The Use and Calibration of the Kern ME5000 Mekometer - SLAC ...
The Use and Calibration of the Kern ME5000 Mekometer - SLAC ...
The Use and Calibration of the Kern ME5000 Mekometer - SLAC ...
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1.2. Path Length Modification<br />
<strong>ME5000</strong> Operation<br />
<strong>The</strong> <strong>Kern</strong> ME3000 <strong>Mekometer</strong> eliminates <strong>the</strong> fractional part f by changing <strong>the</strong> patb distance D until<br />
<strong>the</strong> phase difference is zero, indicating an integral number <strong>of</strong> half-wavelengths, (5) <strong>and</strong> Fig. 2.<br />
D+6D = mf (5)<br />
< D .f SD+<br />
< m.?J2 ><br />
FIGURE 2. Distance determination by changing <strong>the</strong> parh lengrh<br />
As in <strong>the</strong> first approach, m is found by repeating <strong>the</strong> measurement using several predefmed<br />
frequencies.<br />
1.3. Frequency Modification<br />
<strong>The</strong> <strong>Kern</strong> MESO& <strong>Mekometer</strong> also eliminates <strong>the</strong> fractional part f, but by using a different method.<br />
<strong>The</strong> frequency is changed until a zero phase difference is obtained, (6) <strong>and</strong> Fig. 3.<br />
?b<br />
= m.-<br />
D 2<br />
(6)<br />
< D ><br />
FIGURE 3. Distance determination by changing <strong>the</strong> frequency<br />
<strong>The</strong> value <strong>of</strong> m is found in a manner different from <strong>the</strong> frrst two approaches. <strong>The</strong> frequency is<br />
increased in small steps until a zero phase difference is again detected, at which frequency <strong>the</strong> path<br />
contains m+l <strong>of</strong> <strong>the</strong>se new half-wavelengths X1/2,<br />
D = (m+l)$ (7)<br />
<strong>The</strong>se two frequencies provide sufficient information to resolve m <strong>and</strong> thus <strong>the</strong> distance.<br />
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