缺少对其散射特性的认识。本文利用分光光度计设计了在实验室中测量含颗粒水体散射和后向散射特性的方法,并利用标准球形颗粒对该方法的可行性进行验证,结果表明,在400~700 nm范围内,散射测量结果与理论值的一致性较好,最大误差小于3%,而后向散射测量结果在蓝紫光处的一致性较好,在近红外波段处有一定误差。运用这两种测量方法对东中国海常见的赤潮藻种中肋骨条藻Skeletonema costatum和东海原甲藻Prorocentrum donghaiense进行测量,结果显示:中肋骨条藻与东海原甲藻的散射系数幅值相近但谱形差异较大,前者随波长增加散射强度递减,后者则相反;在色素吸收较强的波段,两者散射强度均出现与其它波长位置变化趋势相反的情况,这主要是受细胞物质物理性质的影响。两者的后向散射差异较小,但可以看出其谱形受色素吸收的影响很大,在幅值上,东海原甲藻略高于中肋骨条藻,在550 nm处分别为0.001 74,0.001 43 m2/mg(以藻类叶绿素a浓度归一化),后向散射概率分别为1.104%和0.723%。 相似文献
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Diurnal Cycle of Sound Scatterers and Measurements of Turbidity Using ADCP in Beppu Bay 总被引：2，自引：0，他引：2
Xiao-Hua Zhu Yoshio Takasugi Masayuki Nagao Eisuke Hashimoto 《Journal of Oceanography》2000,56(5):559-565
From September 20 to 22 in 1994, the vertical profiles of echo intensity and three-component velocities were measured with a bottom-mounted 300 kHz broadband acoustic Doppler current profiler (ADCP) in Beppu Bay in the Seto Inland Sea of Japan. A very strong thermocline was observed from 50 to 60 m. A pronounced diurnal cycle of backscatter strength (BS) was found above the thermocline. However, it was not found under the thermocline where there was a lack of dissolved oxygen. We suggest that the diurnal cycle of BS is caused by the vertical migration of zooplankton. The downward and upward migration occurred in early morning and late afternoon, respectively. The migration speeds estimated from BS isopleth displacements were about 1 cm s–1. Further, the contribution of turbidity (Tur) to BS was examined by separating out the effect of migrating zooplankton. There was a significant correlation between BS and turbidity under the thermocline. The maximum contributions of the Tur, migrating zooplankton and non-migrating plankton on BS were estimated at 3, 12, 25 dB, respectively. These data suggest that when using an ADCP to estimate Tur, it is very important to consider carefully the backscatter signal from zooplankton. 相似文献
12.
A.J.F. Hoitink 《Marine Geology》2004,208(1):13-31
The Bay of Banten, West Java, Indonesia represents a shallow coastal embayment harboring coral reefs subject to extremely turbid conditions. The sedimentary regime and flow structure of two contrasting coral reef islands in the embayment were investigated to identify the mechanisms responsible for mean and peak levels of suspended sediment concentration (SSC) around the reefs. Arrays of in situ calibrated optical backscatter (OBS) sensors were deployed across the reef slopes. Far field conditions were simultaneously monitored using an acoustic Doppler current profiler (ADCP) and a conductivity temperature and depth (CTD) probe, equipped with an OBS sensor. In addition, hydrographic surveys were conducted using the ADCP attached to a small fishing boat, navigating transects perpendicular to the reef islands. The direct influence of river plumes was found to be insignificant. Waves act only in the uppermost few meters of the reef slopes, where coral growth is most abundant and little sediment is available for resuspension. Tidal currents are the primary cause of high turbidity, which was inferred from peaks in the diurnal and semidiurnal frequency bands of SSC spectra, and the large depths where the turbidity variation sometimes initiates. The entrained sediment disperses upward across the reef slopes, which is likely due to a secondary current associated with bending of the flow along the curved, hydraulically rough reef slopes, in weakly stratified ambient waters. Changes in sediment availability, variable critical shear stresses for erosion and deposition, and the formation and evanescence of island wakes may explain the high variability of SSC at the reef slopes. 相似文献
13.
基于水下滑翔机观测资料,对南海北部一个反气旋涡旋的温度细结构进行了特征分析.温度细结构强度由温度的脉动值确定,并随着尺度的增加呈指数衰减.在垂直方向上,细结构强度随着深度的加深而减弱,细结构特征在海洋表层(0～100m)和表层以下(＞100 m)存在显著区别.表层内,垂向混合和水平混合对细结构强度均有贡献,细结构强度大... 相似文献
14.
