Direct Determination of Manganese in Sea Water by
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Direct Determination of Manganese in Sea Water by
Direct Determination of Manganese in Sea Water by Electrothermal Atomic Absorption Spectrometry with Deuterium Background Correction Using a Platform and Platinum Matrix Modifier Application Note Atomic Absorption Authors Introduction Michel Hoenig The determination of manganese in sea water samples using electrothermal atomic absorption spectrometry (ET-AAS) has been investigated by many workers [1-9]. Sea water has been found to be difficult to analyze because of the matrix. If the matrix is vaporized simultaneously with the analyte, the result is a large background signal which is often beyond the correcting capabilities of current deuterium devices. The presence of large amounts of chlorides has also been shown to provide interferences, making direct analysis difficult [10]. Paul Van Hoeyweghen Institute of Recherches Chimiques Ministere de l’Agriculture Museumlaan 5 — 1980 Tervuren Belgium To reduce the problems associated with the determination of manganese in sea water, most authors have used matrix modification [2,4,7] or have extracted the analyte from the sea water matrix [3,5]. Few workers have been successful with the direct manganese determination after volatilization of the matrix during the pyrolysis step [1,4,6]. Slavin and Manning [11] have shown that by using the platform, the interference of a salt matrix on cadmium, lead and thallium was greatly reduced. The same authors [12] have also shown that direct manganese determination in sea water is possible by using platform and Zeeman background correction. The reported sensitivity of this method is about 2.2 pg Mn for 0.0044 absorbance unit. We describe in this work a rapid method for the direct determination of manganese in sea water at sub µg L-1 levels using deuterium background correction, platform and platinum as matrix modifier. Experimental First, it was important to determine the correct electrothermal program using the platform technique. The ash study illustrated in Figure 1 showed that manganese can be thermally pretreated up to 1000 °C without losses for both aqueous standard and sea water sample (curves a and b). At this temperature the background absorbance generated by the salt matrix during the atomization step (curve c) is still relatively high (about 0.2 Abs). The addition of platinum as matrix modifier to the sample permits a pyrolysis temperature up to 1400 °C without loss of manganese (curves d and e). All the absorbance measurements reported here were made using an Agilent SpectrAA-10 Spectrometer with an Agilent GTA-96 graphite furnace and programmable sample dispenser. The furnace was fitted with pyrolytically coated tubes and solid pyrolytic graphite platforms. A Hewlett-Packard 82905-A printer was used for plotting the absorbance-time profiles. All measurements were performed in the peak-height mode. A manganese hollow cathode lamp operated at 4 mA current, spectral width of 0.2 nm and manganese resonance line at 279.5 nm were used throughout. The manganese aqueous standards were prepared in 5% nitric acid, (Suprapure Merck) from commercial standard solution (Titrisol Merck). Platinum matrix modifier solution (0.1% Pt) was prepared by dissolving the platinum metal in the aqua regia, followed by adequate dilution. Natural sea water samples were collected in the NE Atlantic and the North Sea. They had a salinity of approximate 3.5%. After sampling, the sea water was filtered through a nominal 0.45 µm membrane filter and acidified (5% HNO3). Results and Discussion Figure 1. A review of papers which report direct determination of manganese in sea water reveals a contradictory situation and a very difficult analysis. Earliest papers reported a reduced sensitivity for manganese in a sea water matrix and attributed it to covolatilization of analyte with the salt matrix. More recent reports suggest that this reduced sensitivity is a vapor-phase binding of a portion of the manganese by chlorine [13,14]. The experiments of Ediger et al [15] established that the decrease in signal for manganese in the presence of large amounts of NaCl is a chemical interference. The authors showed that it is necessary to char away as much as possible of the sea water matrix to get maximum sensitivity for manganese and to be relatively free of interference. Pritchard and Reeves [16] reported that sodium chloride is vaporized from a heated graphite surface in a few seconds at temperatures a little higher than 700 °C. According to Nakahara and Chakrabarti [17], the large amounts of NaCl present in sea water are volatilized below 950 °C: this temperature seems to be in agreement with our own experiences. On the other hand, Hoenig et al. [18] showed that other sea water matrix elements remain in the tube up to 1700 °C. At higher pyrolysis temperatures the background signal disappears entirely. Ash temperature The effect on the atomization signal is plotted as a function of different char temperatures for an aqueous standard and a sea water sample. Manganese concentration was 2 µg L-1 in both samples (5 µL dispensing). (a) — Aqueous standard (5% HNO3) (b) — Sea water (5% HNO3) (c) — Background absorbance (d) — Aqueous standard (5% HNO3) + Pt (2 µL 0.1%) (e) — Sea water (5% HNO3) + Pt (2 µL 0.1%) Finally, the ashing temperature of 1300 °C was set for both media (aqueous standards and sea water samples). With this ashing temperature the background absorbance has decreased to an acceptable value of about 0.04 absorbance. It must be also noted that in the presence of the platinum modifier the manganese peak-height absorbance signal is enhanced by about 30%. The best sensitivity was obtained with an atomization temperature of 2600 °C. Details of electrothermal program and sampler parameters are given in Table 1. Figure 2 shows the absorbance-time profiles of manganese for both media with electrothermal program described. 