Reported are variations measured in tertiary aerosol laser scatter signal i
ntensities in response to changes in the concentration of different dissolv
ed solids in the starting solutions, and to varied DC potentials applied to
a mesh screen positioned in a spray chamber. The scatter signal from an ae
rosol derived from a solution containing one of nine different ionic matric
es would increase when the concentration of that matrix was increased from
10 to 100 mM, but there was no concentration dependence on the scatter sign
al when the matrix was non-ionic (sucrose). The tertiary aerosol droplet si
ze distributions for three of these ionic matrices were then measured, and
for each increase of the matrix concentration, there was an increased abund
ance of small droplets in the tertiary aerosol. We attribute the source of
this droplet size distribution alteration to be the result of a change in t
he net charge acquired by the primary droplets at the nebulization step, in
stigated because of the change in the total concentration of dissolved soli
ds in the starting solution. The net charge acquired by a primary droplet i
s a critical parameter, because during transport through the spray chamber
desolvation can lead to a Coulomb fission event, a process that causes a dr
oplet to split unevenly, releasing numerous new small droplets into the aer
osol. We use this argument to explain how a change in the dissolved ionic s
olids concentration in the starting solution leads to a change in the frequ
ency of Coulomb fission event occurrence within the secondary aerosol. The
assumption that primary droplets carry net charge was then put to the test
by incorporating a mesh screen into the spray chamber to which DC potential
s were then applied. Each starting solution used in this work exhibited a l
arge change in the tertiary aerosol in response to a DC biased mesh screen.
In particular, there was decreased transmission for both large and small d
roplets in each of the tertiary aerosols studied, in response to increased
electric field strengths in the spray chamber. These data provide strong ev
idence that static electrification of aerosols, with subsequent Coulomb fis
sion event occurrence during aerosol transport, are ubiquitous factors in l
iquid sample introduction methodology for atomic spectroscopy.