Abstract

Abstract. Atmospheric dust rich in illite is transported globally from arid regions and impacts cloud properties through the nucleation of ice. We present measurements of ice nucleation in water droplets containing known quantities of an illite rich powder under atmospherically relevant conditions. The illite rich powder used here, NX illite, has a similar mineralogical composition to atmospheric mineral dust sampled in remote locations, i.e. dust which has been subject to long range transport, cloud processing and sedimentation. Arizona Test Dust, which is used in other ice nucleation studies as a model atmospheric dust, has a significantly different mineralogical composition and we suggest that NX illite is a better surrogate of natural atmospheric dust. Using optical microscopy, heterogeneous nucleation in the immersion mode by NX illite was observed to occur dominantly between 246 K and the homogeneous freezing limit. In general, higher freezing temperatures were observed when larger surface areas of NX illite were present within the drops. Homogenous nucleation was observed to occur in droplets containing low surface areas of NX illite. We show that NX illite exhibits strong particle to particle variability in terms of ice nucleating ability, with ~1 in 105 particles dominating ice nucleation when high surface areas were present. In fact, this work suggests that the bulk of atmospheric mineral dust particles may be less efficient at nucleating ice than assumed in current model parameterisations. For droplets containing ≤2 × 10−6 cm2 of NX illite, freezing temperatures did not noticeably change when the cooling rate was varied by an order of magnitude. The data obtained during cooling experiments (surface area ≤2 × 10−6 cm2) is shown to be inconsistent with the single component stochastic model, but is well described by the singular model (ns(236.2 K ≤ T ≤ 247.5 K) = exp(6.53043 × 104− 8.2153088 × 102T + 3.446885376T2 − 4.822268 × 10−3T3). However, droplets continued to freeze when the temperature was held constant, which is inconsistent with the time independent singular model. We show that this apparent discrepancy can be resolved using a multiple component stochastic model in which it is assumed that there are many types of nucleation sites, each with a unique temperature dependent nucleation coefficient. Cooling rate independence can be achieved with this time dependent model if the nucleation rate coefficients increase very rapidly with decreasing temperature, thus reconciling our measurement of nucleation at constant temperature with the cooling rate independence.

Highlights

  • Ice formation is difficult to quantitatively understand in the Earth’s atmosphere. This is in part because it is governed by kinetics, with phase changes only occurring under nonequilibrium conditions (Martin, 2000)

  • Shown for comparison is an experimental fice(T ) curve for pure water droplets for the same cooling rate (5 K min−1) (Murray et al, 2010), which indicates that the NX illite caused heterogeneous nucleation

  • Heterogeneous nucleation by NX illite was found to occur over a range of temperatures, dominantly between 246 K and the homogeneous limit

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Summary

Introduction

Ice formation is difficult to quantitatively understand in the Earth’s atmosphere. This is in part because it is governed by kinetics, with phase changes only occurring under nonequilibrium conditions (Martin, 2000). Montmorillonite and kaolinite are both present in the atmosphere, illite has often been observed to be the most abundant airborne clay mineral (Chester et al, 1972; Glaccum and Prospero, 1980; Delany et al, 1967; Arnold et al, 1998) Arizona Test Dust (ATD) has been widely used as a surrogate of atmospheric dust in ice nucleation studies, but X-ray diffraction analysis reveal that it has a substantially different composition to sampled atmospheric dusts (see Fig. 1) It is much richer in feldspars and contains a high proportion of uncommon clays. The results are interpreted using several theoretical approaches and parameterised for use in atmospheric models

Theoretical background
The singular model
The single component stochastic model
Methods of combining time dependence with particle to particle variability
Experimental
Materials
Characterisation of NX illite
Heterogeneous freezing temperatures
Cooling rate dependence
K min-1
A high and low surface area regime
The single component stochastic model versus the singular model
Isothermal experiments in the low surface area regime
Summary and conclusions
Full Text
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