The Fifth International Workshop on Ice Nucleation phase 2 (FIN-02): laboratory intercomparison of ice nucleation measurements
<p>The second phase of the Fifth International Ice Nucleation Workshop (FIN-02) involved the gathering of a large number of researchers at the Karlsruhe Institute of Technology's Aerosol Interactions and Dynamics of the Atmosphere (AIDA) facility to promote characterization and underst...
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Format: | Article |
Language: | English |
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Copernicus Publications
2018-11-01
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Series: | Atmospheric Measurement Techniques |
Online Access: | https://www.atmos-meas-tech.net/11/6231/2018/amt-11-6231-2018.pdf |
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collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
P. J. DeMott O. Möhler D. J. Cziczo D. J. Cziczo N. Hiranuma N. Hiranuma M. D. Petters S. S. Petters S. S. Petters F. Belosi H. G. Bingemer S. D. Brooks C. Budke M. Burkert-Kohn K. N. Collier A. Danielczok A. Danielczok O. Eppers L. Felgitsch S. Garimella S. Garimella H. Grothe P. Herenz T. C. J. Hill K. Höhler Z. A. Kanji A. Kiselev T. Koop T. B. Kristensen T. B. Kristensen K. Krüger K. Krüger G. Kulkarni E. J. T. Levin B. J. Murray A. Nicosia A. Nicosia D. O'Sullivan D. O'Sullivan A. Peckhaus A. Peckhaus M. J. Polen H. C. Price H. C. Price N. Reicher D. A. Rothenberg Y. Rudich G. Santachiara T. Schiebel J. Schrod T. M. Seifried F. Stratmann R. C. Sullivan K. J. Suski K. J. Suski M. Szakáll H. P. Taylor R. Ullrich J. Vergara-Temprado J. Vergara-Temprado R. Wagner T. F. Whale T. F. Whale D. Weber A. Welti A. Welti T. W. Wilson T. W. Wilson M. J. Wolf J. Zenker |
spellingShingle |
P. J. DeMott O. Möhler D. J. Cziczo D. J. Cziczo N. Hiranuma N. Hiranuma M. D. Petters S. S. Petters S. S. Petters F. Belosi H. G. Bingemer S. D. Brooks C. Budke M. Burkert-Kohn K. N. Collier A. Danielczok A. Danielczok O. Eppers L. Felgitsch S. Garimella S. Garimella H. Grothe P. Herenz T. C. J. Hill K. Höhler Z. A. Kanji A. Kiselev T. Koop T. B. Kristensen T. B. Kristensen K. Krüger K. Krüger G. Kulkarni E. J. T. Levin B. J. Murray A. Nicosia A. Nicosia D. O'Sullivan D. O'Sullivan A. Peckhaus A. Peckhaus M. J. Polen H. C. Price H. C. Price N. Reicher D. A. Rothenberg Y. Rudich G. Santachiara T. Schiebel J. Schrod T. M. Seifried F. Stratmann R. C. Sullivan K. J. Suski K. J. Suski M. Szakáll H. P. Taylor R. Ullrich J. Vergara-Temprado J. Vergara-Temprado R. Wagner T. F. Whale T. F. Whale D. Weber A. Welti A. Welti T. W. Wilson T. W. Wilson M. J. Wolf J. Zenker The Fifth International Workshop on Ice Nucleation phase 2 (FIN-02): laboratory intercomparison of ice nucleation measurements Atmospheric Measurement Techniques |
author_facet |
