Formation of highly porous aerosol particles by atmospheric freeze-drying in ice clouds

Significance Aerosols cycling through clouds affect particle morphological and chemical properties, thus modifying aerosol effects on cloud microphysics and climate. Previous studies have focused on aerosol processing in warm clouds via aqueous-phase reactions. Here we investigate the physical modifications of aerosols following processing within ice clouds using a unique laboratory setup that simulates ice cloud processes. The processed particles have a porous structure due to phase separation upon freezing, subsequent glass transition, and ice sublimation. Such modified aerosols can be better ice and cloud condensation nuclei and scatter less light. These changes have implications for aerosol–cloud interactions and optical properties of aerosols in the vicinity of clouds. The cycling of atmospheric aerosols through clouds can change their chemical and physical properties and thus modify how aerosols affect cloud microphysics and, subsequently, precipitation and climate. Current knowledge about aerosol processing by clouds is rather limited to chemical reactions within water droplets in warm low-altitude clouds. However, in cold high-altitude cirrus clouds and anvils of high convective clouds in the tropics and midlatitudes, humidified aerosols freeze to form ice, which upon exposure to subsaturation conditions with respect to ice can sublimate, leaving behind residual modified aerosols. This freeze-drying process can occur in various types of clouds. Here we simulate an atmospheric freeze-drying cycle of aerosols in laboratory experiments using proxies for atmospheric aerosols. We find that aerosols that contain organic material that undergo such a process can form highly porous aerosol particles with a larger diameter and a lower density than the initial homogeneous aerosol. We attribute this morphology change to phase separation upon freezing followed by a glass transition of the organic material that can preserve a porous structure after ice sublimation. A porous structure may explain the previously observed enhancement in ice nucleation efficiency of glassy organic particles. We find that highly porous aerosol particles scatter solar light less efficiently than nonporous aerosol particles. Using a combination of satellite and radiosonde data, we show that highly porous aerosol formation can readily occur in highly convective clouds, which are widespread in the tropics and midlatitudes. These observations may have implications for subsequent cloud formation cycles and aerosol albedo near cloud edges.

[1]  Woodley,et al.  Deep convective clouds with sustained supercooled liquid water down to -37.5 degrees C , 2000, Nature.

[2]  C. Marcolli Deposition nucleation viewed as homogeneous or immersion freezing in pores and cavities , 2013 .

[3]  W. Paul Menzel,et al.  The MODIS cloud products: algorithms and examples from Terra , 2003, IEEE Trans. Geosci. Remote. Sens..

[4]  Daniel M. Murphy,et al.  In‐situ observations of mid‐latitude forest fire plumes deep in the stratosphere , 2004 .

[5]  Sonia M. Kreidenweis,et al.  Observations of organic species and atmospheric ice formation , 2004 .

[6]  H. Köhler The nucleus in and the growth of hygroscopic droplets , 1936 .

[7]  Frank Stratmann,et al.  Hygroscopic growth and activation of HULIS particles: Experimental data and a new iterative parameterization scheme for complex aerosol particles , 2007 .

[8]  Douglas R. Worsnop,et al.  The deposition ice nucleation and immersion freezing potential of amorphous secondary organic aerosol: Pathways for ice and mixed‐phase cloud formation , 2012 .

[9]  L. Qian,et al.  Controlled freezing and freeze drying: a versatile route for porous and micro‐/nano‐structured materials , 2011 .

[10]  D. M. Murphy,et al.  Measurements of the concentration and composition of nuclei for cirrus formation , 2003, Proceedings of the National Academy of Sciences of the United States of America.

[11]  C. Jakob,et al.  The variability of tropical ice cloud properties as a function of the large-scale context from ground-based radar-lidar observations over Darwin, Australia , 2010 .

[12]  J. Carpenter,et al.  Annealing to optimize the primary drying rate, reduce freezing-induced drying rate heterogeneity, and determine T(g)' in pharmaceutical lyophilization. , 2001, Journal of pharmaceutical sciences.

[13]  Gerard Capes,et al.  Exploring the vertical profile of atmospheric organic aerosol: comparing 17 aircraft field campaigns with a global model , 2011 .

[14]  H. Christenson Two-step crystal nucleation via capillary condensation , 2013 .

[15]  M. Wendisch,et al.  In Situ, Airborne Instrumentation: Addressing and Solving Measurement Problems in Ice Clouds , 2012 .

[16]  Douglas R. Worsnop,et al.  Particle Morphology and Density Characterization by Combined Mobility and Aerodynamic Diameter Measurements. Part 1: Theory , 2004 .

[17]  William L. Woodley,et al.  Deep convective clouds with sustained supercooled liquid water down to -37.5 °C , 2000, Nature.

[18]  A. Pier Siebesma,et al.  Entrainment and detrainment in cumulus convection: an overview , 2013 .

[19]  Davide Fissore,et al.  Freeze Drying of Pharmaceutical Excipients Close to Collapse Temperature: Influence of the Process Conditions on Process Time and Product Quality , 2009 .

