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The significance of coherent flow structures for the turbulent mixing ...

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Æ<br />

e¼c’„ïG<br />

ù<br />

#<br />

#dc’e<br />

›<br />

B<br />

›<br />

J<br />

ù<br />

ÿ©«ªa¬<br />

B<br />

›<br />

B<br />

›<br />

z<br />

­<br />

J<br />

ù<br />

©<br />

&<br />

o<br />

º"»<br />

‘a#a¸<br />

­<br />

¯<br />

3.1 Principles<br />

In case <strong>of</strong> <strong>the</strong> angular displacement arrangement <strong>the</strong> variation <strong>of</strong> <strong>the</strong> relative out-<strong>of</strong>-plane error<br />

as a function <strong>of</strong> <strong>the</strong> T coordinate is given by expression 3.3. Compared with <strong>the</strong> translation<br />

set-up, <strong>the</strong> dependence is ra<strong>the</strong>r weak as can be seen by comparing <strong>the</strong> upper plots <strong>of</strong> figure<br />

3.5.<br />

­ <br />

­µ´«´ ·<br />

¬v® o<br />

°²±0³ J<br />

· (3.3)<br />

B œ<br />

¨v¯<br />

©«ªa¬<br />

° ± ³ J<br />

­µ´¡<br />

By substituting in equation 3.3 it turns out that <strong>the</strong> relative out-<strong>of</strong>-plane error at <strong>the</strong><br />

optical axis is <strong>the</strong> reciprocal <strong>of</strong> <strong>the</strong> tangents <strong>of</strong> <strong>the</strong> T<br />

<strong>of</strong>f-axis angle , according to <strong>the</strong><br />

}<br />

following<br />

equation, and <strong>for</strong> ­ B œ<br />

(opening angle ¹ e¸ ) <strong>the</strong> out-<strong>of</strong>-plane error › becomes<br />

comparable with <strong>the</strong> in-plane error ­ J at <strong>the</strong> centre <strong>of</strong> <strong>the</strong> field <strong>of</strong> view, see lower right plot<br />

›<br />

<strong>of</strong> figure<br />

ù<br />

3.5.<br />

ù<br />

Bmœ<br />

­ (3.4)<br />

¬v® o<br />

¨ &<br />

©«ªa¬<br />

3.1.2 Scheimpflug condition<br />

Un<strong>for</strong>tunately, large opening angles are <strong>of</strong>ten not feasible by using standard equipment due<br />

to <strong>the</strong> limited depth <strong>of</strong> focus, see section 4.7 <strong>for</strong> fur<strong>the</strong>r details. For a typical configuration<br />

nm, <strong>for</strong> example, <strong>the</strong> depth <strong>of</strong> focus is only ¾<br />

ù<br />

with<br />

ù<br />

z fÀ¿ _<br />

f<br />

½<br />

© ÃÂ b<br />

and<br />

#]c’“•e mm. To overcome <strong>the</strong>se difficulties, <strong>the</strong> conditions which<br />

diffîG<br />

&óÁG<br />

improve <strong>the</strong> imaging when <strong>the</strong> object plane is tilted relative to <strong>the</strong> main plane <strong>of</strong> <strong>the</strong> lens, will<br />

be briefly derived.<br />

ù<br />

e“<br />

œ ù<br />

P<br />

2<br />

P<br />

1<br />

-Y<br />

A<br />

-Z<br />

a<br />

y<br />

z<br />

-Z o<br />

z o<br />

FIGURE 3.6: Scheimpflug condition: <strong>The</strong> image-, object- and main plane <strong>of</strong> <strong>the</strong> lens need to intersect<br />

in a common line <strong>for</strong> ideal imaging (Ä r +€Ä ).<br />

Assuming that <strong>the</strong> main-plane <strong>of</strong> <strong>the</strong> lens intersects with <strong>the</strong> object- and image-planes at Å r<br />

and Å respectively according to figure 3.6, it follows from geometrical considerations that<br />

<strong>the</strong> distance from <strong>the</strong> centre <strong>of</strong> <strong>the</strong> lens to <strong>the</strong> points <strong>of</strong> intersection can be expressed as<br />

Å r 0Ç ã<br />

ÁÇ ùÉÈ<br />

and Æ Å<br />

.îÊȤï0 Ç ódenotes <strong>the</strong> coordinates <strong>of</strong> a non-axial objectpoint<br />

(measured from <strong>the</strong> intersection <strong>of</strong> <strong>the</strong> optical axis <strong>of</strong> <strong>the</strong> lens with <strong>the</strong> object plane)<br />

<strong>the</strong> corresponding image coordinates. Using <strong>the</strong> definition <strong>for</strong> <strong>the</strong> transversal<br />

Eã ù§ñE<br />

andîñ\ïEó<br />

are<br />

41

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