Departure from Clausius‐Clapeyron scaling of water entering the stratosphere in response to changes in tropical upwelling. Issue 4 (25th February 2014)

• Record Type: Journal Article
• Authors: Fueglistaler, S.; Liu, Y. S.; Flannaghan, T. J.; Ploeger, F.; Haynes, P. H.
• Is Part Of: Journal of geophysical research. Volume 119:Issue 4(2014:Apr.)
• Page Start: 1962
• Page End: 1972
• Publication Date: 2014-02-25
• Subjects: Atmospheric physics -- Periodicals; Geophysics -- Periodicals; 551.5
• DOI: 10.1002/2013JD020772
• Languages: English
• ISSNs: 2169-897X

Abstract

<abstract abstract-type="main" id="jgrd51188-abs-0001"> <title> <x xml:space="preserve">Abstract</x> </title> <p id="jgrd51188-para-0001">Water entering the stratosphere ([H<sub>2</sub>O]<sub>entry</sub>) is strongly constrained by temperatures in the tropical tropopause layer (TTL). Temperatures at tropical tropopause levels are 15–20 K below radiative equilibrium. A strengthening of the residual circulation as suggested by general circulation models in response to increasing greenhouse gases is, based on radiative transfer calculations, estimated to lead to a temperature decrease of about 2 K per 10% change in upwelling (with some sensitivity to vertical scale length). For a uniform temperature change in the inner tropics, [H<sub>2</sub>O]<sub>entry</sub> may be expected to change as predicted by the temperature dependence of the vapor pressure, referred here as "Clausius‐Clapeyron (CC) scaling." Under CC scaling, this corresponds to ∼1 ppmv change in [H<sub>2</sub>O]<sub>entry</sub> per 10% change in upwelling. However, the change in upwelling also changes the residence time of air in the TTL. We show with trajectory calculations that this affects [H<sub>2</sub>O]<sub>entry</sub>, such that [H<sub>2</sub>O]<sub>entry</sub> changes ∼10 % less than expected from CC scaling. This <italic>residence time</italic> effect for water vapor is a consequence of the spatiotemporal variance in the temperature field. We show that for the present‐day TTL, a little more than half of the effect is due to the systematic relation between flow and temperature field. The remainder can be understood from the perspective of a random walk problem, with slower ascent (longer path) increasing each air parcel's probability to encounter anomalously low temperatures. Our results show that atmospheric water vapor may depart from CC scaling with mean temperatures even when all physical processes of dehydration remain unchanged.</p> </abstract>