Abstract

Abstract. Atmospheric ice formation in cirrus clouds is often initiated by aerosol particles that act as ice-nucleating particles. The aerosol–cloud interactions of soot and associated feedbacks remain uncertain, in part because a coherent understanding of the ice nucleation mechanism and activity of soot has not yet emerged. Here, we provide a new framework that predicts ice formation on soot particles via pore condensation and freezing (PCF) that, unlike previous approaches, considers soot particle properties, capturing their vastly different pore properties compared to other aerosol species such as mineral dust. During PCF, water is taken up into pores of the soot aggregates by capillary condensation. At cirrus temperatures, the pore water can freeze homogeneously and subsequently grow into a macroscopic ice crystal. In the soot-PCF framework presented here, the relative humidity conditions required for these steps are derived for different pore types as a function of temperature. The pore types considered here encompass n-membered ring pores that form between n individual spheres within the same layer of primary particles as well as pores in the form of inner cavities that form between two layers of primary particles. We treat soot primary particles as perfect spheres and use the contact angle between soot and water (θsw), the primary particle diameter (Dpp), and the degree of primary particle overlap (overlap coefficient, Cov) to characterize pore properties. We find that three-membered and four-membered ring pores are of the right size for PCF, assuming primary particle sizes typical of atmospheric soot particles. For these pore types, we derive equations that describe the conditions for all three steps of soot PCF, namely capillary condensation, ice nucleation, and ice growth. Since at typical cirrus conditions homogeneous ice nucleation can be considered immediate as soon as the water volume within the pore is large enough to host a critical ice embryo, soot PCF becomes limited by either capillary condensation or ice crystal growth. We use the soot-PCF framework to derive a new equation to parameterize ice formation on soot particles via PCF, based on soot properties that are routinely measured, including the primary particle size, overlap, and the fractal dimension. These properties, along with the number of primary particles making up an aggregate and the contact angle between water and soot, constrain the parameterization. Applying the new parameterization to previously reported laboratory data of ice formation on soot particles provides direct evidence that ice nucleation on soot aggregates takes place via PCF. We conclude that this new framework clarifies the ice formation mechanism on soot particles in cirrus conditions and provides a new perspective to represent ice formation on soot in climate models.

Highlights

  • Incomplete combustion of biomass or fossil fuel produces copious quantities of soot particles, encompassing mixtures of black carbon and organic carbon that are of particular importance in the Earth’s atmosphere

  • A size dependency of ice nucleation was found in the studies of Zhang et al (2020) and Mahrt et al (2018). While these studies reveal significant scatter in terms of the ice nucleation activity, as evident from e.g. the range of onset RHi values observed for different soot types at a given temperature, they indicate that soot particles could represent an eminent source of ice-nucleating particles (INPs) in upper tropospheric conditions, with potentially important implications for cirrus cloud formation and climate

  • The trend of increasing primary particle diameters with increasing thrust levels is consistent with other studies of aircraft soot emissions (Delhaye et al, 2017; Liati et al, 2019; Marhaba et al, 2019). In their detailed transmission electron microscopy (TEM) characterization of aircraft soot from the same engine type, Liati et al (2019) investigated the effect of fuel type on the soot morphology. This was achieved by comparing the primary particle size when burning standard Jet A-1 fuel and a blend of the same fuel, along with 32 % hydro-processed esters and fatty acids (HEFA) biofuel, and analysing soot aggregates collected at thrust levels of 85 % and 4 %

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Summary

Introduction

Incomplete combustion of biomass or fossil fuel produces copious quantities of soot particles, encompassing mixtures of black carbon and organic carbon that are of particular importance in the Earth’s atmosphere. A size dependency of ice nucleation was found in the studies of Zhang et al (2020) and Mahrt et al (2018) While these studies reveal significant scatter in terms of the ice nucleation activity, as evident from e.g. the range of onset RHi values observed for different soot types at a given temperature, they indicate that soot particles could represent an eminent source of INPs in upper tropospheric conditions, with potentially important implications for cirrus cloud formation and climate. Relevant properties for PCF are pore shape, pore size, and the contact angle between the pore surface with water and ice. In the following, we discuss these particle properties with respect to atmospheric soot. The number of pores in a soot aggregate depends on the number of primary particles in the aggregate and their compaction, i.e. fractal dimension

Primary particle size
Overlap between primary particles
Soot aggregate size and compaction
Contact angle
Critical pore size for PCF
Nucleation rates in cirrus conditions
Pore geometry in tetrahedral packing arrangement
Three-membered ring pore
Concave octahedron
Pore geometry in cubic packing arrangement
Four-membered ring pore
Concave cube
Kelvin equation for conical and cylindrical pores
Cylindrical pores
Conical pores
Findings
Slit filling between two adjacent primary particles with liquid water
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