School of Engineering and Science - Jacobs University
School of Engineering and Science - Jacobs University
School of Engineering and Science - Jacobs University
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the concentration <strong>of</strong> the major element being considered, since as concentrations<br />
increase (e.g., to 500 mg/kg) the high TDS content <strong>of</strong> the solution begins to suppress<br />
analyte intensities, similar to that observed for rock samples that are only minimally<br />
diluted before analysis.<br />
The quantification <strong>of</strong> the observed interferences as concentrations in mg/kg<br />
allows predictions to be made regarding the potential impact these interferences might<br />
have upon trace metal determinations. For example, as the CaO content in a carbonate<br />
rock increases from 10% to 40%, then Ni concentrations determined in an HCl acid<br />
matrix would be expected to increase from ~2.5 mg/kg to ~6 mg/kg, due to Ca<br />
interferences on 60 Ni (Fig. A2.1). These calculated interferences in concentration<br />
units <strong>of</strong> m/kg are obtained from the long term average instrument response as<br />
determined from the 10 μg/kg calibration st<strong>and</strong>ard (described in Fig. 2, Section 4).<br />
For example, the 60 Ni isotope has an average instrument response <strong>of</strong> 2158 cps/μg·kg -1<br />
in 0.5 M HCl, <strong>and</strong> a sample containing 14% CaO <strong>and</strong> diluted 1000x would be<br />
expected to generate an CaO(H) interference <strong>of</strong> ~6700 cps on mass 60. Therefore, Ni<br />
quantified in this sample using measurement <strong>of</strong> the 60 Ni isotope would be erroneously<br />
overestimated by approximately 3.1 μg/kg (i.e., 2158/6700 = 3.1).<br />
It should be noted that, similar to estimates <strong>of</strong> interferences based upon raw<br />
data (cps), interference estimates reported as concentrations (mg/kg) will vary with<br />
instrument performance. As the long term average instrument response for the 10<br />
μg/kg calibration st<strong>and</strong>ard varies by as much as 30% (RSD), <strong>and</strong> this is the basis for<br />
the calculation <strong>of</strong> the interference magnitude in mg/kg, then these calculated<br />
concentrations will vary similarly.<br />
Data for interferences are presented for the following isotopes in the order;<br />
60 Ni, 62 Ni, 88 Sr, 89 Y, 90 Zr, 91 Zr, 93 Nb, <strong>and</strong> 95 Mo. Regardless <strong>of</strong> the element <strong>of</strong> interest,<br />
or the specific interferences that inhibit accurate concentration measurements <strong>of</strong> these<br />
elements, the key factor is always the relative abundance <strong>of</strong> the interfering species to<br />
the isotope <strong>of</strong> interest. In other words, the greatest analytical difficulties arise when<br />
trying to quantify small concentrations <strong>of</strong> an element in the presence <strong>of</strong> large<br />
concentrations <strong>of</strong> interfering elements. As a result, while some interferences may be<br />
large, e.g., several mg/kg in the case <strong>of</strong> Ca 2 <strong>and</strong> ArCa on Sr, the effect <strong>of</strong> these<br />
interferences is minor if the element being measured is abundant in the sample (e.g.,<br />
115 mg/kg Sr in the JDo-1 dolomite).<br />
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