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1.
ADCP模拟信号源谭小勇1前言ADCP是“声学多普勒海流剖面仪”的英文缩写,它是根据多普勒原理用矢量合成法,遥测海流的垂直分布。目前国际海委会以将ADCP定为四种先进的海洋观测仪器之一。现在我们进行的ADCP工作研制已接近尾声,我们希望进一步完备AD...  相似文献   

2.
在金塘水道西口门2006年冬季和2007年夏季大、小潮期间应用美国RDI公司生产的300 kHz声学多普勒流速剖面仪(ADCP)进行25 h的走航式断面观测,同步采集水样过滤获得悬沙浓度.实测断面流速、流向表明:落潮时流向为东南向,涨潮时分两股,靠近北仑为西南向,靠近金塘岛为西北向;夏季大潮最大流速为260 cm/s,大于冬季大潮;观测期间断面悬沙浓度为0.4~1.5 g/L,冬季大于夏季约0.3~0.5 g/L;ADCP后向散射强度冬季大于夏季约5 dB.应用实测CTD数据进行声吸收系数校正,通过计算,断面后向散射强度分布趋势基本不变.后向散射强度与悬沙浓度成正比,与水深成正比,垂向分布与潮时有关,冬季小潮水深增大时,后向散射强度反而减小.回归ADCP后向散射强度与水样悬沙浓度之间半经验半理论统计关系,发现冬季不成线性关系,夏季成线性关系,且相关性较好,相关系数为0.7,说明夏季较高浓度下后向散射强度可以表示悬沙浓度的大小.夏季大、小潮期间高分辨率的悬沙浓度断面数据分析表明,反演后的悬沙浓度值与流速成正比;近岸悬沙浓度大于断面中部;涨急和落急时同一水深高低含沙量值错落分布,涨憩和落憩则分层明显;大潮悬沙浓度大于小潮流约0.05 g/L.断面两端点反演后的悬沙浓度与实测值比较,呈现半日潮含沙量双峰特征,夏季大潮反演后的悬沙浓度与实测值分布一致,实测值大于0.9 g/L时,两者量值相差大,小潮则拟合很好.因此,应用走航式ADCP测量高悬沙浓度是可行的,它可大大提高测量效率,为获取现场悬沙浓度提供了一种新方法.  相似文献   

3.
ADCP测量悬沙浓度的可行性分析与现场标定   总被引:18,自引:3,他引:18  
程鹏  高抒 《海洋与湖沼》2001,32(2):168-176
根据现场观测数据,对ADCP测量悬浮沙浓度的进行标定实验。结果表明,在观测期间悬沙粒径变化较小的条件下,后散射强度与水样悬沙浓度之间存在较好的相关性。悬沙浓度剖面标定公式中的参数C′可用剖面实测水样浓度来确定,该参数与浓度密切相关:同一剖面不同浓度之间有一定的波动,但同一浓度不同潮时的变化很小。使用同一剖面参数C′的平均值计算出的剖面悬沙分布误差较大(29%-43%),而按不同深度段分别标定,误差可以小于20%,能够满足沉积动力学研究的需要。  相似文献   

4.
螺旋藻多糖对CD3AK细胞增殖能力的影响   总被引:7,自引:0,他引:7  
研究了螺旋藻多糖(PS)对CD3McAb激活的杀伤细胞(CD3McAb Activated Killer Cells,CD3AK Cells)增殖能力的影响。结果表明,当PS浓度为2.5μg·ml^-1培养体系条件下,对CD3AK细胞具有明显的刺激细胞增殖作用(P〈0.02);对培养长达23d的CD3AK细胞杀伤肿瘤细胞(K562细胞)的活性仍维持在较高的水平(46.5% ̄50%)。提示PS对辐射  相似文献   

