Black carbon aerosol mixing state, organic aerosols and aerosol optical properties over the United Kingdom

Abstract. Black carbon (BC) aerosols absorb sunlight thereby leading to a positive radiative forcing and a warming of climate and can also impact human health through their impact on the respiratory system. The state of mixing of BC with other aerosol species, particularly the degree of internal/external mixing, has been highlighted as a major uncertainty in assessing its radiative forcing and hence its climate impact, but few in situ observations of mixing state exist. We present airborne single particle soot photometer (SP2) measurements of refractory BC (rBC) mass concentrations and mixing state coupled with aerosol composition and optical properties measured in urban plumes and regional pollution over the United Kingdom. All data were obtained using instrumentation flown on the UK's BAe-146-301 large Atmospheric Research Aircraft (ARA) operated by the Facility for Airborne Atmospheric Measurements (FAAM). We measured sub-micron aerosol composition using an aerosol mass spectrometer (AMS) and used positive matrix factorization to separate hydrocarbon-like (HOA) and oxygenated organic aerosols (OOA). We found a higher number fraction of thickly coated rBC particles in air masses with large OOA relative to HOA, higher ozone-to-nitrogen oxides (NO x ) ratios and large concentrations of total sub-micron aerosol mass relative to rBC mass concentrations. The more ozone- and OOA-rich air masses were associated with transport from continental Europe, while plumes from UK cities had higher HOA and NO x and fewer thickly coated rBC particles. We did not observe any significant change in the rBC mass absorption efficiency calculated from rBC mass and light absorption coefficients measured by a particle soot absorption photometer despite observing significant changes in aerosol composition and rBC mixing state. The contributions of light scattering and absorption to total extinction (quantified by the single scattering albedo; SSA) did change for different air masses, with lower SSA observed in urban plumes compared to regional aerosol (0.85 versus 0.9–0.95). We attribute these differences to the presence of relatively rapidly formed secondary aerosol, primarily OOA and ammonium nitrate, which must be taken into account in radiative forcing calculations.

[1]  D. Blake,et al.  Evolution of mixing state of black carbon in polluted air from Tokyo , 2007 .

[2]  P. M. Lang,et al.  Distributions and recent changes of carbon monoxide in the lower troposphere , 1998 .

[3]  J. Ogren Comment on “Calibration and Intercomparison of Filter-Based Measurements of Visible Light Absorption by Aerosols” , 2010 .

[4]  Martin Gallagher,et al.  2. Measurements of fine particulate chemical composition in two U.K. cities , 2003 .

[5]  M. Chin,et al.  Evaluation of black carbon estimations in global aerosol models , 2009 .

[6]  D. R. Worsnop,et al.  Evolution of Organic Aerosols in the Atmosphere , 2009, Science.

[7]  D. Ceburnis,et al.  Aerosol properties associated with air masses arriving into the North East Atlantic during the 2008 Mace Head EUCAARI intensive observing period: an overview , 2009 .

[8]  David S. Covert,et al.  Bias in Filter-Based Aerosol Light Absorption Measurements Due to Organic Aerosol Loading: Evidence from Ambient Measurements , 2008 .

[9]  Peter Clark,et al.  Prediction of visibility and aerosol within the operational Met Office Unified Model. I: Model formulation and variational assimilation , 2008 .

[10]  T. Bond,et al.  Light Absorption by Carbonaceous Particles: An Investigative Review , 2006 .

[11]  M. Petters,et al.  Influences on the fraction of hydrophobic and hydrophilic black carbon in the atmosphere , 2011 .

[12]  James D. Lee,et al.  Contributions from transport, solid fuel burning and cooking to primary organic aerosols in two UK cities , 2009 .

[13]  M. Stephens,et al.  Particle identification by laser-induced incandescence in a solid-state laser cavity. , 2003, Applied optics.

[14]  P. Quinn,et al.  Modification, Calibration and a Field Test of an Instrument for Measuring Light Absorption by Particles , 2005 .

[15]  Tami C. Bond,et al.  Calibration and Intercomparison of Filter-Based Measurements of Visible Light Absorption by Aerosols , 1999 .

[16]  T. Bond,et al.  Yellow Beads and Missing Particles: Trouble Ahead for Filter-Based Absorption Measurements , 2007 .

[17]  Matthew West,et al.  Particle‐resolved simulation of aerosol size, composition, mixing state, and the associated optical and cloud condensation nuclei activation properties in an evolving urban plume , 2010 .

[18]  Michael Flynn,et al.  Black carbon measurements in the boundary layer over western and northern Europe , 2010 .

[19]  M. Esselborn,et al.  Enhancement of the aerosol direct radiative effect by semi-volatile aerosol components: airborne measurements in North-Western Europe , 2010 .

[20]  J. Allan,et al.  Interactive comment on “Vertical distribution of sub-micron aerosol chemical composition from North-Western Europe and the North-East Atlantic” by W. T. Morgan et al , 2009 .

[21]  H. Burtscher,et al.  Hygroscopic properties of carbon and diesel soot particles , 1997 .

