Turbulent Flux Transfer over Bare-Soil Surfaces: Characteristics and Parameterization

Parameterization of turbulent flux from bare-soil and undercanopy surfaces is imperative for modeling land–atmosphere interactions in arid and semiarid regions, where flux from the ground is dominant or comparable to canopy-sourced flux. This paper presents the major characteristics of turbulent flu...

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Veröffentlicht in:Journal of applied meteorology (1988) 2008-01, Vol.47 (1), p.276-290
Hauptverfasser: Yang, Kun, Koike, Toshio, Ishikawa, Hirohiko, Kim, Joon, Li, Xin, Liu, Huizhi, Liu, Shaomin, Ma, Yaoming, Wang, Jieming
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container_issue 1
container_start_page 276
container_title Journal of applied meteorology (1988)
container_volume 47
creator Yang, Kun
Koike, Toshio
Ishikawa, Hirohiko
Kim, Joon
Li, Xin
Liu, Huizhi
Liu, Shaomin
Ma, Yaoming
Wang, Jieming
description Parameterization of turbulent flux from bare-soil and undercanopy surfaces is imperative for modeling land–atmosphere interactions in arid and semiarid regions, where flux from the ground is dominant or comparable to canopy-sourced flux. This paper presents the major characteristics of turbulent flux transfers over seven bare-soil surfaces. These sites are located in arid, semiarid, and semihumid regions in Asia and represent a variety of conditions for aerodynamic roughness length (z 0m; from
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This paper presents the major characteristics of turbulent flux transfers over seven bare-soil surfaces. These sites are located in arid, semiarid, and semihumid regions in Asia and represent a variety of conditions for aerodynamic roughness length (z 0m; from &lt;1 to 10 mm) and sensible heat flux (from −50 to 400 W m−2). For each site, parameterkB −1[=ln(z 0m/z 0h), wherez 0his the thermal roughness length] exhibits clear diurnal variations with higher values during the day and lower values at night. Mean values ofz 0hfor the individual sites do not change significantly withz 0m, resulting inkB −1increasing withz 0m, and thus the momentum transfer coefficient increases faster than the heat transfer coefficient withz 0m. The termkB −1often becomes negative at night for relatively smooth surfaces (z 0m∼ 1 mm), indicating that the widely accepted excess resistance for heat transfer can be negative, which cannot be explained by current theories for aerodynamically rough surfaces. Last, severalkB −1schemes are evaluated using the same datasets. The results indicate that a scheme that can reproduce the diurnal variation ofkB −1generally performs better than schemes that cannot.</description><identifier>ISSN: 1558-8424</identifier><identifier>ISSN: 0894-8763</identifier><identifier>EISSN: 1558-8432</identifier><identifier>EISSN: 1520-0450</identifier><identifier>DOI: 10.1175/2007jamc1547.1</identifier><identifier>CODEN: JOAMEZ</identifier><language>eng</language><publisher>Boston, MA: American Meteorological Society</publisher><subject>Aerodynamics ; Arid regions ; Arid zones ; Atmosphere ; Computational fluid dynamics ; Convection, turbulence, diffusion. Boundary layer structure and dynamics ; Datasets ; Diurnal variations ; Earth, ocean, space ; Exact sciences and technology ; External geophysics ; Fluctuations ; Flux ; General circulation models ; Geographic regions ; Geophysics. Techniques, methods, instrumentation and models ; Heat transfer ; Meteorology ; Momentum transfer ; Parameterization ; Parametrization ; Remote sensing ; Research universities ; Reynolds number ; River basins ; Roughness ; Semiarid lands ; Sensible heat ; Soil surfaces ; Studies ; Surface roughness ; Surface temperature ; Theory ; Turbulence ; Vegetation canopies</subject><ispartof>Journal of applied meteorology (1988), 2008-01, Vol.47 (1), p.276-290</ispartof><rights>2008 American Meteorological Society</rights><rights>2008 INIST-CNRS</rights><rights>Copyright American Meteorological Society Jan 2008</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c517t-afe759bf23be0dc2f14dad4445f609794a8d13a5727f723cea13ed49ec65e7263</citedby><cites>FETCH-LOGICAL-c517t-afe759bf23be0dc2f14dad4445f609794a8d13a5727f723cea13ed49ec65e7263</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.jstor.org/stable/pdf/26172144$$EPDF$$P50$$Gjstor$$H</linktopdf><linktohtml>$$Uhttps://www.jstor.org/stable/26172144$$EHTML$$P50$$Gjstor$$H</linktohtml><link.rule.ids>314,776,780,799,3668,4010,27900,27901,27902,57992,58225</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=20116520$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Yang, Kun</creatorcontrib><creatorcontrib>Koike, Toshio</creatorcontrib><creatorcontrib>Ishikawa, Hirohiko</creatorcontrib><creatorcontrib>Kim, Joon</creatorcontrib><creatorcontrib>Li, Xin</creatorcontrib><creatorcontrib>Liu, Huizhi</creatorcontrib><creatorcontrib>Liu, Shaomin</creatorcontrib><creatorcontrib>Ma, Yaoming</creatorcontrib><creatorcontrib>Wang, Jieming</creatorcontrib><title>Turbulent