State transformations and ice nucleation in amorphous (semi-)solid organic aerosol

Amorphous (semi-)solid organic aerosol particles have the potential to serve as surfaces for heterogeneous ice nucleation in cirrus clouds. Raman spectroscopy and optical microscopy have been used in conjunction with a cold stage to examine water uptake and ice nucleation on individual amorphous (se...

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Main Authors: K. J. Baustian, M. E. Wise, E. J. Jensen, G. P. Schill, M. A. Freedman, M. A. Tolbert
Format: Article
Language:English
Published: Copernicus Publications 2013-06-01
Series:Atmospheric Chemistry and Physics
Online Access:http://www.atmos-chem-phys.net/13/5615/2013/acp-13-5615-2013.pdf
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spelling doaj-eec523b9ff40468182c4c365790b31af2020-11-25T00:24:15ZengCopernicus PublicationsAtmospheric Chemistry and Physics1680-73161680-73242013-06-0113115615562810.5194/acp-13-5615-2013State transformations and ice nucleation in amorphous (semi-)solid organic aerosolK. J. BaustianM. E. WiseE. J. JensenG. P. SchillM. A. FreedmanM. A. TolbertAmorphous (semi-)solid organic aerosol particles have the potential to serve as surfaces for heterogeneous ice nucleation in cirrus clouds. Raman spectroscopy and optical microscopy have been used in conjunction with a cold stage to examine water uptake and ice nucleation on individual amorphous (semi-)solid particles at atmospherically relevant temperatures (200–273 K). Three organic compounds considered proxies for atmospheric secondary organic aerosol (SOA) were used in this investigation: sucrose, citric acid and glucose. Internally mixed particles consisting of each organic and ammonium sulfate were also investigated. <br><br> Results from water uptake experiments followed the shape of a humidity-induced glass transition (<i>T</i><sub>g</sub>(RH)) curve and were used to construct state diagrams for each organic and corresponding mixture. Experimentally derived <i>T</i><sub>g</sub>(RH) curves are in good agreement with theoretical predictions of <i>T</i><sub>g</sub>(RH) following the approach of Koop et al. (2011). A unique humidity-induced glass transition point on each state diagram, <i>T</i><sub>g</sub>'(RH), was used to quantify and compare results from this study to previous works. Values of <i>T</i><sub>g</sub>'(RH) determined for sucrose, glucose and citric acid glasses were 236, 230 and 220 K, respectively. Values of <i>T</i><sub>g</sub>'(RH) for internally mixed organic/sulfate particles were always significantly lower; 210, 207 and 215 K for sucrose/sulfate, glucose/sulfate and citric acid/sulfate, respectively. <br><br> All investigated SOA proxies were observed to act as heterogeneous ice nuclei at tropospheric temperatures. Heterogeneous ice nucleation on pure organic particles occurred at <i>S</i><sub>ice</sub> = 1.1–1.4 for temperatures below 235 K. Particles consisting of 1:1 organic-sulfate mixtures took up water over a greater range of conditions but were in some cases also observed to heterogeneously nucleate ice at temperatures below 202 K (<i>S</i><sub>ice</sub>= 1.25–1.38). <br><br> Polynomial curves were fitted to experimental water uptake data and then incorporated into the Community Aerosol Radiation Model for Atmospheres (CARMA) along with the predicted range of humidity-induced glass transition temperatures for atmospheric SOA from Koop et al. (2011). Model results suggest that organic and organic/sulfate aerosol could be glassy more than 60% of the time in the midlatitude upper troposphere and more than 40% of the time in the tropical tropopause region (TTL). At conditions favorable for ice formation (<i>S</i><sub>ice</sub> > 1), particles in the TTL are expected to be glassy more than 50% of the time for temperatures below 200 K. Results from this study suggests that amorphous (semi-)solid organic particles are often present in the upper troposphere and that heterogeneous ice formation on this type of particle may play an important role in cirrus cloud formation.http://www.atmos-chem-phys.net/13/5615/2013/acp-13-5615-2013.pdf
collection DOAJ
language English
format Article
sources DOAJ
