Engineering Simulation Software for the Offshore, Marine and Wave/Tidal Renewable Energy Industries. Viscous CFD Applications. Phil Stopford ANSYS UK
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1 Engineering Simulation Software for the Offshore, Marine and Wave/Tidal Renewable Energy Industries Viscous CFD Applications Phil Stopford ANSYS UK 2011 ANSYS, Inc. All rights reserved. 1 ANSYS, Inc. Proprietary
2 Agenda Introduction to viscous CFD CFD capabilities Offshore and marine applications Hydrodynamic characterisation/loading Motion response Vortex-induced vibration Added mass and damping Two-way fluid structure interaction Wind/Tidal renewable energy applications Oscillating water columns Tidal turbines Wind farm layouts Summary 2011 ANSYS, Inc. All rights reserved. 2 ANSYS, Inc. Proprietary
3 Fluid dynamics Complex and sometimes non-intuitive Depends on the interaction of multiple features Which situation will see the highest velocity? A B 1m/s 1m/s 2011 ANSYS, Inc. All rights reserved. 3 ANSYS, Inc. Proprietary
4 Results Adverse pressure gradient ~60% higher Velocity (m/s) Pressure Field 2011 ANSYS, Inc. All rights reserved. 4 ANSYS, Inc. Proprietary
5 What is CFD? Computational Fluid Dynamics (CFD) is the science of predicting fluid flow, heat transfer, mass transfer and related phenomena by solving the mathematical equations which govern these physical processes, using a numerical approach (i.e. on a computer) including viscous effects Flow simulation allows a prototype to be modelled on the PC workstation Complementing physical testing CFD can be used on Any geometry at any scale Most flow physics including free surfaces and motion 2011 ANSYS, Inc. All rights reserved. 5 ANSYS, Inc. Proprietary
6 Introduction to CFD applications Many applications for fluid flow analysis with viscous CFD Hydrodynamic characterisation and loading of floating and submerged hull forms, structures and devices Viscous drag, form drag Wave-making, sea-keeping Motion response Vortex induced vibration Added mass and damping analysis Tidal turbine hydraulic performance Tidal/wind turbine farm layout and wake effects Providing fluid loading results for fluid-structure-interaction assessment 2011 ANSYS, Inc. All rights reserved. 6 ANSYS, Inc. Proprietary
7 CFD capabilities CFD capabilities for offshore, marine and wave/tidal Flow visualisation Quantitative information Pressures, velocities,... Viscous/pressure forces, drag, lift,... Free surface models Simple wave generation Wave/body interactions Dynamic response Rigid body 6-DOF solutions Added mass and damping calculations Tidal/Wind turbine-specific tools Rotating and stationary components Performance and power extraction Cavitation modelling 2011 ANSYS, Inc. All rights reserved. 7 ANSYS, Inc. Proprietary
8 Hydrodynamic characterisation 2011 ANSYS, Inc. All rights reserved. 8 ANSYS, Inc. Proprietary
9 Hydrodynamic Characterisation and Loading Viscous CFD provides a way to characterise the overall forces on a floating or submerged body Viscous and form drag 5415 Destroyer test case At 4.03 knots Drag CFD /- 2 N Experiment 44.3 N 2011 ANSYS, Inc. All rights reserved. 9 ANSYS, Inc. Proprietary
10 Free-surface flows Wigley Hull test-case Validation of ANSYS CFD capability to calculate wave structure for an analytical hull shape Excellent agreement with experiment 2011 ANSYS, Inc. All rights reserved. 10 ANSYS, Inc. Proprietary
11 Racing Yacht CFD Racing yacht geometry at model scale Fully appended with rudders, keel and bulb Different speeds give different hull orientation 2011 ANSYS, Inc. All rights reserved. 11 ANSYS, Inc. Proprietary
12 Side Force [N] Total Drag [N] Validation: Racing Yacht Forces at 20 heel Constant speed Variation of yaw angle Good agreement Drag vs Side Force 20 Heel & 14 knots Side Force [N] CFX Experiment Side Force vs. Yaw Angle 20 Heel & 14 knots Yaw [deg] CFX Tank 2011 ANSYS, Inc. All rights reserved. 12 ANSYS, Inc. Proprietary
