Abstract

Abstract. A new method for parameterizing the subgrid variations of vertical velocity and cloud droplet number concentration (CDNC) is presented for general circulation models (GCMs). These parameterizations build on top of existing parameterizations that create stochastic subgrid cloud columns inside the GCM grid cells, which can be employed by the Monte Carlo independent column approximation approach for radiative transfer. The new model version adds a description for vertical velocity in individual subgrid columns, which can be used to compute cloud activation and the subgrid distribution of the number of cloud droplets explicitly. Autoconversion is also treated explicitly in the subcolumn space. This provides a consistent way of simulating the cloud radiative effects with two-moment cloud microphysical properties defined at subgrid scale. The primary impact of the new parameterizations is to decrease the CDNC over polluted continents, while over the oceans the impact is smaller. Moreover, the lower CDNC induces a stronger autoconversion of cloud water to rain. The strongest reduction in CDNC and cloud water content over the continental areas promotes weaker shortwave cloud radiative effects (SW CREs) even after retuning the model. However, compared to the reference simulation, a slightly stronger SW CRE is seen e.g. over mid-latitude oceans, where CDNC remains similar to the reference simulation, and the in-cloud liquid water content is slightly increased after retuning the model.

Highlights

  • Cloud droplet formation Iins tshtervuemrtiecanl tvaeltoiocinty of an ascending air vapour ptharrocuegl,hsiandcieabiattiacffceoMcotsleintthghe. oTsadhteusrcaautinrornednrtastitoateo-fofw-tahteerart cloud activation paramDeatetraizaStioynsste(em.g.sAbdul-Razzak

  • Compared to the refer- vertical velocity for cloud activaStiocn.ieTunrcbuelesnt variability of ence simulation, a slightly stronger shortwave cloud radiative effects (SW cloud radiative effects (CREs)) is seen e.g. over vertical velocity has a strong impact on the number of cloud mid-latitude oceans, where cloud droplet number concentration (CDNC) remains similar to the ref- droplets in stratiform clouds, and it takes place at scales conerence simulation, and the in-cloud liquid water content is siderably smaller than the, typically, rather large grid spacing slightly increased after retuning the model

  • This paper reported the implementation of a subgrid vertical velocity parameterization and subgrid versions of cloud microphysical parameterizations describing processes such as cloud droplet activation and autoconversion of cloud droplets to rain

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Summary

Introduction

Cloud droplet formation Iins tshtervuemrtiecanl tvaeltoiocinty of an ascending air vapour ptharrocuegl,hsiandcieabiattiacffceoMcotsleintthghe. oTsadhteusrcaautinrornednrtastitoateo-fofw-tahteerart cloud activation paramDeatetraizaStioynsste(em.g.sAbdul-Razzak. Autoconversion is treated explicitly in the subcolumn and Ghan, 2000; Fountoukis and Nenes, 2005; Ming et al., space This provides a consistent way of simulating the cloud 2006; Khvorostyanov and Curry, 2009) rely on this assumpradiative effects with two-moment cloud microphysical properties defined at subgrid scale. Compared to the refer- vertical velocity for cloud activaStiocn.ieTunrcbuelesnt variability of ence simulation, a slightly stronger SW CRE is seen e.g. over vertical velocity has a strong impact on the number of cloud mid-latitude oceans, where CDNC remains similar to the ref- droplets in stratiform clouds, and it takes place at scales conerence simulation, and the in-cloud liquid water content is siderably smaller than the, typically, rather large grid spacing slightly increased after retuning the model.

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