Landsat-8热红外数据监测田湾核电站温排水分布

基于2015—2017年的多景Landsat-8热红外数据,采用辐射传输方程法反演田湾核电站邻近海域海面温度,依据反演所得海面温升分布图对温排水的分布特征进行分析。结果表明:田湾核电站温排水的扩散方向和影响范围与潮汐状态密切相关。在涨潮中期阶段,温排水分布范围较小,其中1℃以上温升区域面积不足10 km~2;在高、低平潮阶段,温排水扩散面积相近,其中1℃以上温升区域面积约15 km~2;在落潮中期阶段温排水分布范围最大,1℃以上温升区域面积可达30 km~2,但4℃以上高温升区域面积较小。高温升区域多出现在排水口以南至以东附近海域,随着温排水向周围海域扩散,温升逐渐呈衰减分布。     

基于POM模型的后石电厂附近海域热环境容量计算

阐述了热环境容量的含义,并在POM模型的基础上建立了热传输模型,考虑了热能在垂直方向上的扩散。采用模型试算法计算了后石电厂附近海域的热环境容量和剩余热环境容量,结果表明,后石电厂附近海域的热环境容量为1 496(℃·m3)/s,一、二期工程的剩余热环境容量为350.2(℃·m3)/s,在允许的排放范围;三期扩建后的剩余热环境容量为–413.6(℃·m3)/s,超过该海域的热环境容量。研究结果可为电厂扩建及其附近海域生态环境保护提供参考依据。     

台湾以东海域黑潮热结构的一个简单模型

多年来,对紧邻台湾东侧的黑潮区域,已积累了一定数量的温、盐度观测资料。从实测的水温垂直断面图上,可以看出该区域的水温分布有如下特点。 1.在水平方向上:水温自西向东逐渐增加,其最大值在离岸70km左右(即所谓“热核”所在处);再向东温度开始递减,其低温区呈现在“热核”东侧。图1示台湾以东海域100m层的水温分布,可看出温度水平分布的这些特点。     

基于无人机的用海项目施工期悬浮泥沙监测

为实现对用海项目施工期悬浮泥沙扩散的实时跟踪监测,尝试采用无人机携带可见光、多光谱传感器对古雷围填海项目的围堰区进行遥感探测。利用Pix4d软件对无人机携带的可见光及多光谱照片进行处理,结果表明,可见光及多光谱影像对水体中的悬浮泥沙分布均具有一定的识别能力。通过研究分析多光谱影像的光谱特征发现,近红外波段对悬浮泥沙含量的升高较为敏感,运用波段比值公式计算结果显示,围堰内含沙水体经溢流口排入海域后浓度明显降低,并可向南继续扩散约300 m。该方法可克服遥感卫星影像时空分辨率低的特点,为用海项目资源环境影响跟踪监测提供新的技术手段。     

2011年春、夏季黄、东海水团与水文结构分布特征

根据2011年春季(4月)夏季(8月)两个航次调查的CTD温盐资料,获得观测期间黄、东海主要水团特征:(1)夏季黄海冷水团10℃等温线在黄海海域中部30m以深,影响范围西至122°E南至34°N,最低温度为6.2℃,比气候态平均冷水团温度低约2℃;(2)夏季冲淡水以长江口为中心,呈半圆形向外扩展,并无明显NE转向,30.00等盐线在32°N断面上东至124°E,南至29.5°N,扩展范围与往年相比偏西1°左右,而在SE方向较往年有明显延伸扩展。水文结构特征为:(1)春季,温跃层主要在南黄海中部以西,跃层强度仅为0.10—0.40℃/m;密跃层主要在长江口以东,跃层强度0.20—0.30kg/m4;(2)夏季,温跃层强度最高值在长江口东北,跃层强度达到2.41℃/m,上界深度5.5m,厚度2.5m;黄海温跃层强度普遍强于东海,主要是冷水团区域表底显著的温度差异造成;密跃层强度高值区在33°N断面西侧海区,强度达到1.38kg/m4,上界深度5.5m,厚度约为1.5m;沿长江冲淡水舌轴方向的密跃层强度为0.30—0.60kg/m4,自西向东逐渐减弱。     

