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1.
黑河下游绿洲地表辐射平衡及小气候特征分析 总被引：1，自引：0，他引：1
利用额济纳绿洲2004年5~10月微气象站观测资料,分析了该地区地表能量平衡及小气候特征.结果表明:在绿洲内太阳总辐射、光合有效辐射、净辐射有明显的季节变化及日变化,日峰值及月总量在7月份达到最高.地表能量平衡季节变化显著,5、8、9、10月份,地面能量交换基本以感热通量为主,Bowen比值在日间>4;6、7月份,潜热蒸发是能量平衡的主要部分,Bowen比基本<1.5~10月土壤热通量值始终较小,约占净辐射的15%~20%.绿洲内近地层风速基本在0~5 m·s-1之间,夜间风速变化很小,日间风速较大.随着土壤深度的增加,土壤温度变化趋势越来越缓慢,地表温度波动变化最大,而在40 cm深处土壤温度日变化很小. 相似文献
2.
为探究寒区冰封水库热状况的时空演变规律,于2010年6月~2011年8月对丰满水库的水温和冰情进行了原型观测。基于现场观测资料,阐述了丰满库区不同季节热结构的变化规律,重点分析了汛期洪水过程对分层结构的影响,并发现解冻初期水库表层浮力流动现象。同时,典型水温分层期1月和6月的坝前75~800m范围4条水温观测垂线基本一致,且同期电站下泄水温与坝前取水口对应高程平均水温差异较小,说明该水域范围内无三维水温效应。由于深层取水影响,丰满电站下泄水温过程较为稳定,但与坝址天然水温相比,5~7月、10~12月分别表现出月平均高达10.8℃、7.9℃的春夏低温水和秋冬高温水现象。此外,冰情监测结果表明,丰满水库冬季基本全库封冻,坝前最大冰厚约0.7m,且库区冰厚沿程出现不均匀分布的规律。 相似文献
3.
Jimin Yao Lianglei Gu Haidong Han Yuyu Wang Shiyin Liu 《Environmental Earth Sciences》2014,72(11):4503-4510
Energy fluxes were measured by using the eddy covariance system plus an automatic weather station at the debris-covered area on Koxkar Glacier from March to August, 2009. The coldest month of the glacier was January, and air temperature reached a maximum in July and August. Wind velocity at 2.0 m was higher in summer and lower in winter as a whole. Precipitation was concentrated from May to September and accounted for about 80 % of the total. Daily latent heat fluxes were higher than daily sensible heat fluxes during the observation period. The main reason for higher latent heat fluxes from March to April was snow cover. From June to August, latent heat fluxes during the daytime were limited by surface water content, and were lower than sensible heat fluxes, but latent heat fluxes were higher than sensible heat fluxes during summer nights because of air convection in the debris layer. Summer evaporation was higher than in the spring, and evaporation was 53.7 % of the precipitation from 19 June to 23 August. The Bowen ratio ranged from ?2.0 to 2.0 at the site. 相似文献
4.
V. S. N. Murty V. Ramesh Babu L. V. G. Rao Charuta V. Prabhu V. Tilvi 《Journal of Earth System Science》2000,109(2):267-277
Time-series data on upper-ocean temperature, Vessel-Mounted Acoustic Doppler Current Profiler (VM-ADCP) measured currents
and surface meteorological parameters have been obtained for the first time in the southern Bay of Bengal at 7‡N, 10‡N, and
13‡N locations along 87‡E during October–November, 1998 under BOBMEX-Pilot programme. These data have been analysed to examine
the diurnal variability of upper oceanic heat budget and to estimate the eddy diffusivity coefficient of heat in the upper
layer. Diurnal variation of near-surface temperature is typical at northern location (13‡N) with a range of 0.5‡C while the
diurnal range of temperature is enhanced to 0.8‡C at the central location (10‡N) due to intense solar radiation (1050 W/m2), clear skies and low wind speeds. At the southern location (7‡N), the diurnal variation of temperature is atypical with
the minimum temperature occurring at 2000 hrs instead of at early morning hours. In general, the diurnal curve of temperature
penetrated up to 15 to 20 m with decreasing diurnal range with depth. The VM-ADCP measured horizontal currents in the upper
ocean were predominantly easterly/northeasterly at southern location, north/northerly at central location and northwesterly
at northern location, thus describing a large-scale cyclonic gyre with the northward meridional flow along 87‡E. The magnitudes
of heat loss at the surface due to air-sea heat exchanges and in the upper 50 m layer due to vertical diffusion of heat are
highest at the southern location where intense convective activity followed by overcast skies and synoptic disturbance prevailed
in the lower atmosphere. This and the estimated higher value (0.0235 m2/s) of eddy diffusivity coefficient of heat in the upper ocean (0–50 m depth) suggest that 1-D processes controlled the upper
layer heat budget at the southern location. On the other hand, during the fair weather conditions, at the central and northern
locations, the upper layer gained heat energy, while the sea surface lost (gained) heat energy at northern (central) location.
