effect of accelerometer mass on thin plate vibration - Jurnal Mekanikal
effect of accelerometer mass on thin plate vibration - Jurnal Mekanikal
effect of accelerometer mass on thin plate vibration - Jurnal Mekanikal
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
<strong>Jurnal</strong> <strong>Mekanikal</strong>, December 2009<br />
Experiment<br />
Finite Element<br />
(a) Accelerometer at P1<br />
(b) Accelerometer at P1<br />
(c) Accelerometer at P2<br />
(d) Accelerometer at P2<br />
(e) Accelerometer at P3<br />
(f) Accelerometer at P3<br />
Figure 4 : Comparis<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the mode shape for mode 2 with 5.84 gm <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
<str<strong>on</strong>g>accelerometer</str<strong>on</strong>g> <str<strong>on</strong>g>mass</str<strong>on</strong>g> located at P1, P2 and P3.<br />
Figure 4 shows the mode shape <str<strong>on</strong>g>of</str<strong>on</strong>g> mode 2 for 5.84 gm <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>accelerometer</str<strong>on</strong>g><br />
<str<strong>on</strong>g>mass</str<strong>on</strong>g> obtained through experiment and finite element analysis. The <str<strong>on</strong>g>effect</str<strong>on</strong>g>s <strong>on</strong> the<br />
mode shapes as the locati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the <str<strong>on</strong>g>accelerometer</str<strong>on</strong>g> varied were portrayed clearly.<br />
The mode shapes for <str<strong>on</strong>g>accelerometer</str<strong>on</strong>g> located at P2 and P3 were looked similar.<br />
While, the mode shapes <str<strong>on</strong>g>of</str<strong>on</strong>g> the mode for <str<strong>on</strong>g>accelerometer</str<strong>on</strong>g> located at P1 was slightly<br />
different compared to the other locati<strong>on</strong>.<br />
Figure 5 illustrates the mode shape <str<strong>on</strong>g>of</str<strong>on</strong>g> the mode 2 for <strong>thin</strong> <strong>plate</strong> with 45.84<br />
gm <str<strong>on</strong>g>of</str<strong>on</strong>g> the <str<strong>on</strong>g>accelerometer</str<strong>on</strong>g> obtained through experiment and finite element analysis.<br />
The mode shapes <str<strong>on</strong>g>of</str<strong>on</strong>g> the mode were significantly different for different locati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
the <str<strong>on</strong>g>accelerometer</str<strong>on</strong>g> mounted <strong>on</strong> the <strong>thin</strong> <strong>plate</strong> although all the mode shapes were <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
the same mode.<br />
It can be c<strong>on</strong>cluded that varying the locati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>accelerometer</str<strong>on</strong>g> mounted <strong>on</strong><br />
the <strong>thin</strong> <strong>plate</strong>, will give different results. An <str<strong>on</strong>g>accelerometer</str<strong>on</strong>g> placed <strong>on</strong> a nodal line<br />
did not cause <str<strong>on</strong>g>mass</str<strong>on</strong>g> loading <str<strong>on</strong>g>effect</str<strong>on</strong>g>, while it str<strong>on</strong>gly influence the measured data if<br />
place at anti nodal locati<strong>on</strong>.<br />
109