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1.
Turbulence Intensity Parameters over a Very Complex Terrain 总被引:1,自引:1,他引:0
Cintya A. Martins Osvaldo L. L. Moraes Otávio C. Acevedo Gervásio A. Degrazia 《Boundary-Layer Meteorology》2009,133(1):35-45
Detailed knowledge of turbulence structure is important for the understanding of atmospheric phenomena in the boundary layer,
especially over complex terrain. In the present study, turbulence intensity parameters are analyzed for different conditions
regarding stability, wind speed and wind direction over a mountainous region. The purpose of the analysis is to verify whether
the observed parameters follow Monin–Obukhov similarity theory (MOST), despite the terrain heterogeneity. The dataset was
collected during an experimental campaign at the Nova Roma do Sul site, in southern Brazil, with a micrometeorological tower
located near a sharp slope, approximately 400 m high. The results show that the normalized standard deviations of the vertical
velocity component as well as the normalized standard deviation of temperature follow Monin–Obukhov similarity for all stability
regimes, regardless of the wind direction. However the normalized standard deviation of the horizontal components of the turbulent
velocity obeys the similarity relationship only for a limited range of the stability parameters. 相似文献
2.
The Near-Calm Stable Boundary Layer 总被引:3,自引:3,他引:0
Larry Mahrt 《Boundary-Layer Meteorology》2011,140(3):343-360
For the near-calm stable boundary layer, nominally 2-m mean wind speed <0.5 ms−1, the time-average turbulent flux is dominated by infrequent mixing events. These events are related to accelerations associated
with wave-like motions and other more complex small-scale motions. In this regime, the relationship between the fluxes and
the weak mean flow breaks down. Such near-calm conditions are common at some sites. For very weak winds and strong stratification,
the characteristics of the fluctuating quantities change slowly with increasing scale and the separation between the turbulence
and non-turbulent motions can become ambiguous. Therefore, a new analysis strategy is developed based on the scale dependence
of selected flow characteristics, such as the ratio of the fluctuating potential energy to the kinetic energy. In contrast
to more developed turbulence, correlations between fluctuating quantities are small, and a significant heat flux is sometimes
carried by very weak vertical motions with large temperature fluctuations. The relation of the flux events to small-scale
increases of wind speed is examined. Large remaining uncertainties are noted. 相似文献
3.
L. Zubair 《Theoretical and Applied Climatology》2002,71(1-2):119-127
Summary Hourly measurements of surface winds at Sita Eliya (6° 58′ N, 80° 46′ E, 1860 m a.s.l.) located atop the North-South mountain ridge in Sri Lanka were analyzed to investigate the diurnal and seasonal variation
in the wind climate. Surface winds are dominated by the monsoon regimes, with Northeasterlies from November to January, Southwesterlies
from February to May and Westerlies and Northwesterlies from June to October. Through most of the year, the average wind speed
is around 6–8 m/s. However from June to August, it is around 10–14 m/s. Wind in June is gusty due the location of the low-level
Easterly jet over Sri Lanka. The wind undergoes a reversal in both zonal and meridional directions in March and November coincident
with the migration of the Inter-Tropical Convergence Zone. Notwithstanding the period from May to September being designated
as the Southwest monsoon, the wind is from West, South-West-West and North-North-West. During the Southwest monsoon, wind
speed during the night is nearly as high as that during the day. This anomalous diurnal variation in wind speeds may be related
to orographic influences. The high wind speeds at Sita Eliya, in conjunction with the moderate diurnal and seasonal variability
in wind speed, is suitable for wind-energy generation.
Received January 2, 2001 Revised May 26, 2001 相似文献
4.
