GAS AND ION DYNAMICS OF A 3-APERTURE VACUUM INTERFACE FOR INDUCTIVELY-COUPLED PLASMA-MASS SPECTROMETRY

Citation
Sd. Tanner et al., GAS AND ION DYNAMICS OF A 3-APERTURE VACUUM INTERFACE FOR INDUCTIVELY-COUPLED PLASMA-MASS SPECTROMETRY, Applied spectroscopy, 48(11), 1994, pp. 1373-1378
Citations number
10
Categorie Soggetti
Instument & Instrumentation",Spectroscopy
Journal title
ISSN journal
00037028
Volume
48
Issue
11
Year of publication
1994
Pages
1373 - 1378
Database
ISI
SICI code
0003-7028(1994)48:11<1373:GAIDOA>2.0.ZU;2-I
Abstract
The equations describing the pressure, density, and temperature charac teristics of isentropic flow and of the formation of a shock structure due to the sudden termination of the directed motion of a flowing pla sma are reviewed. The results are applied to describe the flow charact eristics of a novel ICP-MS vacuum interface which consists of three ap ertures: a conventional sampler and skimmer and a third aperture conta ined in a blunt support which is normal to (or nearly normal to) the a xis of the primary expansion through the sampler and skimmer. The flow through the interface apertures is characterized as continuum, effusi ve, or transitional, and the impact of these forms of expansion on the ion dynamics (kinetic energies and plasma neutrality) is examined. A shock wave may form in front of the third aperture. The effect of this flow disturbance on the gas and ion dynamics in the vicinity of the a perture is discussed. Experimental neutral and ion flow results are co mpared to the theoretical predictions. It is concluded that the plasma retains its charge neutrality as it flows through the sampler and ski mmer and, under the conditions studied, also through the shock and sub sequent expansion through the third aperture. The gas behind the shock flows across the surface of the blunt tip of the third aperture, and the aperture itself may be offset from the axis of the original expans ion to eliminate clogging of the aperture by unvaporized particles and condensed salts from the plasma and to prevent source plasma photons from contributing to the background signal continuum. The reduction in the ion current introduced into the ion optics region of the mass spe ctrometer reduces the magnitude of the space charge field and results in a gain in ion transmission efficiency which offsets the reduction o f the ion flow.