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Dynamics of Machines - Part II - IFS.pdf

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presented in section 1.6.9, to learn how to deal with experimental data and how to extract<br />

important information. H1(ω) as well as H2(ω) are obtained when an excitation force<br />

is horizontally acting on the platform mass and its value is measured by using a force<br />

transducer, and simultaneously the acceleration response <strong>of</strong> the platform is measured using<br />

a acceleration sensor. The experimental setup can be seen in figure 36(b). The most<br />

common ways <strong>of</strong> representing the frequency response functions H1(ω) and H2(ω) are in<br />

the form <strong>of</strong> amplitude and phase, or real and imaginary. In table 6 such values are presented<br />

in the real and imaginary forms and in figure 37 they are plotted. Please, plot H1(ω) and<br />

H2(ω) in terms <strong>of</strong> magnitude and phase.<br />

Frequency - H1 - H2 COHERENCE<br />

[Hz] [(m/s 2 )/N] [(m/s 2 )/N]<br />

1.6250 0.0490 - 0.0040i 0.0595 - 0.0049i 0.8236<br />

1.7500 0.0610 - 0.0051i 0.0698 - 0.0058i 0.8745<br />

1.8750 0.0750 - 0.0071i 0.0855 - 0.0080i 0.8776<br />

2.0000 0.0826 - 0.0068i 0.0945 - 0.0078i 0.8744<br />

2.1250 0.0974 - 0.0025i 0.1093 - 0.0028i 0.8907<br />

2.2500 0.1124 + 0.0015i 0.1204 + 0.0016i 0.9335<br />

2.3750 0.1310 - 0.0018i 0.1393 - 0.0019i 0.9403<br />

2.5000 0.1411 - 0.0100i 0.1477 - 0.0105i 0.9555<br />

2.6250 0.1540 - 0.0112i 0.1601 - 0.0116i 0.9621<br />

2.7500 0.1817 - 0.0040i 0.1889 - 0.0041i 0.9619<br />

2.8750 0.2113 - 0.0145i 0.2184 - 0.0150i 0.9677<br />

3.0000 0.2474 - 0.0172i 0.2520 - 0.0176i 0.9819<br />

3.1250 0.2676 - 0.0230i 0.2726 - 0.0234i 0.9817<br />

3.2500 0.3016 - 0.0364i 0.3080 - 0.0371i 0.9792<br />

3.3750 0.3460 - 0.0487i 0.3536 - 0.0497i 0.9787<br />

3.5000 0.4072 - 0.0467i 0.4173 - 0.0479i 0.9758<br />

3.6250 0.4601 - 0.0673i 0.4697 - 0.0687i 0.9795<br />

3.7500 0.5107 - 0.0903i 0.5165 - 0.0914i 0.9887<br />

3.8750 0.5894 - 0.1239i 0.5974 - 0.1256i 0.9866<br />

4.0000 0.6862 - 0.1427i 0.6994 - 0.1454i 0.9812<br />

4.1250 0.8110 - 0.1959i 0.8228 - 0.1987i 0.9857<br />

4.2500 0.9381 - 0.2824i 0.9539 - 0.2872i 0.9834<br />

4.3750 1.1113 - 0.4002i 1.1429 - 0.4116i 0.9723<br />

4.5000 1.3290 - 0.5385i 1.3711 - 0.5556i 0.9693<br />

4.6250 1.5586 - 0.8030i 1.6312 - 0.8405i 0.9555<br />

4.7500 1.8764 - 1.4666i 1.9844 - 1.5509i 0.9456<br />

4.8750 1.8832 - 2.0905i 2.0664 - 2.2938i 0.9114<br />

