Page 122 - Inorganic Mass Spectrometry : Fundamentals and Applications
P. 122

l12                                                         Olesik


                       Load Coil                            Load Coil
              12







                                                                             1  '
               0                                    -5'   i   +.l   1   '4   8   l   *   l
               -30   -20   -10   0   10   20   30    -30  -20   -10   0   10   20   30
                   Height above load coil (mm)           Height above load coil (mm)
                   1'7  The  eEect of  center (nebuli~er) gas  flow  rate  plasma  temperature  and  gas
            velocity  profiles.  Calculations  were  performed  by using a simulation  program,  HiFI  2.0.
            (From  Ref.  424.)



            a  fixed  sampling  depth,  an  increase   in  nebulizer  gas  flow  rate  decreases   the
            distance  in  the  plasma  that  the sample travels  before  reaching  the  sampling  orifice.
            ~urthermore, for pneumatic  nebulizers  and  conventional  spray  chambers  without
            desolvation, the aerosol  and  water  vapor  transport into the plasma  increases  with
            increasing  nebulizer  gas  flow  rate.  This  tends  to   cool the plasma  and  delay
            completion of  vaporization  and  ionization.
                 A certain  amount of  time is required to desolvate,  vaporize,  atomize,  and
            ionize a  drop  of  sample. If  the  ions  are  sampled  too  early, vaporization  and
            ionization of the  sample  may not be complete, F~he~ore, a si~ni~cant number
            of  incompletely  desolvated  droplets  may  survive  to  the  sampling  orifice [ 1571.
            Even  a  small  number   of  incompletely  desolvated  droplets  can  affect  signals
             sig~ficantly because  each  droplet can cool a  1-  to 12-m-wide region  of  the
            plasma [l 581, After  the  sample is completely  vaporized  and  converted into ions,
            the  ions  diffuse  outward  in  the  plasma,  reducing  the  number ions that enter the
                                                             of
            mass  spectrometer  [159,160]. The optimal  sampling  location  depends  on  a  trade
            off  between  a  distance far enough so that  most of  the  sample  aerosol  has  been
            converted into ions and  a  distance  not  so far that  diffusion  reduces  the  number of
            ions  sampled by the mass  spectrometer.
                 If  the  plasma  power   is increased,  the  location  where  the  plasma  begins
             along  the  center axis moves  upstream  (closer  to the injector tube of the torch)  and
            the  plasma  temperature  increases.  Therefore,  if  the  nebulizer  gas  flow  rate  were
             optimized at a  power of  1.0 kW  and the power  were  increased  to  1.2 kW, ions
             would  be  produced   farther from  the  sampling  orifice.   There would  be  more
                                                    the
             extensive diffusion of the  ions  before  they  reached sampling  ori
             be overcome by  either moving  the sampling  orifice  closer  to the  load  coil  or
             increasing the nebulizer  gas  flow  rate.
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