5.
通过实时观测黄河口洪季(9月)潮滩潮周期内悬沙浓度和波潮流等水动力因素的变化,并结合边界层悬浮物剖面测量仪(ASM-4)数据,讨论了悬沙浓度在潮周期内的变化及其影响因素,计算了再悬浮通量、分析了悬沙浓度的垂向分布特征。结果表明,一级海况下海流对再悬浮的贡献较大,二级海况下波浪对再悬浮的贡献较大。观测点悬沙浓度多以浓度峰的形式出现,既有潮流冲刷床面所引起的悬沙浓度峰,也存在由波致再悬浮和潮流输运所引起的悬沙浓度峰。  相似文献   

6.
根据连云港近岸海域15个测站的大、中潮6层位垂向同步连续海流、悬沙浓度和盐度等观测资料,分析了悬沙浓度的时空分布特征、潮周期内的变化及其影响因素,计算了再悬浮通量.结果表明,连云港近岸海域悬沙浓度在空间分布上符合悬沙分布的一般规律,在时间域中多以浓度峰的形式出现,并多集中在底层某一深度内,悬沙浓度峰主要发生在高低潮位以...  相似文献   

7.
椒江河口悬沙浓度垂向分布和泥跃层发育   总被引:14,自引:2,他引:12  
论述了椒江河口粘性细颗粒泥沙洪、枯季及大、小潮悬沙浓度分布.椒江河口水体高度混浊,近底层悬沙浓度可达71kg/m3以上.在河口最大混浊带,小潮期水体层化现象明显,悬沙浓度垂向分布呈三层结构,即活动悬沙层、泥跃层和浮泥层.泥跃层是水体中悬沙浓度分布剧变层,梯度大.在河口咸、淡水互相作用下,悬沙浓度大于3kg/m3、盐度在4~16及水流速度中等的条件下泥跃层发育.  相似文献   

8.
时钟 《海洋科学》2000,24(4):56-56
1连续的、高时空分辨率的河口细颗粒悬沙浓度垂线分布在长江口深水航道北槽,利用"声学是沙观测系统"观测到大潮典型的高时空分辨率细颗粒是沙浓度声学垂向分布图和垂线分布曲线。研究结果表明:(1)在涨潮时呈L形,是沙浓度的垂向变化梯度小(浓度小于1.0gL-1)。(2)在涨急时呈射流形,射流项悬沙浓度达10gL-1,悬沙浓度的垂向变化梯度大。(3)在接近涨想时,是沙浓度的垂向梯度小。(4)在落潮时从水面到水底是沙浓度按指数增加,代表恒定均匀流中悬沙处于平衡条件的分布,泥沙垂向扩散系数。在数值上大约是泥沙颗粒沉降速度Ws的两…  相似文献   

9.
廉州湾海域的悬沙分布特征   总被引:1,自引:0,他引:1  
本文根据67个大面积观测站和14个周日连续观测站的水文和悬沙观测资料,通过对悬沙浓度和单宽输沙特征值的计算,讨论了该湾悬沙浓度的分布规律以及单宽输沙与悬沙运移的特点。  相似文献   

10.
盐藻的室温光抑制   总被引:2,自引:0,他引:2  
实验用盐藻取自天津塘沽轻工业部制盐研究所,采用ASP2培养液为培养基,研究了盐藻的室温光抑制现象,并探讨了盐藻的光保护反应机理,结果表明,盐藻对高辐照有很强的忍耐力,且光合能力的恢复也很强,氯霉素(CAP)或二硫苏糖醇(DTT)在高光下强烈地加深了对PSII光化学效率(Fv/Fm)和光合量子效率(Φi)的抑制,但CAP或DTT单独作用并不抑制盐藻的光化学系统在低光下的可逆恢复;盐藻在CAP+DTT  相似文献   

