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西太平洋暖池区的海气通量及整体交换系数 总被引：3，自引：1，他引：2
根据西太平洋海域弱风、高温、潮湿的大气状态特征,提出了在光滑面存在粘性副层气流中的廓线的层结订正方案。用此模式对西太平洋暖池区ＴＯＧＡＣＯＡＲＥＩＯＰ期间,在向阳红５号船（２°Ｓ,１５４°Ｅ）获取的海面风、温、湿梯度资料进行了处理。计算结果显示西太平洋暖池区贴水层气流中不稳定层结占５０％－８０％,其中很不稳定的占１０．３％;该海区海气通量和整体交换系数受层结影响远大于受风速的影响;海气通量和整体交换系数随不稳定程度增加而增大,在相同风速下量值可相差４倍以上;其变化范围为０．３×１０－３—３．２×１０－３。由此可见,层结的影响使它们的变化大于其它海区的结果。在ｕ１０＝０－１０ｍ／ｓ范围内,中性化整体交换系数平均为ＣＤＮ＝１．２×１０－３,ＣＨＮ＝１．１４×１０－３,ＣＥＮ＝１．１９×１０－３,与Ｌａｒｇｅ和Ｐｏｎｄ（１９８１,１９８２）不稳定条件的研究结果相差无几。 相似文献
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农田植被层上方湍流通量输送特征分析 总被引：6，自引：0，他引：6
根据宵田植被层上方的温湿风梯度观测资料,采用基于莫宁－奥布霍夫相似理论的廓线梯度法计算了农田植被层上方的湍流通量,进而确定出拖曳系数、斯坦顿数和道尔顿数。文中检验了用于农田植被层上方湍流通量计算的普适函数的适用性,讨论了湍流通量以及拖曳系数等随稳定度参数、粗糙度高、平均风速等因子的变化规律。结果表明,农田植被层上方的湍流通量随层结构稳定度变化而变化;拖曳系数、斯坦顿数和道尔顿数也不是常数,而是层结 相似文献
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应用含湍流频散效应的近地面层的运动方程求解了不同层结下的风速廓线，着重分析了湍流频散效应对近地面层平稳运动的影响。分析指出：湍流的频散效应对经典的幂律廓线一对数修正，该修正在不稳定层结时比稳定层时明显；利用相似理论也得到了该常数。 相似文献
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西太平洋热带海域湍流通量以及海面粗糙度和曳力系数的观测研究 总被引：2，自引：0，他引：2
本文利用1987年西太平洋热带海域考察期间系留气艇所取得的廓线资料,用相似理论半经验的通量-廓线关系,给出这一海域的湍流热通量和动量通量,并且对海面粗糙度长度Z_0,曳力系数C_D及其与风速的关系等作了初步的研究,给出了一些经验公式,并与其他研究者的研究结果作了比较。 相似文献
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本文利用1987年西太平洋热带海域考察期间系留气艇所取得的廓线资料,用相似理论半经验的通量-廓线关系,给出这一海域的湍流热通量和动量通量,并且对海面粗糙度长度Z_0,曳力系数C_D及其与风速的关系等作了初步的研究,给出了一些经验公式,并与其他研究者的研究结果作了比较。 相似文献
8.
近海层大气湍流通量系数研究 总被引：1，自引：0，他引：1
根据１９９４年９月１８～３０日南沙群岛海域渚碧礁的近海面大气湍流观测实验资料,分别计算了该海域光滑海面和粗糙海面上的空气动力粗糙度（ｚ０ ）、中性曳力系数（ Ｃ Ｄ Ｎ）。利用 Ｂｕｔｓａｅｒｔ 的假定,推导了求取标量粗糙度（ｚ Ｔ、ｚ Ｑ）、整体输送系数（感热交换系数 Ｃ Ｈ Ｎ、水汽交换系数 Ｃ Ｅ Ｎ ）的一组公式。在此基础上,分别计算和分析了该海域光滑海面和粗糙海面上空气动力粗糙度（ｚ０ ）、标量粗糙度（ｚ Ｔ、ｚ Ｑ ）、中性曳力系数（ Ｃ Ｄ Ｎ）、整体输送系数（感热交换系数 Ｃ Ｈ Ｎ、水汽交换系数 Ｃ Ｅ Ｎ）及其关于水平风速分量的分布,并得到了一些有益的结论。 相似文献
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湍流频散对边界层风廓线的影响 总被引：2，自引：0，他引：2
应用包括湍流粘性和频散的新的Reynolds平均动量方程，分析了边界层的垂直风速廓线，发现包含湍流频散的地面层的风速廓线对经典的风廓线指数规律有一个对数规律的修改；而且在不稳定层结下比在稳定层结下，湍流的频散效应更为显；在中性条件下，指数规律退化为对数规律并且Karman常数被另外一个常数所代替，而这个新常数也可以通过相似理论来获得。 相似文献
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A theory for the scalar roughness and the scalar transfer coefficients over snow and sea ice 总被引：1，自引：0，他引：1
Edgar L. Andreas 《Boundary-Layer Meteorology》1987,38(1-2):159-184
Although the bulk aerodynamic transfer coefficients for sensible (C
H
) and latent (C
E
) heat over snow and sea ice surfaces are necessary for accurately modeling the surface energy budget, they have been measured rarely. This paper, therefore, presents a theoretical model that predicts neutral-stability values of C
H
and C
E
as functions of the wind speed and a surface roughness parameter. The crux of the model is establishing the interfacial sublayer profiles of the scalars, temperature and water vapor, over aerodynamically smooth and rough surfaces on the basis of a surface-renewal model in which turbulent eddies continually scour the surface, transferring scalar contaminants across the interface by molecular diffusion. Matching these interfacial sublayer profiles with the semi-logarithmic inertial sublayer profiles yields the roughness lengths for temperature and water vapor. When coupled with a model for the drag coefficient over snow and sea ice based on actual measurements, these roughness lengths lead to the transfer coefficients. C
E
is always a few percent larger than CH. Both decrease monotonically with increasing wind speed for speeds above 1 m s–1, and both increase at all wind speeds as the surface gets rougher. Both, nevertheless, are almost always between 1.0 × 10–3 and 1.5 × 10–3. 相似文献
12.
