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1.
给出一种利用测定圆管对流换热温度场求解湍流流体热物性参数的方法。根据边界层理论,对管内湍流强制对流换热控制方程组进行简化,并通过考虑湍流运输中的密度脉动,对传统的混合长度湍流模型进行改进,基于该计算模型求解圆管湍流模型的温度场。采用Levenberg-Marquardt方法通过测量温度场反演了湍流对流换热控制方程中的黏度系数。结果表明,利用反问题方法通过测定温度场反演湍流流动流体的热物性参数具有可行性,精确度较高。 相似文献
2.
浮冰界面融化速率参数化方案的实验室研究 总被引：2，自引：2，他引：0
融冰季节时天然浮冰表面、底面和侧向融化共存,三者融化速率是底面大于侧向,侧向大于表面。而且浮冰尺寸越小,侧向速率占比越高。为了解决将小尺度浮冰块尺度指标计入融化参数化方案,在低温环境实验室无辐射、无流速、控制气温和水温条件下对天然海冰和人工冻结淡水冰的圆盘试样,开展了不同初始水温和不同初始直径的圆盘试样融化过程实验,获得了圆盘试样直径、厚度和质量融化过程。依据这些实验数据,构建试样直径厚度比这一新指标,通过物理分析和数学统计手段,建立了海冰和淡水冰试样表面、底面融化速率同温度梯度,侧向融化速率和温差以及直径厚度比的关系式。这些关系式能够应用于天然直径100 m范围内浮冰的融化参数化方案,期望能解决北冰洋海冰和入海口近岸淡水冰夏季融化季节能量和质量平衡数值模拟的需求。 相似文献
3.
本文将海面上的大气边界层简化为水平平板上湍流边界层的混合对流问题,并考虑大气与海浪之间的动量交换,计算出海面上风速、海气温差和风区等诸因素对海气动量输运的影响.边界层计算需用的湍流模式采用包含浮力效应的混合长模式,在考虑海浪作用的计算中采用理论与半经验公式相结合的方法.我们发现在有限风区情况下(刮离岸风的近海区域),风区会显着影响不同海气温差下海气动量交换过程,这一点在以往的研究中从未涉及到. 相似文献
4.
5.
北极多年海冰的渡夏与冰脊形成的初始阶段均属于海冰升温的热力学过程。在卤水作用下，海冰在升温过程中需要融化内部的固态冰以达到温盐平衡。为研究海冰升温过程中盐度对宏观热力学性质的影响，本文设计了冰块试样在水中的一维浸没试验。将具有相同初始温度 （-32℃）、不同盐度 （0 ppt, 2.65 ppt, 12 ppt） 的冰试样浸至 0.2 ℃的淡水环境中，并测试试样内部温度场与厚度变化。试验结果表明，高盐度海冰的最终冰厚增加量超过 31%，而淡水冰则仅为 15%。海冰内部卤水的活跃改变了海冰的宏观比热并大幅度提高了其潜在的内能变化量。同时，将内能变化的实测结果与 Schwerdfeger 模型理论计算结果进行了对比。分析得出，真实环境中在海冰卤水迁移引起的盐度不均匀分布与卤水外排使得 Schwerdfeger 模型无法准确描述海冰升温过程中热力学性质。此外，通过对新生冰进行冰晶测试中所观测的柱状结构及晶粒尺寸特征也进一步验证了试验结果的可靠性。 相似文献
6.
利用一次冷空气过程的14组GPS探空数据,采用位温梯度法确定了冷空气过境前后大气边界层高度,并分析了冷空气过程对大气边界层结构的影响。结果表明:冷锋过境加大了海洋大气边界层的静力不稳定度,使边界层内对流活动增强,且锋面过后距离锋面越近的区域边界层的静力不稳定度越大;冷锋过境使边界层的平均高度升高,边界层顶处逆温梯度增大。结合ERAInterim再分析资料,分析认为大气边界层高度与静力稳定度(海气温差)存在显著的正相关关系(相关系数达0.73),海气温差越大,大气边界层高度越高。 相似文献
7.