13 Transient wave-loading with CFD CFD can be used to look at transient loadings on structures Extreme wave events Peak load transfer to ANSYS Mechanical model Automated 1-way transfer of load from ANSYS CFD to Mechanical within Workbench 2011 ANSYS, Inc. All rights reserved. 13 ANSYS, Inc. Proprietary
14 Motion response 2011 ANSYS, Inc. All rights reserved. 14 ANSYS, Inc. Proprietary
15 CFD simulations with moving bodies It is also possible to use viscous CFD to understand The effect of geometry motion on fluid flow (a prescribed motion) Geometry motion due to fluid flow and resulting loads (a flow-driven motion) All this can be done in ANSYS CFD software if moving solids are: Rigid bodies Have deformations that are simple to describe in the CFD software Prescribed motion Flow-driven motion 2011 ANSYS, Inc. All rights reserved. 15 ANSYS, Inc. Proprietary
16 Rigid Body CFD Solution Dynamic Sink and Trim Speedboat example Six degree of freedom Free surface flow 2011 ANSYS, Inc. All rights reserved. 16 ANSYS, Inc. Proprietary
17 Rigid Body CFD Solution Dynamic Sink and Trim Mono-chromatic waves generated at inlet by simple linear theory Pitch and heave from 6-DOF solution 2011 ANSYS, Inc. All rights reserved. 17 ANSYS, Inc. Proprietary
18 Mooring example 2011 ANSYS, Inc. All rights reserved. 18 ANSYS, Inc. Proprietary
19 Mooring Model The addition of mooring lines as part of a CFD calculation is now possible Complementing AQWA capability Simple Spring-Damper model for tethers Includes capability to have multiple mooring points Implemented to allow for 3D cases Moving Body Force Applied By Mooring c ẋ F = k x + c ẋ k x 2011 ANSYS, Inc. All rights reserved. 19 ANSYS, Inc. Proprietary
20 Model Setup For each mooring: Specify an arbitrary mooring point, (x,y,z) Provide an initial location for the attachment point on the moving body, (x,y,z) Input values for stiffness and damping coefficients, k and c Set the length of the tether, L L, k, c Attachment Point Mooring Point 2011 ANSYS, Inc. All rights reserved. 20 ANSYS, Inc. Proprietary
21 Mooring example Two moorings defined Open Channel Flow Direction 2011 ANSYS, Inc. All rights reserved. 21 ANSYS, Inc. Proprietary
22 Vortex Induced Vibration 2011 ANSYS, Inc. All rights reserved. 22 ANSYS, Inc. Proprietary
23 Vortex induced vibrations An important topic for the offshore industry Offshore platforms need to be placed in more and more hostile environments A challenging fluid-structure interaction (FSI) application Complex response of riser, etc to ocean waves and currents Length to diameter ratios of order 10 3 Reynolds numbers of order 10 4 Several simulation approaches of varying complexity CFD with embedded rigid-body mechanics CFD with coupling to flexible structural mechanics An offshore platform near Sakhalin (Russia) 2011 ANSYS, Inc. All rights reserved. 23 ANSYS, Inc. Proprietary
24 Simple 2-D VIV Use 2-D CFD with 2 degrees of freedom and numerical tethers to understand riser motion Computationally inexpensive 2011 ANSYS, Inc. All rights reserved. 24 ANSYS, Inc. Proprietary
25 More advanced methods for VIV Strip theory Fluid flow fields are computed in multiple two-dimensional planes positioned along the riser Computationally cheaper than full 3-D CFD Doesn t take into account threedimensional flow features Only resolves flow forces at specific locations Potentially useful methodology for coupling ANSYS CFD to beam (riser specific) structural simulation software 2011 ANSYS, Inc. All rights reserved. 25 ANSYS, Inc. Proprietary
26 More advanced methods for VIV Full 3-D CFD simulations dynamically to structural simulations (ANSYS Mechanical) Two-way fluid-structure-interaction Fluid flow field is computed with a full 3D CFD model CFD results passed to ANSYS Mechanical as loads ANSYS Mechanical calculates deformation and passes geometry displacement back to ANSYS CFD Computationally expensive but shows potential 2011 ANSYS, Inc. All rights reserved. 26 ANSYS, Inc. Proprietary
