Model calculation of the characteristic mass for convective and diffusive vapor transport in graphite furnace atomic absorption spectrometry

• Published in: Spectrochimica acta. Part B: Atomic spectroscopy Vol. 109; pp. 52 - 59
• Main Authors: Bencs, László, Laczai, Nikoletta, Ajtony, Zsolt
• Format: Journal Article
• Language: English
• Published: Elsevier B.V 01.07.2015
• Subjects: Accuracy; Atomic absorption analysis; Computer model; Convective vapor transport; Design standards; Diffusion; Diffusion coefficient; Furnaces; Graphite; Internal furnace gas flow; Mathematical models; Transversely heated graphite furnace; Computer model; Diffusion coefficient; Transversely heated graphite furnace; Convective vapor transport; Internal furnace gas flow
• ISSN: 0584-8547; 1873-3565
• DOI: 10.1016/j.sab.2015.05.001

A combination of former convective–diffusive vapor-transport models is described to extend the calculation scheme for sensitivity (characteristic mass — m0) in graphite furnace atomic absorption spectrometry (GFAAS). This approach encompasses the influence of forced convection of the internal furnace gas (mini-flow) combined with concentration diffusion of the analyte atoms on the residence time in a spatially isothermal furnace, i.e., the standard design of the transversely heated graphite atomizer (THGA). A couple of relationships for the diffusional and convectional residence times were studied and compared, including in factors accounting for the effects of the sample/platform dimension and the dosing hole. These model approaches were subsequently applied for the particular cases of Ag, As, Cd, Co, Cr, Cu, Fe, Hg, Mg, Mn, Mo, Ni, Pb, Sb, Se, Sn, V and Zn analytes. For the verification of the accuracy of the calculations, the experimental m0 values were determined with the application of a standard THGA furnace, operating either under stopped, or mini-flow (50cm3min−1) of the internal sheath gas during atomization. The theoretical and experimental ratios of m0(mini-flow)-to-m0(stop-flow) were closely similar for each study analyte. Likewise, the calculated m0 data gave a fairly good agreement with the corresponding experimental m0 values for stopped and mini-flow conditions, i.e., it ranged between 0.62 and 1.8 with an average of 1.05±0.27. This indicates the usability of the current model calculations for checking the operation of a given GFAAS instrument and the applied methodology. •A calculation scheme for convective–diffusive vapor loss in GFAAS is described.•Residence time (τ) formulas were compared for sensitivity (m0) in a THGA furnace.•Effects of the sample/platform dimension and dosing hole on τ were assessed.•Theoretical m0 of 18 analytes were calculated for stopped & mini furnace gas flows.•Experimental m0 data were determined & compared with theoretical values.