This and lower values of eddy diffusivity coefficient of heat (0.0045 and 0.0150 m2/s) and the northward intensification of horizontal currents at these locations suggest the greater role of horizontal heat
advection over the 1-D processes in the upper ocean heat budget at these two locations. 相似文献
5.
选取高放射核废物处置库重要预选场区甘肃北山地区的花岗岩,制作750 mm（宽）×300 mm（厚）×1 000 mm（高）的稀疏不规则裂隙岩体模型,该模型由18块花岗岩和竖向与斜向各两条裂隙组成,在裂隙及岩石内部埋置温度传感器、水压计、直角应变花,并在模型一侧设置局部热源,研究热源温度和裂隙水流速对岩石温度和应力的影响。结果表明,竖裂隙水主要从顶部进水口流向底部出水口,斜裂隙水主要从侧部进水口流向侧部出水口,竖裂隙与斜裂隙在交汇处存在微小流量交换;由于热源处在两条斜裂隙进水口之间,并且斜裂隙长度小于竖裂隙,岩石热传导与斜裂隙水流对岩石温度分布起控制作用,竖裂隙水流对岩石横向热传导起阻滞作用;由于热传导和水流传热的不规则性,上层岩石形成从左向右为主的传热路径,中层和下层岩石形成从上向下为主的传热路径;由于上、下层岩石温度梯度较小,岩石收缩受热拉应力,而中层岩石温度梯度较大,岩石膨胀受热压应力,大主应力的方向大致垂直于斜裂隙面与竖裂隙面的交线,岩石应力增量随斜平面方向的温度梯度增大而增大;热源温度越高,裂隙水流速越低,岩石温度越高、岩石应力越大,系统达到稳态需要的时间越长。 相似文献
6.
The summer cooling of the Arabian Sea has been reviewed in relation to the dynamic and thermodynamic processes. The differences in the quantum of cooling in the coastal regions have been attributed to the variations in the strength of coastal upwelling along the respective coasts. In the central portions of the Arabian Sea, the thickness of the surface layer and the thermal structure appear to be predominantly governed by the turbulent mixing of cold waters entrained into the surface layer in association with the deepening of current shear zone. The surface heat losses during the passage of a cyclone over the east central Arabian Sea account for only 40% of the total heat change in the surface layer while the rest is lost into the interior. Also presented are climatological mean patterns of the forcing parameters and their variations during certain years. 相似文献
7.
根据2001年6月～2002年5月在天目湖进行的每月一次的全湖水温观测以及2002年5月25～26日在1号点的定点24h连续水温观测资料,分析研究了天目湖水温时空分布、垂直分布、温跃层的形成与变化以及湖泊热力学对溶解氧、营养盐的影响,揭示了各自的基本变化规律。结果表明:天目湖水温的日变化、年变化及垂直分布明显,而其水平差异不大;温跃层随着季节的变化而呈现增强-稳定-减弱-消失的周期变化;水温的变化以及温跃层的存在引起了水中溶解氧以及营养盐的变化。 相似文献
8.
Variability of the oceanic boundary layer characteristics in the northern Bay of Bengal during MONTBLEX-90 总被引：1，自引：0，他引：1
Variability of the ocean surface boundary layer characteristics on daily time-scale is studied utilizing the 3-hourly hydrographic data collected at a stationary location (20°N, 89°E) in the Bay of Bengal during August (18th–31st) and September (9th–19th), 1990 under MONTBLEX-90 field programme. The daily variations of temperature, salinity, σ0, mixed layer thickness, stability, heat content and rate of change of heat content in the upper 100 m are discussed in relation to prevailing weather (depressions) and hydrographic conditions (influx of fresh water, presence of eddies). The mixed layer thickness is examined through temperatureand σ0-based criteria considering also the surface salinity in the latter. TheT-based mixed layer thickness is always higher than that of σ0-based thickness. The rate of change of heat content is also computed up to the depth of 20°C and 14°C isotherms which takes into account the vertical motion and hence divergence. With the development of a low into a deep depression close to the study area, intense upwelling of subsurface cold waters is noticed from 100 m to the bottom of the surface mixed layer (20m) from 18th to 20th August. The upwelling is weakened by 21st August when the depression moved away from the study location. This variation of upwelling is supported by the variation of surface mixed layer thickness, static stability at 30 m depth, heat content in the upper 100 m and the heat content up to the depth of 20°C isotherm from 18th to 21st August. The rate of change of heat content in the upper 100 m and up to the depths of 20°C and 14°C isotherms leads to net heat storage during August and to net heat depletion during September. This together with the net surface heat gain lead to an import (197Wm?2) and export (233 Wm?2) of heat during August and September respectively through horizontal advective processes. These advective processes are attributed to the presence and movement of a warm core eddy through the study location. 相似文献
9.