27 Experimental Set-up Delta Flume in Holland Inlet velocity: 0.16m/s Top tension: 405N Bending stiffness: 29.9NM 2 Axial stiffness: 5.88MN Structural dumping: 0.33% Mass ratio relative to the surrounding water: 3 Riser diameter: 28mm Length to diameter ratio ~470 Submerged part: 42.5% of the riser length Re ~5000 Cabin Water surface inside the vacuum tank Water surface in the flume 13.12m Riser Vacuum tank Incident velocity profile at the riser from Chaplin et al. (2004) 2011 ANSYS, Inc. All rights reserved. 27 ANSYS, Inc. Proprietary
28 ANSYS CFD Set-up Computational domain and boundary conditions inlet top surface (free slip) tank walls (no slip) water surface (free slip) outlet Floor (free slip) Fluid/solid interface The case was run as laminar Time discretization scheme: Second Order Backwards Euler Spatial discretization scheme: Second Order Upwind Convergence criterion: 10-5 for RMS Residual Maximum number of coefficient loops: ANSYS, Inc. All rights reserved. 28 ANSYS, Inc. Proprietary
29 ANSYS Structural Set-up Boundary conditions F=405N (applied to the central node) No movement in xz No constraint in y No movement in xz No constraint in y No movement in xyz Fluid/solid interface - All nodes but central - central node The nonlinear transient solver (i.e. the large displacement transient option) was used Riser was modeled as a solid cylinder with Solid185 elements (3D 8-node structural solid) Young's modulus of Pa was chosen to match the axial stiffness Ramped loading was switched off 2011 ANSYS, Inc. All rights reserved. 29 ANSYS, Inc. Proprietary
30 View of Flow Structure A view of vorticity field at different heights. Red and blue colours represent positive and negative vorticity respectively 2011 ANSYS, Inc. All rights reserved. 30 ANSYS, Inc. Proprietary
31 Results Riser Motion Moving riser started from rest 2011 ANSYS, Inc. All rights reserved. 31 ANSYS, Inc. Proprietary
32 Added-Mass and Damping Calculation 2011 ANSYS, Inc. All rights reserved. 33 ANSYS, Inc. Proprietary
33 Added Mass and Damping When simulating floating bodies, or mooring systems, some 3D-panel method codes and multi-body dynamics codes require additional coefficients in order to get an accurate response. The effect of these coefficients is implicitly included in full CFD analyses Sometimes coefficients can be estimated for simple geometries For complex geometry we can calculate them quickly using CFD 2011 ANSYS, Inc. All rights reserved. 34 ANSYS, Inc. Proprietary
34 Added Mass and Damping Perform transient simulation with prescribed sinusoidal motion, e.g. heave, sway, and look at variation with amplitude and frequency Examine reaction force response of the structure and the phase change (compared to displacement) Coefficients obtained by extracting Fourier coefficients of the fundamental frequency over a time period Higher order components of coefficients could also have been extracted using similar techniques based on Fourier analysis 2011 ANSYS, Inc. All rights reserved. 35 ANSYS, Inc. Proprietary
35 Damping Example Eni G R O U P Lowering of structure to seabed Need added mass and damping for accurate dynamics simulation Perform transient CFD calculation on one mudmat Separate horizontal and vertical motion prescribed Sinusoidal moving mesh Simulation duration of 3-5 cycles only Information courtesy of Saipem (UK) Ltd 2011 ANSYS, Inc. All rights reserved. 36 ANSYS, Inc. Proprietary
36 Force (kn) Damping Example Same geometry and mesh can be used for heave and sway calculations 3.E+05 2.E+05 1.E+05 0.E+00-1.E+05-2.E+05-3.E+05-4.E+05-5.E Time (Seconds) Hydrodynamic Forces in Heave Direction (Inverted Can) 2011 ANSYS, Inc. All rights reserved. 37 ANSYS, Inc. Proprietary
37 Damping Example Results analysed in CFD-Post Coefficients extracted from amplitude and phase of reaction force plot Also examined: Effects of holes in geometry Effect of proximity to sea bed Sway Motion Added Mass in Heave Period (s) Heave Motion Amplitude (cm) Calculated Value (no holes) Model Tests (4 holes) Damping in Heave Period (s) Amplitude (cm) Calculated Value (no holes) Model Tests (4 holes) ANSYS, Inc. All rights reserved. 38 ANSYS, Inc. Proprietary
