Abstract

A semi-analytical scheme is proposed to parametrize the Obukhov stability parameter \(\zeta \) (= \(z/L\); \(z\) is the height above the ground and \(L\) is the Obukhov length) in terms of the bulk Richardson number (\(R_{iB}\)) in unstable conditions within the framework of Monin–Obukhov similarity (MOS) theory. The scheme involves, (i) a solution of a cubic equation in \(\zeta \) whose coefficients depend on the gradient Richardson number (\(R_{i}\)), and (ii) a relationship between \(R_{i}\) and \(R_{iB}\). The proposed scheme is applicable for a wide range (i) \(-5\le R_{iB}\le 0\), (ii) \(0\le \hbox {ln}(z_{0}/z_{h})\le 29.0\), and (iii) \(10\le z/z_{0}\le 10^{5}\) and performs relatively better than all other schemes in terms of accuracy in computation of surface-layer transfer coefficients. The absolute errors in computing the transfer coefficients do not exceed 7 %. The analysis presented here is found to be valid for different \(\gamma _{m}\) and \(\gamma _{h}\) appearing in the expressions of the similarity functions \(\varphi _{m}\) and \(\varphi _{h}\) (representing non-dimensional wind and temperature profiles), so long as the ratio of \(\gamma _{m}\) to \(\gamma _{h} \ge 1\). The improved scheme can be easily employed in atmospheric modelling for a comprehensive range of \(R_{iB}\) and a variety of surfaces.

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