Ren Li Lin Zhao Tonghua Wu Yongjian Ding Yao Xiao Guojie Hu Defu Zou Wangping Li Wenjun Yu Yongliang Jiao Yanhui Qin 《Environmental Earth Sciences》2014,72(6):2091-2099
In this study, we collected radiation and active layer temperature data observed in the northern Qinghai–Xizang Plateau during the period 2006–2008 in order to analyze the impact of surface energy balance on the thawing process of the active layer. Results show that surface energy exhibits an obvious seasonal variation. The largest values of energy variables including global radiation, net radiation, soil heat flux and surface heat source intensity occur during June and July, while the smallest values occur in November and December. The active layer is generally dominated by an endothermic process. During the freeze–thaw period, the variation process of the active layer temperature is similar to that of surface energy. The seasonal thawing depth is closely related to the process of surface energy exchange. During the thawing period, seasonal thawing depth gradually increases as more solar energy enters the surface. When the surface energy accumulation is 0.0 MJ m?2 d?1, the seasonal thawing depth is the smallest. The seasonal thawing depth gradually increases with further accumulation of surface energy. Thus, the variation processes between the surface energy and seasonal thawing depth can be expressed by a power relation. The values of seasonal thawing depth calculated with the empirical relationship provided in this study agree well with the observed values. The relative error between calculated and observed values is less than 12 %. These results show that this empirical relationship can be successfully used to describe the behavior of active layers. 相似文献
10.
利用2010年6-7月鄂陵湖野外试验的近地层观测数据,分析了在不同天气条件下黄河源鄂陵湖地区辐射分量、地表能量分量、土壤温度和反照率的变化特征. 结果表明：不同天气条件下,辐射和地表能量各分量日变化差异较大,晴天、阴天和雨天的地表反照率依次递减,平均反照率约为0.21;观测期内,平均辐射贡献从大到小依次为向上长波、向下长波、向下短波、向上短波,日积分值分别为31.4 MJ·m-2、25.6 MJ·m-2、22.4 MJ·m-2、4.2 MJ·m-2,净辐射(12.5 MJ·m-2)占向下短波辐射的55.7%;平均地表能量和土壤温度的变化幅度较晴天小,感热、潜热、0 cm土壤热通量的平均日积分值分别占净辐射的21.2%、43.1%、8.2%;平均土壤温度变化幅度随深度增加逐渐减小,浅层土壤温度峰值较晴天低2 ℃,深层土壤温度相差不大. 云和降水的扰动削弱了向下短波辐射,导致平均感热通量和0 cm土壤热通量的峰值比晴天小,而平均潜热通量的峰值大于晴天. 由于湖泊水体巨大的热容量和水分供应,鄂陵湖地区的气温日较差较小,地表温度变化幅度变小,附近地表温度升高缓慢. 鄂陵湖区的地表能量平衡中,潜热通量占主导,感热和地表土壤热通量次之. 研究结果有助于理解气候变化背景下黄河源区湖泊的能量水分循环过程,为促进该地区光热资源的合理利用和畜牧业的可持续发展提供数据支持. 相似文献
11.
利用Scripps海温再分析资料,对赤道印度洋0～400m深度范围内海温变化和偶极子异常变化特征进行了初步分析。结果显示,赤道印度洋上层海温呈现西低东高,而次表层以下海温则为西高东低。同时发现,温跃层是赤道印度洋上、下层很好的分界面。温跃层之上海温变化受海气相互作用明显,之下海温变化主要受海洋自身的运动影响。赤道印度洋偶极子现象存在于各个深度,其偶极子指数变化存在半年周期,季节变化表现为双峰双谷型,并从深层（400m）向表层传递。分析发现,海气相互作用不是表层赤道印度洋偶极子变化的决定因素。较深层偶极子变化决定于海洋自身的运动变化特征（如洋流）,并向上层传输,进而影响上层偶极子的异常变化。赤道印度洋偶极子指数由西印度洋和东印度洋海温变化共同制约,但西印度洋海温变化起主导作用,东印度洋仅起到加强或减弱偶极子强度变化的作用。 相似文献
12.
