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1.
云贵高原西部大理地区近地层湍流特征分析 总被引：4，自引：1，他引：3
利用大理国家气候观象台2007年3—12月观测资料,采用涡动相关法等计算方法分析了该地区湍流强度、湍流方差、湍流通量等特征量的日变化和干湿季变化特征。结果表明,湍流强度干季大于湿季;湍流方差与稳定度满足1／3次方定律,风速方差在稳定条件下比不稳定条件下离散,水平方向比垂直方向离散;湍流通量有明显日变化特征,感热、动量通量干季大于湿季,潜热通量湿季大于干季,干湿季热量交换以潜热为主;干季能量闭合率大于湿季;不同风向条件下平均水汽密度存在差异. 相似文献
2.
南海西南季风爆发前后海-气通量交换系 数研究 总被引：7，自引：1，他引：7
动量交换系数(CD)、感热交换系数(CH)和潜热(或水汽)交换系数(CE)是气候模式中参数化海-气通量必需的参数,不同地区、天气、海况的试验中计算结果各异。文章利用2002年4月24日至6月20日在西沙海区进行的第3次南海海-气通量观测试验资料,使用涡旋相关法和TOGA COARE2.5b版本通量计算方案,计算了西南季风爆发前后海-气界面动量、感热通量、潜热通量等的湍流交换系数,讨论了各通量交换系数的变化特征及其与气象要素变化的关系。结果表明:西南季风爆发前后,随着风向、风速、云量、降水、湿度及海面状态等变化,通量交换系数也发生变化:中性条件动量交换系数(CDn)在季风爆发前数值略小,季风爆发后数值增大;中性条件感热交换系数和潜热交换系数(CHn,CEn)对天气变化的反应不够敏感。动量交换系数主要受风速影响,但在不同风速区间相关关系有异。(CH)与海-气温差呈现正相关关系,和气温有明显的负相关关系。CE与风速的关系密切,但当风速>12 m/s,CE随风速的变化趋向一个稳定值。另外当海-气温差大约<2℃时,CE随着海-气温差增大相应增大,反映了通量交换系数不仅与风影响下的下垫面特性有关,而且还与稳定度参数有关。各通量交换系数与气象要素变化的关系可以拟合为多项式或者简单的线性关系式。 相似文献
3.
青藏高原东南缘大理地区近地层微气象特征及能量交换分析 总被引：2，自引：0，他引：2
利用2008年1月-2010年2月青藏高原东南缘大理站的长期观测资料,初步分析了该地区近地层基本气象要素、辐射通量和湍流通量的日变化和季节变化.结果表明,各参数均表现出显著的日循环结构和干、湿季变化特征.近地层的风速、气温和动量通量等均在早晨最小、午后最大;相对湿度、地表温度等均是湿季高于干季.近地层2 m高度处的盛行风向,白天以东东南风和东风为主,夜间以静风和偏西风为主,并且盛行风向转变与日出、日落时间有较好的对应关系.地表辐射四分量最高值出现在正午,最低值出现在日出前.除向上短波辐射通量干季大于湿季外,其他辐射分量都是湿季大于干季.地表反照率表现出非对称的“U”形分布,早晨最大、傍晚次之及中午最小.早晚地表反照率差异可能是由于露水、东西两面山体不同程度遮挡以及云的影响造成的.感热、潜热通量全年有相似的日变化过程,变化幅度随季节变化,但潜热通量明显大于感热通量,表明地气热量交换中,感热作用小,潜热输送占主导地位.感热通量一天之中约在20:00出现最小值,这主要是由于风速减弱和地气温差回升影响热量交换系数造成的.地面对大气的加热作用明显,主要是以潜热方式加热大气;地面全年均为大气热源,白天表现为强热源,夜间则表现为较弱的冷源. 相似文献
4.
5.
利用2008年4~5月大理国家气候观象台近地面层观测系统的梯度、涡动相关通量观测资料,结合背景场环流分析,分析了西南季风爆发前后大理近地面层的风速、风向变化特征、风速廓线和垂直切变变化特征以及动量、感热和潜热通量变化特征。结果显示:西南季风爆发前,大理近地层风向以东南风为主,平均风速较大;风速日变化的双峰型特征较显著,风速的垂直切变大,动量通量数值较大且日变化特征较明显。西南季风爆发后,大理近地层西北风频率显著增加,平均风速减小;风速日变化以单锋型为主,风速垂直切变较前期显著减小,动量通量数值减小而日变化特征较不显著。西南季风开始前后大理地气热量交换都以潜热为主,西南季风开始前一旬期间,潜热通量的逐日变化特点是随时间逐渐减少,感热通量逐渐增大,二者差值逐渐减小;西南季风开始后潜热通量的逐日变化为逐渐增大而感热通量逐渐减少,二者差值逐渐增大。就月平均值的日变化而言,潜热通量峰值变化不大,雨季略低于干季的4月;感热通量4~6月的月平均逐月降低。其原因既与雨季天气的变化有关,也与下垫面状况的改变相联系。 相似文献
6.
