Page 190 - Tandem Techniques
P. 190

Page 173

            Methane produces more aggressive reagent ions than isobutane, and thus whereas methane ions produce
            a number of fragments by protonation, isobutane, by a similar protonation process, will produce almost
            exclusively the protonated molecular ion. This is clearly demonstrated by the mass spectrum of methyl
            stearate shown in Figure 5.6. Spectrum (A) was produced by chemical ionization using methane as the
            reagent gas and exhibits fragments other than the protonated parent ion. In contrast, spectrum  (B)
            obtained with butane as the reagent gas exhibits the protonated molecular ion only.

            The chemical ionization source is very similar to the simple ion impact source; in fact most mass
            spectrometer electron impact sources can perform the dual role, and in addition, act as a chemical
            ionization source. Dual-action sources do not perform quite as well as dedicated electron impact sources
            when used in the electron impact mode, but the loss of ionization efficiency is certainly no more than
            50%. Continuous use of a chemical ionization source results in significant source contamination which
            impairs the performance of the spectrometer. This results from the build-up of residues from the
            ionization process and thus the source requires cleaning by baking-out fairly frequently. A diagram of a
            typical gas inlet system for a chemical ionization source is shown in Figure 5.7,



















                                                          Figure 5.7
                                             A Gas Inlet System for Chemical Ionization

            The diagram illustrates the use of three different reagent gases but any number could be incorporated if
            desired. The source pressure is usually held at 0.1-0.5 torr and a low pressure regulator is incorporated
            to
   185   186   187   188   189   190   191   192   193   194   195