[22]  R. Draxler HYSPLIT (HYbrid Single-Particle Lagrangian Integrated Trajectory) Model access via NOAA ARL READY Website , 2010 .

[23]  J. Peischl,et al.  Measurement of the mixing state, mass, and optical size of individual black carbon particles in urban and biomass burning emissions , 2008 .

[24]  P. Massoli,et al.  Absorption Enhancement of Coated Absorbing Aerosols: Validation of the Photo-Acoustic Technique for Measuring the Enhancement , 2009 .

[25]  Jim Haywood,et al.  Evolution of biomass burning aerosol properties from an agricultural fire in southern Africa , 2003 .

[26]  P. Chazette,et al.  Airborne measurements of trace gases and aerosols over the London metropolitan region , 2011 .

[27]  R. C. Easter,et al.  Estimating Black Carbon Aging Time-Scales with a Particle-Resolved Aerosol Model , 2009, 0903.0029.

[28]  Yutaka Kondo,et al.  Effects of Mixing State on Black Carbon Measurements by Laser-Induced Incandescence , 2007 .

[29]  Meridional gradients of light absorbing carbon over northern Europe , 2008 .

[30]  K. Prather,et al.  Aircraft measurements of vertical profiles of aerosol mixing states , 2010 .

[31]  Qi Zhang,et al.  Ubiquity and dominance of oxygenated species in organic aerosols in anthropogenically‐influenced Northern Hemisphere midlatitudes , 2007 .

[32]  J. Jimenez,et al.  Interpretation of organic components from Positive Matrix Factorization of aerosol mass spectrometric data , 2008 .

[33]  K. Prather,et al.  In-situ measurements of the mixing state and optical properties of soot with implications for radiative forcing estimates , 2009, Proceedings of the National Academy of Sciences.

[34]  O. Boucher,et al.  Estimates of the direct and indirect radiative forcing due to tropospheric aerosols: A review , 2000 .

[35]  W. T. Rawlins,et al.  Observation of hydration of single, modified carbon aerosols , 1994 .

[36]  Stephan Borrmann,et al.  A New Time-of-Flight Aerosol Mass Spectrometer (TOF-AMS)—Instrument Description and First Field Deployment , 2005 .

[37]  M. Steinbacher,et al.  Single particle characterization of black carbon aerosols at a tropospheric alpine site in Switzerland , 2010 .

[38]  Y. Kondo,et al.  Amplification of Light Absorption of Black Carbon by Organic Coating , 2010 .

[39]  B. Stephens,et al.  Black carbon over Mexico: the effect of atmospheric transport on mixing state, mass absorption cross-section, and BC/CO ratios , 2009 .

[40]  J. Allan,et al.  Vertical distribution of sub-micron aerosol chemical composition from North-Western Europe and the North-East Atlantic , 2009 .

[41]  Mark Z. Jacobson,et al.  Short-term effects of controlling fossil-fuel soot, biofuel soot and gases, and methane on climate, Arctic ice, and air pollution health , 2010 .

[42]  E. Highwood,et al.  Airborne measurements of the spatial distribution of aerosol chemical composition across Europe and evolution of the organic fraction , 2010 .

[43]  P. Paatero,et al.  Positive matrix factorization: A non-negative factor model with optimal utilization of error estimates of data values† , 1994 .

[44]  P. Mcmurry,et al.  Variability in morphology, hygroscopicity, and optical properties of soot aerosols during atmospheric processing , 2008, Proceedings of the National Academy of Sciences.

[45]  P. Paatero Least squares formulation of robust non-negative factor analysis , 1997 .

[46]  Axel Lauer,et al.  Single‐particle measurements of midlatitude black carbon and light‐scattering aerosols from the boundary layer to the lower stratosphere , 2006 .

[47]  J. Haywood,et al.  Prediction of visibility and aerosol within the operational Met Office Unified Model. II: Validation of model performance using observational data , 2008 .

[48]  D. Blake,et al.  Evolution of mixing state of black carbon particles: Aircraft measurements over the western Pacific in March 2004 , 2007 .

[49]  T. Onasch,et al.  Collection Efficiencies in an Aerodyne Aerosol Mass Spectrometer as a Function of Particle Phase for Laboratory Generated Aerosols , 2008 .

[50]  G. Mann,et al.  Aerosol mass spectrometer constraint on the global secondary organic aerosol budget , 2011 .

[51]  J. Dorsey,et al.  Carbonaceous aerosols contributed by traffic and solid fuel burning at a polluted rural site in Northwestern England , 2010 .

[52]  James B. Burkholder,et al.  Bias in Filter-Based Aerosol Light Absorption Measurements Due to Organic Aerosol Loading: Evidence from Laboratory Measurements , 2008 .

[53]  W. Malm,et al.  Effects of mixing on extinction by carbonaceous particles , 1999 .

[54]  J. Ogren,et al.  Determining Aerosol Radiative Properties Using the TSI 3563 Integrating Nephelometer , 1998 .

[55]  U. Lohmann,et al.  Coatings and their enhancement of black carbon light absorption in the tropical atmosphere , 2008 .