根据2012年5、11月2次船载GPS探空资料,结合CFSR再分析、OISST海温、沿岸站位L波段雷达数据等,对黄东海海洋大气边界层(MABL)的时空变化特征及影响因子进行了分析。GPS探空数据表明,正的海气温差产生对流边界层,负的为稳定边界层。相比陆地边界层,MABL的日变化很小。5月份,MABL较低,暖区的海气温差大小与MABL高度相关,而冷区风切变的影响较为显著,太阳辐射也能一定程度上影响MABL高度。11月,MABL远高于5月,海气温差、太阳辐射均能影响MABL高度,风切变贡献很小。5月份海洋锋暖水侧的水汽能到达MABL以上,冷水侧水汽则维持在MABL中;11月水汽被限制在MABL以内。通过青岛、洪家站的L波段雷达数据对比,得到沿岸地区的大气边界层具有与MABL相同的季节变化,能够代表黄、东海MABL特征,但日变化更加剧烈,因此在替代研究海上MABL日变化时具有局限性。 相似文献
8.
海上溢油油膜厚度实验室模拟和理论模型对比研究 总被引：1，自引：0，他引：1
溢油量是衡量溢油规模的关键指标,是处理溢油事故的重要依据。油膜厚度是确定溢油量的基本前提,是一个尚未解决的国际难题。实验室中模拟了不同阶段和不同环境条件下扩展油膜的厚度变化特征。结果表明,实验室模拟与理论模型分析具有基本一致的变化趋势,扩展速度与扩展时间成反比;温度是影响油膜厚度的重要因素,相同条件下,温度越高,油膜厚度越小;海水盐度会影响溢油扩展,但这种影响并未延伸到对油膜厚度的控制上。由于实验室模拟限定在平静海面条件下,并未考虑风和海流等扩展中不容忽视的因素,故与理论构建模型相比系数相差较大。通过对比分析,前期构建的理论模型更能准确地反映海洋溢油的实际情况,加之在实例验证中的较高准确性,该模型具有业务化实施和广泛推广的潜力。 相似文献
9.
航行体近水面航行时会引起周围流场中流体的惯性运动,动能会随波浪扩散而耗散,航行体近水面运动时固有周期和幅值衰减率受水的影响可以用附加质量和阻尼系数描述。运用计算流体力学软件 STAR-CCM+开展航行体近水面自由横摇与纵摇衰减运动的数值仿真,根据不同初始角度条件下仿真得到的自由衰减时历曲线,分别计算横摇与纵摇的附加质量与阻尼系数,并结合实际运动情况,对不同初始角度条件下附加质量与阻尼系数的变化成因分别进行分析。 相似文献
10.
对传统可拆式板式换热器进行了改良,以适用于海洋温差能发电系统工况,并对改良后的板式换热器进行了理论数值分析。研建了海洋温差发电系统测试平台,对系统内的换热器换热特性进行测试,在不同工况下对换热器换热特性进行了实验研究,得到了板式换热器瞬态运行特性,同时还得到了换热器换热特性随热流密度的变化曲线及压降随工质流量的变化关系。结合实验数据拟合了换热器换热特性经验关联式和压降随工质流量关联式,预测值和实验值偏差均在20%以内。结果表明:在实验系统运行工况范围内,换热器的换热系数随着热流密度的增加而增大,当热流密度大于3 kW/m2时,换热系数随热流密度变化的曲线斜率变小;换热器压降随着工质流量增大而增加,压降随工质流量变化的曲线斜率变大。 相似文献
11.
雪热传导系数是海冰质量平衡过程中的重要物理参数，决定了穿透海冰的热传导通量。北冰洋海冰质量平衡浮标观测获得多年冰上冬季温度链剖面可以明显地区分冰雪界面。本文考虑到冰雪界面处温度随时间变化，再根据冰雪界面热传导通量连续假定，提出了新的雪热传导系数计算方法。受不同环境因素影响，多年冰上各个浮标的雪热传导系数在0.23~0.41 W/（m·K）之间，均值为（0.32±0.08） W/（m·K）。北冰洋多年冰上冬季穿过海冰的热传导通量最大发生在11月至翌年3月，约14~16 W/m2。结冰季节，来自海冰自身降温的热量对穿过海冰向大气传输的热量贡献逐月减少，从9月100%减小到12月的35%，翌年的1月至3月稳定在10%左右。夏季，短波辐射通能量通过热传导自上而下加热海冰，海冰上层温度高于下层，热量传播方向与冬季反向，往海冰内部传递。直到9月短波辐射完全消失，气温下降，热量再次转变为自下往上传递。从冰底热传导来看，夏季出现海冰向冰水界面传递热量现象。由于雪较好的绝热性，冰上覆雪极大地削弱了海冰上层热传导通量，从而减缓了秋冬季节的结冰速度。尽管受雪厚影响，多年冰上层热传导通量与气温依旧具有很好的线性关系，气温每降低1℃，热传导通量增加约0.59 W/m2。 相似文献
12.
