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Among the atomic spectral lines that overlap and that can results in spectral interference

               are

                       285.2 nm lines of Tb (Terbium) and Mg (Magnesium)
                       290.0 nm lines of Cr (Chromium) and Os (Osmium)

                       422.7 nm lines of Ge (Germanium) and Ca (Calcium)
                       The easiest way to eliminate a spectral Interference is to use a different spectral line of

               the analyte for the assay. A chemical separation prior to the assay can also be used to eliminate

               Interference.
                       Another factor which must be considered while performing assays with flame AAS is

               potential difference between the viscosity of the standard and sample solutions. The Viscosity of
               the solution affects its rate of aspiration into the flame. More viscous solutions are not aspirated

               into the flame as rapidly as less viscous solutions. If the viscosity of the standard is less than that
               of the sample, a negative error is introduced into the assay.

                       Similarly if the viscosity of the standard is more than that of the sample, a positive error

               occurs. The viscosity of a solution is determined by the component of the solution. Errors owing
               to changes in viscosity can be eliminated by matrix matching, i.e. by preparing the standard in

               exactly the same matrix as that of the sample.
                       Zeeman Background Correction

                       Atomic absorption lines occur at discrete wavelengths because the transition that gives

               rise to the absorption is between two discrete energy levels. However, when a vapor phase atom
               is placed in a strong magnetic field the electronic energy levels split. This gives rise to several

               absorption lines for a given transition in place of the single absorption line in the absence of a
               magnetic field. This occurs in all atomic spectra and is called Zeeman splitting or the Zeeman

               effect.



























                       In the simplest case, the Zeeman effect splits an absorption line into two components.

               The  first  component  is  the  π  component,  at  the  same  wavelength  as  before  (unshifted);  the


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