author K. J. Baustian
M. E. Wise
E. J. Jensen
G. P. Schill
M. A. Freedman
M. A. Tolbert
spellingShingle K. J. Baustian
M. E. Wise
E. J. Jensen
G. P. Schill
M. A. Freedman
M. A. Tolbert
State transformations and ice nucleation in amorphous (semi-)solid organic aerosol
Atmospheric Chemistry and Physics
author_facet K. J. Baustian
M. E. Wise
E. J. Jensen
G. P. Schill
M. A. Freedman
M. A. Tolbert
author_sort K. J. Baustian
title State transformations and ice nucleation in amorphous (semi-)solid organic aerosol
title_short State transformations and ice nucleation in amorphous (semi-)solid organic aerosol
title_full State transformations and ice nucleation in amorphous (semi-)solid organic aerosol
title_fullStr State transformations and ice nucleation in amorphous (semi-)solid organic aerosol
title_full_unstemmed State transformations and ice nucleation in amorphous (semi-)solid organic aerosol
title_sort state transformations and ice nucleation in amorphous (semi-)solid organic aerosol
publisher Copernicus Publications
series Atmospheric Chemistry and Physics
issn 1680-7316
1680-7324
publishDate 2013-06-01
description Amorphous (semi-)solid organic aerosol particles have the potential to serve as surfaces for heterogeneous ice nucleation in cirrus clouds. Raman spectroscopy and optical microscopy have been used in conjunction with a cold stage to examine water uptake and ice nucleation on individual amorphous (semi-)solid particles at atmospherically relevant temperatures (200–273 K). Three organic compounds considered proxies for atmospheric secondary organic aerosol (SOA) were used in this investigation: sucrose, citric acid and glucose. Internally mixed particles consisting of each organic and ammonium sulfate were also investigated. <br><br> Results from water uptake experiments followed the shape of a humidity-induced glass transition (<i>T</i><sub>g</sub>(RH)) curve and were used to construct state diagrams for each organic and corresponding mixture. Experimentally derived <i>T</i><sub>g</sub>(RH) curves are in good agreement with theoretical predictions of <i>T</i><sub>g</sub>(RH) following the approach of Koop et al. (2011). A unique humidity-induced glass transition point on each state diagram, <i>T</i><sub>g</sub>'(RH), was used to quantify and compare results from this study to previous works. Values of <i>T</i><sub>g</sub>'(RH) determined for sucrose, glucose and citric acid glasses were 236, 230 and 220 K, respectively. Values of <i>T</i><sub>g</sub>'(RH) for internally mixed organic/sulfate particles were always significantly lower; 210, 207 and 215 K for sucrose/sulfate, glucose/sulfate and citric acid/sulfate, respectively. <br><br> All investigated SOA proxies were observed to act as heterogeneous ice nuclei at tropospheric temperatures. Heterogeneous ice nucleation on pure organic particles occurred at <i>S</i><sub>ice</sub> = 1.1–1.4 for temperatures below 235 K. Particles consisting of 1:1 organic-sulfate mixtures took up water over a greater range of conditions but were in some cases also observed to heterogeneously nucleate ice at temperatures below 202 K (<i>S</i><sub>ice</sub>= 1.25–1.38). <br><br> Polynomial curves were fitted to experimental water uptake data and then incorporated into the Community Aerosol Radiation Model for Atmospheres (CARMA) along with the predicted range of humidity-induced glass transition temperatures for atmospheric SOA from Koop et al. (2011). Model results suggest that organic and organic/sulfate aerosol could be glassy more than 60% of the time in the midlatitude upper troposphere and more than 40% of the time in the tropical tropopause region (TTL). At conditions favorable for ice formation (<i>S</i><sub>ice</sub> > 1), particles in the TTL are expected to be glassy more than 50% of the time for temperatures below 200 K. Results from this study suggests that amorphous (semi-)solid organic particles are often present in the upper troposphere and that heterogeneous ice formation on this type of particle may play an important role in cirrus cloud formation.
url http://www.atmos-chem-phys.net/13/5615/2013/acp-13-5615-2013.pdf
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