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Highly Viscous States Affect the Browning of Atmospheric Organic Particulate Matter Pengfei Liu 1 , Yong Jie Li 1 , Yan Wang 1 , Adam Bateman 1 , Yue Zhang 1 , Zhaoheng Gong 1 Allan K Bertram 2 and Scot T Martin 1,* Introduction Zhaoheng Gong , Allan K. Bertram , and Scot T . Martin 1 Harvard University, Cambridge, MA, USA; 2 University of British Columbia, Vancouver, BC, Canada blah blah blah Light-absorbing organic carbon is of great interest because it potentially affects climate and photochemistry. Some types of secondary organic material (SOM) can become light Optical properties Abstract: Initially transparent organic particulate matter (PM) can become shades of light-absorbing brown via particle-phase reactions. When semisolid or solid physical states of organic PM a. blah blah blah organic material (SOM) can become light- absorbing via multiphase reactive processing in the atmosphere, and thereby contribute to so- called “brown carbon” (Updyke et al. 2012). These multiphase browning reactions, however, can possibly be limited by the slow diffusion of reactant molecules in organic matrix under conditions that semisolids or solids prevail (Kuwata & Martin. 2012; Li et al., 2015). semisolid or solid physical states of organic PM prevail, however, the diffusion of reactant molecules can become sufficiently slow to inhibit browning reactions. Experiments show that the production of light-absorbing organonitrogen species from ammonia exposure strongly depended on the RH value. The observed RH-dependent behavior was well captured by a model that considered the diffusivities of both the large molecules making up the organic PM and the small reactant guest b. 280-320 nm Diffusivities Physical state Diffusivity Reactivity Optical properties molecules taken up by the PM. c. 380-420 nm Experimental Figure 5. Changed optical properties of toluene- derived SOM exposed to ammonia at different RH values. (a) Mass absorption coefficient as a function of wavelength; (b) Absorptive indices on left axis and mass absorption coefficients on right axis from 280 to 320 nm (c) Same as panel (b) but for 380 to 420 nm Organic particles were produced by photooxidation of toluene in an Oxidation Flow Reactor (OFR) (Kang et al. 2007; Lambe et al. 2011); In-particle diffusivities of both small (water) and large (organic) molecules were measured by a Q C l Mi bl (QCM) Conclusions Figure 3. (left axis) Self-diffusivity D org and water diffusivity D H2O for toluene-derived SOM; (right axis) mixing timescale for a 100-nm particle. Below 20% RH, fast browning reactions associated with ammonia uptake were kinetically limited by a shallow diffusoreactive length, even as the comparative physical mixing timescale of small molecules was short. Self-diffusivity of large organic molecules making up PM was 10 4 to 10 6 times smaller than Dry Flow cell SOM fil N 2 Quartz Crystal Microbalance (QCM); Toluene-derived SOM particles were exposed to ammonia; Organonitrogen species (C x H y N z + ) were analyzed by the AMS Absorption spectra before and after ammonia exposure were recorded by a UV-VIS spectrometer. Organonitrogen References Upkyke, K.M., et al. Atmos. Environ., 2012, 63, 22-31.. Kuwata, M. & Martin, S.T. PNAS, 2012, 109(43), 17354- 17359. Li, Y.J., et al., Environ. Sci. Tech. 2015, 49, 13264-13274. the small-molecule diffusivity, further inhibiting reactant refreshing near the particle surface. Water uptake Evaporation of organic material Water Figure 1. Diagram of the experimental apparatus for diffusivity measurements RH Quartz crystal SOM film 2 SOM particles NH3 exposure RH Kang, E., et al., Atmos. Chem. Phys. 2007, 7(22), 5727-5744. Lambe, A.T., et al., Atmos. Meas. Tech. 2011, 4, 445-461. Bateman, A.P., Bertram, A.K. & Martin, S.T., J. Phys. Chem. A, 2015, 119, 4386-4395. Song, M. et al., Atmos. Chem. Phys., 2016, 16, 8817-8830. Liu, P.F., et al., PNAS, 2016, 113, 12643-12648. Liu, P.F., et al., in preparation. 2017 Contact: [email protected] Water desorption content Dry RH = 11% Dry Figure 2. Illustration of QCM analysis (data shown for an α‐pinene-derived thin film) Figure 4. Organonitrogen production of toluene- derived SOM exposed to ammonia at different RH values. The red curve represents model results based on obtained diffusivities (Fig. 3). Water diffusivity was taken as a surrogate for NH3 diffusivity.