Young-Hee Lee 《Asia-Pacific Journal of Atmospheric Sciences》2012,48(3):243-252
We have analyzed eddy covariance data collected within open canopy to investigate the influence of non-flat terrain and wind direction shear on the canopy turbulence. The study site is located on non-flat terrain with slopes in both south-north and east-west directions. The surface elevation change is smaller than the height of roughness element such as building and tree at this site. A variety of turbulent statistics were examined as a function of wind direction in near-neutral conditions. Heterogeneous surface characteristics results in significant differences in measured turbulent statistics. Upwind trees on the flat and up-sloping terrains yield typical features of canopy turbulence while upwind elevated surface with trees yields significant wind direction shear, reduced u and w skewness, and negligible correlation between u and w. The directional dependence of turbulence statistics is due that strong wind blows more horizontally rather than following terrain, and hence combination of slope related momentum flux and canopy eddy motion decreases the magnitude of Sk w and r uw for the downslope flow while it enhances them for the upslope flow. Significant v skewness to the west indicates intermittent downdraft of northerly wind, possibly due to lateral shear of wind in the presence of significant wind direction shear. The effects of wind direction shear on turbulent statistics were also examined. The results showed that correlation coefficient between lateral velocities and vertical velocity show significant dependence on wind direction shear through change of lateral wind shear. Quadrant analysis shows increased outward interaction and reduced role of sweep motion for longitudinal momentum flux for the downslope flow. Multi-resolution analysis indicates that uw correlation shows peak at larger averaging time for the upslope flow than for the downslope flow, indicating that large eddy plays an active role in momentum transfer for the upslope flow. On the other hand, downslope flow shows larger velocity variances than other flows despite similar wind speed. These results suggest that non-flatness of terrain significantly influences on canopy-atmosphere exchange. 相似文献
5.
Variability of Sub-Canopy Flow,Temperature, and Horizontal Advection in Moderately Complex Terrain 总被引:1,自引:1,他引:0
We examine the space–time structure of the wind and temperature fields, as well as that of the resulting spatial temperature
gradients and horizontal advection of sensible heat, in the sub-canopy of a forest with a dense overstorey in moderately complex
terrain. Data were collected from a sensor network consisting of ten stations and subject to orthogonal decomposition using
the multiresolution basis set and stochastic analyses including two-point correlations, dimensional structure functions, and
various other bulk measures for space and time variability. Despite some similarities, fundamental differences were found
in the space–time structure of the motions dominating the variability of the sub-canopy wind and temperature fields. The dominating
motions occupy similar spatial, but different temporal, scales. A conceptual space–time diagram was constructed based on the
stochastic analysis that includes the important end members of the spatial and temporal scales of the observed motions of
both variables. Short-lived and small-scale motions govern the variability of the wind, while the diurnal temperature oscillation
driven by the surface radiative transfer is the main determinant of the variability in the temperature signal, which occupies
much larger time scales. This scale mismatch renders Taylor’s hypothesis for sub-canopy flow invalid and aggravates the computation
of meaningful estimates of horizontal advective fluxes without dense spatial information. It may further explain the ambiguous
and inconclusive results reported in numerous energy and mass balance and advection studies evaluating the hypothesis that
accounting for budget components other than the change in storage term and the vertical turbulent flux improves the budget
closure when turbulent diffusion is suppressed in plant canopies. Estimates of spatial temperature gradients and advective
fluxes were sensitive to the network geometry and the spatial interpolation method. The assumption of linear spatial temperature
gradients was not supported by the results, and leads to increased spatial and temporal variability of inferred spatial gradients
and advection estimates. A method is proposed to estimate the appropriate minimum network size of wind and temperature sensors
suitable for an evaluation of energy and mass balances by reducing spatial and temporal variability of the spatially sampled
signals, which was estimated to be on the order of 200 m at the study site. 相似文献
6.
Ann-Sofi Smedman 《Boundary-Layer Meteorology》1988,44(3):231-253
Boundary-layer measurements conducted at the Marsta site in Sweden from a winter-time situation (23–25 Feb.) with stable stratification have been analysed. The data comprise wind and temperature profile measurements up to 30 m, turbulence measurements at 2, 6 and 30 m and Doppler acoustic sounder data up to about 150 m. The upwind fetch at the site is flat and free from obstacles to a distance of ca 5 km for the particular sector chosen for the experiment.During the night, a two-layer vertical structure developed. Analysis of power spectra, co-spectra and variances in a shallow and very stable turbulent boundary layer near the ground show that the turbulence is fully developed and follow the universal behaviour.Above, at a height of 30 m, another turbulent layer is produced by increased wind shear near a low-level jet. This turbulent upper layer can be regarded as a layer of free shear flow. At this height, there also exist wave-turbulence interactions at low frequencies which sometimes cause a countergradient heat flux. 相似文献
7.
