A general study of performance attributes was conducted for a prototypical electrothermal vaporization (ETV) sample introduction system, in which induction heating (IH) was used to facilitate the drying, pyrolysis, and vaporization of samples from long, undercut graphite cup probes in a radio-frequency (RF) induction field. In the first part of this study, experiments were carried out to determine the heating characteristics and temperature control aspects of an IH-ETV arrangement. Using a remote-sensing infrared thermocouple, it was determined that a 3/8-inch (9.53-mm) outer diameter graphite cup sample probe could be heated to a maximum temperature of 1860°C in the induction field of the IH-ETV under full forward power (1.5 kW). The IH-ETV device was found to have a rapid heating response (1/ e time-constant of 2.0±0.2 s) that was independent of the initial/final temperatures chosen. Linear temperature control was possible by regulating either the DC voltage applied to the plate or the current flowing to the grid of the RF generator oscillator tube. The second part of this work consisted of studies to establish benchmarks, such as limits of detection (LOD) with inductively coupled plasma optical emission spectrometry (ICP-OES) and transport efficiency for analyte vaporization under several x–Ar mixed gas atmospheres [where x=15% N 2, 10% O 2, HCl (sparged), or 15% SF 6 (v/v)]. In general, reproducible transient signals with evolution times of 5–15 s were seen for the vaporization of most elements studied, with peak area intensity and reproducibility generally being the best with SF 6–Ar. A 10-fold increase in transport efficiency was seen for refractory carbide-forming analytes (Cr, V) when vaporization was conducted in a halogenous ( x=HCl, SF 6) versus non-halogenous ( x=N 2, O 2) environment, with a two-fold improvement being observed for most other non-refractory elements (Cd, Cu, Fe, Mn, Ni, Pb, Zn). The transport of arsenic proved to be a special case unto itself, with its transport efficiency increasing to 90% when vaporized in the presence of SF 6 (a three-fold improvement over all other carrier mixtures) due to the formation of volatile AsF 5. Using the concept of transport-independent analyte sensitivity, the introduction of the aforementioned x–Ar mixtures into the center channel of the plasma appeared to not have any appreciable effect on plasma excitation conditions, with N 2 being the only exception (a 70% reduction in transport-independent sensitivity was observed). Detection limits ranged from 0.08 to 70 ng absolute and were highly dependent on the analyte studied and the vaporization atmosphere used. Based on the above information, the feasibility of an induction heating arrangement for thermal sample introduction was evaluated, with recommendations being made for the future design of IH-ETV instrumentation.
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