[20]  Ulrich Pöschl,et al.  Atmospheric aerosols: composition, transformation, climate and health effects. , 2005, Angewandte Chemie.

[21]  J. Flink,et al.  ‘Collapse’, a structural transition in freeze dried carbohydrates: III. Prerequisite of recrystallization , 2007 .

[22]  B. Barkstrom,et al.  Cloud-Radiative Forcing and Climate: Results from the Earth Radiation Budget Experiment , 1989, Science.

[23]  S. McFarlane,et al.  Tropical anvil characteristics and water vapor of the tropical tropopause layer: Impact of heterogeneous and homogeneous freezing parameterizations , 2010 .

[24]  Yoram J. Kaufman,et al.  On the twilight zone between clouds and aerosols , 2007 .

[25]  Klaus Gierens,et al.  Ice supersaturation in the ECMWF integrated forecast system , 2007 .

[26]  P. Alpert,et al.  A water activity based model of heterogeneous ice nucleation kinetics for freezing of water and aqueous solution droplets. , 2013, Faraday discussions.

[27]  T. L. Malkin,et al.  Ice cloud processing of ultra-viscous/glassy aerosol particles leads to enhanced ice nucleation ability , 2012 .

[28]  L. Pfister,et al.  Impact of radiative heating, wind shear, temperature variability, and microphysical processes on the structure and evolution of thin cirrus in the tropical tropopause layer , 2011 .

[29]  U. Lohmann,et al.  Global simulations of aerosol processing in clouds , 2008 .

[30]  B. Turpin,et al.  Secondary organic aerosol formation in cloud droplets and aqueous particles (aqSOA): a review of laboratory, field and model studies , 2011 .

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

[32]  C. Bretherton,et al.  Convective Influence on the Heat Balance of the Tropical Tropopause Layer: A Cloud-Resolving Model Study , 2004 .

[33]  K. Froyd,et al.  Aerosol composition of the tropical upper troposphere , 2009 .

[34]  Yinon Rudich,et al.  Extinction efficiencies of coated absorbing aerosols measured by cavity ring down aerosol spectrometry , 2007 .

[35]  T. Ackerman,et al.  Maintenance of tropical tropopause layer cirrus , 2010 .

[36]  Y. Rudich,et al.  Alternative pathway for atmospheric particles growth , 2012, Proceedings of the National Academy of Sciences.

[37]  Jonathan P. Reid,et al.  Measurements of the timescales for the mass transfer of water in glassy aerosol at low relative humidity and ambient temperature , 2011 .

[38]  S. Martin,et al.  Phase of atmospheric secondary organic material affects its reactivity , 2012, Proceedings of the National Academy of Sciences.

[39]  E. Jensen,et al.  State transformations and ice nucleation in amorphous (semi-)solid organic aerosol , 2013 .

[40]  L. Pfister,et al.  Ice nucleation and cloud microphysical properties in tropical tropopause layer cirrus , 2009 .

[41]  U. Pöschl,et al.  Amorphous and crystalline aerosol particles interacting with water vapor: conceptual framework and experimental evidence for restructuring, phase transitions and kinetic limitations , 2009 .

[42]  Scot T. Martin,et al.  Phase Transitions of Aqueous Atmospheric Particles. , 2000, Chemical reviews.

[43]  C. Twohy,et al.  Clarifying the Dominant Sources and Mechanisms of Cirrus Cloud Formation , 2013, Science.

[44]  Ulrich Pöschl,et al.  Glass transition and phase state of organic compounds: dependency on molecular properties and implications for secondary organic aerosols in the atmosphere. , 2011, Physical chemistry chemical physics : PCCP.

[45]  T. L. Malkin,et al.  Glassy aerosols with a range of compositions nucleate ice heterogeneously at cirrus temperatures , 2012 .

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

[47]  K. Froyd,et al.  Aerosols that form subvisible cirrus at the tropical tropopause , 2010 .

[48]  Klaus Gierens,et al.  The global distribution of ice‐supersaturated regions as seen by the Microwave Limb Sounder , 2003 .

[49]  Yinon Rudich,et al.  Atmospheric HULIS : how humic-like are they ? A comprehensive and critical review , 2005 .

[50]  Mark Pinsky,et al.  Turbulent effects on the microphysics and initiation of warm rain in deep convective clouds: 2-D simulations by a spectral mixed-phase microphysics cloud model , 2012 .

[51]  B. Turpin,et al.  Aqueous chemistry and its role in secondary organic aerosol (SOA) formation , 2010 .

[52]  Y. Rudich,et al.  The complex refractive index of atmospheric and model humic-like substances (HULIS) retrieved by a cavity ring down aerosol spectrometer (CRD-AS). , 2008, Faraday discussions.

[53]  William R. Cotton,et al.  Convective cloud downdraft structure: An interpretive survey , 1985 .

[54]  Pablo G. Debenedetti,et al.  Engineering pharmaceutical stability with amorphous solids , 2002 .