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1.
自动剖面浮标研究现状及展望   总被引:1,自引:0,他引:1  
回顾了自动剖面浮标的发展历程,自动剖面浮标由Swollow提出的中性浮子发展而来,演变到现在的PROVOR型、APEX型、SOLO型等自动剖面浮标。文中介绍了Argo计划中几种主要的自动剖面浮标,其浮力调节原理主要是通过改变浮标在水中的排水体积实现自动沉浮,从而测量水的温度、盐度、深度等数据。对常规(2 000 m)和深海(2 000 m)自动剖面浮标进行比较,大部分深海自动剖面浮标耐压结构已经采用球形设计,浮标受压后变形小且可减轻浮标自重;单冲程柱塞泵改变为体积较小的液压泵,提供超高压的同时可以充分利用球体空间。目前,常规自动剖面浮标已广泛应用到海洋环境数据的调查、收集,而深海自动剖面浮标仍处于研发与试验阶段,面临诸多的技术挑战,对浮标的可靠性提出了更高的要求。  相似文献   

2.
剖面浮标被广泛应用在国际"Argo"计划中,通过在海洋中上浮下潜运动来收集海水温、盐、深等物理参数。为了满足科学研究的需要,将常规2 000 m的剖面观测深度延伸至更深的海区十分有必要。为了设计一款性能优越的4 500 m深海剖面浮标,文章针对深海剖面浮标的特点,以液压系统的性能参数为依据,以100个测量剖面为设计目标,同时考虑到浮标露出水面的干舷高度、在深海环境下体积压缩以及其内部各模块之间的关联与耦合,建立深海剖面浮标概念设计的多学科设计优化模型,应用BLISCO多学科设计优化算法框架进行总体设计优化,优化后的总重量为48.773 kg,与日本的4 000 m的深海剖面浮标相比,重量减小了2.52%,测量剖面数增加了30个。设计优化结果表明,该型深海浮标的设计能满足深海环境下的测量要求,且性能优于日本的4 000 m级深海剖面浮标。  相似文献   

3.
以新型激光雷达浮标系统为研究对象,基于ANSYS/AQWA开展了激光雷达浮标系统运动响应特性数值研究,研究了浮标吃水深度、形状参数对于激光雷达浮标运动响应的影响规律,分析了附加质量、辐射阻尼、运动响应RAO及一阶、二阶波浪力等水动力参数。采用时域分析方法对不同风浪流荷载入射角度下的激光雷达浮标锚泊系统张力特性进行了计算分析。研究结果表明:随着浮标吃水深度的增加,浮标纵荡方向响应无明显变化,垂荡响应显著增大;随着浮标底部圆台直径的增大,浮标纵荡方向响应变化较小,而圆柱形浮标垂荡运动响应显著大于圆台形浮标;当浮标系泊锚链发生松弛—张紧状态变化时易出现极端张力,且极端张力出现的幅值和频率随有效波高的增大和谱峰周期的减小而增大。  相似文献   

4.
初探我国Argo浮标下潜深度标定   总被引:1,自引:0,他引:1  
为了使剖面能停留在预定深度,通过水静力学角度对相应的浮标压载标定方法进行研究.试验表明,浮标重量改变1 g,就会造成大约10 m停留深度的变化.论文详细描述了用压力罐进行浮标压载重量标定的方法,并通过一台浮标的压载实验给出浮标配重计算方法.  相似文献   

5.
南海自动剖面浮标轨迹模拟系统包括高分辨率模式流场、拉格朗日追踪模型和垂向浮标运动参数化方案等三个核心部分。该系统可在南海范围内模拟两类自动剖面浮标:传统自动剖面浮标(停滞深度为1000m,最大下潜深度为2000m)和新型深海自动剖面浮标(停滞深度为距海底500m)。通过对南海现有的6个传统浮标的模拟,该系统可以预测其100d内的漂流轨迹。通过与真实浮标轨迹数据的对比,验证了该模拟系统的准确性。此外,根据该系统,我们初步探讨了深海自动剖面浮标阵列(时空分辨率为2°×2°×30d)在南海内区布放方案的可行性。该模拟系统的建立和完善将有助于对现有传统剖面浮标布放策略进行优化,并对未来深海剖面浮标在南海的推广应用提供初步的理论依据。  相似文献   