P. J. DeMott O. Möhler D. J. Cziczo D. J. Cziczo N. Hiranuma N. Hiranuma M. D. Petters S. S. Petters S. S. Petters F. Belosi H. G. Bingemer S. D. Brooks C. Budke M. Burkert-Kohn K. N. Collier A. Danielczok A. Danielczok O. Eppers L. Felgitsch S. Garimella S. Garimella H. Grothe P. Herenz T. C. J. Hill K. Höhler Z. A. Kanji A. Kiselev T. Koop T. B. Kristensen T. B. Kristensen K. Krüger K. Krüger G. Kulkarni E. J. T. Levin B. J. Murray A. Nicosia A. Nicosia D. O'Sullivan D. O'Sullivan A. Peckhaus A. Peckhaus M. J. Polen H. C. Price H. C. Price N. Reicher D. A. Rothenberg Y. Rudich G. Santachiara T. Schiebel J. Schrod T. M. Seifried F. Stratmann R. C. Sullivan K. J. Suski K. J. Suski M. Szakáll H. P. Taylor R. Ullrich J. Vergara-Temprado J. Vergara-Temprado R. Wagner T. F. Whale T. F. Whale D. Weber A. Welti A. Welti T. W. Wilson T. W. Wilson M. J. Wolf J. Zenker |
author_sort |
P. J. DeMott |
title |
The Fifth International Workshop on Ice Nucleation phase 2 (FIN-02): laboratory intercomparison of ice nucleation measurements |
title_short |
The Fifth International Workshop on Ice Nucleation phase 2 (FIN-02): laboratory intercomparison of ice nucleation measurements |
title_full |
The Fifth International Workshop on Ice Nucleation phase 2 (FIN-02): laboratory intercomparison of ice nucleation measurements |
title_fullStr |
The Fifth International Workshop on Ice Nucleation phase 2 (FIN-02): laboratory intercomparison of ice nucleation measurements |
title_full_unstemmed |
The Fifth International Workshop on Ice Nucleation phase 2 (FIN-02): laboratory intercomparison of ice nucleation measurements |
title_sort |
fifth international workshop on ice nucleation phase 2 (fin-02): laboratory intercomparison of ice nucleation measurements |
publisher |
Copernicus Publications |
series |
Atmospheric Measurement Techniques |
issn |
1867-1381 1867-8548 |
publishDate |
2018-11-01 |
description |
<p>The second phase of the Fifth International Ice Nucleation Workshop (FIN-02)
involved the gathering of a large number of researchers at the Karlsruhe
Institute of Technology's Aerosol Interactions and Dynamics of the Atmosphere
(AIDA) facility to promote characterization and understanding of ice
nucleation measurements made by a variety of methods used worldwide.
Compared to the previous workshop in 2007, participation was doubled,
reflecting a vibrant research area. Experimental methods involved sampling of
aerosol particles by direct processing ice nucleation measuring systems from
the same volume of air in separate experiments using different ice nucleating
particle (INP) types, and collections of aerosol particle samples onto
filters or into liquid for sharing amongst measurement techniques that
post-process these samples. In this manner, any errors introduced by
differences in generation methods when samples are shared across laboratories
were mitigated. Furthermore, as much as possible, aerosol particle size
distribution was controlled so that the size limitations of different methods
were minimized. The results presented here use data from the workshop to
assess the comparability of immersion freezing measurement methods activating
INPs in bulk suspensions, methods that activate INPs in condensation and/or
immersion freezing modes as single particles on a substrate, continuous flow
diffusion chambers (CFDCs) directly sampling and processing particles well
above water saturation to maximize immersion and subsequent freezing of
aerosol particles, and expansion cloud chamber simulations in which liquid
cloud droplets were first activated on aerosol particles prior to freezing.
