submeso motions
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Atmosphere ◽  
2021 ◽  
Vol 12 (9) ◽  
pp. 1095
Author(s):  
Mauro Mazzola ◽  
Angelo Pietro Viola ◽  
Taejin Choi ◽  
Francesco Tampieri

The availability of 5-year time series of velocity and temperature data from two sonic anemometers installed at Jang Bogo Station, Antarctica, allowed a systematic investigation of the turbulence features in a stable layer affected by submeso motions and characterized by the vertical divergence of some second-order moments for a large fraction of time (quite a non-ideal surface layer). The investigation of the effect of the averaging time interval on the statistics of the second-order moments showed that this is greater for the variances of the velocity components with respect to that for the vertical fluxes. This corresponds to a greater contribution from low-frequency motions. The turbulence statistics were investigated and compared with current literature results in terms of vertical structure, share of energy between horizontal and vertical components, skewness of the vertical velocity and turbulent velocities. As a general result, all the normalized second-order moments show a clear change passing from neutral to stable conditions, passing through the range of bulk Richardson number equal to 0.1–1.


2021 ◽  
Author(s):  
Luca Mortarini ◽  
Cléo Quaresma Dias-Júnior ◽  
Otavio Acevedo ◽  
Pablo Oliveira ◽  
Daiane Brondani ◽  
...  

<p>This study provides a detailed analysis of the influence of atmospheric stratification on the flow dynamics above and within a dense forest for a 19-days campaign at the Amazon Tall Tower Observatory (ATTO) site. Observations taken at seven levels within and above the forest along an 81-meter and a 325-meter towers allow a unique investigation of the vertical evolution of the turbulent field in the roughness sublayer and in the surface layer above it.</p><p>Five different stability classes were defined on the basis of the behavior of turbulent heat, momentum and CO<sub>2</sub> fluxes and variance ratio as a function of h/L stability parameter (where h is the canopy height and L is the Obukhov length). The novelty is the identification of a ‘super-stable’ (SS) regime (h/L>3) characterized by extremely low wind speeds, the almost completely suppression of turbulence and a clear dominance of submeso motions both above and within the forest.</p><p>The obtained data classification was used to study the influence of atmospheric stratification on the vertical profiles of turbulent statistics. The spectral characteristics of coherent structures and of submeso motions (that may influence the energy and mass exchange above the Amazon forest) have been analyzed by wavelet analyses. The role of the main structures in momentum, heat and CO<sub>2 </sub>transport at the different levels inside and above the forest and in different diabatic conditions was thoroughly investigated through multiresolution and quadrant analyses.</p><p>In unstable and neutral stability, the flow above the canopy appears modulated by ejections, whereas downward and intermittent sweeps dominate the transport inside the canopy. In the roughness sublayer (z £ 2h) the coherent structures dominating the transport within and above the canopy have a characteristic temporal scale of about 100 sec, whereas above this layer the transport is mainly driven by larger scale convection (temporal scale of about 15 min).</p><p>In stable conditions the height of roughness sublayer progressively decreases with increasing stability reaching the minimum value (z<1.35h) in the SS regime. Above the canopy the flow is clearly dominated by ejections but characterized by a higher intermittency mainly in SS conditions. On the other hand, the rapid shear stress absorption in the highest part of the vegetation produces a less clear dominance of sweeps and a less defined role of odd and even quadrants inside the canopy in the transport of momentum, heat and CO<sub>2</sub>. In the weakly stable regime (0.15<h/L<1) transport is dominated in the roughness sublayer by canopy coherent structures with a characteristic temporal scale of about 60 sec. As stability increases the influence of low-frequency (submeso) processes, with a temporal scale of 20-30 min, on flow dynamics progressively increases and becomes dominant in the SS regime where the buoyancy strongly dampens or completely inhibits turbulent structures whereas the large-scale oscillations propagate in the interior of the canopy modulating the heat and CO<sub>2 </sub>transport.</p><p> </p>


2020 ◽  
Vol 146 (727) ◽  
pp. 889-903 ◽  
Author(s):  
Michel Stefanello ◽  
Daniela Cava ◽  
Umberto Giostra ◽  
Otávio Acevedo ◽  
Gervasio Degrazia ◽  
...  