西太平洋热带海域西风爆发过程湍流通量输送的某些特征 总被引：12，自引：2，他引：12
本文根据中、美、日、澳、法等近20个国家在热带海洋全球大气海气耦合响应试验强化期（1992年11月～1993年2月）定点、连续观测获得大气和海洋资料，使用考虑风速和大气层结影响的整体输送动力学公式，计算动量、感热和潜热等的湍流通量。结果表明，西风爆发过程与其他天气过程相比，无论是大气向海洋输送的动量通量，还是海洋向大气输送的感热通量和潜热通量，其值都是最大的。文中还讨论了整体输送公式中的曳力系数、感热交换系数和潜热交换系数更准确的计算方法。 相似文献
7.
陆—气之间的能量交换是通过近地层湍流热量和水汽通量来实现的.以往的研究表明近地层阻抗对湍流能量通量有着不同程度的影响,但是关于陆面模式中阻抗系数的取值范围却始终没有统一的标准.为了深入了解简单生物圈模式 (SiB2) 中近地层阻抗系数取值变化对湍流能量通量的影响,我们以那曲站为例,分别采用传统的逐个因子分析法和考虑参数间相互作用的部分因子分析法定量地研究了夏季该观测站近地层湍流能量通量分别对冠层阻抗系数C1和地表阻抗系数C2的敏感性响应.结果表明,感热通量对地表阻抗系数C2更为敏感,而潜热通量则对冠层阻抗系数C1较为敏感;感热通量随C1增加而增大,随C2增加而减小,而潜热通量则随C1或C2的增加而减小;不管是感热通量还是潜热通量,它们对阻抗系数的敏感度随阻抗系数的增大而减小,而对阻抗系数的相对敏感度则随阻抗系数的增大而增大.最后,结合那曲站夏季下垫面稀疏短草的分布特点分析了造成感热通量和潜热通量敏感变化各异的原因. 相似文献
8.
利用在陇中黄土高原半干旱区2003年10月—2005年7月获得的近地层梯度观测资料,采用空气动力学法,计算了动量和感热总体输送系数。结果表明,陇中黄土高原半干旱区动量和感热总体输送系数均存在明显的日变化特征,夏季中午左右分别达到5.6×10-3和6.7×10-3。受下垫面植被的影响,在一年中呈现出双峰型特征,第一峰值出现在春小麦拔节—黄熟期,次高值出现在10月初。动量和感热总体输送系数平均值分别为2.9×10-3和3.1×10-3。当大气处于不稳定状态时,总体输送系数随着风速的增大而减小;相反当大气处于稳定状态时,随着风速的增大而增大。陇中黄土高原半干旱区的总体输送系数高于戈壁、平原草地和海洋下垫面的值,但低于青藏高原草地和城市下垫面的值。 相似文献
9.
10.
1998年南海季风爆发期间近海面层大气湍流结构和通量输送的观测研究 总被引：28，自引：1，他引：27
1998年5月14日至6月22日,在西沙永兴岛近海铁塔上进行了一次海-气通量观测试验,观测期包括了西南季风爆发前、爆发、爆发后风速加强等几个阶段。这次试验获得该年西南季风爆发的天气特征以及由涡度相关法、廓线法计算的动量、感热、潜热通量及湍流强度等一些统计量分布。分析结果表明,观测期湍流强度σu、σv、σw与平均风速之比为0.096、0.066、0.045;在近中性条件下（z/L≈0）,各相似函数基本为常数,σu/u＊≈3,σv/u＊≈2,σw/u＊≈1.25;在稳定条件下u、v、w三方向σ/u＊近似相等;在稳定与不稳定条件下σt/t＊随稳定度参数z/L的变化趋势相似,但符号相反。摩擦速度u＊随风速的变化接近于关系式u＊=0.029U10+0.006（U10为10m高度30min平均风速）,空气动力粗糙度长度z0变化在0.01～0.35mm之间。观测期动量通量变化在0.05～0.30N/m2之间,季风爆发期明显增大;曳力系数CD平均为1.12×10-3,它随平均风速变化可以表示为关系式103CD=0.003U210+0.020U10+0.836或103CD=0.056U10+0.732。感热通量由海洋输向大气,平均值为7.8W/m2,数值在0～15W/m2之间变化,季风爆发后明显增大;潜热通量数值一般变化于50～200W/m2,白天中午数值较高,夜间较低。季风爆发后也明显增大。观测期间鲍恩比（BowenRatio）日平均为0.05左右。 相似文献
11.
