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940 A · ANALYTICAL CHEMISTRY, VOL. 58, NO. 8, JULY 1986
Figure 6. Mg (285.2 nm) in an air-acet ylene flame (a) Calibration curves and (b) relative concentra tion errors using the stepped modulation wave form shown In Figure 5. Curves 1 and 2 corre spond to the type 1 and 2 absorbances shown In Figure 5
that reflect either the emphasis of the investigation or a compromise pattern. One compromise sampling pattern is shown in Figure 5. This pattern was designed to optimize sampling at five locations over the course of one modu lation cycle (two passes across the pro file). Sampling points are concentrat ed at the middle of the profile, at both sides two-thirds of the distance to ward the extremes, and at both ex tremes. The type 1 absorbance is com puted using all 40 intensity measure ments, and the less sensitive type 2 absorbance is computed from 24 in tensity measurements in the wings of the absorption profile. This sampling pattern was designed for use with flame atomization where the signal is static. Two full passes require 36 ms, which is a slow response time for car bon furnace atomization. The result ing calibration curves and relative concentration error plots are shown in Figure 6 for Mg (285.2 nm) in an airacetylene flame. Data processing
All the data processing for SIMAAC is handled by three computer pro grams—the data acquisition, the data display, and the data reduction pro grams. The data acquisition program can acquire 18,000 intensity measure ments per second for up to 30 s. This program drives the galvanometer with the appropriate modulation waveform and collects data as described in the previous section. The raw intensity data are stored directly on a disk and