On the relationship between the roughness length of a scalar quantity and the corresponding sublayer-Stanton number

Considering Sheppard's effective diffusivity approach for the molecular-turbulent sublayer, the relationship between the roughness length of a scalar quantity, zp and the corresponding sublayer-Stanton number, Bi, ist re-formulated. This re-formulation leads to Bi-1 = k-1 ln (1+zo/zp), where zo...

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Main Authors: Gerhard Kramm, Hans Müller, Ralph Dlugi
Format: Article
Language:English
Published: Borntraeger 1995-11-01
Series:Meteorologische Zeitschrift
Subjects:
Online Access:http://dx.doi.org/10.1127/metz/4/1995/209
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author Gerhard Kramm
Hans Müller
Ralph Dlugi
author_facet Gerhard Kramm
Hans Müller
Ralph Dlugi
author_sort Gerhard Kramm
collection DOAJ
description Considering Sheppard's effective diffusivity approach for the molecular-turbulent sublayer, the relationship between the roughness length of a scalar quantity, zp and the corresponding sublayer-Stanton number, Bi, ist re-formulated. This re-formulation leads to Bi-1 = k-1 ln (1+zo/zp), where zo is the roughness length for momentum. Based on this equation, it is evident that (a) the relationship Bi-1 = k-1 ln (1+zo/zp commonly used is a doubtful approximation for the interfacial sublayer, and (b) the sublayer-Stanton number is positive-definite even if zp≥zo > 0. This is in contrast to negative Bi-1 values found in the literature. Moreover, it is shown that Bi-1 values derived with Sheppard's approach are much smaller than those provided by the more adequate Reichardt's approach.
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spelling doaj.art-aec6f033c97d450ea7862e4687a9f4412024-02-08T08:12:39ZengBorntraegerMeteorologische Zeitschrift0941-29481995-11-014520921210.1127/metz/4/1995/20989151On the relationship between the roughness length of a scalar quantity and the corresponding sublayer-Stanton numberGerhard KrammHans MüllerRalph DlugiConsidering Sheppard's effective diffusivity approach for the molecular-turbulent sublayer, the relationship between the roughness length of a scalar quantity, zp and the corresponding sublayer-Stanton number, Bi, ist re-formulated. This re-formulation leads to Bi-1 = k-1 ln (1+zo/zp), where zo is the roughness length for momentum. Based on this equation, it is evident that (a) the relationship Bi-1 = k-1 ln (1+zo/zp commonly used is a doubtful approximation for the interfacial sublayer, and (b) the sublayer-Stanton number is positive-definite even if zp≥zo > 0. This is in contrast to negative Bi-1 values found in the literature. Moreover, it is shown that Bi-1 values derived with Sheppard's approach are much smaller than those provided by the more adequate Reichardt's approach.http://dx.doi.org/10.1127/metz/4/1995/209molecular-turbulent sublayerdiffusionskoeffizient
spellingShingle Gerhard Kramm
Hans Müller
Ralph Dlugi
On the relationship between the roughness length of a scalar quantity and the corresponding sublayer-Stanton number
Meteorologische Zeitschrift
molecular-turbulent sublayer
diffusionskoeffizient
title On the relationship between the roughness length of a scalar quantity and the corresponding sublayer-Stanton number
title_full On the relationship between the roughness length of a scalar quantity and the corresponding sublayer-Stanton number
title_fullStr On the relationship between the roughness length of a scalar quantity and the corresponding sublayer-Stanton number
title_full_unstemmed On the relationship between the roughness length of a scalar quantity and the corresponding sublayer-Stanton number
title_short On the relationship between the roughness length of a scalar quantity and the corresponding sublayer-Stanton number
title_sort on the relationship between the roughness length of a scalar quantity and the corresponding sublayer stanton number
topic molecular-turbulent sublayer
diffusionskoeffizient
url http://dx.doi.org/10.1127/metz/4/1995/209
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