The AIDA expansion chamber measurements are expected to be the closest
representation to INP activation in atmospheric cloud parcels in these
comparisons, due to exposing particles freely to adiabatic cooling.</p><p>The different particle types used as INPs included the minerals illite NX and
potassium feldspar (K-feldspar), two natural soil dusts representative of arable sandy loam
(Argentina) and highly erodible sandy dryland (Tunisia) soils, respectively,
and a bacterial INP (Snomax<span style="position:relative; bottom:0.5em; " class="text">®</span>). Considered
together, the agreement among post-processed immersion freezing measurements
of the numbers and fractions of particles active at different temperatures
following bulk collection of particles into liquid was excellent, with
possible temperature uncertainties inferred to be a key factor in determining
INP uncertainties. Collection onto filters for rinsing versus directly into
liquid in impingers made little difference. For methods that activated
collected single particles on a substrate at a controlled humidity at or
above water saturation, agreement with immersion freezing methods was good in
most cases, but was biased low in a few others for reasons that have not been
resolved, but could relate to water vapor competition effects. Amongst
CFDC-style instruments, various factors requiring (variable) higher
supersaturations to achieve equivalent immersion freezing activation dominate
the uncertainty between these measurements, and for comparison with bulk
immersion freezing methods. When operated above water saturation to include
assessment of immersion freezing, CFDC measurements often measured at or
above the upper bound of immersion freezing device measurements, but often
underestimated INP concentration in comparison to an immersion freezing
method that first activates all particles into liquid droplets prior to
cooling (the PIMCA-PINC device, or Portable Immersion Mode Cooling chAmber–Portable Ice Nucleation Chamber), and typically slightly underestimated INP
number concentrations in comparison to cloud parcel expansions in the AIDA
chamber; this can be largely mitigated when it is possible to raise the
relative humidity to sufficiently high values in the CFDCs, although this is
not always possible operationally.</p><p>Correspondence of measurements of INPs among direct sampling and
post-processing systems varied depending on the INP type. Agreement was best
for Snomax<span style="position:relative; bottom:0.5em; " class="text">®</span> particles in the temperature regime
colder than −10 °C, where their ice nucleation activity is nearly
maximized and changes very little with temperature. At temperatures warmer than
−10 °C, Snomax<span style="position:relative; bottom:0.5em; " class="text">®</span> INP measurements (all
via freezing of suspensions) demonstrated discrepancies consistent with
previous reports of the instability of its protein aggregates that appear to
make it less suitable as a calibration INP at these temperatures. For
Argentinian soil dust particles, there was excellent agreement across all
measurement methods; measures ranged within 1 order of magnitude for INP
number concentrations, active fractions and calculated active site densities
over a 25 to 30 °C range and 5 to 8 orders of corresponding
magnitude change in number concentrations. This was also the case for all
temperatures warmer than −25 °C in Tunisian dust experiments. In
contrast, discrepancies in measurements of INP concentrations or active site
densities that exceeded 2 orders of magnitude across a broad range of temperature
measurements found at temperatures warmer than −25 °C in a previous study were
replicated for illite NX. Discrepancies also exceeded 2 orders of magnitude at
temperatures of −20 to −25 °C for potassium feldspar (K-feldspar), but these coincided
with the range of temperatures at which INP concentrations increase rapidly at
approximately an order of magnitude per 2 °C cooling for
K-feldspar.</p><p>These few discrepancies did not outweigh the overall positive outcomes of the
workshop activity, nor the future utility of this data set or future similar