étude expérimentale de la couche limite au-dessus d'un relief modéré proche d'une chaîne de montagne
A. Druilhet J. Noilhan B. Benech G. Dubosclard D. Guedalia J. Frangi 《Boundary-Layer Meteorology》1983,25(1):3-16
For the heterogeneous site described in the first part, some aspects of the turbulent structure of the planetary boundary layer are studied. Using mixed-layer scaling, the normalized profiles are compared with those obtained over flat terrain during convective conditions. The measurements were made with the same instrumented aircraft at both sites. The dissipative and spectral length scales are smaller over complex terrain within the whole boundary layer. This is due to the shifting of the wavelength peak toward the high frequencies by dynamic turbulence.This last effect can also explain the increase of the dissipation rate over the heterogeneous site during strong wind conditions. The vertical profiles of sensible heat flux and temperature-water vapor correlation show a lack of entrainment process at the top of the boundary layer. This fact suggests that the investigated boundary layer is advected from the neighbouring plain over the complex site (plateau de Lannemezan). 相似文献
8.
Aircraft turbulence data from the Autonomous Ocean Sampling Network project were analyzed and compared to the Coupled Ocean–Atmosphere
Response Experiment (COARE) bulk parametrization of turbulent fluxes in an ocean area near the coast of California characterized
by complex atmospheric flow. Turbulent fluxes measured at about 35 m above the sea surface using the eddy-correlation method
were lower than bulk estimates under unstable and stable atmospheric stratification for all but light winds. Neutral turbulent
transfer coefficients were used in this comparison because they remove the effects of mean atmospheric conditions and atmospheric
stability. Spectral analysis suggested that kilometre-scale longitudinal rolls affect significantly turbulence measurements
even near the sea surface, depending on sampling direction. Cross-wind sampling tended to capture all the available turbulent
energy. Vertical soundings showed low boundary-layer depths and high flux divergence near the sea surface in the case of sensible
heat flux but minimal flux divergence for the momentum flux. Cross-wind sampling and flux divergence were found to explain
most of the observed discrepancies between the measured and bulk flux estimates. At low wind speeds the drag coefficient determined
with eddy correlation and an inertial dissipation method after corrections were applied still showed high values compared
to bulk estimates. This discrepancy correlated with the dominance of sea swell, which was a usually observed condition under
low wind speeds. Under stable atmospheric conditions measured sensible heat fluxes, which usually have low values over the
ocean, were possibly affected by measurement errors and deviated significantly from bulk estimates. 相似文献
9.
The scintillation method tested over a dry vineyard area 总被引:8,自引:1,他引:8
H. A. R. De Bruin B. J. J. M. Van Den Hurk W. Kohsiek 《Boundary-Layer Meteorology》1995,76(1-2):25-40
Measurements of a scintillometer device mounted at 4 m above a dry vineyard area in La Mancha, Spain, are used to obtain an average sensible heat flux densityH. Averaging is over a rectangular area determined by the distance between the scintillometer light source and receptor (875 m) and some upwind distance governed by the horizontal wind speed perpendicular to that line. Using similarity relations obtained from La Crau, a good correspondence betweenH measured with the scintillometer and an eddy-correlation device in the centre of a vineyard is obtained. The friction velocityu
* was either measured directly using a sonic anemometer or obtained indirectly from two wind speeds and known values of the roughness length zo and displacementd. The free convection formulation underestimates the sensible heat flux by about 30%. This is due to a significant contribution of mechanically generated turbulence to the total turbulent transport, which was caused by relatively strong winds and rough terrain. 相似文献
10.