38 RAO (m/m) RAO (m/m) Response Amplitude Operators (RAO) Comparison of CFD to Free Floating Calm Buoy measurement Surge RAO Prescribed heave motion 0.6 RAO calculated from Added Mass, Damping and Restoring coefficients Experimental CFD Buoy model Anchored with three mooring lines OPTICAL SYSTEM FOR MEASUREMENT OF BUOY MOTION Full scale period (s) Heave RAO 1.4 LINE #3 LINE # Experimental CFD ANSYS, Inc. All rights reserved. 41 Full scale period (s) ANSYS, Inc. Proprietary
39 Transient two-way fluid-structureinteraction 2011 ANSYS, Inc. All rights reserved. 43 ANSYS, Inc. Proprietary
40 Transient Dynamics: Two-way FSI 2-Way Coupled Fluid Structure Interaction Motion of vessel calculated not prescribed Structural FEA code used to solve for vessel displacement Loads exchanged in both directions Between CFD and FEA code More coupled solution than 1-way Introduce concept of coupling convergence Transient or steady-state Single exchange per timestep explicit Multiple exchange per timestep implicit Important for strongly coupled problems 2011 ANSYS, Inc. All rights reserved. 44 ANSYS, Inc. Proprietary
41 Transient Dynamics: Two-way FSI Basic sea-keeping Two-way FSI Fluid flow simulation in ANSYS CFD Waves generated as boundary condition again Structural mechanics in ANSYS FEA Examine slamming for example, and stress response 2011 ANSYS, Inc. All rights reserved. 45 ANSYS, Inc. Proprietary
42 Guest presentation BMT presentation 2011 ANSYS, Inc. All rights reserved. 46 ANSYS, Inc. Proprietary
43 Wave Energy: Oscillating Water Column Simulation 2011 ANSYS, Inc. All rights reserved. 47 ANSYS, Inc. Proprietary
44 OWC principle Waves in sea generate oscillation in vertical duct Resonance occurs if duct diameter and length are carefully chosen Resonance can increase the wave height significantly Cylinder can be on sea-bed, or at surface Reference: Lighthill, J., 1979, Two-dimensional analyses related to wave-energy extraction by submerged resonant ducts, J. Fluid Mech, 91, part 2, ANSYS, Inc. All rights reserved. 48 ANSYS, Inc. Proprietary
45 OWC example application Compression chamber above OWC Energy can be harnessed (e.g. via Wells turbine) Source: ANSYS, Inc. All rights reserved. 49 ANSYS, Inc. Proprietary
46 Vertical cylinder on sea-bed Pressure distribution at resonance Amplitude elevation in cylinder 2011 ANSYS, Inc. All rights reserved. 51 ANSYS, Inc. Proprietary
47 Vertical cylinder Pressure time trace at monitoring points on seabed Point 1 inside cylinder, Point 2 outside cylinder upstream More resonant 2011 ANSYS, Inc. All rights reserved. 52 ANSYS, Inc. Proprietary
48 Wave-piercing design Air Pressure variation inside cylinder 2011 ANSYS, Inc. All rights reserved. 53 ANSYS, Inc. Proprietary
49 Air movement through the hole at the top of the OWC 2011 ANSYS, Inc. All rights reserved. 54 ANSYS, Inc. Proprietary
50 Tidal turbine simulation using CFD and one-way FSI 2011 ANSYS, Inc. All rights reserved. 55 ANSYS, Inc. Proprietary
51 Tidal turbine CFD CFD provides the ability to perform detailed hydraulic assessment of tidal turbine devices Quantitative results Blade loading Torque Axial thrust Power and efficiency Flow visualisation Streamlines Pressure, temperature, velocity plots It can show why a machine design is good or bad Where are the losses due to separation and swirl at certain operating conditions? CFD also provides pressure loads for structural mechanics 2011 ANSYS, Inc. All rights reserved. 56 ANSYS, Inc. Proprietary
52 Quantitive Analysis Forces and Torque on Blades Resultant Force in X direction [N] Resultant Force in Y direction [N] Resultant Force in Z direction [N] Resultant Torque [Nm] 2011 ANSYS, Inc. All rights reserved. 57 ANSYS, Inc. Proprietary
53 Imported CFD pressure into structural calculation Imported Hydraulic Forces from CFD calculation applied to structural calculation One-way FSI 2011 ANSYS, Inc. All rights reserved. 58 ANSYS, Inc. Proprietary
54 Structural mechanics Displacement due to centrifugal and hydraulic loading Calculated in ANSYS Mechanical 2011 ANSYS, Inc. All rights reserved. 59 ANSYS, Inc. Proprietary
