基于奇异谱分析的静态相对重力观测重力固体潮提取

针对相对重力测量数据中存在的重力固体潮信号,本文提出将奇异谱分析方法（Singular Spectrum Analysis,SSA）应用到相对重力测量数据处理中,在不需要测站坐标等先验信息的条件下从相对重力数据中提取重力固体潮,提供了一种获取重力固体潮的新思路.采用模拟的相对重力数据进行实验,利用SSA方法和小波变换方法分别从模拟信号中提取重力固体潮并进行结果对比,SSA获取的重力固体潮与理论值残差RMS为0.3 μGal,小波方法获取的残差RMS为1.6 μGal.利用CG-5相对重力仪实测数据进行实验,提出一种利用SSA外推时间序列来削弱边界效应的新思路,实验结果显示采用这种方法后重力固体潮值与理论值残差序列的RMS和STD均有所减小.通过实验发现削弱边界效应后SSA提取的重力固体潮与采用Tamura潮波表计算的重力固体潮理论值残差RMS值为2.2 μGal.利用SSA提取的零点漂移值与最小二乘拟合得到的结果基本一致,十天内的差值小于0.4 μGal/d.     

长江口海域赤潮成因及其防治对策

对长江口海域的赤潮发生形势进行了系统总结与分析,探讨了长江口海域赤潮灾害的成因及其防治对策。长江口及邻近海域是我国赤朝高发区,自20世纪80年代以来赤潮发生越来越频繁,赤潮生物种类增加,2002年首次发生了有毒亚历山大藻(Alexandrium sp．)赤潮,赤潮危害程度在增大,这与长江口海域的环境和生物条件、河口最大军浊带、长江上游大型水利工程建设以及全球气候变化对长江口海域赤潮高发区的影响有直接关系,同时河口海域甲藻孢囊也是赤潮发生的种源。建议建立赤潮立体监测体系、赤潮信息管理系统、海产品赤潮毒素卫生检疫制度和赤潮应急响应机制,全面加强长江口海域的赤潮监控与防治工作。     

非迁移潮作用下的电离层赤道异常区单峰现象及其经度分布

当喷泉效应较弱而双峰结构发展不充分的时候,可能在赤道异常区仅能够观测到一个电子密度的峰值,称之为单峰现象.本文利用CHAllenging Minisatellite Payload卫星在2001-2010年的电子密度数据给出了单峰的发生规律,单峰在地方时早上08：00-10：00和下午16：00-19：00发生率高,发生位置在经度上呈现多波数分布,尤其在10：00-18：00明显：在分季时多呈现四波,而在冬至季时以三波为主.单峰发生多的经度,正好对应着双峰的结构特征较弱之处.究其原因,是非迁移潮的DE2和DE3分量调制了背景风场和大气发电机电场,在电场和喷泉效应减弱的经度,双峰结构难以形成时,就会表现为单峰结构.本文扩展了对单峰现象的地方时、季节和经度分布等规律的了解,明确了非迁移潮在其中施加的影响,由此,单峰同双峰现象一样可以用于研究非迁移潮对热层-电离层的作用.     

Time stability of spring and superconducting gravimeters through the analysis of very long gravity records

Long gravity records are of great interest when performing tidal analyses. Indeed, long series enable to separate contributions of near-frequency waves and also to detect low frequency signals (e.g. long period tides and polar motion). In addition to the length of the series, the quality of the data and the temporal stability of the noise are also very important. We study in detail some of the longest gravity records available in Europe: 3 data sets recorded with spring gravimeters in Black Forest Observatory (Germany, 1980–2012), Walferdange (Luxemburg, 1980–1995) and Potsdam (Germany, 1974–1998) and several superconducting gravimeters (SGs) data sets, with at least 9 years of continuous records, at different European GGP (Global Geodynamics Project) sites (Bad Homburg, Brussels, Medicina, Membach, Moxa, Vienna, Wettzell and Strasbourg). The stability of each instrument is investigated using the temporal variations of tidal parameters (amplitude factor and phase difference) for the main tidal waves (O1, K1, M2 and S2) as well as the M2/O1 factor ratio, the later being insensitive to the instrumental calibration. The long term stability of the tidal observations is also dependent on the stability of the scale factor of the relative gravimeters. Therefore we also check the time stability of the scale factor for the superconducting gravimeter C026 installed at the J9 Gravimetric Observatory of Strasbourg (France), using numerous calibration experiments carried out by co-located absolute gravimeter (AG) measurements during the last 15 years. The reproducibility of the scale factor and the achievable precision are investigated by comparing the results of different calibration campaigns. Finally we present a spectrum of the 25 years of SG records at J9 Observatory, with special attention to small amplitude tides in the semi-diurnal and diurnal bands, as well as to the low frequency part.     

