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4 - Memorial University of Newfoundland DAI

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8.2 Experimental Results<br />

8.2.1 Transient Decay Tests to Compute Damping<br />

In-Air Tests. Averqcglobai x and y direction damping ratio variations (us-<br />

ing lhc logarithznie decrement method) were shown in Figure 7.45. In both<br />

twos, thc damping variation is more steady after eight cycles. Therefore, this<br />

mgion war uscd to determine the transienl decay damping. For comparison,<br />

con>putcd damping oatimstes using the above method and the average damp-<br />

ing obtained fmm tho curvc fitting method (i.e., the LarenbereMarquardt<br />

and Pinilc difference Jneobian) are shown here:<br />

Damping Estimates from In-Air Testa<br />

lagnrithmic Decmment Curve Pitting<br />

In-Water Tests. Like the in-air tests, average global r: and y direction<br />

dnrnpi~~g ratio variations (using the logsrithmie decrement method) were<br />

depicted in Pigum 7.18. After six cycles, the variation in damping is more<br />

rtcdy. Thc following am the damping estimates:<br />

Damping Estimates from In-Water Tests<br />

Logarithmic Decmmcnt Curve Pitting<br />

, 3.5755 i 0.15% 3.6576 i 0.04%<br />

( , 1.7033 i 0.04% 1.7221 i 0.02%<br />

These damping rwlors are assoei~ted with the lalgiobal flexural modes in<br />

Lhc global x and y direclions. The values oblained from the in-air tesls corre-

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