Ben Yang Yun Qian Larry K. Berg Po-Lun Ma Sonia Wharton Vera Bulaevskaya Huiping Yan Zhangshuan Hou William J. Shaw 《Boundary-Layer Meteorology》2017,162(1):117-142
We evaluate the sensitivity of simulated turbine-height wind speeds to 26 parameters within the Mellor–Yamada–Nakanishi–Niino (MYNN) planetary boundary-layer scheme and MM5 surface-layer scheme of the Weather Research and Forecasting model over an area of complex terrain. An efficient sampling algorithm and generalized linear model are used to explore the multiple-dimensional parameter space and quantify the parametric sensitivity of simulated turbine-height wind speeds. The results indicate that most of the variability in the ensemble simulations is due to parameters related to the dissipation of turbulent kinetic energy (TKE), Prandtl number, turbulent length scales, surface roughness, and the von Kármán constant. The parameter associated with the TKE dissipation rate is found to be most important, and a larger dissipation rate produces larger hub-height wind speeds. A larger Prandtl number results in smaller nighttime wind speeds. Increasing surface roughness reduces the frequencies of both extremely weak and strong airflows, implying a reduction in the variability of wind speed. All of the above parameters significantly affect the vertical profiles of wind speed and the magnitude of wind shear. The relative contributions of individual parameters are found to be dependent on both the terrain slope and atmospheric stability. 相似文献
11.
Turbulence data collected over a total of 25 days during two summers are used to describe processes responsible for the nonstationarity
of turbulent sensible heat fluxes at Summit, Greenland. A stationarity test shows that about 40% of the data are classified
as nonstationary. Three main factors are explored to account for the large fraction of nonstationary runs: (1) intermittency
of turbulence in stable conditions, (2) changes in net all-wave radiation in response to cloud forcing, and (3) diurnal trends
in stability. A classification procedure that accounts for the intermittent nature of turbulence shows that during stable,
nonstationary conditions 50% of the total sensible heat flux is realized in 22% of the sampling time. Intermittency often
occurs at Summit during periods characterized by weak and irregular horizontal winds in combination with strong stability.
Rapid changes in net all-wave radiation in response to cloud forcing results in nonstationarity during unstable conditions.
Between 0930–1130 and 1900–1930 UTC turbulent heat fluxes are not only small in magnitude but also typically change sign,
with nonstationarity during these periods often as high as 65%. These results should help resolve some of the present uncertainties
in obtaining reliable fluxes at this site, in particular under stable atmospheric conditions. 相似文献
12.
Effects of Thermal Stability and Incoming Boundary-Layer Flow Characteristics on Wind-Turbine Wakes: A Wind-Tunnel Study 总被引:2,自引:1,他引:1
Wind-tunnel experiments were carried out to study turbulence statistics in the wake of a model wind turbine placed in a boundary-layer
flow under both neutral and stably stratified conditions. High-resolution velocity and temperature measurements, obtained
using a customized triple wire (cross-wire and cold wire) anemometer, were used to characterize the mean velocity, turbulence
intensity, turbulent fluxes, and spectra at different locations in the wake. The effect of the wake on the turbulence statistics
is found to extend as far as 20 rotor diameters downwind of the turbine. The velocity deficit has a nearly axisymmetric shape,
which can be approximated by a Gaussian distribution and a power-law decay with distance. This decay in the near-wake region
is found to be faster in the stable case. Turbulence intensity distribution is clearly non-axisymmetric due to the non-uniform
distribution of the incoming velocity in the boundary layer. In the neutral case, the maximum turbulence intensity is located
above the hub height, around the rotor tip location and at a distance of about 4–5.5 rotor diameters, which are common separations
between wind turbines in wind farms. The enhancement of turbulence intensity is associated with strong shear and turbulent
kinetic energy production in that region. In the stable case, the stronger shear in the incoming flow leads to a slightly
stronger and larger region of enhanced turbulence intensity, which extends between 3 and 6 rotor diameters downwind of the
turbine location. Power spectra of the streamwise and vertical velocities show a strong signature of the turbine blade tip
vortices at the top tip height up to a distance of about 1–2 rotor diameters. This spectral signature is stronger in the vertical
velocity component. At longer downwind distances, tip vortices are not evident and the von Kármán formulation agrees well
with the measured velocity spectra. 相似文献
13.
