American Association for Aerosol Research - Abstract Submission

AAAR 35th Annual Conference
October 17 - October 21, 2016
Oregon Convention Center
Portland, Oregon, USA

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Phase Separation, Morphology, and Diffusivity of alpha-Pinene Secondary Organic Matter Determined using Optical Tweezers

KYLE GORKOWSKI, Neil Donahue, Ryan Sullivan, Carnegie Mellon University

     Abstract Number: 127
     Working Group: Single Aerosol Particle Studies - Techniques and Instrumentation

Abstract
Atmospheric aerosols contain a wide variety of organic and/or inorganic components and can phase-separate into distinct liquid phases, resulting in either a core-shell or a partial-shell particle morphology. Understanding and predicting when each of these morphologies forms is critical to understanding gas-particle interactions. We conducted experiments exploring phase-separation of droplets suspended using aerosol optical tweezers (AOT). The droplet levitation and the surface resonant whispering gallery modes (WGMs), retrieved in the cavity enhanced Raman spectrum, provide a unique direct and real-time assessment of the droplet’s morphology.

We performed the first optical tweezers experiment on droplets to which secondary organic matter (SOM) was added through in situ precursor ozonolysis directly in the tweezing chamber. The alpha-pinene SOM formed a composite droplet with separate phases when added to an aqueous salt or a squalane droplet, producing a shell of secondary organic matter. Using this determined morphology and the rapid evaporation of squalane observed by Robinson et al. (2015) in an aerosol population chamber experiment, we can conclude that squalane has no observable diffusion limitations through alpha-pinene secondary organic matter. Using spreading coefficients, we can bound the surface tension of alpha-pinene SOM and conclude that the air-liquid surface tension of alpha-pinene SOM is less than or equal to that of squalane, 28 mN/m. This, in turn, helps to constrain the Kelvin diameter for condensation of alpha-pinene SOM onto ultrafine particles soon after nucleation in the atmosphere. Analysis of the WGMs in the Raman spectrum allows us to conclude that the nucleated submicron SOM particles that coagulated with the trapped droplet must quickly spread across the droplet under a timescale much shorter than the Raman spectrum acquisition time of 2 seconds, otherwise the WGMs would not have been present.