辐射板强化喷管换热与红外抑制效果试验研究

试验研究了在发动机喷管中加装金属辐射板前后,喷管壁面温度、热喷流温度与喷管红外辐射特征的变化。结果表明,加装金属辐射板后,热喷流与喷管壁面之间的热量传递显著增强,热喷流中心温度降低,壁面温度明显升高,在90°方向上,热喷流3～5μm波段的红外辐射强度降低了38.5%。文中从热喷流、喷管壁面以及金属辐射板等相关部件的温度变化情况对红外辐射强度的变化原因进行了解释。      

黄海海水温度月变化与鲑鱼养殖的适应性

鲑鱼(Oncorhynchus)属冷水性鱼,其生长对水温条件极敏感,生存的上限水温一般不超过20℃。本文利用历史上80年的海表和海底的平均温度数据,分析了鲑鱼生长的适宜温度窗口、休眠温度窗口和死亡窗口;结合黄海底层冷水团的年际变化,讨论了不同月份鲑鱼适宜生长的海域。研究发现,黄海冷水团提供了鲑鱼顺利度夏的天然场所;南黄海在一年中适宜窗口出现的时间最长,但不论是表底温差还是海表面温度,变化都比较较大;北黄海在一年中适宜窗口出现的时间短,但表底温度变化较小。研究结果表明,在黄海,养殖鲑鱼的水温条件最佳的位置位于济州岛北部,朝鲜半岛南的近岸海域,对于中国,养殖鲑鱼的水温条件最佳的位置位于辽东半岛南部;但是,台风对相关区域影响较大,生产实践中应充分考虑多种因素的综合影响。     

长江口邻近海域水团特征与影响范围的季节变化

基于2009年—2011年调查资料,研究长江口及其邻近海域水体温度和盐度时空分布特征,剖析该海域水团特征与影响范围的季节变化。结果表明,从春末到秋初,长江水以高温形式向外海扩展,秋末至翌年春初,径流水以低温形式从河口流向东南。西北部海区受黄海冷水团影响,水温较低,东北部受南黄海西部逆时针环流影响,盐度较低,东南部海区受黑潮及分支台湾暖流影响,呈高温高盐状态。受径流量和季风季节差异,长江冲淡水影响一般夏季最强,扩展范围最大,秋末冬初最弱。其双向延伸趋势在夏季有最清晰表现,一支自河口向东北方向延伸,指向南黄海中部,一支穿过杭州湾口及舟山群岛一带沿岸南下,或自长江口向东南方向扩展。温度垂向变化表明夏季存在上升流,并明确处于以31.5°N,122.67°E为中心,在经纬方向上各达1°范围内。     

渤、黄、东海水温季节变化特征分析

利用"908"专项所获取的CTD观测资料,系统地阐述了渤、黄、东海温度的分布特征及季节变化。结果显示,冬季,水平方向上,水温分布呈现多舌状:外海温度多暖舌结构,近岸等温线基本平行于岸线,并出现多个指向南方的冷水舌,且暖流区与近岸冷水区间形成了较强的温度峰。夏季,三大海域底层均出现了各具特色的冷水团和冷水块,最为典型的有"渤中冷水"、"辽东湾冷水"、黄海冷水团、青岛冷水团和东海北部底层冷水。春、秋季水温分布呈现过渡季节的特征。春季,跃层开始出现,"渤中冷水"及黄海冷水团等冷水现象开始形成。进入秋季,跃层明显下沉,直至消失,水温分布逐渐呈现垂向均匀状况。同时,分析还表明,三大海域的水温分布存在明显的区域性差异。水温分布的年变幅从北向南、从近岸向外海递减。     