《Deep Sea Research Part II: Topical Studies in Oceanography》1999,46(6-7):1385-1425
In high-latitude oceans with seasonal ice cover, the ice and the low-salinity mixed layer form an interacting barrier for the heat flux from the ocean to the atmosphere. The presence of a less dense surface layer allows ice to form, and the ice cover reduces the heat loss to the atmosphere. The ice formation weakens the stability at the base of the mixed layer, leading to stronger entrainment and larger heat flux from below. This heat transport retards, and perhaps stops, the growth of the ice cover. As much heat is then entrained from below as is lost to the atmosphere. This heat loss further reduces the stability, and unless a net ice melt occurs, the mixed layer convects. Two possibilities exist: (1) A net ice melt, sufficient to retain the stability, will always occur and convection will not take place until all ice is removed. The deep convection will then be thermal, deepening the mixed layer. (2) The ice remains until the stability at the base of the mixed layer disappears. The mixed layer then convects, through haline convection, into the deep ocean. Warm water rises towards the surface and the ice starts to melt, and a new mixed layer is reformed. The present work discusses the interactions between ice cover and entrainment during winter, when heat loss to the atmosphere is present. One crucial hypothesis is introduced: “When ice is present and the ocean loses sensible heat to the atmosphere and to ice melt, the buoyancy input at the sea surface due to ice melt is at a minimum”. Using a one-dimensional energy-balance model, applied to the artificial situation, where ice melts directly on warmer water, it is found that this corresponds to a constant fraction of the heat loss going to ice melt. It is postulated that this partitioning holds for the ice cover and the mixed layer in the high-latitude ocean. When a constant fraction of heat goes to ice melt, at least one deep convection event occurs, before the ice cover can be removed by heat entrained from below. After one or several convection events the ice normally disappears and a deep-reaching thermal convection is established. Conditions appropriate for the Weddell Sea and the Greenland Sea are examined and compared with field observations. With realistic initial conditions no convection occurs in the warm regime of the Weddell Sea. A balance between entrained heat and atmospheric heat loss is established and the ice cover remains throughout the winter. At Maud Rise convection may occur, but late in winter and normally no polynya can form before the summer ice melt. In the central Greenland Sea the mixed layer generally convects early in winter and the ice is removed by melting from below as early as February or March. This is in agreement with existing observations. 相似文献
13.
A. S. Filimonov V. A. Tarasov M. A. Komkov V. A. Moiseev M. P. Timofeev R. V. Boyarskaya 《Izvestiya Atmospheric and Oceanic Physics》2016,52(8):862-868
In this paper, the hazard of adverse heat effect on permafrost soil as a result of viscous oil production in the Far North is studied with the method of thermocompression supply of superheated water steam to the oil-bearing layer. It is found that, due to the divergent nature of heat transfer and convective complex movement of air in the space between the tubing and the casing, the temperature of the latter in the area of load-bearing elements heated to 130°C is about 70°C. The heterogeneity of the temperature field is leveled up to 4–5% at a distance of 400–420 mm from the axis of the tubing. The thickness of the melting layer of ground ice within 90 days of operation of the tubing depends on the percentage of water-filled pores in the soil. With the minimum (10%) percentage of water-filled pores in the soil layer, the thickness of the ground ice melting layer for 90 days of operation of the tubing does not exceed 2.6 m. 相似文献
14.