55 Structural mechanics Stress contours due to centrifugal and hydraulic loading 2011 ANSYS, Inc. All rights reserved. 60 ANSYS, Inc. Proprietary
56 East River: Verdant Generation 5 Kinetic Hydropower Systems Effect of turbines in East River Non-rotating units create small wake regions, especially behind the pylon, pile, blades and tail cone. Very little flow acceleration is visible; generally well above the river bottom The turbulent wake lead to regions of increased mixing and flow disturbance, however, these regions are generally well above the river bottom. The impact of the pile wake, which is near the river bottom, is reduced by the lower water velocities in the fully developed turbulent boundary layer. Jonathan A Colby, Hydrodynamic Analysis of Kinetic Hydropower arrays, ANSYS, Inc. All rights reserved. 61 ANSYS, Inc. Proprietary
57 Wind and tidal turbine farm layouts 2011 ANSYS, Inc. All rights reserved. 62 ANSYS, Inc. Proprietary
58 Site Specific Issues Trickle down wind -> tidal WindModeller, vertical application based on ANSYS CFD Currently being extended to tidal flows Effect of geometry; Orography / Bathymetry Flow physics; Atmospheric Marine, free surface... Turbulence Inflow / ambient conditions sciencenw.com/uploads/horns_rev.jpg Turbine interactions and the environment Resolved Turbines / Actuator Disk models Wakes, towers 2011 ANSYS, Inc. All rights reserved. 63 ANSYS, Inc. Proprietary
59 Site Specific Studies Geometry available in various formats Point values: x,y,z csv Various GIS formats (.map, NTF, Seazone) Point values of depth, referred to LAT Digitised contours of coastline Convert to STL Morph template mesh to terrain for automation Or ANSYS AMP / ICEM CFD 2011 ANSYS, Inc. All rights reserved. 64 ANSYS, Inc. Proprietary
60 Offshore wind turbine wakes U ref = 10 m/s at 70m, z 0 = m, upstream TI = 6% Wind direction: sector 285 Horizontal velocity Turbulence intensity 2011 ANSYS, Inc. All rights reserved. 65 ANSYS, Inc. Proprietary
61 Tidal Turbine: Fall of Warness Peak mean spring current = 3.6 m/s Typical water depth = 34 m 2011 ANSYS, Inc. All rights reserved. 66 ANSYS, Inc. Proprietary
62 SeaZone Bathymetry Data 2011 ANSYS, Inc. All rights reserved. 67 ANSYS, Inc. Proprietary
63 Processing of Bathymetric Data Seazone Data The reference level of the depth data is Lowest Astronomical Tide (LAT) About 6 m resolution, in places as low as 1 m Data contains approximately 11 million points Gridded data triangulated and converted to STL Basis for meshing Important to have methods that cope well with anisotropic meshes Number of meshing approaches tried Black Box, morph template hex mesh 2011 ANSYS, Inc. All rights reserved. 68 ANSYS, Inc. Proprietary
64 Calculations 18 mins elapsed time, 30 iterations About mins to complete converged run 4 processors nodes Resolution about 25 m square Input profiles Constant and logarithmic (ABL profile) and 1/7 th profile Use tidal diamonds from naval charts for initial studies 2011 ANSYS, Inc. All rights reserved. 69 ANSYS, Inc. Proprietary
65 Results without Turbines 2011 ANSYS, Inc. All rights reserved. 70 ANSYS, Inc. Proprietary
66 Sample results vs Data Figure 10: Comparison between CFD results, Tidal Diamond Information and ADCP Measurements. 1 hour after High Water. Figure 11: Orientation of the velocity at the ADCP locations, 1 hour after High Water 2011 ANSYS, Inc. All rights reserved. 71 ANSYS, Inc. Proprietary
67 Results with Turbines Depth and landmass Turbine wakes zoomed local speed Turbine wakes, colours zoomed to illustrate wakes Overall Flow Speed 2011 ANSYS, Inc. All rights reserved. 72 ANSYS, Inc. Proprietary
68 Conclusions ANSYS viscous CFD provides a useful and complementary simulation technology Offshore and marine applications Hydrodynamic characterisation/loading Motion response Vortex-induced vibration Added mass and damping Two-way fluid structure interaction Wind/Tidal renewable energy applications Oscillating water columns Tidal turbines Tidal farm layouts 2011 ANSYS, Inc. All rights reserved. 73 ANSYS, Inc. Proprietary
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