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1.
海水池塘施肥混养滤食性鱼贝的初步研究   总被引:1,自引:1,他引:0  
实验于1995年7月10日至9月16日,在烟台市黄海水产集团公司第二养虾场进行。采用围隔生态系实验法,利用4个海水池塘陆基围隔(5m×5m)初步研究了台湾红罗非鱼(Ore-ochromismossambicus×O.niloticus)与菲律宾蛤仔(Ruditapesphilippinarum)施肥混养的效果。结果表明:菲律宾蛤仔的生产力为1.24g/m2·d,负荷力为3830.0kg/hm2;罗非鱼的生产力为1.86g·(m2·d)-1,负荷力为1580.8kg/hm2。鱼贝对施入氮、磷的利用率分别为15.06%和6.80%,比单养罗非鱼要高;总生产力和总负荷力都明显高于单养罗非鱼。  相似文献   

2.
利用渤海中部海域泥温实测资料,计算出该海域海底热扩散率及恒温层深度。结果表明,8#平台处的热扩散率为0.001~0.005cm2s-1,A(B)平台处为0.002~0.010cm2s-1。恒温层深度8#平台处为8m,A(B)平台处10m,也有差异。与陆地比较,海底恒温层深度较浅,且水深越深恒温层深度越浅。  相似文献   

3.
本文在σ坐标下建立了一个半诊断计算及预报计算的数值模式,应用于台湾海峡夏季时三维海流计算。计算结果表明,当t=2.5d时,密度场和速度场得到调整,即得到半诊断解,当t=40d以后,解已达到准稳定态;半诊断及预报计算的结果在定性上是与诊断计算结果一致。但它们在定量上有些变化,如表层台湾岛西岸附近的最大水平流速,在t=0时(诊断)为59.1cm/s,t=2.5d时(半诊断)为62.1cm/s,t=300d时(预报)为62.0cm/s.此外,在半诊断及预报计算中,上升流也主嵰⑸诟=ń兜龋魉偌忧浚段б灿兴┐蟆  相似文献   

4.
南麂列岛海域微小型底栖藻类生态研究   总被引:6,自引:0,他引:6  
本文首次报道南麂列岛海域沉积物中的微型(2~20μm)、小型(20~200μm)藻类组成、数量分布及其与环境因子的关系。经初步鉴定,沉积物中共有微小型藻类24属71种,其中小型的底栖圆筛藻属Coscinodiscusspp.为21种,广布于整个海区,春季平均细胞密度为(10.4±3.6)×103个/cm2,占总密度的65.4%;微型藻以中肋骨条藻Skeletonemacostatum占优势,秋季平均细胞密度为(4262.8±11928.2)×103个/cm2,占总细胞密度的98.9%,主要分布在沿岸区。对0~12cm柱状样品中细胞密度分层分析结果表明,0~2cm层的细胞密度大于2~5cm层大于5~12cm层。沿岸区(1,2,5,6,7,8,9站)的种类和细胞密度高于岙口(3站)、远岸(10站)及水道区(4站)。根据微小型底栖藻类组成特点,可划分为三个生态类群:广布性类群、暖水性类群和温带性类群。微小型底栖藻类密度与营养盐浓度的季节变化密切相关,秋季高于春季。  相似文献   

5.
不同孔距固定气泡幕对黑鲷的阻拦效果   总被引:2,自引:0,他引:2  
于1987年3月-1988年1月,在室内水池中观测孔径为0.5mm,孔距分别为2.5,5.0,7.5,10.0,20.0cm5中固定气泡幕的视觉特征和声学特征;对孔距分别为5.0,10.0和20.0cm3种气泡幕对黑鲷的阻拦作用予以重点分析研究,以期探讨适合阻拦黑鲷的最适孔距。结果表明,这3种气泡幕对黑鲷都具有明显的阻拦作用,平均阻拦率分别为75.1%,55.5和54.5%;其中,以5.0cm孔距  相似文献   

6.
根据湾顶Konorihama站和湾外Enoshima站1972年5月至1973年5月Ia的观测资料研究了女川湾的假潮特征,在Konorihama站经常出现7-11cm全振幅假潮,最大达31cm。  相似文献   