Annual observations of first-year ice(FYI) and second-year ice(SYI) near Zhongshan Station, East Antarctica,were conducted for the first time from December 2011 to December 2012. Melt ponds appeared from early December 2011. Landfast ice partly broke in late January, 2012 after a strong cyclone. Open water was refrozen to form new ice cover in mid-February, and then FYI and SYI co-existed in March with a growth rate of 0.8 cm/d for FYI and a melting rate of 2.7 cm/d for SYI. This difference was due to the oceanic heat flux and the thickness of ice,with weaker heat flux through thicker ice. From May onward, FYI and SYI showed a similar growth by 0.5 cm/d.Their maximum thickness reached 160.5 cm and 167.0 cm, respectively, in late October. Drillings showed variations of FYI thickness to be generally less than 1.0 cm, but variations were up to 33.0 cm for SYI in March,suggesting that the SYI bottom was particularly uneven. Snow distribution was strongly affected by wind and surface roughness, leading to large thickness differences in the different sites. Snow and ice thickness in Nella Fjord had a similar "east thicker, west thinner" spatial distribution. Easterly prevailing wind and local topography led to this snow pattern. Superimposed ice induced by snow cover melting in summer thickened multi-year ice,causing it to be thicker than the snow-free SYI. The estimated monthly oceanic heat flux was ～30.0 W/m2 in March–May, reducing to ～10.0 W/m2 during July–October, and increasing to ～15.0 W/m2 in November. The seasonal change and mean value of 15.6 W/m2 was similar to the findings of previous research. The results can be used to further our understanding of landfast ice for climate change study and Chinese Antarctic Expedition services. 相似文献
15.
States of maximum entropy production in a one-dimensional vertical model with convective adjustment 总被引：2，自引：0，他引：2
We investigate the hypothesis that the atmosphere is constrained to maximize its entropy production by using a one-dimensional (1-D) vertical model. We prescribe the lapse rate in the convective layer as that of the standard troposphere. The assumption that convection sustains a critical lapse rate was absent in previous studies, which focused on the vertical distribution of climatic variables, since such a convective adjustment reduces the degrees of freedom of the system and may prevent the application of the maximum entropy production (MEP) principle. This is not the case in the radiative-convective model (RCM) developed here, since we accept a discontinuity of temperatures at the surface similar to that adopted in many RCMs.
For current conditions, the MEP state gives a difference between the ground temperature and the air temperature at the surface ≈10 K. In comparison, conventional RCMs obtain a discontinuity ≈2K only. However, the surface boundary layer velocity in the MEP state appears reasonable (≈m s−1 ). Moreover, although the convective flux at the surface in MEP states is almost uniform in optically thick atmospheres, it reaches a maximum value for an optical thickness similar to current conditions. This additional result may support the maximum convection hypothesis suggested by Paltridge (1978 ). 相似文献
For current conditions, the MEP state gives a difference between the ground temperature and the air temperature at the surface ≈10 K. In comparison, conventional RCMs obtain a discontinuity ≈2K only. However, the surface boundary layer velocity in the MEP state appears reasonable (≈m s
16.
2010年马卡罗夫海盆冰站观测期间垂向热通量时间变化研究 总被引：1，自引：1，他引：0