6.
南海自动剖面浮标轨迹模拟系统包括高分辨率模式流场、拉格朗日追踪模型和垂向浮标运动参数化方案等三个核心部分。该系统可在南海范围内模拟两类自动剖面浮标: 传统自动剖面浮标(停滞深度为1000m, 最大下潜深度为2000m)和新型深海自动剖面浮标(停滞深度为距海底500m)。通过对南海现有的6个传统浮标的模拟, 该系统可以预测其100d内的漂流轨迹。通过与真实浮标轨迹数据的对比, 验证了该模拟系统的准确性。此外, 根据该系统, 我们初步探讨了深海自动剖面浮标阵列(时空分辨率为2°×2°×30d)在南海内区布放方案的可行性。该模拟系统的建立和完善将有助于对现有传统剖面浮标布放策略进行优化, 并对未来深海剖面浮标在南海的推广应用提供初步的理论依据。  相似文献   

7.
文章对正在研制中的“自持式剖面循环探测漂流浮标”完成一个剖面测量任务的过程,进行了运动分析和数值计算。数值计算结果与试验数据的对比显示,数值计算结果是可信的,这对了解浮标在水下的运动状态提供直观的帮助,并为浮标的海上试验提供了参考依据。  相似文献   

8.
利用CFD技术对浮标上浮下潜运动进行数值模拟实验分析,流场求解基于Navier-Stokes方程和RNG k-epsilon湍流模型,压力和速度的耦合采用SIMPLE方法解耦,流场的控制方程采用有限体积法离散且分离式求解。在此基础上揭示了浮标上浮下潜运动过程的流场特性;得到浮标水下运动过程阻力随速度变化的规律,并将仿真结果与浮标海试试验结果进行了对比分析,验证了该方法的可行性。为浮标控制和浮标外形结构的优化提供了理论依据。  相似文献   

9.
基于Argo浮标的热带印度洋混合层深度季节变化研究   总被引:2,自引:0,他引:2  
根据2004-2005年热带印度洋(30°S以北)的Argo浮标(自持式海洋剖面观测浮标)温度-盐度剖面观测资料,采用位势密度判据(Δσθ=0.03 kg/m3),针对每个Argo浮标的温度-盐度观测剖面确定了海洋混合层的深度,然后采用Krig插值方法构建了3°×3°空间分辨率的月平均网格化混合层深度产品。通过与已有气候平均混合层深度资料的比较表明了该产品的合理性,在此基础上进一步对热带印度洋海盆尺度的混合层深度空间特征和季节变化规律进行了讨论。研究结果表明,Argo浮标资料可用于热带印度洋混合层变化的研究,为进一步研究热带印度洋海-气相互作用提供了基础资料。  相似文献   

10.
利用船载CTD仪、国外剖面浮标(APEX)和实验室盐度计等标准仪器设备,在西北太平洋海域对2种型号国产剖面浮标(COPEX和HM2000)进行了现场比测试验,并对观测资料质量进行了定性和定量分析与评价.结果表明:(1) COPEX和HM2000型剖面浮标观测的盐度资料均能达到国际Argo计划提出的±0.01的精度要求;(2)HM2000的最小观测深度离海面1 m以内,最大观测深度基本稳定在2 000 m左右,并能保持在1000 m深度附近漂移,而COPEX的最小观测深度在8~9 m之间,最大观测深度则在1 800~1 900 m之间波动,且漂移深度都在600~800 m之间;(3)COPEX和HM2000都获得了70条以上有效观测剖面.总体而言,两种国产剖面浮标观测的温、盐度资料都是可信、可靠的.但试验中暴露的一些问题和不足仍有待不断改进和完善.  相似文献   