1986年夏季西藏东部近地层湍流输送特征的分析 总被引：3，自引：0，他引：3
本文以1986年夏季西藏高原气象实验(TIPMEX-86)期间获得的资料为基础,运用廓线方法,计算了实验期间感热、潜热和动量湍流通量并分析了与通量输送有关因子的变化。分析结果表明,各种湍流通量都有明显的日变化、日际变化和旬变化。7月份感热通量比6月份大约减少了2/3以上。计算得出那曲6月13—28日拖曳系联C_d的平均值为0.0052,同期感热通量的整体输送系数C_h为0.0075;而拉萨6月11日—7月20日C_d的平均值为0.0056,同期C_h的平均值为0.0085。根据整体输送系数和各种有关因子的关系分析表明,C_d,C_h不可能用一个常数代表,它们不仅仅是风速的函数,而且其变化还包含了稳定度、风速梯度、温度梯度的综合效应。 相似文献
12.
Denny P. Alappattu D. Bala Subrahamanyam P. K. Kunhikrishnan Radhika Ramachandran K. M. Somayaji R. Venkatesh G. S. Bhat A. Bhagavath Singh 《Boundary-Layer Meteorology》2008,126(2):297-309
We report the spatio-temporal variability of surface-layer turbulent fluxes of heat, moisture and momentum over the Bay of
Bengal (BoB) and the Arabian Sea (AS) during the Integrated Campaign for Aerosols, gases Radiation Budget (ICARB) field experiment.
The meteorological component of ICARB conducted during March – May 2006 onboard the oceanic research vessel Sagar Kanya forms
the database for the present study. The bulk transfer coefficients and the surface-layer fluxes are estimated using a modified
bulk aerodynamic method, and then the spatio-temporal variability of these air-sea interface fluxes is discussed in detail.
It is observed that the sensible and latent heat fluxes over the AS are marginally higher than those over the BoB, which we
attribute to differences in the prevailing meteorological conditions over the two oceanic regions. The values of the wind
stress, sensible and latent heat fluxes are compared with those obtained for the Indian Ocean Experiment (INDOEX) period.
The variation of drag coefficient (C
D
), exchange coefficients of sensible heat and moisture (C
H
= C
E
) and neutral drag coefficient (C
DN
) with wind speed is also discussed.
相似文献
13.
Aerodynamic Parameters of Regular Arrays of Rectangular Blocks with Various Geometries 总被引：8，自引：8，他引：0
The aerodynamic effects of various configurations of an urban array were investigated in a wind-tunnel experiment. Three aerodynamic
parameters characterising arrays—the drag coefficient (C
d
), roughness length (z
o) and displacement height (d)—are used for analysis. C
d
is based on the direct measurement of the total surface shear using a floating element, and the other two parameters are
estimated by logarithmic fitting of the measured wind profile and predetermined total drag force. The configurations of 63
arrays used for measurement were designed to estimate the effects of layout, wind direction and the height variability of
the blocks on these parameters for various roughness packing densities. The results are summarised as follows: (1) The estimated
C
d
and z
o of the staggered arrays peak against the plan area index (λ
p
) and frontal area index (λ
f
), in contrast with values for the square arrays, which are less sensitive to λ
p
and λ
f
. In addition, the square arrays with a wind direction of 45° have a considerably larger C
d
, and the wind direction increases z
o/H by up to a factor of 2. (2) The effect of the non-uniformity of roughness height on z
o is more remarkable when λ
f
exceeds 20%, and the discrepancy in z
o is particularly remarkable and exceeds 200%. (3) The effect of the layout of tall blocks on C
d
is stronger than that of short blocks. These results indicate that the effects of both wind direction and the non-uniformity
of the heights of buildings on urban aerodynamic parameters vary greatly with λ
p
and λ
f
; hence, these effects should be taken into account by considering the roughness packing density. 相似文献
14.