南黄海春季水温分布特征的分析

利用美国海军的空间分辩率为10′×10′月平均的GDEM三维水温资料,研究了南黄海春季水温的分布特征及其演变过程。分析结果较清晰地显示了春季南黄海的水温分布如何从冬季的垂直均匀型过渡到夏季的层化结构。分析还表明:春季南黄海水温的水平和垂直结构皆比冬季更为复杂,并出现若干个较特殊的水文现象,例如,在34°40′~36°20′N的南黄海西侧出现了“青岛冷水团”,而在35°30′~37°20′N的南黄海东侧,初次发现存在着一个类似性质的冷水团,称其为“仁川外海冷水团”。此外,在冷水团的邻近海域还存在着中层冷水。     

2002年夏季粤东外海的海洋状况

本文利用2002年7月22日至8月2日对粤东外海进行的水文观测资料，分析了调查海区的水温、盐度和跃层的分布状况，并对粤东沿岸的上升冷水、海洋锋等海洋现象进行了探讨．结果表明，整个粤东沿岸都存在着下层冷水的涌升现象，该现象在大亚湾外海附近和广东总来外海附近尤为明显，从而导致粤东沿岸水等温线非常密集，产生上升流锋．上升流锋随着深度的增加有向外海扩展的趋势．此外，在台湾浅潍的南部，陆架的坡析处和东沙群岛的东例以及西南部海战似乎也有下层冷水涌升的迹象．东沙群岛的北侧和西部海战有暖水中心存在，该暖水中心可能是离岸的表层水离异一定距离后发生下沉所致．珠江口的东例出现高温低盐水，其低盐水舌向东伸展，可达大亚湾口外海，等盐度线非常密集，是一个非常强的冲淡水羽状锋。     

Hamilton Bank,Labrador Shelf: Postglacial sediment dynamics and paleo-oceanography

Sandy glacial sediments on Hamilton Bank have been reworked during postglacial times by the effect of storm waves and the Labrador Current. Gravel to cobble lags are found along the periphery of the bank. A layer of medium to fine sand and silt less than 1 m thick cloaks the bank surface. Toward the center, modal grain size becomes progressively finer reaching a minimum of 5 ?. Silt and clay have accumulated in peripheral basins.Faunal changes in basin sediments and partial covering of the lag deposits by sand imply that the Labrador Current which today flows southward between Hamilton Bank and the coast was, for a period after deglaciation, deflected to the east around Hamilton Bank and down the seaward edge of the Grand Banks. Thus warm water was able to penetrate northward along the continental shelves of the United States and Canada to southern Newfoundland. Warmer coastal waters south of Newfoundland appear to have substantially amplified the effect of the Holocene thermal maximum in coastal areas. Isostatic and eustatic considerations suggest that Hamilton Bank was not emergent in postglacial times and that the depth of water over the bank has been increasing, probably for the last 6,000 years. Deepening water over the inner shelf and a cooling trend in Arctic surface waters beginning 3,500 years ago are probably responsible for the present position and intensity of the Labrador Current.     

On the total geostrophic circulation of the Indian Ocean: flow patterns, tracers, and transports

The large-scale circulation of the Indian Ocean has several major components. There is a cyclonic gyre in the far southwest with its axis along about 60°S. It extends to the bottom. North of this the Circumpolar Current flows eastward south of 40°S to more than 3000 m. The axis of the great anticyclonic gyre lies along 35°S to 40°S down to about 2000 m. Below there the western end shifts northward and the axis lies along the central and southeast Indian ridges, with southward flow west of the ridges and northward flow on the east side.There is a westward flow along 10°S to 15°S, which includes water from the Pacific, through the Banda Sea. The flow near the equator is eastward down to the depth of the ridge near 73°E. Flow within both the Arabian Sea and Bay of Bengal is cyclonic down to great depth.There is a southward flow along the coast of Africa in the upper 2000 m joining the Circumpolar Current, and a southward flow along the coast of Australia that does not reach the Circumpolar Current.Below 2500 m there is a northward flow from the Circumpolar Current along the east coast of Madagascar and on into the Somali and Arabian basins.     

