18 May 2021

18 May 2021

Review status: a revised version of this preprint is currently under review for the journal ACP.

Physical and chemical properties of black carbon and organic matter from different sources using aerodynamic aerosol classification

Dawei Hu1, M. Rami Alfarra1,2,a, Kate Szpek3, Justin M. Langridge3, Michael Cotterell5, Claire Belcher4, Ian Rule4, Zixia Liu4, Chenjie Yu1, Yunqi Shao1, Aristeidis Voliotis1, Mao Du1, Brett Smith6, Greg Smallwood6, Prem Lobo6, Dantong Liu7, Jim M. Haywood4, Hugh Coe1, and James D. Allan1,2 Dawei Hu et al.
  • 1Department of Earth and Environmental Sciences, University of Manchester, UK
  • 2National Centre for Atmospheric Science, University of Manchester, Manchester, UK
  • 3Observation Based Research, Met Office, Exeter, UK
  • 4College for Engineering, Mathematics and Physical Sciences, University of Exeter, Exeter, UK
  • 5School of Chemistry, University of Bristol, Bristol, UK
  • 6Metrology Research Centre, National Research Council Canada, Ottawa, Canada
  • 7Department of Atmospheric Sciences, School of Earth Sciences, Zhejiang University, Hangzhou, Zhejiang, China
  • aCurrently at: Qatar Environment and Energy Research Institute (QEERI), Hamad Bin Khalifa University (HBKU), Doha, Qatar

Abstract. The physical and chemical properties of black carbon (BC) and organic aerosols are important for predicting their radiative forcing in the atmosphere. During the Soot Aerodynamic Size Selection for Optical properties (SASSO) project and a EUROCHAMP-2020 transnational access project, different types of light absorbing carbon were studied, including BC from catalytically stripped diesel exhaust, a flame burner, a colloidal graphite standard (Aquadag), and from controlled flaming wood combustion. Brown carbon (BrC) was also investigated in the form of organic aerosol emissions from wood burning (pyrolysis and smouldering) and from the nitration of secondary organic aerosol (SOA) proxies produced in a photochemical reaction chamber. Here we present insights into the physical and chemical properties of the aerosols, with optical properties being presented in subsequent publications. The dynamic shape factor (χ) of BC particles and material density (ρm) of organic aerosols were investigated by coupling a charging-free Aerodynamic Aerosol Classifier (AAC) with a Centrifugal Particle Mass Analyzer (CPMA) and Scanning Mobility Particle Sizer (SMPS). The morphology of BC particles was captured by transmission electron microscopy (TEM). For BC particles from the diesel engine and flame burner emissions, the primary spherule sizes were similar, around 20 nm. With increasing particle size, BC particles adopted more collapsed/compacted morphologies for the former source but tended to show more aggregated morphologies for the latter source. For particles emitted from the combustion of dry wood samples, the χ of BC particles and the ρm of organic aerosols were observed in the ranges 1.8–2.17 and 1.22–1.32 g/cm3, respectively. Similarly, for wet wood samples, the χ and ρm ranges were 1.2–1.85 and 1.44–1.60 g/cm3, respectively. Aerosol mass spectrometry measurements show no clear difference in mass spectra of the organic aerosols in individual burn phases (pyrolysis or smouldering phase) with the moisture content of the wood samples. This implies that the effect moisture has on the organic chemical profile of wood burning emissions is through changing the durations of the different phases of the burn cycle, not through the chemical modification of the individual phases. In this study, the incandescence signal of a Single Particle Soot Photometer (SP2) was calibrated with three different types of BC particles and compared with that from an Aquadag standard that is commonly used to calibrate SP2 incandescence to a BC mass. A correction factor is defined as the ratio of the incandescence signal from an alternative BC source to that from the Aquadag standard, and took values of 0.82 (or 0.79), 0.88 and 0.84–0.91 for the BC particles emitted from the diesel engine running under hot (or cold idle) conditions, the flame burner and wood combustion, respectively. These correction factors account for differences in instrument response to BC from different sources compared to the standardised Aquadag calibration and are more appropriate than the common value of 0.75 recommended by Laborde et al. (2012b) when deriving the mass concentration of BC emitted from diesel engines. Quantifying the correction factor for many types of BC particles found commonly in the atmosphere may enable better constraints to be placed on this factor depending on the BC source being sampled, and thus improve the accuracy of future SP2 measurements of BC mass concentrations.

Dawei Hu et al.

Status: final response (author comments only)

Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor | : Report abuse
  • RC1: 'Comment on acp-2021-351', Anonymous Referee #1, 19 Jun 2021
  • RC2: 'Comment on acp-2021-351', Anonymous Referee #2, 08 Jul 2021

Dawei Hu et al.


Total article views: 452 (including HTML, PDF, and XML)
HTML PDF XML Total Supplement BibTeX EndNote
307 139 6 452 21 1 1
  • HTML: 307
  • PDF: 139
  • XML: 6
  • Total: 452
  • Supplement: 21
  • BibTeX: 1
  • EndNote: 1
Views and downloads (calculated since 18 May 2021)
Cumulative views and downloads (calculated since 18 May 2021)

Viewed (geographical distribution)

Total article views: 587 (including HTML, PDF, and XML) Thereof 587 with geography defined and 0 with unknown origin.
Country # Views %
  • 1
Latest update: 18 Sep 2021
Short summary
Here, we developed new techniques for investigating these properties in the laboratory and applied these to BC and BrC from different sources, including diesel exhaust, inverted propane flame and wood combustion. These have allowed us to quantify the changes in shape and chemical composition of different soots according to source and variables such as the moisture content of wood.