Stuart Bradley Yvette Perrott Paul Behrens Andy Oldroyd 《Boundary-Layer Meteorology》2012,143(1):37-48
The quality of lidar and sodar wind estimates is generally judged through comparisons with mast-mounted instruments, and the
resulting regressions. Evaluation of the relative merits of lidars versus sodars is complicated by the fact that lidars are
generally placed close to a mast whereas sodars are generally placed some distance from a mast so that acoustic reflections
off the mast are reduced. This leads to the two technologies, lidar and sodar, not being compared in similar situations. Differences
arising from the two geometries can be expected to be larger in complex terrain, where the wind regime can vary significantly
spatially. The current work explores these differences in moderately complex terrain. Lidar–mast comparisons are performed
with the lidar close to an 80 m mast, and sodar–mast comparisons performed with the sodar 300 m from the mast. Systematic
variations in estimated wind speed are found to occur with height, consistent with predictions from a simple flow model. When
the lidar was moved to the sodar location, further from the mast, there were significant changes in the estimated wind speeds
and a reduction in correlation with the mast-based wind speeds, as expected. However, the correlation between collocated lidar and sodar winds was high. This finding emphasizes that any comparison of two remote sensing instruments needs to be
through similar experiments, and that differences in accuracy often reported for the lidar and sodar technologies are likely
to be contaminated due to poor comparison configurations. A method was devised to simulate the sodar being collocated with
the mast, by using the lidar–sodar measurements and the lidar–mast measurements. It was found that there was then no statistically
detectable difference between lidar–mast regressions and sodar–mast regressions for the particular lidar and sodar tested.
Both remote sensing instruments were also found to be good estimators of Weibull parameters, as compared with those derived
from mast data. The conclusion is that the sodar measured the winds above the sodar with a similar accuracy to the lidar measuring
winds above the lidar. 相似文献
14.
15.
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
16.
Hiroshi Takimoto Ayumu Sato Janet F. Barlow Ryo Moriwaki Atsushi Inagaki Shiho Onomura Manabu Kanda 《Boundary-Layer Meteorology》2011,140(2):295-314
We investigate the spatial characteristics of urban-like canopy flow by applying particle image velocimetry (PIV) to atmospheric
turbulence. The study site was a Comprehensive Outdoor Scale MOdel (COSMO) experiment for urban climate in Japan. The PIV
system captured the two-dimensional flow field within the canopy layer continuously for an hour with a sampling frequency
of 30 Hz, thereby providing reliable outdoor turbulence statistics. PIV measurements in a wind-tunnel facility using similar
roughness geometry, but with a lower sampling frequency of 4 Hz, were also done for comparison. The turbulent momentum flux
from COSMO, and the wind tunnel showed similar values and distributions when scaled using friction velocity. Some different
characteristics between outdoor and indoor flow fields were mainly caused by the larger fluctuations in wind direction for
the atmospheric turbulence. The focus of the analysis is on a variety of instantaneous turbulent flow structures. One remarkable
flow structure is termed ‘flushing’, that is, a large-scale upward motion prevailing across the whole vertical cross-section
of a building gap. This is observed intermittently, whereby tracer particles are flushed vertically out from the canopy layer.
Flushing phenomena are also observed in the wind tunnel where there is neither thermal stratification nor outer-layer turbulence.
It is suggested that flushing phenomena are correlated with the passing of large-scale low-momentum regions above the canopy. 相似文献
17.
High-Resolution Fibre-Optic Temperature Sensing: A New Tool to Study the Two-Dimensional Structure of Atmospheric Surface-Layer Flow 总被引:1,自引:0,他引:1
Christoph K. Thomas Adam M. Kennedy John S. Selker Ayla Moretti Martin H. Schroth Alexander R. Smoot Nicholas B. Tufillaro Matthias J. Zeeman 《Boundary-Layer Meteorology》2012,142(2):177-192
We present a novel approach based on fibre-optic distributed temperature sensing (DTS) to measure the two-dimensional thermal
structure of the surface layer at high resolution (0.25 m, ≈0.5 Hz). Air temperature observations obtained from a vertically-oriented
fibre-optics array of approximate dimensions 8 m × 8 m and sonic anemometer data from two levels were collected over a short
grass field located in the flat bottom of a wide valley with moderate surface heterogeneity. The objectives of the study were
to evaluate the potential of the DTS technique to study small-scale processes in the surface layer over a wide range of atmospheric
stability, and to analyze the space–time dynamics of transient cold-air pools in the calm boundary layer. The time response
and precision of the fibre-based temperatures were adequate to resolve individual sub-metre sized turbulent and non-turbulent
structures, of time scales of seconds, in the convective, neutral, and stable surface layer. Meaningful sensible heat fluxes
were computed using the eddy-covariance technique when combined with vertical wind observations. We present a framework that
determines the optimal environmental conditions for applying the fibre-optics technique in the surface layer and identifies
areas for potentially significant improvements of the DTS performance. The top of the transient cold-air pool was highly non-stationary
indicating a superposition of perturbations of different time and length scales. Vertical eddy scales in the strongly stratified
transient cold-air pool derived from the DTS data agreed well with the buoyancy length scale computed using the vertical velocity
variance and the Brunt–Vaisala frequency, while scales for weak stratification disagreed. The high-resolution DTS technique
opens a new window into spatially sampling geophysical fluid flows including turbulent energy exchange. 相似文献
18.