BOUNDARY LAYER STRUCTURE IN TYPHOON SAOMAI (2006): UNDERSTANDING THE EFFECTS OF EXCHANGE COEFFICIENT
Recent studies have shown that surface fluxes and exchange coefficients are particularly important to models attempting to simulate the evolution and maintenance of hurricanes or typhoons.By using an advanced research version of the Weather Research and Forecasting(ARW)modeling system,this work aims to study the impact of modified exchange coefficient on the intensity and structures of typhoon Saomai(2006)over the western North Pacific.Numerical experiments with the modified and unmodified exchange coefficients are used to investigate the intensity and structure of the storm,especially the structures of the boundary layer within the storm.Results show that,compared to the unmodified experiment,the simulated typhoon in the modified experiment has a bigger deepening rate after 30-h and is the same as the observation in the last 12-h.The roughness is leveled off when wind speed is greater than 30 m/s.The momentum exchange coefficient(CD)and enthalpy exchange coefficient(CK)are leveled off too,and CD is decreased more than CK when wind speed is greater than 30 m/s.More sensible heat flux and less latent heat flux are produced.In the lower level,the modified experiment has slightly stronger outflow,stronger vertical gradient of equivalent potential temperature and substantially higher maximum tangential winds than the unmodified experiment has.The modified experiment generates larger wind speed and water vapor tendencies and transports more air of high equivalent potential temperature to the eyewall in the boundary layer.It induces more and strong convection in the eyewall,thereby leading to a stronger storm. 相似文献
15.
Momentum and Heat Transfer over Urban-like Surfaces 总被引：2，自引：2，他引：0
Momentum and heat transfer was examined for the urban-like surfaces used within the Comprehensive Outdoor Scale MOdel (COSMO)
experiments. Simultaneous and comparative meteorological measurements were made over a pair of scale models with different
block geometries. These data were analyzed to investigate the influence of height variations, obstacle elongation, and packing
density, λ
p
, of blocks on the aerodynamic properties. In addition, the robustness of theoretical expressions of bulk transfer coefficients
for momentum and heat with respect to geometric parameters was examined. Our analyses showed: (1) the theoretical framework
for the bulk transfer coefficient for momentum, C
m
, and that for heat, C
h
, was applicable for homogeneous building arrays, (2) the sensitivity of C
h
to the surface geometry was smaller than that of C
m
, (3) the transfer coefficients were increased by variations of block heights, but not by elongation of blocks, (4) first-order
approximations of C
m
and C
h
for an array of blocks with two different heights can be made by applying simple theoretical assumptions to include the effects
of height variation, and (5) variations of block heights increased the momentum flux significantly, but caused little change
in the sensible heat flux. This can be explained by the feedback mechanism of aerodynamic– thermal interaction; aerodynamic
mixing decreased both the advective velocity and the vertical temperature gradient. 相似文献
16.
Kusuma G. Rao 《Boundary-Layer Meteorology》2004,111(2):247-273
For the first time, the exchange coefficient of heat CH has been estimated from eddy correlation of velocity and virtual temperature fluctuations using sonic anemometer measurements made at low wind speeds over the monsoon land atJodhpur (26°18' N, 73°04' E), a semi arid station. It shows strong dependence on wind speed, increasing rapidly with decreasing wind speed, and scales according to a power law CH = 0.025U10
-0.7 (where U10 is the mean wind speed at 10-m height). A similar but more rapid increase in the drag coefficient CDhas already been reported in an earlier study. Low winds (<4 m s-1) are associated with both near neutral and strong unstable situations. It is noted that CH increases with increasing instability. The present observations best describe a low wind convective regime as revealed in the scaling behaviour of drag, sensible heat flux and the non-dimensional temperature gradient. Neutral drag and heat cofficients,corrected using Monin–Obukhov (M–O) theory, show a more uniform behaviour at low wind speeds in convective conditions, when compared with the observed coefficients discussed in a coming paper.At low wind convective conditions, M-O theory is unable to capture the observed linear dependence of drag on wind speed, unlike during forced convections. The non-dimensional shear inferred from the present data shows noticeable deviations from Businger's formulation, a forced convection similarity. Heat flux is insensitive to drag associated with weak winds superposed on true free convection. With heat flux as the primary variable, definition of new velocity scales leads to a new drag parameterization scheme at low wind speeds during convective conditionsdiscussed in a coming paper. 相似文献
17.
