1970
DOI: 10.1002/qj.49709641012
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Flux‐gradient relationships in the constant flux layer

Abstract: SLMMARYAn analysis is made of the Monin-Obukhov function @.*I in the familiar wind profile equation, using data from two recent expeditions to Gurley (New South Wales) and Hay (New South Wales). In one, the friction velocity u1 is determined directly by the eddy correlation method, and in the other, conducted during mid-winter when small heat-fluxes were experienced, by the use of a friction coefficient applied to a low-!eve1 wind.By collating with a similar earlier analysis for heat and water vapour transfer,… Show more

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Cited by 885 publications
(460 citation statements)
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“…According to Large Eddy Simulations [24] and many field experiments [3,[25][26][27], φ m (ζ) = (1 − 16ζ) −1/4 when ζ < 0 and φ m (ζ) = (1 + 4.7ζ) when ζ > 0. A derivation of these φ m (ζ) functions and their links to the energy spectrum is presented elsewhere [28] and is not repeated here.…”
Section: A Background and Definitionsmentioning
confidence: 99%
“…According to Large Eddy Simulations [24] and many field experiments [3,[25][26][27], φ m (ζ) = (1 − 16ζ) −1/4 when ζ < 0 and φ m (ζ) = (1 + 4.7ζ) when ζ > 0. A derivation of these φ m (ζ) functions and their links to the energy spectrum is presented elsewhere [28] and is not repeated here.…”
Section: A Background and Definitionsmentioning
confidence: 99%
“…ϕ m , ϕ h : Dyer and Hicks (1970) in unstable conditions (ς < 0), and Kondo et al (1978) in stable conditions (ς > 0).…”
Section: The Campaignmentioning
confidence: 99%
“…Computation of surface fluxes of heat, moisture and momentum are based on Monin-Obukhov similarity theory using the stability functions from Paulson (1970), Dyer and Hicks (1970) and Webb (1970). Vertical transport and mixing in the boundary layer are accounted for by using the YSU-PBL scheme (Hong and Lim, 2006).…”
Section: Experimental Set-upmentioning
confidence: 99%