辽宁盘锦新近系馆陶组地下热水埋藏较深,开发历史较早,但利用率较低。研究认为,该区地温场变化主要受地幔隆起相对程度控制;东西两侧幔隆带部位,地壳的厚度相对较薄,结晶岩基底埋藏浅,深部热能传导到储热层消耗能量少,地温及地温梯度值相对较高;中部幔凹带地温以中凸起最高,凹陷区相对较低。在地幔隆起的控制下,区内馆陶组地下水水温受储热层埋藏深度的影响,储热层的埋藏深度大,降低了热能向地表的散失速度,所以水温相对较高;反之,水温相对较低。地下水水温变化规律为：西部的谷坡区,受地下水径流影响,水温一般25℃～28℃,而凹陷区则为30℃～35℃;到中部隆起区水温升高到35℃～50℃;东部凹陷区为31℃～38℃,谷坡为29℃。深部上地幔幔源热源（岩浆热）构成本区生热层,经构造导热作用传输到储热层。最后指出,中央凸起区是该区馆陶组地下热水勘查开发的有利地区,重点开发应在温热水（I区）。 相似文献
13.
A two-dimensional numerical model is employed to study the effect of the coastal urban heat island on the sea breeze front
and the thermal internal boundary layer height. The temperature at the land surface is determined by solving an energy budget
equation. The effect of the urban heat island is studied by varying the width of the region and its intensity. During the
early afternoon, the presence of the urban heat island enhances the strength of convergence of the sea breeze front and also
reduces its inland penetration. The presence of the urban heat island causes increased thermal internal boundary layer height.
Larger urban width causes larger vertical velocity and higher thermal internal boundary layer. Stronger convergence and higher
thermal internal boundary layer are also obtained in case of larger heat island intensity. 相似文献
14.
以辽宁省为例,采用统计分析方法,根据辽宁省61个气象站1951-2013年0~320 cm地温资料,分析了季节性冻土区地温场结构和变化特征。结果表明：地温最冷月出现时间随着深度增加而推后,辽宁各地浅层地温最冷月基本均为1月,深层地温最冷月为1-5月,深度越深温度越高。地温最热月出现时间也随深度增加而推后,浅层地温最热月为7、8月,深层地温最热月为8-10月,深度越深温度越低。越深层地温受地表影响越小,320 cm深度与地表的月平均最大温差达到19℃左右,40 cm深度与地表的月平均最大温差仅在8℃左右。随着深度增加,地温的季节变化减小,沈阳320 cm深度地温年内温差不足8℃。5~80 cm深度3-8月为储能期,160 cm深度5-9月为储能期,320 cm深度6-10月为储能期。越接近地表,地温日变化越显著,40 cm以下深度基本可以忽略日变化。沈阳地温升高程度大于气温,以向大气输送热量为主。地表最冷月变暖率明显大于最热月,但随着土层加深各土层最冷月、最热月变暖的程度无明显规律。深层地温的年际变化有时会受到更深层热源的非气候扰动。地温变化对气候、冻土区域工程等的影响不容忽视。 相似文献
15.
16.
基于2005—2016年青藏高原多年冻土区唐古拉和西大滩站的气象、涡动通量以及活动层资料,利用涡动相关法、气象梯度法和SHAW模型等方法探究了气候变化背景下高原多年冻土区地表能量通量变化规律及其对活动层的影响。结果表明：2005—2016年唐古拉和西大滩气温、地气温差有所升高,年降水量、10 cm土壤含水量及风速有所下降。2005年以来唐古拉和西大滩净辐射（Rn ）与感热（H）呈增加趋势,潜热（LE）呈减小趋势,地表土壤热通量（G）变化较小。唐古拉和西大滩地表能量通量季节变化明显,但受海拔、纬度、坡向、土壤冻融过程、降水、下垫面状况等因素的影响,地表能量通量存在区域差异。研究时段内,唐古拉和西大滩地表冻结指数与土壤热通量呈负相关;融化指数、活动层厚度与土壤热通量呈正相关,融化期间土壤热通量积累量与融化深度的变化呈线性增加关系。 相似文献
17.