11.
Wave attenuation characteristics of a tethered float system have been investigated for various wave heights, wave periods, water depths, depths of submergence of floats and float sizes. As the floats are similar in size and shape, only a single tethered spherical float is considered for the theoretical analysis. Float motion is determined through the dynamical equation of motion, developed for a single degree of freedom. From incident and transmitted wave powers, transmission coefficients are computed. The results show that transmission coefficient does not vary with changes in wave height or water depth. When depth of submergence of float increases, wave attenuation decreases, showing that the system performs well when it is just submerged. As float velocity decreases with increase in float size, transmission coefficient increases with increase in float size. The influence of wave period on wave attenuation is remarkable compared to other parameters. The effect of drag on wave attenuation is studied for varying drag coefficient values. Theoretical results are compared with experimental values and it is found that theory overestimates wave attenuation which may probably be due to various linearisations involved in the theoretical formulation.  相似文献   

12.
Estimating the average lifetime of floats is very important for Argo, because the total cost of maintaining the monitoring network largely depends on float lifetime. However, the actual lifetime of floats used in Argo is currently unknown. An estimate can be made by examining past float survival, but this is complicated by floats still operating at sea and continuous improvements in float hardware. Because APEX (Autonomous Profiling Explorer) floats are the most widely deployed type of float in the world oceans, in this study we estimate the lifetime of the latest model of APEX powered by alkaline batteries. The expected lifetime is estimated with a statistical method that allows for floats that are still active and that failed because of a known and now fixed hardware fault that should not cause failure in the latest model of floats. As an example, we analyzed the APEX fleets managed by the Japan Agency for Marine-Earth Science and Technology (JAMSTEC), because we have access to a JAMSTEC database in which the causes of float failure have been carefully correlated to known hardware problems. Analysis of the JAMSTEC fleet (n = 571, as of 7 May 2008) indicated that the expected lifetime of the latest model of APEX is 134.6 (127.6–141.5, considering standard errors) cycles, equivalent to 3.7 years of 10-day cycles. We conclude that the annual deployment of 813 (773–859) APEX floats is needed to maintain the Argo observational network of 3000 floats. Floats with different hardware configurations (e.g., lithium batteries) or different mission programs (e.g., shallower profiling, deeper profiling every several cycles) may be expected to have an even longer lifetime.  相似文献   

13.
We deployed two profiling floats in the region south of the Kuroshio Extension in March 2000. Temperature and salinity profiles from a depth of 1500 × 104 Pa to the surface are reported every two and four weeks, respectively. The floats performed very well for first four months after deployment. Later they failed in surfacing for a few months when the sea surface temperature in the region was high. The salinity sensors seemed to suffer from some damage during their failure-in-surfacing period. Despite this trouble, the results clearly demonstrate that the profiling float is a very useful and cost-effective tool for physical oceanographic observation in the open sea. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

14.
ARGO剖面浮标电导率传感器漂移问题探讨   总被引:3,自引:0,他引:3  
ARGO剖面浮标在海上长期工作,其携带的电导率传感器漂移会导致测量数据误差,从而影响观测资料的质量。文章利用误差理论和回归分析、曲线拟合等数理统计方法,检测和处理由ARGO剖面浮标电导率传感器漂移所带来的测量误差,并对太平洋、大西洋和印度洋上已经发现有电导率传感器漂移的ARGO资料进行了校正,取得了比较理想的结果。  相似文献   