2 Table 1. Operating Parameters for Determination of Manganese A recent review of the literature [19] reported that the base line level of total manganese in unpolluted deep sea samples was expected to be about 0.05 µg L-1. Numerous trace metal measurements in coastal waters reported levels ranging from 0.5 to 50 µg L-1. Furnace parameters (with platform) Step no. Temperature (°C) 1 2 3 4 5 6 7 500 1300 1300 1300 2600 2600 120 Time (sec) 40 8 5 2 0.7 2.5 12.5 Gas flow (L/min-1) Gas type Read command 3 3 3 0 0 0 3 Argon Argon Argon Argon Argon Argon Argon No No No No Yes Yes No The sensitivity of the manganese determination was 1.2 pg Mn for 0.0044 absorbance. For 5 µL natural sea water samples we then estimate that real manganese concentration greater than 0.5 µg L-1 can be easily determined with good accuracy and precision (between 3 and 8% depending on the magnitude of the measured absorbance signal). Sample parameters (Sampler automixing, Mn standard 2 µg L-1) Blank Standard 1 Standard 2 Standard 3 Sample Solution Blank – 4 8 12 5 5 For samples that range lower than 0.5 µg L-1 the problem is more complicated. The dispensing of larger sample volumes on the platform (or multiple injection facility) is simple. Up to 20 µL of sea water sample, the background generated during the atomization step is not excessive and it is easily corrected by the deuterium device. Modifier (Pt 0.1% in HN03 2%) 2 2 2 2 2 However, in this case a larger amount of salt matrix remains on the platform after the ashing step and produces a nonspectral interference resulting in a reduced sensitivity for manganese. The direct calibration method using simple standard solutions then becomes inadequate because the slope of the single element standard curve is steeper than the working curve slope established in sea water. This slope decrease is variable and proportional to the sample volume of sea water. In such cases only the standard addition method is valid. However, for samples larger than 20 µL the curve slope is too low to obtain accurate results, and then the 20 µL method must be considered as a limit. In this case, manganese concentrations of about 0.2 µg L-1 can be determined with a sufficient accuracy. Figure 2. Absorbance-time profiles for manganese in presence of platinum matrix modifier. Manganese concentration was 1.6 µg L-1 in both samples (5 µL dispensing). Conclusions No major analytical problems were encountered in the manganese sea water analysis using the ET-AAS with platform and platinum matrix modifier. The 5 µL method using a direct calibration procedure is very rapid, simple and accurate and thus suitable for routine analysis. For very low manganese concentrations (below 0.5 µg L-1) it is necessary to analyze larger sea water volumes. In this case a matrix effect occurs and the standard addition method must be used. The long lifetime of solid pyrolytic platforms permits numerous determinations without decrease of absorbance signal. The platforms tested provided a lifetime in excess of 500 firing. In the previous paragraph we showed that the background absorbance of 5 µL sea water samples did not exceed 0.04 absorbance. Consequently, it is evident that major analytical problems will not be due to spectral interference. The calibration curve of manganese in a simple nitric acid medium is parallel with the standard addition curves obtained for 5 µL sea water samples. In such cases the direct calibration procedure against simple reference solutions is valid because of the absence of non-spectral interference. 3 References 1. D. A. Segar, J. G. Gonzalez, Anal. Chim. Acta, 58, 7,(1972). 2. J. M. McArthur, Anal. Chim. Acta, 93, 77, (1977). 3. H. M. Kingston, I. L. Barnes, T. J. Brady, T. C. Rains, M. A. Champ, Anal. Chem., 50, 2064 (1978). 4. R. E. Sturgeon, S. S. Berman, A. Desaulniers, D. S. Russell, Anal. Chem., 57, 2364, (1979). 5. G. P. Klinkhammer, Anal. Chem., 52, 117, (1980). 6. D. A. Segar, A. Y. Cantillo, Anal. Chem., 52, 1766, (1980). 7. J. R. Montgomery, G. N. Peterson, Anal. Chim. Acta, 177, 397, (1980). 8. G. R. Carnrick, W. Slavin, D.C. Manning, Anal. Chem., 53, 1866, (1981). 9. M. Hoenig, R. Wollast, Spectrochim. Acta, 37B, 399, (1982). 10. D. C. Manning, W. Slavin, Anal. Chem., 50, 1234, (1978). 11. W. Slavin, D. C. Manning, Anal. Chem., 51, 261, (1979). 12. G. R. Carnrick, W. Slavin, D. C. Manning, Anal Chem, 53, 1866, (1981). 13. B. V. L’vov, Spectrochim. Acta, 33B, 153, (1978). 14. D. C. Manning, W. Slavin, Anal. Chim. Acta, 118, 301, (1980). 15. R. D. Ediger, G. E. Peterson, J. D. Kerber, At. Absorpt. Newsl., 13, 61, (1974). 16. M. W. Pritchard, R. D. Reeves, Anal. Chim. Acta, 82, 103, (1976). 17. T. Nakahara, C. L. Chakrabarti, Anal. Chim. Acta, 104, 99, (1979). 18. M. Woenig, P. Dehairs, A. M. Kersabiec, J. Anal. Atom. Spectrosc., in press. 19. W. Slavin, At. Spectrosc., 1, 66, (1980). 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