Tandem mobility mass spectrometry study of electrosprayed tetraheptyl ammonium bromide clusters

Multiply charged electrospray ions from concentrated solutions of Heptyl(4)N(+)Br(-) (designated A(+)B(-) hereafter) in formamide are analyzed mass spectrometrically (MS) following mobility selection in ambient air in a differential mobility analyzer (DMA). Most of the sharp mobility peaks seen are identified as (AB)(n)A(+) clusters, with 0 <= n <= 5. One anomalously abundant and mobile ion is identified as NH4+(AB)(4). Six ions in the (AB)(n)(A(+))(2) series are also identified, completing and correcting earlier mobility data for singly and doubly charged ions up to masses of almost 9000 Da. The more mobile of two broad humps seen in the mobility spectrum includes m/z values approximately from 2500 up to 12,000 Da. It is formed primarily by multiply charged (AB)(n)(A(+))(z) clusters with multiple ammonium bromide adducts. Because of overlapping of many peaks of different m/z and charge state z, only a few individual species can be identified by MS alone in this highly congested region. However, the spectral simplification brought about by mobility selection upstream of the MS reveals a series of broad modulations in m/z space, with all ions resolved in the second, third,.. sixth modulation being in charge states z = 2, 3,...6, respectively. Extrapolation of this trend beyond the sixth wave fixes the ion charge state (in some cases up to z = 15) and mass (beyond m = 175,000 u). This wavy structure had been previously observed and explained in terms of ion evaporation kinetics from volatile drops, though without mass identification. All observations indicate that the clusters are formed as charged residues, but their charge state is fixed by the Iribarne-Thomson ion evaporation mechanism. Consequently, the measured curve of cluster diameter versus z yields the two parameters governing ion evaporation kinetics. Clusters with z > I and electrical mobility Z > 0.495 cm(2)/V/s are metastable and evaporate a singly charged cluster, probably (AB)(2)A(+), between the DMA and the MS. Plotting the electrical mobilities Z of the clusters in the form (z/Z)(1/2) versus m(1/3) (both proportional to cluster diameter) collapse the data for all cluster sizes and charge states into one single straight line for Z below 0.495 cm(2)/V/s. This linear relation reveals a uniform apparent cluster density of 0.935 g/cm(3) and an effective hard-sphere diameter of the air molecules of 0.44 nm. An anomalous mobility increase is observed at diameters below 3 nm. (c) 2005 American Society for Mass Spectrometry.