Based on hydrographic data obtained at an ice camp deployed in the Makarov Basin by the 4th Chinese Arctic Research Expedition in August of 2010, temporal variability of vertical heat flux in the upper ocean of the Makarov Basin is investigated together with its impacts on sea ice melt and evolution of heat content in the remnant of winter mixed layer(r WML). The upper ocean of the Makarov Basin under sea ice is vertically stratified. Oceanic heat flux from mixed layer(ML) to ice evolves in three stages as a response to air temperature changes, fluctuating from 12.4 W/m2 to the maximum 43.6 W/m2. The heat transferred upward from ML can support(0.7±0.3) cm/d ice melt rate on average, and daily variability of melt rate agrees well with the observed results. Downward heat flux from ML across the base of ML is much less, only 0.87 W/m2, due to enhanced stratification in the seasonal halocline under ML caused by sea ice melt, indicating that increasing solar heat entering summer ML is mainly used to melt sea ice, with a small proportion transferred downward and stored in the r WML. Heat flux from ML into r WML changes in two phases caused by abrupt air cooling with a day lag. Meanwhile, upward heat flux from Atlantic water(AW) across the base of r WML, even though obstructed by the cold halocline layer(CHL), reaches0.18 W/m2 on average with no obvious changing pattern and is also trapped by the r WML. Upward heat flux from deep AW is higher than generally supposed value near 0, as the existence of r WML enlarges the temperature gradient between surface water and CHL. Acting as a reservoir of heat transferred from both ML and AW, the increasing heat content of r WML can delay the onset of sea ice freezing. 相似文献
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温度对墨西哥湾扇贝耗氧率及排泄率的影响 总被引：63，自引：2，他引：61
于1996年12月至1997年1月在实验室内研究了温度对墨西哥湾扇贝(Argopecten irradians concentricus)的耗氧率和排泄(NH4-N)率的影响,实验在投饵后6h,静水(盐度32)条件下进行,溶氧量和氨氮量分别采用Winkler滴定法和次溴酸盐氧化法测定.实验结果表明,在实验温度(10～31℃)条件下,不同规格(壳高1.6～4.8cm,软体部干重0.0342～0.6908g)的墨西哥湾扇贝耗氧率的总平均值为2.35mg/(g·h).排泄率总平均值为350.89μg/(g·h).墨西哥湾扇见的耗氧量和排氧量都与扇贝体重呈明显的幂函数关系.在10～28℃范围内,不同规格的扇贝耗氧率都随温度的升高而增加;当水温继续升高到31℃时,耗氧率反而下降.在实验温度(10～31℃)条件下,扇贝的排泄率随着温度的升高而增加,温度对墨西哥湾扇贝的耗氧率和排泄率的影响都可用指数方程表示.本实验证实,高温(31℃)将进一步提高墨西哥湾扇贝蛋白质的代谢水平.耗氧量(O)和排氨量(N)与温度(t)、扇贝软体部干重(W)二元线性回归方程分别为:O=-587.804+36.787t+1697.864W;N=-92.344 9+4.534 1t+276.781 8W.复相关系数r分别为0.880 6和0.8035 ; F检验表明,两个回归方程均极显著(F>F0.01). 相似文献
19.
Under the influence of global warming, the sea ice in the Arctic Ocean (AO) is expected to reduce with a transition toward a seasonal ice cover by the end of this century. A comparison of climate-model predictions with measurements shows that the actual rate of ice cover decay in the AO is higher than the predicted one. This paper argues that the rapid shrinking of the Arctic summer ice cover is due to its increased seasonality, while seasonal oscillations of the Atlantic origin water temperature create favorable conditions for the formation of negative anomalies in the ice-cover area in winter. The basis for this hypothesis is the fundamental possibility of the activation of positive feedback provided by a specific feature of the seasonal cycle of the inflowing Atlantic origin water and the peaking of temperature in the Nansen Basin in midwinter. The recently accelerated reduction in the summer ice cover in the AO leads to an increased accumulation of heat in the upper ocean layer during the summer season. The extra heat content of the upper ocean layer favors prerequisite conditions for winter thermohaline convection and the transfer of heat from the Atlantic water (AW) layer to the ice cover. This, in turn, contributes to further ice thinning and a decrease in ice concentration, accelerated melting in summer, and a greater accumulation of heat in the ocean by the end of the following summer. An important role is played by the seasonal variability of the temperature of AW, which forms on the border between the North European and Arctic basins. The phase of seasonal oscillation changes while the AW is moving through the Nansen Basin. As a result, the timing of temperature peak shifts from summer to winter, additionally contributing to enhanced ice melting in winter. The formulated theoretical concept is substantiated by a simplified mathematical model and comparison with observations. 相似文献
20.
东南极Princess Elizabeth冰盖近地层大气参数的年变化特征 总被引：4，自引：0，他引：4
利用2002年东南极Princess Elizabeth冰盖自动气象梯度观测点获得的近地层气象资料,分析了冰盖上的感热通量、潜热通量、大气稳定度、整体输送系数及有关气象要素特征,并与中山站同期的的气象要素进行了对比分析.结果表明,由于两站的海拔高度及地理位置的差异,LGB69站的年平均气温为-25.6℃,比中山站低16.4℃,进入内陆每10km,海拔高度上升约110m,温度下降约1℃.南极内陆冰盖的湍流热通量具有明显的年变化,感热通量年平均值为-17.9W/m2,潜热通量为-0.9W/m2,年平均冷源强度(Qh+Qe)为-18.8W/m2,表明地表从大气吸收热量.LGB69站近地层大气以近中性层结为主,中性层结下的整体输送系数为2.6×10-3,当风速大于8m/s后,整体输送系数趋于常数.LGB69站是南极地区典型下降风区,年平均风速比中山站大2.0m/s,其下降风出现的风向频和风速均大于中山站. 相似文献