High frequency measurements of wind velocity and temperature were made during the Ocean Storms Project in November 1987. The dissipation method was applied to the resulting time series in order to determine friction velocities,u
*, and the characteristic temperature scale,t
*, at 1-min intervals. These values were then compared to the 1-min mean wind speed and air-sea temperature differences to determine relationships for the drag coefficient (C
d
) and Stanton number (C
h
). The drag coefficient was comparable to other values reported in the literature, although the variation with wind speed was greater than reported by other investigators. An examination of the residual time series indicated a systematic low frequency periodicity of about 2-hr duration which was attributed to a fluctuating wind interacting with the surface gravity wave field. The temperature fluctuations did not produce meaningful estimates ofC
h
for stable conditions. For unstable conditions, a value of 1.09±0.02×10–3 was found. 相似文献
18.
本工作是在日本京都大学,防灾研究所的龙卷模拟实验室,用流体动力学模似实验方法研究三种不同粗糙表面对龙卷涡旋的影响。实验中,用热线风速表及微型风向标,测定了五个不同高度上的水平风速和风向分布,揭示出在不同粗糙表面上,龙卷涡旋的风速和风向分布特征。通过不断改变模拟装置的涡旋比S,发现当S值超过某一数值后(S>1.5),在不同粗糙表面上,龙卷涡旋的涡核尺寸将趋于一致。实验结果可进一步解释自然界中的观测事实,并对某些理论研究提供实验依据。 相似文献
19.
Andrey A. Grachev Edgar L Andreas Christopher W. Fairall Peter S. Guest P. Ola G. Persson 《Boundary-Layer Meteorology》2007,124(3):315-333
Measurements of atmospheric turbulence made during the Surface Heat Budget of the Arctic Ocean Experiment (SHEBA) are used
to examine the profile stability functions of momentum, φ
m
, and sensible heat, φ
h
, in the stably stratified boundary layer over the Arctic pack ice. Turbulent fluxes and mean meteorological data that cover
different surface conditions and a wide range of stability conditions were continuously measured and reported hourly at five
levels on a 20-m main tower for 11 months. The comprehensive dataset collected during SHEBA allows studying φ
m
and φ
h
in detail and includes ample data for the very stable case. New parameterizations for φ
m
(ζ) and φ
h
(ζ) in stable conditions are proposed to describe the SHEBA data; these cover the entire range of the stability parameter
ζ = z/L from neutral to very stable conditions, where L is the Obukhov length and z is the measurement height. In the limit of very strong stability, φ
m
follows a ζ 1/3 dependence, whereas φ
h
initially increases with increasing ζ, reaches a maximum at ζ ≈ 10, and then tends to level off with increasing ζ. The effects
of self-correlation, which occur in plots of φ
m
and φ
h
versus ζ, are reduced by using an independent bin-averaging method instead of conventional averaging. 相似文献
20.
A nocturnal gravity wave was detected over a south-western Amazon forest during the Large-Scale Biosphere–Atmosphere experiment
in Amazonia (LBA) in the course of the dry-to-wet season campaign on October 2002. The atmospheric surface layer was stably
stratified and had low turbulence activity, based on friction velocity values. However, the passage of the wave, an event
with a period of about 180–300 s, caused negative turbulent fluxes of carbon dioxide (CO2) and positive sensible heat fluxes, as measured by the eddy-covariance system at 60 m (≈30 m above the tree tops). The evolution
of vertical profiles of air temperature, specific humidity and wind speed during the wave movement revealed that cold and
drier air occupied the sub-canopy space while high wind speeds were measured above the vegetation. The analysis of wind speed
and scalars high frequency data was performed using the wavelet technique, which enables the decomposition of signals in several
frequencies allowed by the data sampling conditions. The results showed that the time series of vertical velocity and air
temperature were −90° out of phase during the passage of the wave, implying no direct vertical transport of heat. Similarly,
the time series of vertical velocity and CO2 concentration were 90° out of phase. The wave was not directly associated with vertical fluxes of this variable but the mixing
induced by its passage resulted in significant exchanges in smaller scales as measured by the eddy-covariance system. The
phase differences between horizontal velocity and both air temperature and CO2 concentration were, respectively, zero and 180°, implying phase and anti-phase relationships. As a result, the wave contributed
to positive horizontal fluxes of heat and negative horizontal fluxes of carbon dioxide. Such results have to be considered
in nocturnal boundary-layer surface-atmosphere exchange schemes for modelling purposes. 相似文献