Momentum Transfer within Canopies
To understand the basic characteristics of the observed S-shaped wind profile and the exponential flux profile within forest canopies, three hypotheses are postulated. The relationship between these fundamental profiles is well established by combining the postulated hypotheses with momentum equatio...
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Published in | Journal of applied meteorology and climatology Vol. 47; no. 1; pp. 262 - 275 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
Boston, MA
American Meteorological Society
01.01.2008
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Subjects | |
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Abstract | To understand the basic characteristics of the observed S-shaped wind profile and the exponential flux profile within forest canopies, three hypotheses are postulated. The relationship between these fundamental profiles is well established by combining the postulated hypotheses with momentum equations. Robust agreements between theoretical predictions and observations indicate that the nature of momentum transfer within canopies can be well understood by combining the postulated hypotheses and momentum equations. The exponential Reynolds stress profiles were successfully predicted by the leaf area index (LAI) profile alone. The characteristics of the S-shaped wind profile were theoretically explained by the plant morphology and local drag coefficient distribution. Predictions of maximum drag coefficient were located around the maximum leaf area level for most forest canopies but lower than the maximum leaf area level for a corn canopy. A universal relationship of the Reynolds stress between the top and bottom of the canopy is predicted for all canopies. This universal relationship can be used to understand what percentage of the Reynolds stress at the top of canopy is absorbed by the whole canopy layer from the observed LAI values alone. All of these predictions are consistent with the conclusions from dimensional analysis and satisfy the continuity requirement of Reynolds stress, mean wind speed, and local drag coefficient at the top of canopy. |
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AbstractList | To understand the basic characteristics of the observed S-shaped wind profile and the exponential flux profile within forest canopies, three hypotheses are postulated. The relationship between these fundamental profiles is well established by combining the postulated hypotheses with momentum equations. Robust agreements between theoretical predictions and observations indicate that the nature of momentum transfer within canopies can be well understood by combining the postulated hypotheses and momentum equations. The exponential Reynolds stress profiles were successfully predicted by the leaf area index (LAI) profile alone. The characteristics of the S-shaped wind profile were theoretically explained by the plant morphology and local drag coefficient distribution. Predictions of maximum drag coefficient were located around the maximum leaf area level for most forest canopies but lower than the maximum leaf area level for a corn canopy. A universal relationship of the Reynolds stress between the top and bottom of the canopy is predicted for all canopies. This universal relationship can be used to understand what percentage of the Reynolds stress at the top of canopy is absorbed by the whole canopy layer from the observed LAI values alone. All of these predictions are consistent with the conclusions from dimensional analysis and satisfy the continuity requirement of Reynolds stress, mean wind speed, and local drag coefficient at the top of canopy. [PUBLICATION ABSTRACT] To understand the basic characteristics of the observed S-shaped wind profile and the exponential flux profile within forest canopies, three hypotheses are postulated. The relationship between these fundamental profiles is well established by combining the postulated hypotheses with momentum equations. Robust agreements between theoretical predictions and observations indicate that the nature of momentum transfer within canopies can be well understood by combining the postulated hypotheses and momentum equations. The exponential Reynolds stress profiles were successfully predicted by the leaf area index (LAI) profile alone. The characteristics of the S-shaped wind profile were theoretically explained by the plant morphology and local drag coefficient distribution. Predictions of maximum drag coefficient were located around the maximum leaf area level for most forest canopies but lower than the maximum leaf area level for a corn canopy. A universal