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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

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