efforts for resolving remaining measurement issues. Measurements of the same
materials were repeatable over the time of the workshop and demonstrated
strong consistency with prior studies, as reflected by agreement of data
broadly with parameterizations of different specific or general (e.g., soil
dust) aerosol types. The divergent measurements of the INP activity of illite
NX by direct versus post-processing methods were not repeated for other
particle types, and the Snomax<span style="position:relative; bottom:0.5em; " class="text">®</span> data
demonstrated that, at least for a biological INP type, there is no expected
measurement bias between bulk collection and direct immediately processed
freezing methods to as warm as −10 °C. Since particle size ranges
were limited for this workshop, it can be expected that for atmospheric
populations of INPs, measurement discrepancies will appear due to the
different capabilities of methods for sampling the full aerosol size
distribution, or due to limitations on achieving sufficient water
supersaturations to fully capture immersion freezing in direct processing
instruments. Overall, this workshop presents an improved picture of present
capabilities for measuring INPs than in past workshops, and provides
direction toward addressing remaining measurement issues.</p> |
url |
https://www.atmos-meas-tech.net/11/6231/2018/amt-11-6231-2018.pdf |
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doaj-64c601933748490ca83b47dd984a0ccd2020-11-24T22:18:06ZengCopernicus PublicationsAtmospheric Measurement Techniques1867-13811867-85482018-11-01116231625710.5194/amt-11-6231-2018The Fifth International Workshop on Ice Nucleation phase 2 (FIN-02): laboratory intercomparison of ice nucleation measurementsP. J. DeMott0O. Möhler1D. J. Cziczo2D. J. Cziczo3N. Hiranuma4N. Hiranuma5M. D. Petters6S. S. Petters7S. S. Petters8F. Belosi9H. G. Bingemer10S. D. Brooks11C. Budke12M. Burkert-Kohn13K. N. Collier14A. Danielczok15A. Danielczok16O. Eppers17L. Felgitsch18S. Garimella19S. Garimella20H. Grothe21P. Herenz22T. C. J. Hill23K. Höhler24Z. A. Kanji25A. Kiselev26T. Koop27T. B. Kristensen28T. B. Kristensen29K. Krüger30K. Krüger31G. Kulkarni32E. J. T. Levin33B. J. Murray34A. Nicosia35A. Nicosia36D. O'Sullivan37D. O'Sullivan38A. Peckhaus39A. Peckhaus40M. J. Polen41H. C. Price42H. C. Price43N. Reicher44D. A. Rothenberg45Y. Rudich46G. Santachiara47T. Schiebel48J. Schrod49T. M. Seifried50F. Stratmann51R. C. Sullivan52K. J. Suski53K. J. Suski54M. Szakáll55H. P. Taylor56R. Ullrich57J. Vergara-Temprado58J. Vergara-Temprado59R. Wagner60T. F. Whale61T. F. Whale62D. Weber63A. Welti64A. Welti65T. W. Wilson66T. W. Wilson67M. J. Wolf68J. Zenker69Department of Atmospheric Science, Colorado State University, Fort Collins, CO 80523-1371, USAKarlsruhe Institute of Technology (KIT), Institute of Meteorology and Climate Research (IMK-AAF), Eggenstein-Leopoldshafen, GermanyDepartment of Earth, Atmospheric and Planetary Sciences, Massachusetts Institute of Technology, Cambridge, MA, USADepartment of Civil and Environmental Engineering, Massachusetts Institute of Technology, Cambridge, MA, USAKarlsruhe Institute of Technology (KIT), Institute of Meteorology and Climate Research (IMK-AAF), Eggenstein-Leopoldshafen, Germanynow at: Department of Life, Earth and Environmental Sciences, West Texas A&M University, Canyon, TX, USADepartment of Marine, Earth and Atmospheric Sciences, North Carolina State University, Raleigh, NC, USADepartment of Marine, Earth and Atmospheric Sciences, North Carolina State University, Raleigh, NC, USAnow at: Department of Environmental Sciences and Engineering, University of North Carolina, Chapel Hill, NC, USAInstitute of Atmospheric Sciences and Climate (ISAC-CNR), Bologna, ItalyInstitute for Atmospheric and Environmental Sciences, Goethe University Frankfurt, 60438 Frankfurt am Main, GermanyDepartment of Atmospheric Sciences, Texas A&M University, College Station, TX, USAFaculty of Chemistry, Bielefeld University, Bielefeld, GermanyInstitute for Atmospheric and Climate Science, ETH Zurich, Zurich, SwitzerlandDepartment of Atmospheric Sciences, Texas A&M University, College