A Design Tool for Aerodynamic Lens Systems - Department of ...
A Design Tool for Aerodynamic Lens Systems - Department of ...
A Design Tool for Aerodynamic Lens Systems - Department of ...
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FIG. 10. Particle transmission efficiency as a function <strong>of</strong> the Stokes number<br />
<strong>for</strong> various Reynolds numbers at three different subsonic Mach numbers.<br />
(a) Ma = 0.03; (b) Ma = 0.10; (c) Ma = 0.32.<br />
A DESIGN TOOL FOR AERODYNAMIC LENS SYSTEMS 329<br />
FIG. 11. Cut<strong>of</strong>f Stokes numbers as a function <strong>of</strong> Reynolds number <strong>for</strong> three<br />
different Mach numbers.<br />
lens corresponding to the limiting trajectory <strong>of</strong> particle loss to<br />
the downstream spacer is ri = ds,i/(2ηc,i). The transmission<br />
efficiency can be estimated as the ratio <strong>of</strong> particle flux within ri<br />
to the total flux in that stage. There<strong>for</strong>e,<br />
ηt, spacer, i =<br />
⎧<br />
⎪⎨<br />
1 <strong>for</strong> dB,i ≤ ds,i<br />
⎪⎩<br />
<strong>for</strong> dB,i > ds,i<br />
. [24]<br />
� � d<br />
2 � �<br />
s,i<br />
d<br />
4<br />
s,i<br />
2 ds,i−1η −<br />
c,i ds,i−1ηc,i � � dB,i−1<br />
2 � � dB,i−1<br />
4<br />
2 d −<br />
s,i−1 ds,i−1 Note that dB,i = dB,i−1 ×|ηc,i|, and the diffusion effect is<br />
neglected.<br />
Loss by diffusion at each stage can be estimated through the<br />
Gormley-Kennedy equation (Gormley and Kennedy 1949):<br />
ηt, GK, i =<br />
⎧<br />
⎨1<br />
− 5.50 ξ<br />
⎩<br />
2/3 + 3.77ξ <strong>for</strong> ξ