11.
The purpose of the present contribution is to explore the technique to use Acoustic Doppler Current Pro- filers (ADCPs) for suspended sediment flux measurements, which may be applied to coastal embayment environments such as estuaries and tidal inlets for sediment exchange and budget studies. Based on tidal cycle measurements from the entrance of ]iaozhou Bay, Shandong Peninsula, eastern China, statistical rela- tionships between the suspended sediment concentration (SSC) and ADCP echo intensity output are estab- lished. Echo intensity data obtained during an ADCP survey along two cross-sections during a spring tidal phase were transformed into SSC data. The ADCP current velocity and SSC data were then used to calculate the flux of fine-grained sediment. The results show that net sediment transport at the entrance is directed towards the open sea, with an order of magnitude of 103 t per spring tidal cycle; hence, although Jiaozhou Bay is a low SSC environment, the tidally induced suspended sediment transport can be intense.  相似文献   

12.
ADCP对悬浮沉积物浓度的测量及其误差分析研究   总被引:6,自引:0,他引:6  
为实时、连续地测量海水中悬浮沉积物,利用声学多普勒海流剖面仪(ADCP),可以在测流的同时,测量海洋悬浮沉积物浓度。描述了利用后散射强度,估计悬浮沉积物浓度的原理。在现场测试中,利用采水器采集水样,通过水样分析并结合声信号的衰减特征对AI)CP的测量结果进行修正。作者还结合现场测试结果,对这一测量方法的精度进行了分析。现场实验表明,经公式校正后,ADCP测得的后散射强度与实测水样所获得的悬浮沉积物浓度之间有很好的相关性,相关系数达0.88,由此证明,此测量方法具有很好的实用价值和应用前景。  相似文献   

13.
长江口悬沙动力特征与输运模式   总被引:5,自引:0,他引:5  
本项研究用ADCP在长江河口进行高频、高分辨率三维流速和声学浊度的定点观测,通过对定点站位潮周期内的悬沙浓度、流速和盐度的分析,计算悬沙输运率;悬沙输运机制分析表明平流作用、斯托克斯漂移效应在悬沙输运中占据主导地位.此外,从河口内向河口外,潮周期内的水动力特征与悬沙净输运具有明显的地域性差异,主要表现在悬沙输送的贡献因子、盐度的垂向混合和分布特征、垂向流速等方面.在拦门沙下游和口外地区,悬沙均向西、北方向输送,而拦门沙上游则向东、南方向输送.这种悬沙输运格局,对于长江口拦门沙及附近最大浑浊带的形成有着重要的作用.  相似文献   

14.
ADCP资料处理中的船速计算   总被引:5,自引:0,他引:5  
吴中鼎  梁广建  李占桥  陈淼 《海洋测绘》2004,24(5):13-15,19
船载ADCP具有走航测流的特点,弥补了传统测流仪器只有停船才能观测的不足。它可以同时观测多层海流数据,获取连续性资料。ADCP测得流速是海水相对于船体的速度,在正常观测条件下,船速远大于海水流速,因而船速计算是ADCP资料处理的关键。本文对不同的船速计算方法进行了比较,对使用参考层法计算船速的原理、特点和效果进行了论述。  相似文献   

15.
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   

16.
悬沙的ADCP估测方法   总被引:6,自引:1,他引:6  
ADCP估测悬沙含量是基于声波的背散射强度正比于悬沙浓度的理论。在实际测验中,由于多种因素干扰,ADCP所得到的背散射强度与悬沙浓度之间存在着不定的非线性关系。同传统的回归方法比较,BP网络模型方法可以使含沙估测精度有较大的提高。  相似文献   

17.
基于座底ADCP实测回波强度信号,结合短期实测悬浮体质量浓度,反演长时间序列悬浮体质量浓度,定量分析了渤海湾近一年悬浮体质量浓度变化特征及其影响因素。结果表明:受风浪影响,该区悬浮体质量浓度具有明显季节性变化特征,风浪作用强烈的季节其悬浮体浓度表现为相对高值。悬浮体净输运同样具明显季节性变化,秋冬强风浪作用下,悬浮体的净输运量明显增加;而在不同季节,月净输运方向具有不同的主输运方向。悬浮体质量浓度日变化受潮流控制明显,长周期变化则主要与风场的变化有关。潮流涨急过程与风致大浪过程均可引起沉积物再悬浮,导致悬浮体浓度明显增高。  相似文献   

