Detecting charging state of ultrafine particles : instrumental development and ambient measurements

The importance of ion-induced nucleation in the lower atmosphere has been discussed for a long time. In this article we describe a new instrumental setup – Ion-DMPS – which can be used to detect contribution of ion-induced nucleation on atmospheric new particle formation events. The device measures positively and negatively charged particles with and without a bipolar charger. The ratio between "charger off" to "charger on" describes the charging state of aerosol particle population with respect to equilibrium. Values above one represent more charges than in an equilibrium (overcharged state), and values below unity stand for undercharged situation, when there is less charges in the particles than in the equilibrium. We performed several laboratory experiments to test the operation of the instrument. After the laboratory tests, we used the device to observe particle size distributions during atmospheric new particle formation in a boreal forest. We found that some of the events were clearly dominated by neutral nucleation but in some cases also ion-induced nucleation contributed to the new particle formation. We also found that negative and positive ions (charged particles) behaved in a different manner, days with negative overcharging were more frequent than days with positive overcharging.

[1]  P. Mcmurry,et al.  MEASURED ATMOSPHERIC NEW PARTICLE FORMATION RATES: IMPLICATIONS FOR NUCLEATION MECHANISMS , 1996 .

[2]  R. Turco,et al.  Correspondence [ to “Ultrafine aerosol formation via ion‐mediated nucleation”] , 2000 .

[3]  Richard C. Flagan,et al.  History of Electrical Aerosol Measurements , 1998 .

[4]  M. Kulmala,et al.  Charging state of atmospheric nanoparticles during the nucleation burst events , 2006 .

[5]  A. Berner,et al.  A new electromobility spectrometer for the measurement of aerosol size distributions in the size range from 1 to 1000 nm , 1991 .

[6]  Klaus Willeke,et al.  Aerosol Measurement: Principles, Techniques, and Applications , 2001 .

[7]  F. Arnold,et al.  Cosmic ray‐induced aerosol‐formation: First observational evidence from aircraft‐based ion mass spectrometer measurements in the upper troposphere , 2002 .

[8]  P. Mcmurry,et al.  Measurement of Expected Nucleation Precursor Species and 3–500-nm Diameter Particles at Mauna Loa Observatory, Hawaii , 1995 .

[9]  K. Lehtinen,et al.  Kinetic nucleation and ions in boreal forest particle formation events , 2004 .

[10]  J. Smith,et al.  Contribution of ion‐induced nucleation to new particle formation: Methodology and its application to atmospheric observations in Boulder, Colorado , 2006 .

[11]  M. Kulmala,et al.  Annual and size dependent variation of growth rates and ion concentrations in boreal forest , 2005 .

[12]  H. Tammet Continuous scanning of the mobility and size distribution of charged clusters and nanometer particles in atmospheric air and the Balanced Scanning Mobility Analyzer BSMA , 2006 .

[13]  M. Misaki A Method of Measuring the Ion Spectrum , 1950 .

[14]  P. Hari,et al.  Long-term field measurements of atmosphere-surface interactions in boreal forest combining forest ecology, micrometeorology, aerosol physics and atmospheric chemistry , 1998 .

[15]  R. Turco,et al.  Ultrafine aerosol formation via ion‐mediated nucleation , 2000 .

[16]  M. Kulmala,et al.  Analytical formulae connecting the “real” and the “apparent” nucleation rate and the nuclei number concentration for atmospheric nucleation events , 2002 .

[17]  Ü. Rannik,et al.  Overview of the international project on biogenic aerosol formation in the boreal forest (BIOFOR) , 2001 .

[18]  方郎 三崎 大気イオン・スペクトラムの研究(II) , 1961 .

[19]  A. Wiedensohler,et al.  An approximation of the bipolar charge distribution for particles in the submicron size range , 1988 .

[20]  C. O'Dowd,et al.  Physical characterization of aerosol particles during nucleation events , 2001 .

[21]  G. M. Frick,et al.  Ion—Aerosol Attachment Coefficients and the Steady-State Charge Distribution on Aerosols in a Bipolar Ion Environment , 1986 .

[22]  Peter H. McMurry,et al.  An Ultrafine Aerosol Condensation Nucleus Counter , 1991 .

[23]  J. Seinfeld,et al.  Ion‐induced nucleation. II. Polarizable multipolar molecules , 1995 .

[24]  J. W. Fitzgerald,et al.  Marine boundary layer measurements of new particle formation and the effects nonprecipitating clouds have on aerosol size distribution , 1994 .

[25]  Ari Laaksonen,et al.  Cluster activation theory as an explanation of the linear dependence between formation rate of 3nm particles and sulphuric acid concentration , 2006 .

[26]  J. Smith,et al.  Negative atmospheric ions and their potential role in ion-induced nucleation , 2006 .

[27]  J. Mäkelä,et al.  Closed-loop arrangement with critical orifice for DMA sheath/excess flow system , 1997 .

[28]  K. Lehtinen,et al.  Kinetic nucleation and ions in boreal particle formation events , 2004 .

[29]  K. Froyd,et al.  Atmospheric ion‐induced nucleation of sulfuric acid and water , 2004 .

[30]  Hanna Vehkamäki,et al.  Formation and growth rates of ultrafine atmospheric particles: a review of observations , 2004 .

[31]  L. Pirjola,et al.  Model studies on ion‐induced nucleation in the atmosphere , 2002 .

[32]  L. Pirjola,et al.  Stable sulphate clusters as a source of new atmospheric particles , 2000, Nature.

[33]  G. Reischl,et al.  Bipolar charging of ultrafine particles in the size range below 10 nm , 1996 .

[34]  N. Fuchs,et al.  HIGH-DISPERSED AEROSOLS , 1971 .

[35]  K. Becker,et al.  Bipolar diffusion charging of aerosol particles—I: experimental results within the diameter range 4–30 nm , 1983 .