Climate impacts of ice nucleation

[1] Several different ice nucleation parameterizations in two different General Circulation Models (GCMs) are used to understand the effects of ice nucleation on the mean climate state, and the Aerosol Indirect Effects (AIE) of cirrus clouds on climate. Simulations have a range of ice microphysical states that are consistent with the spread of observations, but many simulations have higher present-day ice crystal number concentrations than in-situ observations. These different states result from different parameterizations of ice cloud nucleation processes, and feature different balances of homogeneous and heterogeneous nucleation. Black carbon aerosols have a small (−0.06 Wm−2) and not statistically significant AIE when included as ice nuclei, for nucleation efficiencies within the range of laboratory measurements. Indirect effects of anthropogenic aerosols on cirrus clouds occur as a consequence of increasing anthropogenic sulfur emissions with different mechanisms important in different models. In one model this is due to increases in homogeneous nucleation fraction, and in the other due to increases in heterogeneous nucleation with coated dust. The magnitude of the effect is the same however. The resulting ice AIE does not seem strongly dependent on the balance between homogeneous and heterogeneous ice nucleation. Regional effects can reach several Wm−2. Indirect effects are slightly larger for those states with less homogeneous nucleation and lower ice number concentration in the base state. The total ice AIE is estimated at 0.27 ± 0.10 Wm−2 (1σ uncertainty). This represents a 20% offset of the simulated total shortwave AIE for ice and liquid clouds of −1.6 Wm−2.

[1]  A. Mangold,et al.  Ice supersaturations and cirrus cloud crystal numbers , 2008 .

[2]  O. Boucher,et al.  The aerosol-climate model ECHAM5-HAM , 2004 .

[3]  Ann M. Fridlind,et al.  Ice supersaturations exceeding 100% at the cold tropical tropopause: implications for cirrus formation and dehydration , 2004 .

[4]  J. Seinfeld,et al.  Ice Initiation by Aerosol Particles: Measured and Predicted Ice Nuclei Concentrations versus Measured Ice Crystal Concentrations in an Orographic Wave Cloud , 2010 .

[5]  S. Ghan,et al.  Inclusion of Ice Microphysics in the NCAR Community Atmospheric Model Version 3 (CAM3) , 2007 .

[6]  Evgueni I. Kassianov,et al.  The multi-scale aerosol-climate model PNNL-MMF: model description and evaluation , 2010 .

[7]  J. Golaz,et al.  Two-moment bulk stratiform cloud microphysics in the GFDL AM3 GCM: description, evaluation, and sensitivity tests , 2010 .

[8]  U. Lohmann,et al.  Impact of ice supersaturated regions and thin cirrus on radiation in the midlatitudes , 2007 .

[9]  A. Nenes,et al.  Parameterizing the competition between homogeneous and heterogeneous freezing in cirrus cloud formation – monodisperse ice nuclei , 2009 .

[10]  Joyce E. Penner,et al.  Ice nucleation parameterization for global models , 2005 .

[11]  A. Nenes,et al.  Parameterizing the competition between homogeneous and heterogeneous freezing in ice cloud formation – polydisperse ice nuclei , 2009 .

[12]  Richard Neale,et al.  Toward a Minimal Representation of Aerosols in Climate Models: Description and Evaluation in the Community Atmosphere Model CAM5 , 2012 .

[13]  Andrew Gettelman,et al.  A new two-moment bulk stratiform cloud microphysics scheme in the NCAR Community Atmosphere Model (CAM3), Part II: Single-Column and Global Results , 2007 .

[14]  C. Bretherton,et al.  The University of Washington Shallow Convection and Moist Turbulence Schemes and Their Impact on Climate Simulations with the Community Atmosphere Model , 2009 .

[15]  W. Cotton,et al.  New primary ice-nucleation parameterizations in an explicit cloud model , 1992 .

[16]  T. Leisner,et al.  Resurgence in Ice Nuclei Measurement Research , 2011 .

[17]  Johannes Hendricks,et al.  Physically based parameterization of cirrus cloud formation for use in global atmospheric models , 2006 .

[18]  A. Nenes,et al.  Parameterization of cirrus cloud formation in large‐scale models: Homogeneous nucleation , 2008 .

[19]  M. Schnaiter,et al.  Supplementary information for ‘ Heterogeneous nucleation of ice particles on glassy aerosols under cirrus conditions ’ , 2010 .

[20]  U. Lohmann,et al.  Solid Ammonium Sulfate Aerosols as Ice Nuclei: A Pathway for Cirrus Cloud Formation , 2006, Science.

[21]  Claudia Marcolli,et al.  Do atmospheric aerosols form glasses , 2008 .

[22]  David R. Doelling,et al.  Toward Optimal Closure of the Earth's Top-of-Atmosphere Radiation Budget , 2009 .

[23]  S. Ghan,et al.  A New Two-Moment Bulk Stratiform Cloud Microphysics Scheme in the Community Atmosphere Model, Version 3 (CAM3). Part II: Single-Column and Global Results , 2008 .

