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NOTICE The quallty of this microfor
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I*I Et"" :lbL="*"" k.. bpilmsa7d Di
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Acknowledgements I should like lo t
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Abstract As a result of the increas
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Contents List of Figures xii List o
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4.6.3 Fnbrieatiox of tllc Rcduced M
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A Selected Algoilthma 278 A.1 Diago
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4.5 Member Configuration at level #
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7.21 Dynamic Mode # 6 (Intact Model
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7.49 Typical Measured lnput Wnve Sp
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7.66 hulls fmm Accelerometer A2 due
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D.ll DynamicMode # I (Intact Model)
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List of Tables 4.1 Symbols, Units a
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8.9 Pacent Changes in Resonant Frrq
- Page 33 and 34: List of Symbols d(k) .i(k) A A(L1 1
- Page 35 and 36: autosp~trni density of r(t) cms-spe
- Page 37 and 38: 0,1,2
- Page 39 and 40: [@I a Pu. P. P:,," P.. o2(k) instan
- Page 41 and 42: een recorded, then it is beneficial
- Page 43: Associated with every vibration mod
- Page 46 and 47: Such s model is called a dynamicall
- Page 48 and 49: presenlcd. Chapter 3 contains the t
- Page 50 and 51: al frequcncic. occurred when member
- Page 52 and 53: detwM from the data roeorded (later
- Page 54 and 55: y Duggan d a!. [a]. This study inve
- Page 56 and 57: ~~lidity of the results war rompsro
- Page 58 and 59: nic~~~aan:immcdiateiyuseful, they a
- Page 60 and 61: tlncayatem hehavior oftrusswork pla
- Page 62 and 63: Chapter 3 Theoretical Modelling Tll
- Page 64 and 65: 3.2 Wave Theories Works by earlier
- Page 66 and 67: F;-RY% WAVE THEORY) 1/20 I "w/Lw DE
- Page 68 and 69: DIRECTION OF WAVE PROPAGATION FIG.
- Page 70 and 71: liero, d and ita wlocity component
- Page 72 and 73: and and a+ "=-. OY = wA~inl~IW(1+ s
- Page 74 and 75: FIG.3.4 ARBITRARILY ORIENTED CYLIND
- Page 76 and 77: ~i n long c mtd wave is being conai
- Page 78 and 79: inrther. Ultimately, the resulting
- Page 80 and 81: equcncia and mode shapes, equalion
- Page 82 and 83: Toestablish tho relationship betwee
- Page 86 and 87: lG.3.6 SIMULATED 3-D AND STICK MODE
- Page 88: 1. priam&tic heam members, 5. sir d
- Page 92 and 93: The equation of motion for each ele
- Page 94: From tho ~tatic dispiaeemont muita,
- Page 97 and 98: instance, the non-dimensional equal
- Page 99 and 100: functional relationship relating th
- Page 101 and 102: whcre F, 't iinstantanmua force at
- Page 103 and 104: Table 4.1 Symbols, Unit. and Dimens
- Page 105 and 106: thc Buckinghm r-Thmrem (i.c., I2 te
- Page 107 and 108: That is, equations (4.28) and (4.29
- Page 109 and 110: C. Ilence, if the dynamic amplifica
- Page 111 and 112: where (2) is the general gmmdric or
- Page 113 and 114: the prolotype. Damping is dcfincd b
- Page 115 and 116: 2 LEVEL # 7 1 28956DO NOTE: ALL DIM
- Page 117: Mataial= Structural Steel, E = 206.
