Page 105 - Inorganic Mass Spectrometry : Fundamentals and Applications
P. 105

Inductively  Coupled  Plasma  Mass  Spectrometry              9s


                                                 0.3  l


                                           a  =I   0.2
                                            4eU
                                           m r2 W*  o.l
                                                 0.0 i.


                                                   0.0   0.2   0.4   0.6   0.8   1 .o
                                                                 2eV

                   Quadrupole mass  filter: (a) Diagram of quadrupole and connections to rf/dc
         power  supply.  (b) Side view of ion trajectories in two planes.




         power  supply  with a direct  current  (dc)  offset. The voltage  on  one  pair is opposite
                                                      is 180" out of phase  with
         to the  polarity of the  other  pair. The rf voltage  on  one  pair
         the rf voltage  on the other  pair.
              Although  the  ideal  cross  section of the  rods is hyperbolic, the best  approx-
         imation  using  circular  rods is obtained  when the radius of each  rod,  r, is equal to
         1.148 times the radius  from  the center of the four rods to the inside edge of the
         rods, ro [ 1261.
              The operation  of  the  quadrupole  can  be  understood  by  considering  the
         movement of the  ions  in  the  two  planes  perpendicular  to  their  flight  through  the
         quadrupole.  When  the  potential  on  two  opposite  rods negative,  positive  ions  are
                                                   is
         attracted  radially  outward  from  the  center the quadrupole  toward  the  negatively
                                          of
         biased  rods.  Conversely,  when  the potential  on  two  opposite  rods   is positive,
         positive  ions  are  repelled from the rods,  effectively  focused  toward the center of
         the  quadrupole.  The alternating  current  (ac) portion  of  the  voltage  waveform
         oscillates  with  time.  The  distance  ions  travel  outward from the  center  during the
         portion of  the waveform  when the ac  potential of two  opposite  rods is negative
         depends  on  the  mass-to-charge  ratio of  the ion, the  time  the potential  remains
         negative  (inversely  proportional to the ac  frequency),  the  magnitude the  applied
                                                               of
         ac  potential,  the  location
                             of the  ion relative to the center of the  quadrupole,  and  the
         velocity of the ion.  If  the  masslcharge  ratio of the ion is large  and  the  ac  frequency
         is high,  the  ion  does  not  move  far during  each  half-cycle  of  the  ac  waveform.
                                              the
         Therefore,  the  heavy  ions  are  most  affected  by average  (dc)  voltage  applied to
                                                            by
         the rods.  In  contrast,  lighter  ions  are  more  significantly  affected the  oscillating,
         ac  voltage.
              If the  average  (dc)  voltage  on  the  rods positive  (as is true for the  rods  in the
                                            is
                                              to
         x-z plane,  as  defined  in  Fig.  3.13a),  ions  tend be repelled  from  the  rods  toward
         the center of  the  quadrupole  on  average. ions that  have a masdcharge ratio  less
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