7.
湛江港污损生物挂板试验   总被引:11,自引:0,他引:11  
严岩  严文侠 《热带海洋》1995,14(3):81-85
1991年4月至1992年3月在湛江港内的试验浮筏上进行了污损生物周年挂板调查。共记录59种生物。优势种是浒苔Entermorpha sp.和网纹藤壶Balanus reliculatus。表层月板附着量变化幅度10.0-250.0g.m^-2,底层月板附着量变化幅度为3.0-5680.5g.m^-2,年板全年附着量炒22347.1g.m^-2。  相似文献   

8.
1991年4月至1992年3月在湛江港内的试验浮筏上进行了污损生物周年挂板调查。共记录59种生物。优势种是浒苔Entermorphasp.和网纹藤壶Balanusreticulatus。表层月板附着量变化幅度10.0—250.0g·m-2,底层月板附着量变化幅度为3.0—5680.5g·m-2,年板全年附着量为22347·1g·m-2。  相似文献   

9.
在室内水池中观察了黑鲷(Sparusmacrocephalus)和青石斑鱼(Epinephelusawoara)对孔径0.5mm、孔距5.0cm,空气压力0.25kg/cm2固定气泡幕的反应。结果表明,气泡幕对两种海水鱼都有显著的阻拦作用,平均阻拦率分别为黑鲷75.1%、青石斑鱼82.4%。分析显示,气泡幕对两种鱼的阻拦率间无显著差异。在本实验中,该两种鱼对气泡幕均无明显的适应现象  相似文献   

10.
厦门黄厝文昌鱼保护区监测与研究   总被引:6,自引:2,他引:6  
曾国寿  何明海 《台湾海峡》1996,15(2):174-181
本文报道了1994年7月至1995年7月厦门黄厝文昌鱼自然保护区的监测结果。表明该区文昌鱼的数量较大,(平均密度142尾/m^2,平均生物量8.10g/m^2),体长组成以11-40mm为多,其性成熟主要在4月上、中旬,生殖期集中在4月下旬至5月上旬;文昌鱼栖息地义南类型以粗中砂为主,有机质含量较低,平均0.14(m/m);区内底栖生物58种,种类以多毛类,软体动物和甲壳动物为主,数量则以棘皮动物  相似文献   

11.
The Tushima Current in the east channel was measured in a site of the strong current between Tushima and Iki Islands for 43 days of the winter in 1986. The primary results are:First, it was highly barotropic and flowed northeastward with a mean speed of about 20 cm sec–1. Second, it was decelerated by northeast winds rather than by northwest winds in a frequency range of 0.3 and 0.4 cpd. Third, the scale analysis showed that the Tushima Current is approximately in geostrophic balance. The best empirical relationship between the measured Tushima Current and cross-channel adjusted sea level difference is given by
  相似文献   