Comparison of two extensometric stations in Hungary

Quartz-tube extensometers are used to measure rock deformations in two geodynamic observatories in Hungary in order to contribute to the investigation of recent tectonic movements on the area of the Pannonian Basin. One of the observatories is situated on the border of the Alps at Sopronbánfalva and is set in the metamorphic (gneiss) material of the mountains. The other station is in the basically karstic environment of the Mátyáshegy (Mátyás Hill) near Budapest. The aim of this paper is to investigate how the local conditions, such as structure of the observatory, topography or geologic features of the surrounding rocks, lead to additional or modified deformations of the extensometric stations. Data collected over eight years were processed and analysed to compare the observatories taking into account geologic, lithologic and topograpic properties of the measurement sites. Tidal and coherence analysis of the continuous strain measurements revealed that the instrument at Sopronbánfalva is more sensitive to atmospheric pressure loading than the extensometer at Mátyáshegy. Signal to noise values from the data processing of the short period variations support the higher stability of tidal strain measurements at Mátyáshegy. The strain rates measured by extensometers in both observatories are in good agreement with the strain rates inferred from GPS measurements of the Hungarian GPS Geodynamic Reference Network and the Central European GPS Reference Network.     

地震周期的数值估计

模拟计算表明,地震有多种成因,多种因素的周期复合掩盖了地震的周期性。环太平洋地震带受板块运动、潮汐波动、厄尔尼诺、拉尼娜、海平面变化、剥蚀沉积、太平洋十年涛动等诸多因素影响,地震活动最为强烈,8．5级以上强震有明显的准60年和1800年潮汐波动周期。     

Microsporidan parasite Thelohania contejeani Henneguy from New Zealand freshwater crayfish

The sporozoan Thelohania contejeani Henneguy (Microsporida: Nosematidae) is recorded from Paranephrops zealandicus (White) for the first time. It is an intracellular parasite invading musculature throughout the crayfish, causing a gradual decrease in locomotor activity, and it may eventually cause the death of the host. Infected crayfish were found in the northern part of Leith Stream, Dunedin, where the infection rate reached a maximum of 20%. This parasite has formerly been recorded only from Northern Europe.     

Contribution of Tides to Sea Level Variations Along Visakhapatnam,India

The sea level variations along Visakhapatnam coast are governed by astronomical tides and nontidal oscillations including atmospheric pressure, winds, coastal currents, Ekman Pumping, and river influx. Tidal and nontidal sea level oscillations are usually studied separately because of the vastly different ways in which they are forced. In this study the tidal oscillations along Visakhapatnam are analyzed using GOTIC2 tidal model. The correlation between monthly mean sea level and monthly mean tides is 47% (r = 0.68) and increases to 54% (r = 0.74) when applied for inverse-barometric effect. The major six partial tides are computed and presented. The tidal variations from Neap tide to Spring tide are studied.     

南海北部东沙岛附近的内潮和余流特征

采用东沙岛附近的一个长达9个月的锚定潜标的观测资料对南海北部的正压潮、内潮和余流情况进行了分析,得到了当地正压潮和内潮的特征。此处正压潮流以全日潮为主,秋、冬季相对较大,春季相对较小;正压余流受海盆尺度环流和地形的限制,在潜标观测期间的秋、冬、春三季基本以偏西向的正压流为主。内潮同正压潮一样,也以全日分潮为主,潮流椭圆随水深发生旋转,在110—120m附近存在内潮非常弱的一层。斜压余流在2009年2—3月比较异常,这是由于在此其间有一个中尺度涡经过。对此潜标数据采用经验正交函数分解的方法进行分析,发现海流的各个主要EOF模态与内波的垂向模态结构有一定的关联。     

Cotidal charts and tidal power input atlases of the global ocean from TOPEX/Poseidon and JASON-1 altimetry

The global distributions of eight principal tidal constituents, M₂ , S₂ , K₁ , O₁ , N₂ , K₂ , P₁ , and Q₁ , are derived using TOPEX/Poseidon and JASON-1（T/P-J） satellite altimeter data for 16 a. The intercomparison of the derived harmonics at 7000 subsatellite track crossover points shows that the root mean square （RMS） values of the tidal height differences of the above eight constituents range from 1.19 cm to 2.67 cm, with an average of about 2 cm. The RMS values of the tidal height differences between T/P-J solutions and the harmonics from ground measurements at 152 tidal gauge stations for the above constituents range from 0.34 cm to 1.08 cm, and the relative deviations range from 0.031 to 0.211. The root sum square of the RMS differences of these eight constituents is 2.12 cm, showing the improvement of the present model over the existing global ocean tidal models. Based on the obtained tidal model the global ocean tidal energetics is studied and the global distribution of the tidal power input density by tide-generating force of each constituent is calculated, showing that the power input source regions of semidiurnal tides are mainly concentrated in the tropical belt between 30 S and 30 N, while the power input source regions of diurnal tides are mainly concentrated off the tropic oceans. The global energy dissipation rates of the M₂ , S₂ , K₁ , O₁ , N₂ , P₁ , K₂ and Q₁ tides are 2.424, 0.401, 0.334, 0.160, 0.113, 0.035, 0.030 and 0.006 TW, respectively. The total global tidal dissipation rate of these eight constituents amounts to 3.5 TW.