In an earlier paper by one of the authors (Smith, 1968), a momentum integral method was developed to parameterize the gross
constraint imposed by the surface boundary layer of a steady, axisymmetric, tropical cyclone on the meridional circulation
within the vortex itself. Specifically, the method provides an effective means of estimating the radial variation of mean
upflow/downflow induced by the boundary layer, compatible with a prescribed radial variation of azimuthal velocity just above
the boundary layer,V
gr. However, it relies on a judicious choice of vertical profiles of radial and azimuthal velocity components within the boundary
layer. An especially suitable set of profiles is discussed herein; these are Ekman-like profiles in which turbulent mixing
is characterized by a vertically constant eddy diffusivityK
M
, matched to a constant stress sublayer just above the sea surface. An attractive feature of the formulation is that a suitable
value forK
M
as a function of radius, which is extremely difficult to extract from observational data, can be calculated when the state
of the sea surface, described by a roughness lengthZ
0, is prescribed. Although observations ofZ
0 at high wind speeds are not yet available, the effect of radial variations in sea surface roughness can be assessed and it
is shown that these affect the upflow to a significant degree. 相似文献
13.
John L. Walmsley 《大气与海洋》2013,51(2):203-233
Abstract In October 1985, the Boundary‐Layer Research Division of the Atmospheric Environment Service conducted an experiment on Sable Island, Nova Scotia, where 10‐m wind measurements were made at a number of locations. Wind data were also collected at 4 levels on one of the 10‐m masts and at 6 levels on a 26‐m mast, both located on the South Beach. Other data used in the present study consisted of air temperature measured at 9 m and sea temperature measured at the beach. The theory for wind speed and temperature profiles over the sea is reviewed. A method of deriving over‐sea profile parameters (u*, θ*, Z0, L) from wind data at one level and the air‐sea temperature difference is described. The method is limited to applications either over homogeneous open ocean or, provided measurements are taken above the internal boundary layer generated by the change of roughness at the coastline, over a flat beach (without coastal orography). The heights at which the method is applied must be within the surface layer which must not have any discontinuities in wind speed or temperature in the vertical, such as are often associated with inversion layers. An application to data collected at beach sites in onshore flow during the October 1985 experiment is illustrated. Once the above parameters are obtained, theoretical wind profiles may be computed and compared with observed profiles. In order to make a proper comparison it is essential to account for internal boundary layers generated at the shoreline by the step‐change in surface roughness. Only the data measured above the internal boundary layer are representative of over‐sea conditions and may, therefore, be used for verifying the theoretical profiles. The agreement between calculated and measured data is generally very good. One complication, however, is a slight upstream‐blockage effect due to a 7‐m high dune located about 140 m downwind of the 26‐m mast. Estimates of the magnitude of this effect partially account for small discrepancies in the results at the 26‐ and 10‐m mast locations. An estimation of the most probable errors in the calculated parameters, based on assumed measurement errors, is included in the computer program. Results suggest that small measurement errors can explain the above discrepancies. 相似文献
14.
