Assessment of the sensitivity of core / shell parameters derived using the single-particle soot photometer to density and refractive index

Black carbon (BC) is the dominant absorbing aerosol in the atmosphere, and plays an important role in climate and human health. The optical properties and cloud condensation nuclei (CCN) activity of soot depend on the amounts (both relative and absolute) of BC and non-refractory material in the part...

Full description

Bibliographic Details
Main Authors: J. W. Taylor, J. D. Allan, D. Liu, M. Flynn, R. Weber, X. Zhang, B. L. Lefer, N. Grossberg, J. Flynn, H. Coe
Format: Article
Language:English
Published: Copernicus Publications 2015-04-01
Series:Atmospheric Measurement Techniques
Online Access:http://www.atmos-meas-tech.net/8/1701/2015/amt-8-1701-2015.pdf
id doaj-a7e53fcee47b428eb26c932dfbb5b6bf
record_format Article
collection DOAJ
language English
format Article
sources DOAJ
author J. W. Taylor
J. D. Allan
D. Liu
M. Flynn
R. Weber
X. Zhang
B. L. Lefer
N. Grossberg
J. Flynn
H. Coe
spellingShingle J. W. Taylor
J. D. Allan
D. Liu
M. Flynn
R. Weber
X. Zhang
B. L. Lefer
N. Grossberg
J. Flynn
H. Coe
Assessment of the sensitivity of core / shell parameters derived using the single-particle soot photometer to density and refractive index
Atmospheric Measurement Techniques
author_facet J. W. Taylor
J. D. Allan
D. Liu
M. Flynn
R. Weber
X. Zhang
B. L. Lefer
N. Grossberg
J. Flynn
H. Coe
author_sort J. W. Taylor
title Assessment of the sensitivity of core / shell parameters derived using the single-particle soot photometer to density and refractive index
title_short Assessment of the sensitivity of core / shell parameters derived using the single-particle soot photometer to density and refractive index
title_full Assessment of the sensitivity of core / shell parameters derived using the single-particle soot photometer to density and refractive index
title_fullStr Assessment of the sensitivity of core / shell parameters derived using the single-particle soot photometer to density and refractive index
title_full_unstemmed Assessment of the sensitivity of core / shell parameters derived using the single-particle soot photometer to density and refractive index
title_sort assessment of the sensitivity of core / shell parameters derived using the single-particle soot photometer to density and refractive index
publisher Copernicus Publications
series Atmospheric Measurement Techniques
issn 1867-1381
1867-8548
publishDate 2015-04-01
description Black carbon (BC) is the dominant absorbing aerosol in the atmosphere, and plays an important role in climate and human health. The optical properties and cloud condensation nuclei (CCN) activity of soot depend on the amounts (both relative and absolute) of BC and non-refractory material in the particles. Mixing between these two components is often represented in models by a core / shell coated sphere. The single-particle soot photometer (SP2) is one of, if not the only, instrument capable of reporting distributions of both core size and coating thickness. Most studies combine the SP2's incandescence and 1064 nm scattering data to report coating properties, but to date there is no consistency in the assumed values of density and refractive index of the core that are used in these calculations, which can greatly affect the reported parameters such as coating thickness. Given that such data are providing an important constraint for model comparisons and comparison between large data sets, it is important that this lack of consistency is addressed. <br><br> In this study we explore the sensitivity of the reported coatings to these parameters. An assessment of the coating properties of freshly emitted, thermodenuded ambient particles demonstrated that a core density of 1.8 g cm<sup>−3</sup> and refractive index of (2.26–1.26<i>i</i>) were the most appropriate to use with ambient soot in the Los Angeles area. Using these parameters generated a distribution with median shell / core ratio of 1.02 ± 0.11, corresponding to a median absolute coating thickness of 2 ± 8 nm. The main source of statistical error in the single-particle data was random variation in the incandescence signals. Other than the sensitivity to core refractive index, the incandescence calibration was the main source of uncertainty when optically determining the average coatings. The refractive index of coatings was found to have only a minor influence. <br><br> This work demonstrates that using this technique the SP2 can accurately determine the average mixing state (externally or internally mixed) of ambient soot within the precision of the instrument calibration. Ambient coatings were measured up to a median shell / core ratio of 1.50 ± 0.11, meaning that this technique is able to resolve absolute changes in mixing state. <br><br> However, when different core parameters were used, the core / shell ratio and the coating thickness were shown to be offset by amounts that could be larger than the atmospheric variability in these parameters, though the results have a similar precision. For comparison, using the core parameters that resulted in the thickest coatings, on the same thermodenuded fresh particles as before, generated a median shell / core ratio of 1.39 ± 0.11, corresponding to a median absolute coating thickness of 30 ± 8 nm. These results must be taken into account when comparing BC coatings measured using this technique, or if using these data for optical or CCN calculations. <br><br> We have determined the most appropriate values of BC density and refractive index to use to measure mixing state at 1064 nm where particle morphology has only a minor effect, but appropriate values to use for optical calculations of nonspherical particles at visible wavelengths will also be subject to similar, significant uncertainties. Without similar constraints as those provided here, constraining the behaviour of BC particles in models using field data will be subject to large systematic measurement uncertainties.