Station, TX, USAInstitute for Atmospheric and Environmental Sciences, Goethe University Frankfurt, 60438 Frankfurt am Main, Germanynow at: German Weather Service, Satellite-based Climate Monitoring, 63067 Offenbach am Main, GermanyInstitute for Atmospheric Physics, Johannes Gutenberg University, Mainz, GermanyInstitute of Materials Chemistry, TU Wien, Vienna, AustriaDepartment of Earth, Atmospheric and Planetary Sciences, Massachusetts Institute of Technology, Cambridge, MA, USAnow at: ACME AtronOmatic, LLC, Portland, OR, USAInstitute of Materials Chemistry, TU Wien, Vienna, AustriaLeibniz Institute for Tropospheric Research, 04318 Leipzig, GermanyDepartment of Atmospheric Science, Colorado State University, Fort Collins, CO 80523-1371, USAKarlsruhe Institute of Technology (KIT), Institute of Meteorology and Climate Research (IMK-AAF), Eggenstein-Leopoldshafen, GermanyInstitute for Atmospheric and Climate Science, ETH Zurich, Zurich, SwitzerlandKarlsruhe Institute of Technology (KIT), Institute of Meteorology and Climate Research (IMK-AAF), Eggenstein-Leopoldshafen, GermanyFaculty of Chemistry, Bielefeld University, Bielefeld, GermanyLeibniz Institute for Tropospheric Research, 04318 Leipzig, Germanynow at: Division of Nuclear Physics, Lund University, Box 118, Lund 22100, SwedenKarlsruhe Institute of Technology (KIT), Institute of Meteorology and Climate Research (IMK-AAF), Eggenstein-Leopoldshafen, GermanyInstitute for Atmospheric and Environmental Sciences, Goethe University Frankfurt, 60438 Frankfurt am Main, GermanyAtmospheric Sciences and Global Change Division, Pacific Northwest National Laboratory, Richland, WA, USADepartment of Atmospheric Science, Colorado State University, Fort Collins, CO 80523-1371, USAInstitute for Climate and Atmospheric Science, School of Earth and Environment, University of Leeds, Woodhouse Lane, Leeds, LS2 9JT, UKInstitute of Atmospheric Sciences and Climate (ISAC-CNR), Bologna, Italynow at: Laboratoire de Méteorologie Physique (LaMP-CNRS), Aubière, FranceInstitute for Climate and Atmospheric Science, School of Earth and Environment, University of Leeds, Woodhouse Lane, Leeds, LS2 9JT, UKnow at: NHS Digital,1 Trevelyan Square, Boar Lane, Leeds, LS1 6AE, UKKarlsruhe Institute of Technology (KIT), Institute of Meteorology and Climate Research (IMK-AAF), Eggenstein-Leopoldshafen, Germanynow at: German Aerospace Center (DLR), Institute of Technical Physics, 70569 Stuttgart, GermanyCenter for Atmospheric Particle Studies, Carnegie Mellon University, Pittsburgh, PA, USAInstitute for Climate and Atmospheric Science, School of Earth and Environment, University of Leeds, Woodhouse Lane, Leeds, LS2 9JT, UKnow at: Facility for Airborne Atmospheric Measurements, Cranfield, MK43 0AL, UKDepartment of Earth and Planetary Sciences, Weizmann Institute, Rehovot 76100, IsraelDepartment of Earth, Atmospheric and Planetary Sciences, Massachusetts Institute of Technology, Cambridge, MA, USADepartment of Earth and Planetary Sciences, Weizmann Institute, Rehovot 76100, IsraelInstitute of Atmospheric Sciences and Climate (ISAC-CNR), Bologna, ItalyKarlsruhe Institute of Technology (KIT), Institute of Meteorology and Climate Research (IMK-AAF), Eggenstein-Leopoldshafen, GermanyInstitute for Atmospheric and Environmental Sciences, Goethe University Frankfurt, 60438 Frankfurt am Main, GermanyInstitute of Materials Chemistry, TU Wien, Vienna, AustriaLeibniz Institute for Tropospheric Research, 04318 Leipzig, GermanyCenter for Atmospheric Particle Studies, Carnegie Mellon University, Pittsburgh, PA, USADepartment of Atmospheric Science, Colorado State University, Fort Collins, CO 80523-1371, USAnow at: Pacific Northwest National Laboratory, Richland, WA, USAInstitute for Atmospheric Physics, Johannes Gutenberg University, Mainz, GermanyDepartment of Marine, Earth and Atmospheric Sciences, North Carolina State University, Raleigh, NC, USAKarlsruhe Institute of Technology (KIT), Institute of Meteorology and Climate Research (IMK-AAF), Eggenstein-Leopoldshafen, GermanyInstitute for Atmospheric and Climate Science, ETH Zurich, Zurich, SwitzerlandInstitute for Climate and Atmospheric Science, School of Earth and