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Page 1: Highly Viscous States Affect the Browning of …...Highly Viscous States Affect the Browning of Atmospheric Organic Particulate Matter Pengfei Liu1, Yong JieLi1, Yan Wang1, Adam Bateman1,

Highly Viscous States Affect the Browning of Atmospheric Organic Particulate MatterPengfei Liu1, Yong Jie Li1, Yan Wang1, Adam Bateman1, Yue Zhang1, Zhaoheng Gong1 Allan K Bertram2 and Scot T Martin1,*

Introduction

Zhaoheng Gong , Allan K. Bertram , and Scot T. Martin1Harvard University, Cambridge, MA, USA; 2University of British Columbia, Vancouver, BC, Canada

blah blah blah

Light-absorbing organic carbon is of greatinterest because it potentially affects climate andphotochemistry. Some types of secondaryorganic material (SOM) can become light

Optical propertiesAbstract:

Initially transparent organic particulate matter(PM) can become shades of light-absorbingbrown via particle-phase reactions. Whensemisolid or solid physical states of organic PM

a.

blah blah blahorganic material (SOM) can become light-absorbing via multiphase reactive processing inthe atmosphere, and thereby contribute to so-called “brown carbon” (Updyke et al. 2012).These multiphase browning reactions, however,can possibly be limited by the slow diffusion ofreactant molecules in organic matrix underconditions that semisolids or solids prevail(Kuwata & Martin. 2012; Li et al., 2015).

semisolid or solid physical states of organic PMprevail, however, the diffusion of reactantmolecules can become sufficiently slow toinhibit browning reactions. Experiments showthat the production of light-absorbingorganonitrogen species from ammonia exposurestrongly depended on the RH value. Theobserved RH-dependent behavior was wellcaptured by a model that considered thediffusivities of both the large molecules makingup the organic PM and the small reactant guest

b. 280-320 nm

Diffusivities

Physical state

Diffusivity Reactivity

Optical properties

p g gmolecules taken up by the PM.

c. 380-420 nm

ExperimentalFigure 5. Changed optical properties of toluene-derived SOM exposed to ammonia at different RHvalues. (a) Mass absorption coefficient as a functionof wavelength; (b) Absorptive indices on left axis andmass absorption coefficients on right axis from 280to 320 nm (c) Same as panel (b) but for 380 to 420nm

Organic particles were produced byphotooxidation of toluene in an Oxidation FlowReactor (OFR) (Kang et al. 2007; Lambe et al.2011);In-particle diffusivities of both small (water) andlarge (organic) molecules were measured by aQ C l Mi b l (QCM)

Conclusions

Figure 3. (left axis) Self-diffusivity Dorg and waterdiffusivity DH2O for toluene-derived SOM; (right axis)mixing timescale for a 100-nm particle.

Below 20% RH, fast browning reactionsassociated with ammonia uptake were kineticallylimited by a shallow diffusoreactive length, evenas the comparative physical mixing timescale ofsmall molecules was short.Self-diffusivity of large organic moleculesmaking up PM was 104 to 106 times smaller than

Dry

Flow cell

SOM filN2

Quartz Crystal Microbalance (QCM);Toluene-derived SOM particles were exposed toammonia;Organonitrogen species (CxHyNz

+) were analyzedby the AMSAbsorption spectra before and after ammoniaexposure were recorded by a UV-VIS spectrometer.

Organonitrogen

References

Upkyke, K.M., et al. Atmos. Environ., 2012, 63, 22-31..

Kuwata, M. & Martin, S.T. PNAS, 2012, 109(43), 17354-17359.

Li, Y.J., et al., Environ. Sci. Tech. 2015, 49, 13264-13274.

g pthe small-molecule diffusivity, further inhibitingreactant refreshing near the particle surface.

Water uptake Evaporation of organic material

Water

Figure 1. Diagram of the experimental apparatusfor diffusivity measurements

RHQuartz crystal

SOM film2

SOM particles

NH3 exposure

RH

Kang, E., et al., Atmos. Chem. Phys. 2007, 7(22), 5727-5744.

Lambe, A.T., et al., Atmos. Meas. Tech. 2011, 4, 445-461.

Bateman, A.P., Bertram, A.K. & Martin, S.T., J. Phys. Chem.A, 2015, 119, 4386-4395.

Song, M. et al., Atmos. Chem. Phys., 2016, 16, 8817-8830.

Liu, P.F., et al., PNAS, 2016, 113, 12643-12648.

Liu, P.F., et al., in preparation. 2017

Contact: [email protected]

Water desorptioncontent

Dry

RH = 11%

Dry

Figure 2. Illustration of QCM analysis (data shownfor an α‐pinene-derived thin film)

Figure 4. Organonitrogen production of toluene-derived SOM exposed to ammonia at different RHvalues. The red curve represents model resultsbased on obtained diffusivities (Fig. 3). Waterdiffusivity was taken as a surrogate for NH3diffusivity.