url http://www.atmos-meas-tech.net/8/1701/2015/amt-8-1701-2015.pdf
work_keys_str_mv AT jwtaylor assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
AT jdallan assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
AT dliu assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
AT mflynn assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
AT rweber assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
AT xzhang assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
AT bllefer assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
AT ngrossberg assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
AT jflynn assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
AT hcoe assessmentofthesensitivityofcoreshellparametersderivedusingthesingleparticlesootphotometertodensityandrefractiveindex
_version_ 1725950872747245568
spelling doaj-a7e53fcee47b428eb26c932dfbb5b6bf2020-11-24T21:34:00ZengCopernicus PublicationsAtmospheric Measurement Techniques1867-13811867-85482015-04-01841701171810.5194/amt-8-1701-2015Assessment of the sensitivity of core / shell parameters derived using the single-particle soot photometer to density and refractive indexJ. W. Taylor0J. D. Allan1D. Liu2M. Flynn3R. Weber4X. Zhang5B. L. Lefer6N. Grossberg7J. Flynn8H. Coe9Centre for Atmospheric Science, School of Earth, Atmospheric and Environmental Sciences, University of Manchester, Manchester, UKCentre for Atmospheric Science, School of Earth, Atmospheric and Environmental Sciences, University of Manchester, Manchester, UKCentre for Atmospheric Science, School of Earth, Atmospheric and Environmental Sciences, University of Manchester, Manchester, UKCentre for Atmospheric Science, School of Earth, Atmospheric and Environmental Sciences, University of Manchester, Manchester, UKGeorgia Institute of Technology, Atlanta, GA, USAGeorgia Institute of Technology, Atlanta, GA, USADepartment of Earth and Atmospheric Sciences, University of Houston, Houston, TX, USADepartment of Earth and Atmospheric Sciences, University of Houston, Houston, TX, USADepartment of Earth and Atmospheric Sciences, University of Houston, Houston, TX, USACentre for Atmospheric Science, School of Earth, Atmospheric and Environmental Sciences, University of Manchester, Manchester, UKBlack carbon (BC) is the dominant absorbing aerosol in the atmosphere, and plays an important role in climate and human health. The optical properties and cloud condensation nuclei (CCN) activity of soot depend on the amounts (both relative and absolute) of BC and non-refractory material in the particles. Mixing between these two components is often represented in models by a core / shell coated sphere. The single-particle soot photometer (SP2) is one of, if not the only, instrument capable of reporting distributions of both core size and coating thickness. Most studies combine the SP2's incandescence and 1064 nm scattering data to report coating properties, but to date there is no consistency in the assumed values of density and refractive index of the core that are used in these calculations, which can greatly affect the reported parameters such as coating thickness. Given that such data are providing an important constraint for model comparisons and comparison between large data sets, it is important that this lack of consistency is addressed. <br><br> In this study we explore the sensitivity of the reported coatings to these parameters. An assessment of the coating properties of freshly emitted, thermodenuded ambient particles demonstrated that a core density of 1.8 g cm<sup>−3</sup> and refractive index of (2.26–1.26<i>i</i>) were the most appropriate to use with ambient soot in the Los Angeles area. Using these parameters generated a distribution with median shell / core ratio of 1.02 ± 0.11, corresponding to a median absolute coating thickness of 2 ± 8 nm. The main source of statistical error in the single-particle data was random variation in the incandescence signals. Other than the sensitivity to core refractive index, the incandescence calibration was the main source of uncertainty when optically determining the average coatings. The refractive index of coatings was found to have only a minor influence. <br><br> This work demonstrates that using this technique the SP2 can accurately determine the average mixing state (externally or internally mixed) of ambient soot within the precision of the instrument calibration. Ambient coatings were measured up to a median shell / core ratio of 1.50 ± 0.11, meaning that this technique is able to resolve absolute changes in mixing state. <br><br> However, when different core parameters were used, the core / shell ratio and the coating thickness were shown to be offset by amounts that could be larger than the atmospheric variability in these parameters, though the results have a similar precision. For comparison, using the core parameters that resulted in the thickest coatings, on the same thermodenuded fresh particles as before, generated a median shell / core ratio of 1.39 ± 0.11, corresponding to a median absolute coating thickness of 30 ± 8 nm. These results must be taken into account when comparing BC coatings measured using this technique, or if using these data for optical or CCN calculations. <br><br> We have determined the most appropriate values of BC density and refractive index to use to measure mixing state at 1064 nm where particle morphology has only a minor effect, but appropriate values to use for optical calculations of nonspherical particles at visible wavelengths will also be subject to similar, significant uncertainties. Without similar constraints as those provided here, constraining the behaviour of BC particles in models using field data will be subject to large systematic measurement uncertainties.http://www.atmos-meas-tech.net/8/1701/2015/amt-8-1701-2015.pdf