relationship of the Reynolds stress between the top and bottom of the canopy is predicted for all canopies. This universal relationship can be used to understand what percentage of the Reynolds stress at the top of canopy is absorbed by the whole canopy layer from the observed LAI values alone. All of these predictions are consistent with the conclusions from dimensional analysis and satisfy the continuity requirement of Reynolds stress, mean wind speed, and local drag coefficient at the top of canopy. Abstract To understand the basic characteristics of the observed S-shaped wind profile and the exponential flux profile within forest canopies, three hypotheses are postulated. The relationship between these fundamental profiles is well established by combining the postulated hypotheses with momentum equations. Robust agreements between theoretical predictions and observations indicate that the nature of momentum transfer within canopies can be well understood by combining the postulated hypotheses and momentum equations. The exponential Reynolds stress profiles were successfully predicted by the leaf area index (LAI) profile alone. The characteristics of the S-shaped wind profile were theoretically explained by the plant morphology and local drag coefficient distribution. Predictions of maximum drag coefficient were located around the maximum leaf area level for most forest canopies but lower than the maximum leaf area level for a corn canopy. A universal relationship of the Reynolds stress between the top and bottom of the canopy is predicted for all canopies. This universal relationship can be used to understand what percentage of the Reynolds stress at the top of canopy is absorbed by the whole canopy layer from the observed LAI values alone. All of these predictions are consistent with the conclusions from dimensional analysis and satisfy the continuity requirement of Reynolds stress, mean wind speed, and local drag coefficient at the top of canopy. |
Author | Yi, Chuixiang |
Author_xml | – sequence: 1 givenname: Chuixiang surname: Yi fullname: Yi, Chuixiang organization: Queens College, City University of New York, Flushing, New York |
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Keywords | Reynolds stress Wind field Momentum transfer Air biosphere interaction Atmospheric boundary layer Turbulent transfer turbulent flow forests Drag coefficient Canopy(vegetation) Leaf area index |
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22 Allen (2020061306432985700_i1558-8432-47-1-262-Allen1) 1968; 7 Mohan (2020061306432985700_i1558-8432-47-1-262-Mohan1) 2004; 113 Landsberg (2020061306432985700_i1558-8432-47-1-262-Landsberg1) 1971; 8 2020061306432985700_i1558-8432-47-1-262-Lalic1 Massman (2020061306432985700_i1558-8432-47-1-262-Massman3) 1999; 91 Poggi (2020061306432985700_i1558-8432-47-1-262-Poggi1) 2004; 111 Turnipseed (2020061306432985700_i1558-8432-47-1-262-Turnipseed1) 2003; 119 Bohm (2020061306432985700_i1558-8432-47-1-262-Bohm1) 2000 Wyngaard (2020061306432985700_i1558-8432-47-1-262-Wyngaard1) 1973 Obukhov (2020061306432985700_i1558-8432-47-1-262-Obukhov1) 1953; 93 Grant (2020061306432985700_i1558-8432-47-1-262-Grant1) 1983; 27 Legg (2020061306432985700_i1558-8432-47-1-262-Legg1) 1975; 101 Katul (2020061306432985700_i1558-8432-47-1-262-Katul2) 1999; 38 Denmead (2020061306432985700_i1558-8432-47-1-262-Denmead1) 1985 Bergen (2020061306432985700_i1558-8432-47-1-262-Bergen1) 1971; 17 Cionco (2020061306432985700_i1558-8432-47-1-262-Cionco1) 1965; 4 |
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Snippet | To understand the basic characteristics of the observed S-shaped wind profile and the exponential flux profile within forest canopies, three hypotheses are... Abstract To understand the basic characteristics of the observed S-shaped wind profile and the exponential flux profile within forest canopies, three... |
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SubjectTerms | Animal and plant ecology Animal, plant and microbial ecology Biological and medical sciences Canopies Chemical compounds Convection, turbulence, diffusion. Boundary layer structure and dynamics Dimensional analysis Drag coefficient Drag coefficients Earth, ocean, space Exact sciences and technology External geophysics Forest canopy Forests Fundamental and applied biological sciences. Psychology Hypotheses Leaf area Leaves Mathematical analysis Meteorology Meteors Modeling Momentum Momentum transfer Plant morphology Reynolds stress Synecology Terrestrial ecosystems Theory Vegetation canopies Wind profiles Wind speed Wind velocity |
Title | Momentum Transfer within Canopies |
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