Environment, University of Leeds, Woodhouse Lane, Leeds, LS2 9JT, UKKarlsruhe Institute of Technology (KIT), Institute of Meteorology and Climate Research (IMK-AAF), Eggenstein-Leopoldshafen, GermanyInstitute for Climate and Atmospheric Science, School of Earth and Environment, University of Leeds, Woodhouse Lane, Leeds, LS2 9JT, UKnow at: School of Chemistry, University of Leeds, Leeds, LS2 9JT, UKInstitute for Atmospheric and Environmental Sciences, Goethe University Frankfurt, 60438 Frankfurt am Main, GermanyLeibniz Institute for Tropospheric Research, 04318 Leipzig, Germanynow at: Finnish Meteorological Institute, 00101 Helsinki, FinlandInstitute for Climate and Atmospheric Science, School of Earth and Environment, University of Leeds, Woodhouse Lane, Leeds, LS2 9JT, UKnow at: Owlstone Medical Ltd., 162 Cambridge Science Park, Milton Road, Cambridge, CB4 0GH, UKDepartment of Earth, Atmospheric and Planetary Sciences, Massachusetts Institute of Technology, Cambridge, MA, USADepartment of Atmospheric Sciences, Texas A&M University, College Station, TX, USA<p>The second phase of the Fifth International Ice Nucleation Workshop (FIN-02) involved the gathering of a large number of researchers at the Karlsruhe Institute of Technology's Aerosol Interactions and Dynamics of the Atmosphere (AIDA) facility to promote characterization and understanding of ice nucleation measurements made by a variety of methods used worldwide. Compared to the previous workshop in 2007, participation was doubled, reflecting a vibrant research area. Experimental methods involved sampling of aerosol particles by direct processing ice nucleation measuring systems from the same volume of air in separate experiments using different ice nucleating particle (INP) types, and collections of aerosol particle samples onto filters or into liquid for sharing amongst measurement techniques that post-process these samples. In this manner, any errors introduced by differences in generation methods when samples are shared across laboratories were mitigated. Furthermore, as much as possible, aerosol particle size distribution was controlled so that the size limitations of different methods were minimized. The results presented here use data from the workshop to assess the comparability of immersion freezing measurement methods activating INPs in bulk suspensions, methods that activate INPs in condensation and/or immersion freezing modes as single particles on a substrate, continuous flow diffusion chambers (CFDCs) directly sampling and processing particles well above water saturation to maximize immersion and subsequent freezing of aerosol particles, and expansion cloud chamber simulations in which liquid cloud droplets were first activated on aerosol particles prior to freezing. The AIDA expansion chamber measurements are expected to be the closest representation to INP activation in atmospheric cloud parcels in these comparisons, due to exposing particles freely to adiabatic cooling.</p><p>The different particle types used as INPs included the minerals illite NX and potassium feldspar (K-feldspar), two natural soil dusts representative of arable sandy loam (Argentina) and highly erodible sandy dryland (Tunisia) soils, respectively, and a bacterial INP (Snomax<span style="position:relative; bottom:0.5em; " class="text">®</span>). Considered together, the agreement among post-processed immersion freezing measurements of the numbers and fractions of particles active at different temperatures following bulk collection of particles into liquid was excellent, with possible temperature uncertainties inferred to be a key factor in determining INP uncertainties. Collection onto filters for rinsing versus directly into liquid in impingers made little difference. For methods that activated collected single particles on a substrate at a controlled humidity at or above water saturation, agreement with immersion freezing methods was good in most cases, but was biased low in a few others for reasons that have not been resolved, but could relate to water vapor competition effects. Amongst CFDC-style instruments, various factors requiring (variable) higher supersaturations