12.
A review is presented of the ocean circulation along Australia’s southern shelves and slope. Uniquely, the long, zonal shelf is subject to an equatorward Sverdrup transport that gives rise to the Flinders Current - a small sister to the world’s major Western Boundary Currents. The Flinders Current is strongest near the 600 m isobath where the current speeds can reach 20 cm/s and the bottom boundary layer is upwelling favourable. It is larger in the west but likely intermittent in both space and time due to possibly opposing winds, thermohaline circulation and mesoscale eddies. The Flinders Current may be important to deep upwelling within the ubiquitous canyons of the region.During winter, the Leeuwin Current and local winds act to drive eastward currents that average up to 20-30 cm/s. The currents associated with the intense coastal-trapped wave-field (6-12 day band) are of order 25-30 cm/s and can peak at 80-90 cm/s. Wintertime winds and cooling also lead to downwelling to depths of 200 m or more and the formation of dense coastal water within the Great Australian Bight and the South Australian Sea. Within the Great Australian Bight, the thermohaline circulation associated with this dense water is unknown, but may enhance the eastward shelf-edge, South Australian Current. The dense salty water formed within Spencer Gulf is known to cascade as a gravity current to depths of 200 m off Kangaroo Island. This dense water outflow and meanders in the shelf circulation also fix the locations of a sequence of quasi-permanent mesoscale eddies between the Eyre Peninsula and Portland.During summer, the average coastal winds reverse and surface heating leads to the formation of warm water in the western Great Australian Bight and the South Australian Sea. No significant exchange of shelf water and gulf water appears to occur due to the presence of a dense, nutrient-rich (sub-surface) pool that is upwelled off Kangaroo Island. The winds lead to weak average coastal currents (<10 cm/s) that flow to the north-west. In the Great Australian Bight, the wind stress curl can lead to an anticyclonic circulation gyre that can result in shelf-break downwelling in the western Great Australian Bight and the formation of the eastward, South Australian Current. In the east, upwelling favourable winds and coastal-trapped waves can lead to deep upwelling events off Kangaroo Island and the Bonney Coast that occur over 3-10 days and some 2-4 times a season. The alongshore currents here can be large (∼40 cm/s) and the vertical scales of upwelling are of order 150 m (off Kangaroo Island) and 250 m (off the Bonney Coast).Increasing evidence suggests that El Nino events (4-7 year period) can have a major impact on the winter and summer circulation. These events propagate from the Pacific Ocean and around the shelf-slope wave-guide of West Australia and into the Great Australian Bight. During winter El Nino events, the average shelf currents may be largely shut-down. During summer, the thermocline may be raised by up to 150 m. The nature and role of tides and surface waves is also discussed along with uncertainties in the general circulation and future research.  相似文献   

13.
14.
The response of wind-drift currents to the prevailing summer wind regime is reported for Simpson Lagoon on the Beaufort Sea (Arctic Ocean) coast of Alaska. Wind and current measurements were taken over the period July 17 to October 20 and August 11 to September 18, 1972, respectively, at a site eastward of the Colville River delta. Mean wind speeds and the frequency of occurrence of westerly storms tend to increase from July to October. Prevailing currents within the lagoon are towards the W to NW driven by the prevailing northeasterly winds. Relatively rapid reversals of current direction occur in response to alternating easterly and westerly winds. Cross correlations of power spectra of the filtered E-W components of the lagoon current record with the concurrent wind data gave a periodicity of 4–5 days at a 70% level of coherence. A linear correlation of −0·83 was obtained between the E-W components of the filtered current record and the wind record, and net water transport (from a progressive current vector analysis) over this period was determined to be towards the WNW with a mean vector velocity of 10·6 cm/sec.  相似文献   

15.
An autumnal upwelling event was observed in the Ria of Vigo (NW Iberian Peninsula) on 15th November 2001. This event was analyzed by means of thermohaline variables measured at CTD stations located in the study area, satellite sea surface temperature and wind data provided by QuikSCAT. Salinity and temperature distributions revealed that the upwelled water mass was Eastern North Atlantic Central Water (ENACW), typically observed during summer upwelling events. However, previous to the upwelling event, the characteristic autumnal body of water was recorded on 31st October 2001. Subsequent sea surface temperature and upwelling index corroborated the presence of an autumnal upwelling event of approximately 15 days duration. The probability of upwelling-favorable winds (from 1999 to 2004) was lower during autumn–winter than during spring–summer, although they may occur at any time of the year. Probabilities of 45% were calculated for February and November, with the highest probability (65%) corresponding to July.  相似文献   

