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The Use and Calibration of the Kern ME5000 Mekometer - SLAC ...

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<strong>ME5000</strong> Operation<br />

4&l 470 480 4Kl SW 510<br />

fmqwncy (MHzl<br />

Figure 5. Actual Characteristic Curves for Instruments 357037 <strong>and</strong> 357081<br />

For short-distance measurements, below 20 m, <strong>the</strong> normal 15 MHz b<strong>and</strong>width is insufficient (for<br />

reasons explained below), so <strong>the</strong> intensity threshold is reduced to 75% <strong>of</strong> maximum to give a wider<br />

b<strong>and</strong>width, nominally 30 MHz. In practice, this b<strong>and</strong>width is dependent upon <strong>the</strong> characteristics <strong>of</strong> <strong>the</strong><br />

individual crystal, <strong>and</strong> has been found to vary in <strong>the</strong> range 18 - 29 MHz. Table 1 shows <strong>the</strong> normal <strong>and</strong><br />

extended b<strong>and</strong>widths for <strong>the</strong> two instruments shown in Fig. 5.<br />

357037 (LBL)<br />

357081. (SSC)<br />

3.1 Normal Mode<br />

Table 1. Modulation b<strong>and</strong>width <strong>of</strong> instruments 357037 <strong>and</strong> 357081<br />

NORMAL. EXTENDED<br />

Range (MHz) B<strong>and</strong>width Rarqe (MHz) B<strong>and</strong>width<br />

472.112 - 486.915 14.803 465.383 - 494.644 28.261<br />

472.785 - 486.915 14.130 469.420 - 490.280 20.859<br />

3. RESOLVING THE DISTANCE<br />

<strong>SLAC</strong>’s field measurement <strong>and</strong> data collection program ME5COO.BAS mimics <strong>the</strong> operation <strong>of</strong> <strong>the</strong><br />

onboard program in <strong>the</strong> ME5OOO’s EPROM for <strong>the</strong> measurement <strong>of</strong> distances in <strong>the</strong> normal operating range<br />

<strong>of</strong> <strong>the</strong> instrument, 20 - 8000 m.<br />

3.1.1. Calculation <strong>of</strong> distance from frequency<br />

Starting at <strong>the</strong> lower end <strong>of</strong> <strong>the</strong> b<strong>and</strong>width an upward sweep is made until a frequency F1 is found at<br />

which <strong>the</strong> phase difference is zero. This nodal point occurs when <strong>the</strong>re is an integer number ml <strong>of</strong> half-<br />

wavelengths along <strong>the</strong> measurement path. <strong>The</strong> sweep is continued until a second nodal point is found at<br />

frequency Fl,.+ at which <strong>the</strong>re are ml+1 half-wavelengths. <strong>The</strong> distance can be determined from <strong>the</strong><br />

frequency difference FM-FI, (S-10).<br />

12<br />

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