[24]  R. Lawson,et al.  Aircraft measurements of microphysical properties of subvisible cirrus in the tropical tropopause layer , 2007 .

[25]  W. Cooper,et al.  Ice Initiation in Natural Clouds , 1986 .

[26]  U. Lohmann,et al.  Sensitivity studies of different aerosol indirect effects in mixed-phase clouds , 2009 .

[27]  U. Schumann,et al.  Aerosol-cirrus interactions: a number based phenomenon at all? , 2003 .

[28]  S. Klein,et al.  Global simulations of ice nucleation and ice supersaturation with an improved cloud scheme in the Community Atmosphere Model , 2010 .

[29]  Joyce E. Penner,et al.  Possible influence of anthropogenic aerosols on cirrus clouds and anthropogenic forcing , 2008 .

[30]  E. Bigg The formation of atmospheric ice crystals by the freezing of droplets , 1953 .

[31]  Athanasios Nenes,et al.  Sensitivity of the global distribution of cirrus ice crystal concentration to heterogeneous freezing , 2010 .

[32]  Paul J. DeMott,et al.  Insights into the role of soot aerosols in cirrus cloud formation , 2007 .

[33]  U. Lohmann,et al.  Total aerosol effect: forcing or radiative flux perturbation , 2009 .

[34]  M. Petters,et al.  Ice nucleation behavior of biomass combustion particles at cirrus temperatures , 2009 .

[35]  U. Lohmann,et al.  Sensitivity studies of cirrus clouds formed by heterogeneous freezing in the ECHAM GCM , 2004 .

[36]  J. Penner,et al.  Cirrus clouds in a global climate model with a statistical cirrus cloud scheme , 2009 .

[37]  D. Barahona On the ice nucleation spectrum , 2011 .

[38]  Qiang Fu,et al.  Mean radiative energy balance and vertical mass fluxes in the equatorial upper troposphere and lower stratosphere , 2005 .

[39]  U. Lohmann,et al.  Cirrus cloud formation and ice supersaturated regions in a global climate model , 2008 .

[40]  M. Schnaiter,et al.  Studies of propane flame soot acting as heterogeneous ice nuclei in conjunction with single particle soot photometer measurements , 2011 .

[41]  Paul J. DeMott,et al.  An Empirical Parameterization of Heterogeneous Ice Nucleation for Multiple Chemical Species of Aerosol , 2008 .

[42]  Johannes Quaas,et al.  Total aerosol effect: radiative forcing or radiative flux perturbation? , 2009 .

[43]  Andrew Gettelman,et al.  Sensitivity studies of dust ice nuclei effect on cirrus clouds with the Community Atmosphere Model CAM5 , 2012 .

[44]  J. Penner,et al.  Influence of anthropogenic sulfate and black carbon on upper tropospheric clouds in the NCAR CAM3 model coupled to the IMPACT global aerosol model , 2009 .

[45]  U. Lohmann,et al.  A Parameterization of cirrus cloud formation: Homogeneous freezing including effects of aerosol size , 2002 .

[46]  Ulrike Lohmann,et al.  Oxalic acid as a heterogeneous ice nucleus in the upper troposphere and its indirect aerosol effect , 2006 .

[47]  J. Curry,et al.  A New Double-Moment Microphysics Parameterization for Application in Cloud and Climate Models. Part I: Description , 2005 .

[48]  S. Twomey The Influence of Pollution on the Shortwave Albedo of Clouds , 1977 .

[49]  Johannes Hendricks,et al.  Do aircraft black carbon emissions affect cirrus clouds on the global scale? , 2005 .

[50]  Johannes Hendricks,et al.  Effects of ice nuclei on cirrus clouds in a global climate model , 2011 .

[51]  U. Lohmann,et al.  Global indirect aerosol effects: a review , 2004 .

[52]  Ulrike Lohmann,et al.  A parameterization of cirrus cloud formation: Heterogeneous freezing , 2003 .

[53]  Steven Platnick,et al.  Interactive comment on “On the importance of small ice crystals in tropical anvil cirrus” by E. J. Jensen et al , 2009 .

[54]  W. Collins,et al.  Description of the NCAR Community Atmosphere Model (CAM 3.0) , 2004 .

[55]  K. C. Young The Role of Contact Nucleation in Ice Phase Initiation in Clouds , 1974 .

[56]  A. Mangold,et al.  Effect of sulfuric acid coating on heterogeneous ice nucleation by soot aerosol particles , 2005 .

[57]  U. Lohmann,et al.  Cloud microphysics and aerosol indirect effects in the global climate model ECHAM5-HAM , 2007 .

[58]  J. Penner,et al.  Coupled IMPACT aerosol and NCAR CAM3 model: Evaluation of predicted aerosol number and size distribution , 2009 .

[59]  Ulrike Lohmann,et al.  Global anthropogenic aerosol effects on convective clouds in ECHAM5-HAM , 2007 .