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81.
82.
钛胶海水提铀动力学研究Ⅱ——吸附机理的推断 总被引:1,自引:0,他引:1
海水提铀机理的研究,已逐渐受到重视,然而,至今研究还不是很深入,观点也各有差别.例如,Keen等[1]认为钛胶从海水中吸附铀是阳离子交换过程,即海水中的铀是UO22+离子的形式与钛胶进行交换;尾方升等[2]则倾向于阴离子吸着,即铀是以UO2(CO3)34-的形式被吸附.我们曾于1973年在海洋局系统的一次会议上提出阳离子给合交换的看法,并在后来的两次专业会议上予以补充发展.张正斌[3]认为是阳离子交换或一价阳离子失水络合.最近崔清晨[4]提出可能是UO2(OH)3-的络合吸附.根据几年来的工作,我们仍认为,钛胶从海水中的吸铀机理可能是一种阳离子形式的络合交换过程. 相似文献
83.
河口沉积物中的有机物质和营养成分,部分直接来自陆源,部分则源于河口水体的生物化学作用。在有污染源的地区,水体携带着无机和有机污染物的微粒和某些洛于水的化学物质,它们在海水与河水混合的河口环境条件下发生沉淀;另一些溶解性的营养物质能促使浮游生物繁殖,这些生物死亡后也变为沉淀性的有机物质,致使底质状况恶化,在一定条件下会形成对海洋生物异常有害的腐泥。国内外关于利用底泥的有机组分来探讨河口水域有机污染状况的资料目前还较少,对衡量有机污染或海域富营养化程度的底泥测定项目也研究得很不够。通常只用底泥中的硫化物、有机碳(或COD)和氮等成分的含量来反映底质的状况,但由于海域自然环境状况不同,这些成分的背景含量也有很大的差异,往往难以对比。为对本河口区底泥中的有机组分的含量状况及其与有机污染的关系有较全面的了解,我们分析测定了河口区沉积物中的有机碳(TOC),有机氮(TON),总磷(TP),腐植酸量(HA)、硫化物(S),烧失量(IL)和阴离子表面活性剂(AS)等成分的含量。沉积物样品主要采于1984年5月。采样站位示于图1。根据站位设置的具体自然条件,可将调查区划分为三个区段:永定新河河口段,系指受潮汐影响的河段,包括A,B,C 和D站;大沽排污口区,系指天津南排污河河口段的E和11b站,以及海河防潮闸外侧的11a站;河口近岸海区,系指上述两区段站位以外的其他调查水域,包括北塘口、大沽口及其口外海域。对沉积物中的有机组分采用下列分析方法:有机碳——重格酸钾氧化法;有机氮——元素仪测定法;硫化物——腆量法;腐植酸——碱液提取法;阴离子表面活性剂——乙基紫光度法和原子吸收间接法(吴景阳等,1986 ;本集吴景阳等另文);磷——比色法;烧失量——重量法。
本文着重讨论这些有机组分的含量分布特征及其规律。 相似文献
84.
The upper layer (above 140 m depth) temperature in the western Philippine Sea near Taiwan was sampled using a coastal monitoring
buoy (CMB) with 15 attached thermistors during July 28–August 7, 2005. The data were collected every 10 min at 1, 3, 5, 10,
15, and 20 m using the CMB sensors, and every 15 sec at 15 different depths between 25 m and 140 m. Internal waves and solitons
were identified from the time-depth plot of the temperature field. Without the internal waves and solitons, the power spectra,
structure functions, and singular measures (representing the intermittency) of temperature field satisfy the power law with
multi-scale characteristics at all depths. The internal waves do not change the basic characteristics of the multifractal
structure. However, the internal solitons change the power exponent of the power spectra drastically, especially in the low
wave number domain; they also break down the power law of the structure function and increase the intermittency parameter.
The physical mechanisms causing these different effects need to be explored further. 相似文献
85.
86.