to achieve equivalent immersion freezing activation dominate the uncertainty between these measurements, and for comparison with bulk immersion freezing methods. When operated above water saturation to include assessment of immersion freezing, CFDC measurements often measured at or above the upper bound of immersion freezing device measurements, but often underestimated INP concentration in comparison to an immersion freezing method that first activates all particles into liquid droplets prior to cooling (the PIMCA-PINC device, or Portable Immersion Mode Cooling chAmber–Portable Ice Nucleation Chamber), and typically slightly underestimated INP number concentrations in comparison to cloud parcel expansions in the AIDA chamber; this can be largely mitigated when it is possible to raise the relative humidity to sufficiently high values in the CFDCs, although this is not always possible operationally.</p><p>Correspondence of measurements of INPs among direct sampling and post-processing systems varied depending on the INP type. Agreement was best for Snomax<span style="position:relative; bottom:0.5em; " class="text">®</span> particles in the temperature regime colder than −10 °C, where their ice nucleation activity is nearly maximized and changes very little with temperature. At temperatures warmer than −10 °C, Snomax<span style="position:relative; bottom:0.5em; " class="text">®</span> INP measurements (all via freezing of suspensions) demonstrated discrepancies consistent with previous reports of the instability of its protein aggregates that appear to make it less suitable as a calibration INP at these temperatures. For Argentinian soil dust particles, there was excellent agreement across all measurement methods; measures ranged within 1 order of magnitude for INP number concentrations, active fractions and calculated active site densities over a 25 to 30 °C range and 5 to 8 orders of corresponding magnitude change in number concentrations. This was also the case for all temperatures warmer than −25 °C in Tunisian dust experiments. In contrast, discrepancies in measurements of INP concentrations or active site densities that exceeded 2 orders of magnitude across a broad range of temperature measurements found at temperatures warmer than −25 °C in a previous study were replicated for illite NX. Discrepancies also exceeded 2 orders of magnitude at temperatures of −20 to −25 °C for potassium feldspar (K-feldspar), but these coincided with the range of temperatures at which INP concentrations increase rapidly at approximately an order of magnitude per 2 °C cooling for K-feldspar.</p><p>These few discrepancies did not outweigh the overall positive outcomes of the workshop activity, nor the future utility of this data set or future similar efforts for resolving remaining measurement issues. Measurements of the same materials were repeatable over the time of the workshop and demonstrated strong consistency with prior studies, as reflected by agreement of data broadly with parameterizations of different specific or general (e.g., soil dust) aerosol types. The divergent measurements of the INP activity of illite NX by direct versus post-processing methods were not repeated for other particle types, and the Snomax<span style="position:relative; bottom:0.5em; " class="text">®</span> data demonstrated that, at least for a biological INP type, there is no expected measurement bias between bulk collection and direct immediately processed freezing methods to as warm as −10 °C. Since particle size ranges were limited for this workshop, it can be expected that for atmospheric populations of INPs, measurement discrepancies will appear due to the different capabilities of methods for sampling the full aerosol size distribution, or due to limitations on achieving sufficient water supersaturations to fully capture immersion freezing in direct processing instruments. Overall, this workshop presents an improved picture of present capabilities for measuring INPs than in past workshops, and provides direction toward addressing remaining measurement issues.</p>https://www.atmos-meas-tech.net/11/6231/2018/amt-11-6231-2018.pdf |