Wind speed and temperature profiles to a height of 8 m were recorded for 30-, 60-, and 90-min averaging times over a striated snow surface at the geographic South Pole during the austral winter of 1975. A gradient Richardson number was calculated for each averaging time to determine conditions of neutral stability under which the logarithmic wind law would hold. A log-linear regression technique was used to determine values of aerodynamic roughness height (Z
0) for those profile averages recorded in conditions of neutral stability. A plot of Z
0 as a function of average wind direction revealed a variation in Z
0 of almost three orders of magnitude, from 0.01 to 7 cm, over 120 deg of wind direction. A simple model is presented to justify the fact that aerodynamic roughness is a function of wind direction and erosion history. 相似文献
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Air-sea bulk transfer coefficients in diabatic conditions 总被引：13，自引：0，他引：13
Junsei Kondo 《Boundary-Layer Meteorology》1975,9(1):91-112
On the basis of recent data for the roughness Reynolds number of the sea surface, and using the Owen-Thomson theory on the transfers of heat and mass between a rough surface and the flow above it, the bulk transfer coefficients of the sea surface have been estimated. For a reference height of 10 m, the neutral-lapse transfer coefficient for water vapor is larger by only a few percent than that for sensible heat. When the wind speed at the 10-m height is u
10>3 m s–1, the coefficient for sensible heat C
H
is larger by about 10% than that for momentum C
D
. For u
10<5 m s–1, however, the value of C
D
exceeds the value of C
H
, and for u
10=15 m s–1 it is shown that C
H
0.8C
D
. It may be also proposed that 103
C
D
=1.11 to 1.70, 103
C
E
=1.18 to 1.30, and 103
C
H
=1.15 to 1.26 for a range of u
10=4 to 20 m s–1. A plot of diabatic transfer coefficients versus wind speed is obtained by using a parameter of the sea-air temperature difference. For practical purposes, the coefficients are approximated by empirical formulae. 相似文献
16.
The surface flux calculation method proposed by Louis (1979) is extended by allowing momentum and heat to have different roughness lengths (z
0 andz
T respectively). Our approach is to extend the traditional analysis by a more careful consideration of potential temperature structure near the surface. This consideration leads to a redefinition of the bulk Richardson number. For bulk transfer coefficients, our method shows a significant improvement over the original Louis method when compared with the theoretical surface-layer model applied to rough surfaces. Numerical experiments simulating sea breezes in 2D show that our extension is crucially important in simulating light wind and low humidity conditions. 相似文献
17.
Koen De Ridder 《Boundary-Layer Meteorology》2010,134(2):257-267
In the roughness sublayer (RSL), Monin–Obukhov surface layer similarity theory fails. This is problematic for atmospheric
modelling applications over domains that include rough terrain such as forests or cities, since in these situations numerical
models often have the lowest model level located within the RSL. Based on empirical RSL profile functions for momentum and
scalar quantities, and scaling the height with the RSL height z
*, we derive a simple bulk transfer relation that accounts for RSL effects. To verify the validity of our approach, these relations
are employed together with wind speed and temperature profiles measured over boreal forest during the BOREAS experimental
campaign to estimate momentum and heat fluxes. It is demonstrated that, when compared with observed flux values, the inclusion
of RSL effects in the transfer relations yields a considerable improvement in the estimated fluxes. 相似文献
18.
Wilfried Brutsaert 《Boundary-Layer Meteorology》1979,16(4):365-388
A differential equation is obtained to describe the concentration of passive admixtures (water vapor, sensible heat, pollutants, CO2, etc.) of turbulent flow inside a dense and uniform vegetational canopy. The profiles of eddy diffusivity, wind speed and shear stress are assumed to be exponential decay functions of depth below the top of the canopy. This equation is solved for the case of a vegetation with constant concentration of the admixture at the foliage surfaces. The solution is used to formulate bulk mass or heat transfer coefficients, which can be applied to practical problems involving surfaces covered with a vegetation or with similar porous or fibrous roughness elements. The results are shown to be consistent with experimental data presented by Chamberlain (1966), Garratt and Hicks (1973) and Garratt (1978). Calculations with the model illustrate that, as compared to its behavior over surfaces with bluff roughness elements, ln(z
0/z
0c
) (wherez
0 is the momentum roughness andz
0c
, the scalar roughness) for permeable roughness elements is relatively insensitive tou
* and practically independent ofz
0. 相似文献
19.
An analysis tool for the study of wind speed profiles over the water has been developed. The profiles are analysed using a
modified dimensionless wind speed and dimensionless height, assuming that the sea surface roughness can be predicted by Charnock’s
roughness length model. In this form, the roughness dependency on wind speed is extracted and the variations on the wind profile
are due solely to atmospheric stability. The use of the Charnock’s non-dimensional wind profile is illustrated using data
collected from a meteorological mast installed in the Danish North Sea. The best fit with the observed mean non-dimensional
wind profile under neutral atmospheric conditions is found using a value of 1.2 × 10−2 for Charnock’s parameter. The stability correction on the neutral wind profile suggested by the Businger-Dyer relations was
found to perform well over the sea. 相似文献
20.
M. Segal 《Boundary-Layer Meteorology》1990,52(1-2):193-198
Calculations are made of the effects of thermal stability under a range of conditions, over the sea and land, on the physical factors (including the critical wind speed) affecting dust-storm generation, snow drift, and rough sea conditions. The computational procedure involves the surface friction velocity, u
*, and its relation with the aerodynamic roughness over aerodynamically rough, mobile surfaces. The results indicated that even at relatively high wind speeds, thermal effects under extreme advection situations may be significant, particularly for those properties of the agitated surface dependent on u
*
3 and u
*
4. 相似文献