Riyad S. Manasrah Fuad A. Al-Horani Mohammad Y. Rasheed Saber A. Al-Rousan Marouf A. Khalaf 《Estuarine, Coastal and Shelf Science》2006,69(3-4):567
This study was focused on analysis of the horizontal and vertical current components with correspondence to tide variation, heat flux, seiches and relative backscatter intensity in coastal waters of the northern Gulf of Aqaba during the summers of 2001–2004. Spectrum analysis has shown eight distinguishable peaks of the tide measurements. In addition to semidiurnal and diurnal barotropic tides, signal periods of 8.13, 5.89–6.32 and 4.06 h were related to shallow water compound and overtides of the principal solar and lunar constituent and to seiches (second and third mode) generated in the Red Sea, whereas seiches of the first mode might enhance the semidiurnal tide signal. The shortest periods of 1.02–1.05, 0.50 and 0.36 h were related to seiches (first, second and third mode, respectively) generated in the Gulf of Aqaba. The spectrum analysis and cross-correlation tests of the horizontal and vertical current components and relative backscatter intensity suggested that the vertical motion at the diurnal period was either due to migration of zooplankton or to water convection. Both of which were of the same order as vertical motion induced by horizontal motions of water particles projected parallel on the bottom gradient line. On the other hand, semidiurnal and diurnal periods detected in the vertical currents were caused by the strong signal in the cross-shore current component, first mode seiches generated from the Red Sea and tide. This could be considered as an indicator of the dominant force influencing the currents, such as winds, thermocline depth, seiches and tidal forcing. A permanent convection during summer is likely to occur in the shallow coastal waters due to relatively high inclined bottom, high evaporation and blowing of dry air, as well as the observed dominance of the downward vertical currents in coastal waters. 相似文献
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北黄海海底麻坑群形态的定量研究及控制因素 总被引：1，自引：0，他引：1
本文基于高分辨率多波束水深数据和反向散射强度数据，对北黄海海底麻坑群的形态参数进行定量研究，结合水深、地形坡度和后向散射强度的变化准确界定了麻坑的轮廓，识别出圆形、椭圆形、拉长型麻坑共282个，并在ArcGIS软件中对其形态参数进行了分析计算，麻坑的平均长轴1.36 km，短轴0.78 km，直径0.94 km，面积0.88 km2，平均周长3.82 km，长宽比1.83，深度0.3~2.5 m，平均面积密集度13%，麻坑的剖面形态有麻坑边缘凹陷、中部有明显凸起（W1型），麻坑边缘凹陷、中部略凸起（W2型），麻坑中部单纯凹陷（V型），分别集中分布在麻坑群的北部、南部、西部。麻坑的平面规模大、深度小的原因与地层中形成麻坑的游离气体浓度较小有关，也可能受到了地震、海啸等外力的诱发。麻坑的长轴优势走向为ENE-WSW、NNE-SSW，底流对其形状的塑造起了较大作用，部分麻坑成串排列，形成串珠状的麻坑链，其排列方式受到海底古河道、古潟湖等沉积地层结构的控制。海底麻坑群发育区反向散射强度为-60~-71 dB，麻坑内部较麻坑外部平均高5 dB，可能为麻坑内部气体泄漏引起海底沉积物被剥蚀后残留下的粗颗粒物质或海底生物活动留下的遗迹导致的。 相似文献
17.
基于2016?2017年4个季节航次数据,分析了湛江湾真光层深度与初级生产力的时空变化特征及其影响因素。结果表明,湛江湾真光层深度平均值为（6.95±3.17）m,空间变化比季节变化明显,Kd(PAR)与浊度存在显著的正相关关系,建立的线性回归模型R2为0.73（p<0.01）,表明悬浮颗粒物对湛江湾真光层深度的影响占主导地位。利用VGPM模型得到初级生产力（以碳计）的平均值为（639.53±427.95）mg/(m2·d),其时空特征与真光层深度基本保持一致,真光层深度比叶绿素a浓度更能解释初级生产力的时空分布模式。 相似文献
18.
《Coastal Engineering》2005,52(2):103-118
The ability of a 1.2-MHz Acoustic Doppler Current Profiler (ADCP) to measure suspended sediment concentration (SSC) and particle size variation in a mud-dominated environment has been investigated. Experiments were conducted in the Bay of Banten, Indonesia, where clays and silts in the range of 3–55 μm are prevalent. The ADCP backscatter depends both on SSC and on the size of the scatterers. Over the time span of several separate deployments, which lasted 20 days at most, SSC was found to be proportional to the acoustically normative grain size squared. Using this relation, the ADCP could be calibrated to yield depth profiles of SSC. The obtained calibrations, however, were spatially and seasonally dependent. Differences between the calibrations could not be completely ascribed to variation in grain size distributions, due to the largely unknown influences of aggregates and organic scatterers. The ADCP backscatter measurements provided insight into diurnal events of erosion and subsequent deposition. An increase or decrease of SSC generally coincided with a raise or decline of the average grain size in the sediment suspension (respectively). 相似文献
19.
A new highly precise source of data has recently become available using multibeam sonar systems in hydrography. Multibeam sonar systems can provide hydrographic quality depth data as well as high-resolution seafloor sonar images. We utilize the seafloor backscatter strength data of each beam from multibeam sonar and the automatic classification technology so that we can get the seafloor type identification maps. In this article, analyzing all kinds of error effects in backscatter strength, data are based on the relationship between backscatter strength and seafloor types. We emphasize particularly analyzing the influences of local bottom slope and near nadir reflection in backscatter strength data. We also give the correction algorithms and results of these two influent factors. After processing the raw backscatter strength data and correcting error effects, we can get processed backscatter strength data which reflect the features of seafloor types only. Applying the processed backscatter strength data and mosaicked seafloor sonar images, we engage in seafloor classification and geomorphy interpretation in future research. 相似文献