Flux Transfer over Bare-Soil Surfaces: Characteristics and Parameterization</title><title>Journal of applied meteorology (1988)</title><description>Parameterization of turbulent flux from bare-soil and undercanopy surfaces is imperative for modeling land–atmosphere interactions in arid and semiarid regions, where flux from the ground is dominant or comparable to canopy-sourced flux. This paper presents the major characteristics of turbulent flux transfers over seven bare-soil surfaces. These sites are located in arid, semiarid, and semihumid regions in Asia and represent a variety of conditions for aerodynamic roughness length (z 0m; from &lt;1 to 10 mm) and sensible heat flux (from −50 to 400 W m−2). For each site, parameterkB −1[=ln(z 0m/z 0h), wherez 0his the thermal roughness length] exhibits clear diurnal variations with higher values during the day and lower values at night. Mean values ofz 0hfor the individual sites do not change significantly withz 0m, resulting inkB −1increasing withz 0m, and thus the momentum transfer coefficient increases faster than the heat transfer coefficient withz 0m. The termkB −1often becomes negative at night for relatively smooth surfaces (z 0m∼ 1 mm), indicating that the widely accepted excess resistance for heat transfer can be negative, which cannot be explained by current theories for aerodynamically rough surfaces. Last, severalkB −1schemes are evaluated using the same datasets. The results indicate that a scheme that can reproduce the diurnal variation ofkB −1generally performs better than schemes that cannot.</description><subject>Aerodynamics</subject><subject>Arid regions</subject><subject>Arid zones</subject><subject>Atmosphere</subject><subject>Computational fluid dynamics</subject><subject>Convection, turbulence, diffusion. Boundary layer structure and dynamics</subject><subject>Datasets</subject><subject>Diurnal variations</subject><subject>Earth, ocean, space</subject><subject>Exact sciences and technology</subject><subject>External geophysics</subject><subject>Fluctuations</subject><subject>Flux</subject><subject>General circulation models</subject><subject>Geographic regions</subject><subject>Geophysics. 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This paper presents the major characteristics of turbulent flux transfers over seven bare-soil surfaces. These sites are located in arid, semiarid, and semihumid regions in Asia and represent a variety of conditions for aerodynamic roughness length (z 0m; from &lt;1 to 10 mm) and sensible heat flux (from −50 to 400 W m−2). For each site, parameterkB −1[=ln(z 0m/z 0h), wherez 0his the thermal roughness length] exhibits clear diurnal variations with higher values during the day and lower values at night. Mean values ofz 0hfor the individual sites do not change significantly withz 0m, resulting inkB −1increasing withz 0m, and thus the momentum transfer coefficient increases faster than the heat transfer coefficient withz 0m. The termkB −1often becomes negative at night for relatively smooth surfaces (z 0m∼ 1 mm), indicating that the widely accepted excess resistance for heat transfer can be negative, which cannot be explained by current theories for aerodynamically rough surfaces. Last, severalkB −1schemes are evaluated using the same datasets. The results indicate that a scheme that can reproduce the diurnal variation ofkB −1generally performs better than schemes that cannot.</abstract><cop>Boston, MA</cop><pub>American Meteorological Society</pub><doi>10.1175/2007jamc1547.1</doi><tpages>15</tpages><oa>free_for_read</oa></addata></record>
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subjects Aerodynamics
Arid regions
Arid zones
Atmosphere
Computational fluid dynamics
Convection, turbulence, diffusion. Boundary layer structure and dynamics
Datasets
Diurnal variations
Earth, ocean, space
Exact sciences and technology
External geophysics
Fluctuations
Flux
General circulation models
Geographic regions
Geophysics. Techniques, methods, instrumentation and models
Heat transfer
Meteorology
Momentum transfer
Parameterization
Parametrization
Remote sensing
Research universities
Reynolds number
River basins
Roughness
Semiarid lands
Sensible heat
Soil surfaces
Studies
Surface roughness
Surface temperature
Theory
Turbulence
Vegetation canopies
title Turbulent Flux Transfer over Bare-Soil Surfaces: Characteristics and Parameterization
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