R. E. Mickle N. J. Cook A. M. Hoff N. O. Jensen J. R. Salmon P. A. Taylor G. Tetzlaff H. W. Teunissen 《Boundary-Layer Meteorology》1988,43(1-2):143-169
This is one of a series of papers on the Askervein Hill Project. It presents results from the Askervein 1982 and 1983 experiments
in the form of vertical profiles of mean wind and turbulence integral statistics at upwind reference locations and at two
hilltop sites. The data were obtained from a variety of sensors including sonic, Gill UVW and cup anemometers mounted on 50,
30, 17 and 10 m towers and TALA kite systems. Comparisons with numerical-model predictions are discussed. 相似文献
19.
Impact of Sea-Spray on the Atmospheric Surface Layer 总被引:1,自引:0,他引:1
The feedback effects of sea-spray on the heat and momentum fluxes under equilibrium conditions associated with winds of tropical
cyclones are investigated using a one-dimensional coupled sea-spray and atmospheric surface-layer (ASL) model. This model
is capable of simulating the microphysical aspects of the evaporation of saline water droplets of various sizes and their
dynamic and thermal interaction with the turbulence mixing that is simulated by the Mellor–Yamada 1.5-order closure scheme.
Sea-spray droplet generation is described by a state-of-the-art parametrization that predicts the size spectrum of sea-spray
droplets for a given surface forcing. The results from a series of simulations indicate the way in which evaporating droplets
of various sizes modify the turbulence mixing near the surface, which in turn affects further droplet evaporation. All these
results are direct consequences of the effects of sea-spray on the balance of turbulent kinetic energy in the spray-filled
surface layer. In particular, the overall impact of sea-spray droplets on the mean wind depends on the wind speed at the level
of sea-spray generation. When the wind speed is below 40 m s−1, the droplets are small in size and tend to evaporate substantially and thus cool the spray-filled layer, while for wind
speeds above 50 m s−1, the size of the droplets is so large that they do not have enough time to evaporate much before falling back into the sea.
The sensible heat carried by the droplets is released to the ambient air, increasing the buoyancy of the surface layer and
enhancing the turbulent mixing. The suspension of sea-spray droplets reduces the buoyancy and makes the surface layer more
stable, decreasing the friction velocity and the downward turbulent mixing of momentum. The results from the numerical experiments
also suggest that, in order not to violate the constant flux assumption critical to the Monin–Obukhov similarity theory, a
displacement equal to the mean wave height should be included in the logarithmic profiles of the wind and thermal fields. 相似文献
20.
Two mathematical models are proposed detailing the influence of ocean spray on vertical momentum transport under high-wind
conditions associated with a hurricane or severe storm. The first model is based on a turbulent kinetic energy (TKE) equation
and accounts for the so-called lubrication effect due to the reduction of turbulence intensity. The second model is based
on Monin–Obukhov similarity (MOS) and uses available experimental data. It is demonstrated that the flow acceleration is negligible
for wind speeds below a certain critical value due to the fact that the spray volume concentration is low for such speeds.
For wind speeds higher than the critical value, the spray concentration rapidly increases, which results in significant flow
acceleration. Both models produce qualitatively similar results for all turbulent flow parameters considered. It was found
that the MOS-based model tends to predict a noticeably stronger lubrication effect than the TKE-based model, especially for
lower wind speeds. The results of model calculations are in very good agreement with available experimental data for the spray
production values near the upper bound. It is also shown that neither the value of the turbulent Schmidt number in the TKE-based
model nor the choice of a stability profile function affects the spray-laden flow dynamics significantly. 相似文献