- Page 122 and 123: LEVEL C6 NOTE: ALL DlMENStONS IN m
- Page 124 and 125: Table 4.5 Relevant Materiel Propert
- Page 128 and 129: FlG.4.9 COMPLETED STRUCTURE. 89
- Page 132 and 133: Since the de& sertioo of the struct
- Page 134 and 135:
% FINITE ELEMENT ANALYSIS (COMPUTER
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3 53 I CONTROL RM SECTION A-D. MEZZ
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I I SERVO CONTROLLER MODEL 408.1% j
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LEGEND FI B F2 FREE VlBllTlDN INITI
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5.1.4 Response Circuit Data acquisi
- Page 146 and 147:
I ~T.UG~U~E LEGEND: DYIIYT I., 10 A
- Page 150 and 151:
the basis upon which the irregular
- Page 152 and 153:
then manipulated by the computer ro
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,.. G STRUCTURE IN STILL WATER STRU
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dter every set of hen wave excitati
- Page 158 and 159:
To gather spectral information fmm
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is the timelag between silrnplev~l~
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ics, with a lew notable exceptions,
- Page 164 and 165:
If bath aides of the dove cguntion
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Conversely, r(1) can be estimated b
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quires ahout N(M + 1) + 9Y1 arithme
- Page 170 and 171:
So equation (6.18) become: I, i = C
- Page 172 and 173:
At each resonant frequency, the hdl
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6.5 Impact Testing Impact testa wer
- Page 179 and 180:
Chapter 7 Theoretical and Experimen
- Page 181 and 182:
Table 7.1 Natural Wequeney Comparis
- Page 188:
Therefore, with the natural freluen
- Page 199:
Pi7 Be: kD! SF:& iid id . -5 i#@ Ba
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(i.o., at noder 6, 12, 18, 22 and 2
- Page 208:
tirne dntn;lis reprcsez~lnlioti of
- Page 214:
-CUI~IW~~~ anstmr 9~1sn-mmu3n DL um
- Page 218:
the posilivc and nogntivr peaks. Re
- Page 224 and 225:
Table 7.7 X-Direction Results From
- Page 226:
2 GEhEnnlEO FRDM TdE WrllTE hOISE l
- Page 230 and 231:
FIG. 7.53 MEASURED INPUT WRVE FROM
- Page 236:
'IUnU133dS 3SIR1 31IHI 9NISn--91 30
- Page 244 and 245:
Table 7.9 MEM Damping Estimates fro
- Page 246:
7.2.3 Impact Test Results In Chsptc
- Page 252 and 253:
(K 01 0 01- OZ- DE- 0,- OBI (KI 09
- Page 257 and 258:
Chapter 8 Discussion of Results In
- Page 260 and 261:
of rnemhcr removal can he visually
- Page 263 and 264:
emoved is a cancellation offecl, an
- Page 265 and 266:
Force Variation Along the Jacket. P
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fi~t on the lower rrequency end of
- Page 271 and 272:
pond approximately to thasc which c
- Page 273 and 274:
'Ikble 8.1 Measured Resonant Rsquen
- Page 275 and 276:
Table 8.6 Measured Resonant Wequenc
- Page 277 and 278:
After a close look at the measured
- Page 279 and 280:
Table 8.11 Percent Changes in Reson
- Page 281 and 282:
Table 8.16 Percent Changes in Reson
- Page 283:
apprmiably. Since the tmnsa of the
- Page 286 and 287:
'*~+12 \5 \8 h4 h7 $0 FREOUENCY IHz
- Page 288 and 289:
8.2.4 Impact Test Results 'l'incobj
- Page 293 and 294:
I able 8.20 Comparison of the Reson
- Page 295 and 296:
'Phc invalidity of thc lumped mass
- Page 297 and 298:
Chapter 9 Concluding Remarks and Re
- Page 299 and 300:
general agreement. 5. An investigat
- Page 301 and 302:
mode, br example, might have been e
- Page 303 and 304:
References K I'o,lnt~n~. 'A Sludy o
- Page 305 and 306:
[21] .I.K. Vandiver, "Structo~ral D
- Page 307 and 308:
1431 D.J. Kartewcg and G. d-Vria "O
- Page 309 and 310:
1671 I..S. Marplo, "A NCW Autorepes
- Page 311 and 312:
(111 J. Zhou "Ocean Wave Simulation
- Page 313 and 314:
[Ill M.C. Ilallsm, N.J. Hcaf and L.
- Page 315 and 316:
Appendix A Selected Algorithms Tllr
- Page 317 and 318:
- M = the total mass of the slructu
- Page 319 and 320:
Suhrtituting qualion (A.5) in equal
- Page 321 and 322:
..3 Longuet-Higgins and Cokelet Smo
- Page 323 and 324:
Appendix B Sample Calculations Typi
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The dcnsity of ABS plsstic (p.,,) i
- Page 327:
C.l Calibration and Instrumentation
- Page 330:
D.l Mode Shape (Members 70 and 68 R
- Page 340 and 341:
D.2 Results for an Impact Initiated
- Page 343:
i W 4 P Li I 2: 5: E B '5 2- d :" i
- Page 347:
oa m 01 o or- QZ- oe- om Q Z ~ oo a
- Page 353:
D.3 MEM Damping Estimates for the D
- Page 357:
Table D.4 MEM Damping Estimate. fro