16.
Changes from winter (July) to summer (February) in mixed layer carbon tracers and nutrients measured in the sub-Antarctic zone (SAZ), south of Australia, were used to derive a seasonal carbon budget. The region showed a strong winter to summer decrease in dissolved inorganic carbon (DIC;  45 µmol/kg) and fugacity of carbon dioxide (fCO2;  25 µatm), and an increase in stable carbon isotopic composition of DIC (δ13CDIC;  0.5‰), based on data collected between November 1997 and July 1999.The observed mixed layer changes are due to a combination of ocean mixing, air–sea exchange of CO2, and biological carbon production and export. After correction for mixing, we find that DIC decreases by up to 42 ± 3 µmol/kg from winter (July) to summer (February), with δ13CDIC enriched by up to 0.45 ± 0.05‰ for the same period. The enrichment of δ13CDIC between winter and summer is due to the preferential uptake of 12CO2 by marine phytoplankton during photosynthesis. Biological processes dominate the seasonal carbon budget (≈ 80%), while air–sea exchange of CO2 (≈ 10%) and mixing (≈ 10%) have smaller effects. We found the seasonal amplitude of fCO2 to be about half that of a study undertaken during 1991–1995 [Metzl, N., Tilbrook, B. and Poisson, A., 1999. The annual fCO2 cycle and the air–sea CO2 flux in the sub-Antarctic Ocean. Tellus Series B—Chemical and Physical Meteorology, 51(4): 849–861.] for the same region, indicating that SAZ may undergo significant inter-annual variations in surface fCO2. The seasonal DIC depletion implies a minimum biological carbon export of 3400 mmol C/ m2 from July to February. A comparison with nutrient changes indicates that organic carbon export occurs close to Redfield values (ΔP:ΔN:ΔC = 1:16:119). Extrapolating our estimates to the circumpolar sub-Antarctic Ocean implies a minimum organic carbon export of 0.65 GtC from the July to February period, about 5–7% of estimates of global export flux. Our estimate for biological carbon export is an order of magnitude greater than anthropogenic CO2 uptake in the same region and suggests that changes in biological export in the region may have large implications for future CO2 uptake by the ocean.  相似文献   

17.
用小麦岛和团岛观测站提供的青岛近海气象和水温资料,以适于SO2气体和硫酸盐(SO42-)气溶胶的干沉降模型研究了模型中的输送阻尼对两种污染物质干沉降速率的贡献,并计算了2003年青岛近海地区两种污染物质干沉降速率的季节变化。结果表明:对SO2而言,粘性副层传输系数对沉降速率的贡献大于空气动力学传输系数;对于SO42-,空气动力学传输系数对沉降速率的贡献要大于表面传输系数。SO2和SO42-的干沉降速率变化范围分别为0.187~0.868cm/s和0.188~0.532cm/s。两种污染物质干沉降速率的四季变化有相似的规律,即冬季>秋季>春季>夏季。  相似文献   

18.
COARE算法估算海气界面热通量的个例对比分析   总被引:2,自引:1,他引:1  
本文先对NCEP分析风、QSCAT/NCEP混合风、MM5中尺度模式分析风场进行了比对分析,发现具有高分辨率的QSCAT/NCEP混合风资料给出的高风速数值较好,但给出的高风速开始时间相对较早;NCEP分析风资料给出的高风速数值明显偏小;MM5分析风场较为可信,只不过模拟的高风速数值还是相对偏小.使用COARE算法(版本3.0)计算了四种资料情况下的渤、黄海海域一次冷空气大风过程的海表面湍流热通量,并与MM5诊断分析结果进行了对比分析.结果发现相同资料情况下,MM5结果跟COARE算法所算海气热通量(包括感热和潜热)在区域分布和时间变化规律上均较为一致,中、低风速情况下,结果比较接近;但是高风速情况下两者差异显著.  相似文献   

19.
利用山东省122个国家级地面气象观测站的风速数据与欧洲中期天气预报中心(ECMWF)提供的ERA-interim再分析数据,采用小波分析、带通滤波等方法对2015年9月—2020年9月山东的大风天气及相应的低频大气环流形势进行分析.结果表明,近几年山东的大风天气有增加的趋势,春季大风发生频次最多,秋季最少;山东半岛东部...  相似文献   

20.
The phase of the sea surface height annual variation in the East China Sea along China’s continental coast is delayed from that in the open ocean area, most probably because of seasonal strong monsoon winds. To elucidate this mechanism, we conducted an idealized model experiment using a rectangular shallow ocean with a sloped seafloor forced by southward blowing winds. We obtain a locally confined high SSH near the western boundary found in the East China Sea. The delay of the phase of the sea surface height (SSH) along the China coast can be interpreted as follows. The SSH of the East China Sea is high over large areas in September and low in March due to the expansion/contraction of seawater, which is attributable to the sea surface heat flux. However, near the continental boundary SSH becomes high in January and low in July under the influence of a monsoon winds. The phase delay along the continental boundary should appear by superposing these two time series with a phase difference near the boundary.  相似文献   

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