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9.1 Computation of Wave Kinematics. Problems of computing wave kinematics using Linear wave theory Revisit of HW 3Modifications to LWT (widely used by the offshore industry)(see Zhang et al. 1991, OTC 6522) Wheeler Stretching Linear Extrapolation Vertical Extrapolation
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1. Chapter 9 Applications of Hybrid Wave Models to Irregular Waves 9.1 Computation of Wave Kinematics
9.2 Prediction of Wave Elevation
9.3 Prediction of Wave Elevation Based on Wave Pressures
9.4 Prediction of Wave Properties of Short-crested Waves.
9.5 Accurate determine Wave Energy Loss Due to Wave Breaking.
9.6 Wave Forces on Slender Bodies
2. 9.1 Computation of Wave Kinematics
5. Heuristic Interpretations for the horizontal velocity under the crest -Steep wave crests are caused by many waves of different frequencies. -Waves of high frequencies are on the top of waves of low frequencies.Hybrid Wave Model (HWM) considers these factors -The still water level to a SW is the LWs surface - Considering Waves of high frequencies are on the top of waves of low frequencies
8. Wave Kinematics Prediction
27. Plan View of Sensor Layout
28.
29. Fig. 4 Power spectrum density according to pressure head time series
30. Fig. 5 Initial phases of each component of pressure and velocity
32. Fig. 7 Comparison of free-wave directions based on DHWM and Waverider (9803011020)
33. Comparison between prediction & measurement of Marex before & after the orientation of S4 was corrected
34. Comparison between prediction & measurement of SAAB before and after the orientation of S4 was corrected
35. Comparison of free-wave directions based on DHWM and Waverider (9803051040)
36. Comparison between prediction & measurement of SAAB before & after the orientation of S4 was corrected
37. Comparison of free-wave directions based on DHWM and Waverider (9804131100)
38. Comparison between prediction & measurement of Marex before & after the orientation of S4 was corrected
39. Comparison between prediction & measurement of SAAB before & after the orientation of S4 was corrected
52. Spar Platform
55. Quasi-static Analysis
mooring/tendon/risers modeled as nonlinear springs.
mooring line damping estimated or neglected
Coupled Dynamic Analysis
structure motion equations and mooring/tendon /riser dynamic equations solved simultaneously.
mooring line damping included.
Empirical formulation for VIV.
56. Numerical Code: COUPLE
57. Methodology of Coupled Dynamic Analysis
hinged boundary condition
Motion equations of a structure
58.
Two Choices of Computation Methods
Morison equation (Slender Body Structure)
Wave Kinematics using Hybrid Wave Model
(HWM). Inertia, drag and lifting (VIV) forces.
Ship Type Structures, (2nd order Wave Diffraction numerical codes, i.e.WAMIT)
Drag and lifting force based on Morison Equation
59. Use of the Hybrid Wave Models
61. Comparison with Measurements
62. Main Characteristics of JIP Spar (1:55)
66. Environment Conditions
Wave 100-year West Africa storm (JONSWAP Spectrum, H1/3=4m & TP =16 s). (Wind & Current).
0 and 45 degree wave heading.
Set-up (1:40)
Fixed model tests (no risers and tendons)
Compliant model tests (4 tendons & 4 (12) risers).
Measurements
Motions of Hull (TLP) in 6 degrees of freedom.
Tensions at the bottom of each riser and tendon.
71. Numerical Code: COUPLE
74.
Approach A: Morsion equation+HWM, quasi-static
Approach B: WAMIT+viscous, quasi-static
Approach C: Morison equation+HWM, coupled dynamic
Approach D: WAMIT+viscous, coupled dynamic
75. Morison Element Model
Four Column
diameter: 8.64m, length: 43.5m
Cm=1.0 (Guichard,2001)
Cd=0.7 ( 0 degree heading) (Teign & Niedzwechi,1998)
Cd=1.0 (45 degrees heading)
Four Pontoons
diameter: 7.02m, length: 19.935m
Cm=1.5
Cd=1.2 ( 0 degree heading)
Cd=1.4 (45 degrees heading)
83. Accurate Boundary Conditions for Numerical SimulationT. Liu & Prof. Chen