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Formula 4-2<br />
Stability parameter a<br />
Formula 4-3<br />
Stability parameter q<br />
Ideal quadrupole fields require rods that have a hyperbolic profile. In actual practice, however,<br />
round rods are used, with the rod radius being equal to 1.144 times the field radius r . 0<br />
An electrical quadrupole field is formed between the rods. Ions of varying mass are shot<br />
axially into the rod system at approximately equal energy and move through the rod system<br />
at uniform velocity. The applied quadrupole field deflects the ions in the X and Y directions,<br />
causing them to describe helical trajectories through the mass filter. To solve the movement<br />
equations, the dimensionless variables<br />
and<br />
www.pfeiffer-vacuum.net<br />
Ions created through<br />
electron bombardment<br />
in the ion source<br />
Ion Optics<br />
Cathode<br />
Formation<br />
Area<br />
Ions separated by the m / e<br />
ratio in the rod system<br />
Figure 4.4: Operating principle of a quadrupole mass spectrometer<br />
a =<br />
q =<br />
8 . e . U<br />
m . 2 r . � 0<br />
2<br />
4 . e . V<br />
m . 2<br />
r0 . � 2<br />
are introduced to obtain Mathieu‘s differential equations. Their solutions yield the stable area<br />
with oscillation amplitudes of less than r beneath the triangle formed by the two solubility<br />
0<br />
curves in Figure 4.5. The values a = 0.23699 and q = 0.706 apply for the apex of the triangle.<br />
p p<br />
All solutions outside result in increasing oscillation amplitudes and thus in neutralization of<br />
the ions on the rods of the quadrupole filter.<br />
Dividing the two equations by one another yields:<br />
a U<br />
= 2 .<br />
q V<br />
This is the pitch of the so-called load line of the mass filter.<br />
Ions detected in the<br />
ion detector<br />
Page 89<br />
<strong>Vacuum</strong><br />
<strong>Technology</strong>