Abstract

Abstract. Secondary organic aerosol (SOA) accounts for a large fraction of submicron particles in the atmosphere. SOA can occur in amorphous solid or semi-solid phase states depending on chemical composition, relative humidity (RH), and temperature. The phase transition between amorphous solid and semi-solid states occurs at the glass transition temperature (Tg). We have recently developed a method to estimate Tg of pure compounds containing carbon, hydrogen, and oxygen atoms (CHO compounds) with molar mass less than 450 g mol−1 based on their molar mass and atomic O : C ratio. In this study, we refine and extend this method for CH and CHO compounds with molar mass up to ∼ 1100 g mol−1 using the number of carbon, hydrogen, and oxygen atoms. We predict viscosity from the Tg-scaled Arrhenius plot of fragility (viscosity vs. Tg∕T) as a function of the fragility parameter D. We compiled D values of organic compounds from the literature and found that D approaches a lower limit of ∼ 10 (±1.7) as the molar mass increases. We estimated the viscosity of α-pinene and isoprene SOA as a function of RH by accounting for the hygroscopic growth of SOA and applying the Gordon–Taylor mixing rule, reproducing previously published experimental measurements very well. Sensitivity studies were conducted to evaluate impacts of Tg, D, the hygroscopicity parameter (κ), and the Gordon–Taylor constant on viscosity predictions. The viscosity of toluene SOA was predicted using the elemental composition obtained by high-resolution mass spectrometry (HRMS), resulting in a good agreement with the measured viscosity. We also estimated the viscosity of biomass burning particles using the chemical composition measured by HRMS with two different ionization techniques: electrospray ionization (ESI) and atmospheric pressure photoionization (APPI). Due to differences in detected organic compounds and signal intensity, predicted viscosities at low RH based on ESI and APPI measurements differ by 2–5 orders of magnitude. Complementary measurements of viscosity and chemical composition are desired to further constrain RH-dependent viscosity in future studies.

Highlights

  • Secondary organic aerosol (SOA) accounts for a large fraction of submicron particles in the atmosphere and plays an important role in climate, air quality, and public health (Goldstein and Galbally, 2007; Jimenez et al, 2009)

  • SOA particles were assumed to be liquid with dynamic viscosity η below 102 Pa s, but a number of recent studies have shown that they can adopt amorphous semisolid (102 ≤ η ≤ 1012 Pa s) or glassy solid (η > 1012 Pa s) states depending on chemical composition and temperature (Zobrist et al, 2008; Koop et al, 2011; Huang et al, 2018; Reid et al, 2018)

  • In this study we have developed an improved parameterization to predict Tg of CH and CHO compounds using the number of carbon, hydrogen, and oxygen that can be applied to higher-molar-mass compounds

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Summary

Introduction

Secondary organic aerosol (SOA) accounts for a large fraction of submicron particles in the atmosphere and plays an important role in climate, air quality, and public health (Goldstein and Galbally, 2007; Jimenez et al, 2009). We have developed a parameterization to estimate Tg of pure organic compounds comprised of carbon, hydrogen, and oxygen (CHO compounds) with molar mass less than 450 g mol−1 based on their molar mass and atomic O : C ratio (Shiraiwa et al, 2017) It has been applied successfully in a global chemistry– climate model to predict Tg and the phase state of atmospheric SOA, which indicated that SOA particles are mostly liquid or semi-solid in the planetary boundary layer, while. This method will be useful for estimations of viscosity of organic particles, for which high-resolution mass spectra are available It can be applied in global or regional models to evaluate the impacts of the particle phase state on the role of SOA in climate and air quality

Glass transition temperature
Viscosity
SOA formed from α-pinene and isoprene
SOA formed from toluene
Biomass burning particles
Findings
Conclusions
Full Text
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