Following our previous study (Sugimoto and Hanawa, 2005b), we further investigate the reason why reemergence of winter sea
surface temperature anomalies does not occur in the North Pacific eastern subtropical mode water (NPESTMW) area, despite its
occurrence in the North Pacific subtropical mode water and North Pacific central mode water areas. We use vertical temperature
and salinity profiles of the World Ocean Circulation Experiment Hydrographic Program and Argo floats with high vertical and
temporal resolution, together with heat flux data through the sea surface. We point out first that one of the causes for non-occurrence
of reemergence is that the thickness of NPESTMW is very thin. In addition to this basic cause, two major reasons are found:
a vigorous mixing in the lower portion of NPESTMW and less heat input from the atmosphere in the warming season. Since, in
the lower portion of NPESTMW and deeper, the stratification is favorable for salt-finger type convection to occur compared
with the other mode water areas, vigorous mixing takes place. This is confirmed by both a large Turner Angle there and the
existence of staircase structures in vertical temperature and salinity profiles. From the viewpoint of heat input, the NPESTMW
area gradually gains heat in the warming season compared with other mode water areas. As a result, NPESTMW cannot be capped
so quickly by the shallow summer mixed layer, and water properties of NPESTMW are to be gradually modified, even in the upper
portion. 相似文献
87.
A geomorphological and statistical analysis of slope canyons from the northern KwaZulu-Natal continental margin is documented
and compared with submarine canyons from the Atlantic margin of the USA. The northern KwaZulu-Natal margin is characterized
by increasing upslope relief, concave slope-gradient profiles and features related to upslope growth of the canyon forms.
Discounting slope-gradient profile, this morphology is strikingly similar to canyon systems of the New Jersey slope. Several
phases of canyon incision indicate that downslope erosion is also an important factor in the evolution of the northern KwaZulu-Natal
canyon systems. Despite the strong similarities between the northern KwaZulu-Natal and New Jersey slope-canyon systems, key
differences are evident: (1) the concavity of the northern KwaZulu-Natal slope, contrasting with the ∼linear New Jersey slope;
(2) the relative isolation of the northern KwaZulu-Natal canyons, rather than the dense clustering of the New Jersey canyons;
and (3) the absence of strongly shelf-breaching canyons along the northern KwaZulu-Natal margin. In comparison with the New
Jersey margin, we surmise a more youthful stage of canyon evolution, a result of either the canyons themselves being younger
or the formative processes being less active. Less complicated patterns of erosion resulting from reduced sediment availability
have developed in northern KwaZulu-Natal. The reduction in slope concavity on the New Jersey margin may be the result of grading
of the upper slope by intensive headward erosion, a process more subdued—or less evident—on the KwaZulu-Natal margin. 相似文献
88.
海洋生态监测包括自然环境和生物群落的监测两部分。海洋生态系统中绝大多数生物群落生活在水中。因此,能真实反映水下自然环境和生物群落状况及其变化的水下图像,对海洋生态监测显得尤为重要。水下照相和水下摄像作为获取水下图像的主要手段已被广泛利用。 相似文献
89.
本文主要介绍了1988年寿光县对虾养殖期间(5~9月)水环境和底泥环境中微生物种群的变化。据不同的地理位置,选择不同的养殖虾池;分别将水样和底泥环境中的弧菌、异养菌,及硫酸盐还原菌进行培养、分离计数。据对虾养殖期5个月的数据分析,不同的养殖虾池有不同的菌数波动范围。底泥与水环境中的菌数分布各有不同。异养菌在水样中的分布最高值为736×10~2个/ml,最低值为268.1×10~2个/ml;湿泥样中的最高值为372.7×10~4个/g最低值为125.9×10~4个/g。弧菌在水样中的最高值为12.33×10~2个/ml,最低值为0.5×10~4个/ml。据综合资料分析,对虾养殖池中的各种细菌分布,底泥高于水样,高温季节高于低温季节。底泥和水环境中有机物的含量与细菌数的分布成正比。底泥中硫酸盐还原菌的数量,是底泥环境中有机物污染程度的标志之一。根据硫酸盐还原菌的数量分布,可以有效地控制有机质(如对虾饵料)的投放量等。 相似文献
90.
Based on the ray theory and Longuet-Higgins’s linear model of sea waves, the joint distribution of wave envelope and apparent wave number vector is established. From the joint distribution, we define a new concept, namely the outer wave number spectrum, to describe the outer characteristics of ocean waves. The analytical form of the outer wave number spectrum, the probability distributions of the apparent wave number vector and its components are then derived. The outer wave number spectrum is compared with the inner wave number spectrum for the average status of wind-wave development corresponding to a peakness factor P = 3. Discussions on the similarity and difference between the outer wave number spectrum and inner one are also presented in the paper. 相似文献