Drifting and Meandering of Olive Ridley Sea Turtles in the Bay of Bengal: Role of Oceanic Rossby Waves

Olive Ridley turtles in the Bay of Bengal are previously thought to migrate southward from their nesting ground, along the east coast of India (Orissa coast), towards Sri Lanka. Surprisingly, three of the four Platform Transmitter Terminal (PTT) attached turtles in April-June 2001 meandered off the east coast of India for about two months. It is found that these turtles meandered at the peripherals of cold core cyclonic eddy surrounded by warm core eddies on either side. Concentrations of prey for the turtles in those frontal regions are known to be abundant. Only one of the four PTT attached turtles migrated to the south along the frontal regions in the direction of geostrophic currents. It is found that the locations of these thermal fronts in the Bay of Bengal are primarily determined by the Oceanic Rossby waves and local Ekman pumping.     

Summertime hydrographic features in the southeastern Hwanghae

CTD casts in the southeastern Hwanghae (Yellow Sea) were made in August 1983 and 1984 to describe the spatial structure of the summertime hydrographic features. Cold coastal water appeared around the southwestern coast of Korea, which was formed by strong tidal stirring. Tidal mixing in the study area seems to have been enhanced by the presence of many small islands. In the deeper region beyond the tidal front, stratification became much stronger and the bottom layer below seasonal thermocline was occupied mostly by the Hwanghae Cold Water characterized by a temperature lower than 10°C and salinity of 32.5–33.0%.The northeastward extension of the Changjiang Diluted Water was shown by a tongue-like plume of relatively warm fresh water, confined to the thin surface layer 10 m thick. There was no evidence for the Hwanghae Warm Current carrying high salinity water into the eastern Hwanghae along the Korean coast. The warm current was found to flow in a narrow band close to the west and north coast of Chejudo (Cheju Island) and then to pass eastward through the Cheju Strait. Thus the eastern part of the cyclonic circulation in the surface layer cannot be considered to be a northward continuation of the Hwanghae Warm Current. The local salinity maximum in the lower layer off Kunsan and the higher salinity on the west side of the central trough than on the east side would imply a northward flow on the west flank of the trough to compensate for the southward intrusion of the Hwanghae Cold Water, from which an anticyclonic circulation could be expected in the lower layer.     

Structure of Subsurface Intrusion of the Oyashio Water into the Kuroshio Extension and Formation Process of the North Pacific Intermediate Water

In order to understand the actual formation process of the North Pacific Intermediate Water (NPIW), structure of subsurface intrusions of the Oyashio water and the mixing of the Oyashio and the Kuroshio waters in and around the Kuroshio Extension (KE) were examined on the basis of a synoptic CTD observation carried out in May-June 1992. The fresh Oyashio water in the south of Hokkaido was transported into KE region through the Mixed Water Region (MWR) in the form of subsurface intrusions along two main paths. The one was along the east coast of northern Japan through the First Branch of the Oyashio (FBO) and the other along the eastern face of a warm streamer which connected KE with a warm core ring through the Second Branch of the Oyashio (SBO). The fresh Oyashio water extended southward through FBO strongly mixed with the saline NPIW transported by the Kuroshio in the south of Japan (old NPIW) in and around the warm streamer. On the other hand, the one through SBO well preserved its original properties and extended eastward beyond 150°E along KE with a form of rather narrow band. The intrusion ejected Oyashio water lens with a diameter of 50–60 km southward across KE axis and split northward into the MWR involved in the interaction of KE and a warm core ring, which were supposed to be primary processes of new NPIW formation.     

Ocean wave characteristics around New Zealand

Nearly 17 years wave records from deep water and shore‐based stations are used to describe the ocean wave characteristics around New Zealand. The wave environment is dominated by west and southwest swell and storm waves generated in the temperate latitude belt of westerly winds. As a result, the west and south coasts are exposed, high energy shores, the east coast is a high energy lee shore, and the northern coast from North Cape to East Cape is a low energy lee shore sheltered from these winds and waves. South of New Zealand, wave energies are extremely high; the prevailing deep water wave is 3.5–4.5 m high and has a 10–12 s period, with a slight increase in wave heights in winter.