18.
In order to study the mechanism of flow-sediment movement, it is essential to obtain measured data of water hydrodynamic and sediment concentration process with high spatial and temporal resolution in the bottom boundary layer (BBL). Field observations were carried out in the northwest Caofeidian sea area in the Bohai Bay. Near 2 m isobath (under the lowest tidal level), a tripod system was installed with AWAC (Acoustic Wave And Current), ADCP (Acoustic Doppler Current Profilers), OBS-3A (Optical Backscatter Point Sensor), ADV (Acoustic Doppler Velocimeters), etc. The accurate measurement of the bottom boundary layer during a single tidal period was carried out, together with a long-term sediment concentration measurement under different hydrological conditions. All the measured data were used to analyze the characteristics of wave-current-sediment movement and the BBL. Analysis was performed on flow structure, shear stress, roughness, eddy viscosity and other parameters of the BBL. Two major findings were made. Firstly, from the measured data, the three-layer distribution model of the velocity profiles and eddy viscosities in the wave-current BBL are proposed in the observed sea area; secondly, the sediment movement is related closely to wind-waves in the muddy coast area where sediment is clayey silt: 1) The observed suspended sediment concentration under light wind conditions is very low, with the peak value generally smaller than 0.1 kg/m3 and the average value being 0.03 kg/m3; 2) The sediment concentration increases continuously under the gales over 6-7 in Beaufort scale, under a sustained wind action. The measured peak sediment concentration at 0.4 m above the seabed is 0.15-0.32 kg/m3, and the average sediment concentration during wind-wave action is 0.08-0.18 kg/m3, which is about 3-6 times the value under light wind conditions. The critical wave height signaling remarkable changes of sediment concentration is 0.5 m. The results show that the suspended load sediment concentration is mainly influenced by wave-induced sediment suspension.  相似文献   

19.
In order to study the mechanism of flow-sediment movement, it is essential to obtain measured data of water hydrodynamic and sediment concentration process with high spatial and temporal resolution in the bottom boundary layer (BBL). Field observations were carried out in the northwest Caofeidian sea area in the Bohai Bay. Near 2 m isobath (under the lowest tidal level), a tripod system was installed with AWAC (Acoustic Wave And Current), ADCP (Acoustic Doppler Current Profilers), OBS-3A (Optical Backscatter Point Sensor), ADV (Acoustic Doppler Velocimeters), etc. The accurate measurement of the bottom boundary layer during a single tidal period was carried out, together with a long-term sediment concentration measurement under different hydrological conditions. All the measured data were used to analyze the characteristics of wave-current-sediment movement and the BBL. Analysis was performed on flow structure, shear stress, roughness, eddy viscosity and other parameters of the BBL. Two major findings were made. Firstly, from the measured data, the three-layer distribution model of the velocity profiles and eddy viscosities in the wave-current BBL are proposed in the observed sea area; secondly, the sediment movement is related closely to wind-waves in the muddy coast area where sediment is clayey silt: 1) The observed suspended sediment concentration under light wind conditions is very low, with the peak value generally smaller than 0.1 kg/m^3 and the average value being 0.03 kg/m^3; 2) The sediment concentration increases continuously under the gales over 6-7 in Beaufort scale, under a sustained wind action. The measured peak sediment concentration at 0.4 m above the seabed is 0.15-0.32 kg/m^3, and the average sediment concentration during wind-wave action is 0.08-0.18 kg/m^3, which is about 3-6 times the value under light wind conditions. The critical wave height signaling remarkable changes of sediment concentration is 0.5 m. The results show that the suspended load sediment concentration is mainly influenced by wave-induced sediment suspension.  相似文献   

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