5.0000 1.2159 - 3.1027i 1.3216 - 3.3723i 0.9201<br />

5.1250 0.2098 - 3.6778i 0.2413 - 4.2301i 0.8694<br />

5.2500 -1.6165 - 3.2734i -1.7564 - 3.5568i 0.9203<br />

5.3750 -2.2154 - 2.3597i -2.3326 - 2.4844i 0.9498<br />

5.5000 -2.1657 - 1.4778i -2.2476 - 1.5337i 0.9635<br />

5.6250 -1.9289 - 1.1157i -1.9659 - 1.1371i 0.9812<br />

5.7500 -1.7058 - 0.8104i -1.7278 - 0.8208i 0.9873<br />

5.8750 -1.5511 - 0.6322i -1.5665 - 0.6384i 0.9902<br />

6.0000 -1.4389 - 0.5016i -1.4438 - 0.5033i 0.9966<br />

6.1250 -1.3520 - 0.4295i -1.3559 - 0.4307i 0.9971<br />

6.2500 -1.2591 - 0.3428i -1.2621 - 0.3436i 0.9976<br />

6.3750 -1.1843 - 0.3000i -1.1866 - 0.3006i 0.9980<br />

6.5000 -1.1241 - 0.2668i -1.1264 - 0.2673i 0.9980<br />

6.6250 -1.0716 - 0.2302i -1.0725 - 0.2304i 0.9991<br />

6.7500 -1.0206 - 0.2121i -1.0216 - 0.2123i 0.9990<br />

6.8750 -0.9715 - 0.1980i -0.9722 - 0.1981i 0.9993<br />

7.0000 -0.9376 - 0.1766i -0.9384 - 0.1767i 0.9992<br />

7.1250 -0.9073 - 0.1613i -0.9077 - 0.1614i 0.9995<br />

7.2500 -0.8793 - 0.1528i -0.8797 - 0.1529i 0.9995<br />

7.3750 -0.8516 - 0.1459i -0.8519 - 0.1459i 0.9996<br />

7.5000 -0.8271 - 0.1377i -0.8273 - 0.1377i 0.9998<br />

7.6250 -0.8107 - 0.1259i -0.8109 - 0.1260i 0.9997<br />

7.7500 -0.7879 - 0.1204i -0.7881 - 0.1204i 0.9997<br />

7.8750 -0.7695 - 0.1170i -0.7696 - 0.1170i 0.9998<br />

8.0000 -0.7513 - 0.1098i -0.7515 - 0.1098i 0.9998<br />

8.1250 -0.7374 - 0.1058i -0.7376 - 0.1059i 0.9998<br />

8.2500 -0.7240 - 0.1038i -0.7242 - 0.1038i 0.9998<br />

8.3750 -0.7122 - 0.0994i -0.7123 - 0.0994i 0.9998<br />

8.5000 -0.6963 - 0.0949i -0.6964 - 0.0950i 0.9998<br />

8.6250 -0.6861 - 0.0930i -0.6862 - 0.0930i 0.9999<br />

8.7500 -0.6792 - 0.0897i -0.6793 - 0.0897i 0.9998<br />

8.8750 -0.6705 - 0.0886i -0.6706 - 0.0886i 0.9998<br />

9.0000 -0.6606 - 0.0847i -0.6607 - 0.0847i 0.9999<br />

9.1250 -0.6544 - 0.0815i -0.6545 - 0.0815i 0.9998<br />

9.2500 -0.6463 - 0.0793i -0.6465 - 0.0794i 0.9997<br />

9.3750 -0.6365 - 0.0765i -0.6367 - 0.0765i 0.9997<br />

9.5000 -0.6287 - 0.0774i -0.6289 - 0.0774i 0.9997<br />

9.6250 -0.6250 - 0.0762i -0.6253 - 0.0762i 0.9996<br />

9.7500 -0.6207 - 0.0722i -0.6209 - 0.0722i 0.9997<br />

9.8750 -0.6160 - 0.0711i -0.6162 - 0.0711i 0.9997<br />

10.0000 -0.6081 - 0.0741i -0.6083 - 0.0741i 0.9998<br />

Table 6: Two experimental frequency response functions H1(ω) and H2(ω) <strong>of</strong> the test rig.<br />

3. Identification <strong>of</strong> model parameters – Suppose you have no access to the values <strong>of</strong> mass<br />

62

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