2019 ◽  
Vol 172 (1) ◽  
pp. 17-43 ◽  
Author(s):  
Daniela Cava ◽  
Luca Mortarini ◽  
Umberto Giostra ◽  
Otavio Acevedo ◽  
Gabriel Katul

2019 ◽  
Vol 171 (2) ◽  
pp. 151-173 ◽  
Author(s):  
Daniela Cava ◽  
Luca Mortarini ◽  
Domenico Anfossi ◽  
Umberto Giostra

2017 ◽  
Vol 144 (710) ◽  
pp. 172-183 ◽  
Author(s):  
L. Mortarini ◽  
D. Cava ◽  
U. Giostra ◽  
O. Acevedo ◽  
L.G. Nogueira Martins ◽  
...  

2016 ◽  
Vol 143 (703) ◽  
pp. 661-669 ◽  
Author(s):  
D. Cava ◽  
L. Mortarini ◽  
U. Giostra ◽  
R. Richiardone ◽  
D. Anfossi

2016 ◽  
Vol 46 (1) ◽  
pp. 95-105 ◽  
Author(s):  
L. Mahrt ◽  
Edgar L Andreas ◽  
James B. Edson ◽  
Dean Vickers ◽  
Jielun Sun ◽  
...  

AbstractSummertime eddy correlation measurements from an offshore tower are analyzed to investigate the dependence of the friction velocity for stable conditions on the mean wind speed V, air–sea difference of virtual potential temperature δθυ, and nonstationary submeso motions. The quantity δθυ sometimes exceeds 3°C, usually because of the advection of warm air from land over cooler water at this site. Thin stable boundary layers result. Unexpectedly, does not depend systematically on the stratification δθυ even for weak winds. For weak winds, increases systematically with increasing submeso variations of the wind. The relationship for a given V is greater in nonstationary conditions. Additionally, this study examines as a function of wind direction. The relationship appears to be affected by swell direction for weak winds and advection from land for short fetches.


2015 ◽  
Vol 54 (2) ◽  
pp. 352-369 ◽  
Author(s):  
Joshua D. Hoover ◽  
David R. Stauffer ◽  
Scott J. Richardson ◽  
Larry Mahrt ◽  
Brian J. Gaudet ◽  
...  

AbstractTo better understand the physical processes of the stable boundary layer and to quantify “submeso motions” in moderately complex terrain, exploratory case-study analyses were performed using observational field data supplemented by gridded North American Regional Reanalysis data and Pennsylvania State University real-time Weather Research and Forecasting Model output. Submeso motions are nominally defined as all motions between the largest turbulent scales and the smallest mesoscales. Seven nighttime cases from August and September of 2011 are chosen from a central Pennsylvania [“Rock Springs” (RS)] network of eight ground-based towers and two sound detection and ranging (sodar) systems . The observation network is located near Tussey Ridge, ~15 km southeast of the Allegheny Mountains. The seven cases are classified by the dominant synoptic-flow direction and proximity to terrain to assess the influence of synoptic conditions on the local submeso and mesogamma motions. It is found that synoptic winds with a large crossing angle over nearby Tussey Ridge can generate mesogamma wave motions and larger-magnitude submeso temperature and wind fluctuations in the RS network than do winds from the direction of the more distant Allegheny Mountains. Cases with synoptic winds that are nearly parallel to the topographic contours or are generally weak exhibit the smallest fluctuations. Changes in the magnitude of near-surface submeso temperature and wind fluctuations in response to local indicator variables are also analyzed. The observed submeso wind and temperature fluctuations are generally larger when the low-level wind speed and thermal stratification, respectively, are greater, but the synoptic flow and its relation to the terrain also play an important role.


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