The effect of the marine environment upon a vented Ir-encapsulated238Pu heat source was investigated. The heat source was emplaced in coastal submarine feldspathic sediment. In less than a month it became encased in a rock-like concretion. The capsule was cemented initially with a white deposit of anhydrite, a mineral identified with high temperature deep-sea springs. As the concentration increased in thickness sedimentary particles were incorporated by the cementing agent. A non-porous barrier was formed such that decay product He was impeded from escape. This property protected the heat source against intrusion by the corrosive marine waters.As determined by neutron activation, the major and minor elements within the coastal sediment, various fractions of the concretion, and certain discrete entities within or on the surface of the concretion, are included. 相似文献
18.
济阳坳陷地幔热流和深部温度 总被引：8，自引：2，他引：6
济阳坳陷深部地热状况对于分析岩石圈深部结构特征、探索该盆地形成和演化的地球动力学过程具有重要意义.依据济阳坳陷最新的钻探资料和深部地球物理探测结果, 按沉积盖层、上、中、下地壳4层结构, 建立了分别代表该区凹陷部位和凸起及斜坡带上的2种地壳结构模型.通过多道能谱分析, 测试了区内4 3块岩心样品的放射性元素U、Th、40K含量, 统计得出了济阳坳陷沉积盖层的平均生热率为(1.40±0.26) μW/m3.在研究大地热流分布的基础上, 结合济阳坳陷地壳各岩层放射性生热率, 采用“剥层”法, 从地表开始, 由浅到深逐步扣除各层段所提供的热量, 得到了济阳坳陷的地幔热流.并且采用相似的方法, 利用一维稳态热传导方程, 分析了地壳上地幔顶部的温度状况.结果表明, 济阳坳陷的地幔热流约为38.4~39.2 mW/m2, 占整个地表总热流量的5 8%;地幔顶部温度约为602~636℃.与世界上其他各类地质构造单元相比, 济阳坳陷无论是地幔热流值或其与地表热流之比值都是比较高的, 其深部地热状态具有介于稳定地区和构造活动区之间的特点. 相似文献
19.
边界条件对碎石层降温效果及机理的影响 总被引：22，自引：14，他引：8
对平均粒径为22.1 cm, 厚度1.3 m, 边界为开放和封闭的碎石层进行了一系列的实验. 从环境温度为最高和最低时刻封闭碎石层内的温度和速度分布可知: 当碎石层上表面温度低于下表面时,碎石层自下向上的散热由空气对流和碎石间的热传导来完成; 当上表面温度高于下表面时, 自上向下传递的热量由碎石接触面间的热传导完成, 此时, 由于其内部的空气几乎静止, 能阻隔热量的传入, 因此封闭边界的碎石层具有热半导体特性. 而开放边界的碎石层, 当平均温度为 0.5℃的空气从上表面吹过时, 碎石体内的热量传递主要是靠强迫对流来完成, 热半导体效果不明显, 不利于使其下面的冻土降温. 相似文献
20.
Christopher Uche Ezeh Michael Chukwuma Obeta Raymond N. C. Anyadike 《Arabian Journal of Geosciences》2016,9(16):681
The study compared the sequences of daily rainfall over coastal southern and semi-arid northern Nigeria. Daily rainfall occurrences for 41 years (1971–2011) over four meteorological stations in Lagos, Rivers, Borno, and Katsina were analyzed using frequency analysis and Markov chain model. Findings indicate that the coastal area had a predominance of 2–4-day wet spells while the semi-arid area showed a wet spell distribution that is geometric in nature with 1-day spell predominance. The dry spell behavior was nearly the opposite of the wet spell occurrence. The coastal region showed a dry spell of 1–4-day spell predominance while the semi-arid region showed a predominance of higher dry spells of 2–6 days. Accumulation of the amount of rainfall in each spell also showed that much rainfall from the coastal area was obtained from rains of spells of 3 days and above while the semi-arid had more of its rain from spells of 1–3 days. The mean annual rainfall was 1423.75 mm (Lagos), 2173.56 mm (Rivers), 517.50 mm (Katsina), and 578.34 mm (Borno). The wettest month was June (274.08 mm) in Lagos, September (378.18 mm) in Rivers, and August in Katsina and Borno (172.98 and 184.81 mm, respectively). The driest months were January for Lagos and Rivers (15.77 and 18.96 mm, respectively) and November–February for Katsina and Borno (0–0.06 mm). This showed that the coastal areas had nearly three times the volume of rain in the semi-arid area. The study further showed that onset of rain for the coastal area was March/April while the cessation of rainy season was October/November. On the other hand, the onset of rainy season in the semi-arid area was May/June and cessation of rainy season was September. Findings portend drier days for the semi-arid area due to dry spell persistence and hence, the consequent challenges of providing artificial water supply for agriculture and other purposes especially from October to May. 相似文献