15.
An improved method to estimate the time-varying drift of measured conductivity from autonomous CTD profiling floats has been developed. This procedure extends previous methods developed by Wong, Johnson and Owens [2003. Delayed-mode calibration of autonomous CTD profiling float salinity data by θS climatology. Journal of Atmospheric and Oceanic Technology, 20, 308–318] and Böhme and Send [2005. Objective analyses of hydrographic data for referencing profiling float salinities in highly variable environments. Deep-Sea Research Part II, 52, 651–664]. It uses climatological salinity interpolated to the float positions and observed θ surfaces and chooses 10 ‘best’ levels that are within well-mixed mode waters or deep homogeneous water masses. A piece-wise linear fit is used to estimate the temporally varying multiplicative adjustment to the float potential conductivities. An objective, statistical method is used to choose the breakpoints in the float time series where there are multiple drift trends. In the previous methods these breakpoints were chosen subjectively by manually splitting the time series into separate segments over which the fits were made. Our statistical procedure reduces the subjectivity by providing an automated way for doing the piece-wise linear fit. Uncertainties in this predicted adjustment are estimated using a Monte-Carlo simulation. Examples of this new procedure as applied to two Argo floats are presented.  相似文献   

16.
Long-term Sensor Drift Found in Recovered Argo Profiling Floats   总被引:5,自引:0,他引:5  
We recovered three Argo profiling floats after 2 to 2.5 years of operation, and recalibrated their temperature, conductivity, and pressure sensors. The results demonstrate that these floats exhibited a significant drift in salinity of −0.0074 to −0.0125, primarily due to the conductivity sensor drift. Combined with the recalibration result for another previously recovered float, the indication is that the negative salinity drift increases nearly in proportion to the operating period of floats. The increasing rate is −0.0041 (±0.0015) year−1, which yields a salinity drift of −0.016 (±0.006) for the expected float lifetime of four years. The present result suggests that reducing the float surfacing time would improve the accuracy of the salinity measurements.  相似文献   

17.
多点液压式波浪能海水淡化系统建模与仿真   总被引:1,自引:1,他引:0  
为缓解淡水资源短缺及化石能源过度使用问题,提出多点液压式波浪能海水淡化系统,该系统主要由采能装置、液压传递系统与反渗透膜海水淡化设备组成。系统的采能装置采用振荡浮子式,可将波浪能转换为浮子振荡从而被液压系统吸收达到采集波浪能的目的。为了提高液压式波浪能海水淡化系统的采能效率及淡水率,利用AMEsim软件对液压传递系统进行建模与仿真,分析了蓄能器、浮子个数及波高对液压传递系统输出响应的影响。结果表明:蓄能器能够使液压马达的输出响应更加稳定;当浮子的数量增加时,液压系统达到稳定的运行状态所需的时间更短,从而有利于提高系统的效率;波高在2 m左右时,本系统的产水量达到最大。  相似文献   

18.
HM2000 型剖面浮标是一种新颖的国产海洋观测仪器,可以长期在海上自由漂移并连续测量 0~2 000 m 水深内的海水温、盐度剖面数据,已被国际 Argo 组织用于全球 Argo 实时海洋观测网建设和维护。 详细介绍了该型浮标的工作原理、结构、功能和主要技术指标等,并与 APEX 型浮标进行了比较分析, 表明了 HM2000 型剖面浮标具有明显的功能优势,且测量的温、盐度质量是有足够保证的,完全可以替代国外浮标用来主导建设我国的 Argo 区域海洋观测网。  相似文献   

19.
Stability of Temperature and Conductivity Sensors of Argo Profiling Floats   总被引:7,自引:3,他引:7  
After recalibration of the temperature and conductivity sensors of three Argo profiling floats recovered after operations for four to nine months, the results indicate that the floats basically showed no significant drift, either in temperature or salinity, and adequately fulfilled the accuracy requirement of the Argo project (0.005°C for temperature and 0.01 psu for salinity). Only the third float showed a significant offset in salinity of about −0.02 psu, as expected from comparison between the float data and the shipboard conductivity-temperature-depth data. This offset was caused by the operational error of the PROVOR-type float, in which the surface water was pumped immediately after the launch, fouling the conductivity sensor cell. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

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