The west coast wave environment is mixed, and consists of locally generated westerly and southerly storm waves, and swell waves generated to the south. The prevailing wave is t.0–3.0 m and 6–8 s period. There are no strong seasonal rhythms, only shorter period cycles of wave height (5 day) associated with similar quasi‐rhythmic cycles in the weather.

The east coast also has a mixed wave climate with southerly swells, originating in the westerlies south of New Zealand, and locally generated southerly and northerly storm waves. The prevailing wave is 0.5–2.0 m and 7–11 s period. A short period rhythmic cycle, similar to that on the west coast, is superimposed on a weak seasonal cycle. The seasonal, cycle results from an increase in the frequency of local northerly waves in summer.

The prevailing wave on the north coast is a northeasterly, 0.5–1.5 m high and 5–7 s period. Subtropical disturbances and southward‐moving depressions generate a mixed wave environment and a possible seasonally reflecting a winter increase in. storminess.     

台湾海峡中、北部海域温、盐度特征

台湾海峡中、北部海域海水温、盐度分布随季风进退而异。东北季风期(10月—翌年5月),进入调查海域的浙闽沿岸水(低温、低盐)顺海域西岸海区南下的同时,在海坛岛外有一分支向东南扩展,其扩展范围随浙闽沿岸水强弱而异,而且在24°30′N,119°30′E附近有海峡暖流水(高温、高盐)向北伸展,它随西南风增强而向北推移。海域温、盐度值自西北向东南递增。西南季风期(6—9月),调查海域基本上为海峡暖流水所控制。在6—8月,海域西岸海区有上升流产生,上升流中心在海坛岛附近。海域盐度值自西北向东南递增,而温度分布趋势与盐度分布相反。 温、盐度的垂直分布大致分均匀型、正梯度型和负梯度型三类。     

丹麦日德兰半岛西海岸典型岸段地貌概况及研究现状

通过实地调查和资料搜集,对丹麦日德兰半岛西海岸典型岸段的地貌类型和研究现状进行了总结。丹麦日德兰半岛西海岸岸线长度约为470km,海岸类型可以分为无障壁海岸和有障壁海岸2大类。无障壁海岸以沙丘为主,并有海蚀崖,主要分布在斯卡恩(Skagen)到布劳万角(Bl?vands Huk);有障壁海岸地貌类型以障壁岛—潟湖、盐沼为主,主要分布在布劳万角到勒姆岛(R?m?),并向南进入德国。丹麦西海岸北部属于冰后期地壳回弹上升区,向南地壳回弹幅度逐渐减弱,至Ringk?bing峡湾地区变为地壳稳定区,再向南地壳变为下降区,因此,全新世地层中分别记录了不同的相对海面变化信息。距今7 150a以来,北部的Skagen岬角地区的相对海面下降了16~25m;Skallingen地区过去5 000a间海面在现代海面附近波动,其后侧Ho Bugt盐沼地区4 000a以来相对海面上升了4m;过去8 000a间,R?m?障壁岛的相对海面上升了15m。欧洲学者在丹麦西海岸地区取得的典型成果包括:海面变化重建(包括海面变化标志点、泥炭层压实校正、定年等)、全新世地质环境演化、开放潮坪现代沉积定量研究等,为海岸带研究提供了有益参考。     

Trajectories of drift bottles released in the Tsushima Strait

Kyungsang-Namdo Fisheries Experimental Station released 620 drift bottles in the west strait of the Tsushima Strait from 1932 to 1939. Among them 183 were recovered. Fukuoka Prefectural Fisheries Experimental Station also released 1930 bottles in the east strait between 1954 and 1969. Recovered bottles were 442.The bottles drifted to the south in winter owing to a northwesterly wind, and drifted to the northeast in spring and summer with the Tsushima warm current. Bottles released at the west strait drifted to the north along the east shore of Korea, went around the Ullung Island, and then to the northeast. Drift bottles released at the east strait drifted to the north along the shore of Japan and washed ashore on the coast.