Express Introductory Training in ANSYS Fluent Workshop 06 Using Moving Reference Frames and Sliding Meshes

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Express Introductory Training in ANSYS Fluent Workshop 06 Using Moving Reference Frames and Sliding Meshes Dimitrios Sofialidis Technical Manager, SimTec Ltd. Mechanical Engineer, PhD PRACE Autumn School 2013 - Industry Oriented HPC Simulations, September 21-27, University of Ljubljana, Faculty of Mechanical Engineering, Ljubljana, Slovenia 2012 ANSYS, Inc. September 19, 2013 1 Release 14.5

Workshop 06 Using Moving Reference Frames and Sliding Meshes 14.5 Release Introduction to ANSYS Fluent 2012 ANSYS, Inc. September 19, 2013 2 Release 14.5

I Introduction [1] Workshop Description: The flow simulated is a vertical axis wind turbine in which 4 outer blades rotate relative to an inner hub, itself turning about a central axis. Learning Aims: This workshop teaches two different strategies for handling moving objects within the flow domain. 1. Using a Moving Reference Frame approach (which uses a steady state solution). 2. Using a Sliding Mesh approach (a transient calculation in which the parts are actually moved each timestep). Learning Objectives: To understand ways of simulating moving parts, as well as introducing transient simulations and generating images on the fly. 2012 ANSYS, Inc. September 19, 2013 3 Release 14.5

Introduction [2] To understand the motion we will be simulating, play the supplied movie file "ws6 mesh animation.avi". The centers of the blades rotate about the axis displayed in the picture while each individual blade simultaneously rotates about its own center. The first part of this workshop will simulate this motion without actually moving the parts. Local accelerations can be added as source terms to each grid cell to account for the motion of the parts. This technique is known as a Moving Reference Frame (MRF) approach. The second part of this workshop will actually move the parts relative to each other. This technique is known as a Sliding Mesh approach. Blade "xneg" Blade "ypos" Blade "xpos" Blade "yneg" 2012 ANSYS, Inc. September 19, 2013 4 Release 14.5

Part 1: Using Moving Reference Frames 2012 ANSYS, Inc. September 19, 2013 5 Release 14.5

Starting Fluent in Workbench 1. Launch Workbench. Start>Programs>ANSYS 14.5>Workbench 14.5. 2. Drag Fluent ("Component Systems") into the project schematic. 3. Change the name to Moving Reference Frame. 4. Double click on Setup. 5. Choose 2D and "Double Precision" under Options and retain the other default settings. 2012 ANSYS, Inc. September 19, 2013 6 Release 14.5

Import Mesh [In Fluent] File>Import>Mesh. Select the mesh file "ws6 simple wind turbine.msh" and OK. Check the scale (Problem Setup>General>Scale). The blades are 1m radius from the origin (0,0), with the outer bounding box +/ 5m in all directions. After reading the mesh, check the grid using Mesh>Check option or by using Check under Problem Setup>General. The mesh check will fail! A number of warning messages such as "WARNING: Unassigned interface zone detected for interface xx" will be displayed. To allow for the motion later in this workshop, there are intentional non conformal interfaces (where the mesh nodes do not match across an interface). These need to be paired up in the solver so that interpolation across the interface can occur so fluid can flow freely through. More generally, if in DesignModeler you produce several different parts, the mesh will also be non conformal, and you will need to perform the next step to make sure the solver interpolates across the interface, otherwise the interfaces would act like walls when the flow is calculated. 2012 ANSYS, Inc. September 19, 2013 7 Release 14.5

Display Mesh To display the mesh such that the zones have different colors, as in the picture on slide 3, select "Display>Mesh" from the menu bar, click the Colors button, and select Color by ID. 2012 ANSYS, Inc. September 19, 2013 8 Release 14.5

Mesh Interfaces [1] Under Problem Setup>Mesh Interfaces. Click Create/Edit. Enter "in hub" in the field below Mesh Interface. Select "int hub a" in the column below Interface Zone 1. Select "int hub b" in the column below Interface Zone 2. Click Create. Note how the nodes do not match across the interface. The boundary on the black side is "Int hub a" and the red side is "Int hub b". 2012 ANSYS, Inc. September 19, 2013 9 Release 14.5

Mesh Interfaces [2] Create the interfaces "in_xneg", "in_xpos", "in_yneg" and "in_ypos" as described in the table below to the left. After all the interfaces have been created the mesh interface panel should appear as it does on the right: Mesh Interface Interface Zone 1 Interface Zone 2 in_hub int hub a int hub b in_xneg int xneg a int xneg b in_xpos int xpos a int xpos b in_yneg int yneg a int yneg b in_ypos int ypos a int ypos b 2012 ANSYS, Inc. September 19, 2013 10 Release 14.5

Setting up the Models Keep the Pressure Based, Steady State solver. Problem Setup>General>Solver. Turbulence model. Problem Setup>Models>Viscous. Double click and select k epsilon (2 eqn) under Model and Realizable under k epsilon model and retain the other default settings. Materials. For Materials, keep the default properties of the material air: density: 1.225 [kg/m³] viscosity: 1.7894e 5 [kg/(ms)] 2012 ANSYS, Inc. September 19, 2013 11 Release 14.5

Cell Zone Conditions [1] Under Problem Setup>Cell Zone Conditions. Select fluid outer domain and click Edit. Observe air is already selected and click OK. fluid outer domain fluid blade ypos centroid at (0,1) fluid rotating core centroid at (0,0) fluid blade xneg centroid at ( 1,0) fluid blade xpos centroid at (1,0) fluid blade yneg centroid at (0, 1) 2012 ANSYS, Inc. September 19, 2013 12 Release 14.5

Cell Zone Conditions [2] Select "fluid rotating core" and click Edit. Observe air is already selected. Click Frame Motion, to activate the Moving Reference Frame model. Retain the (0,0) as Rotational Axis Origin. Select 4 rad/s as Rotational Velocity and click OK. We can account for the motion of the parts, even in a steady state solver by using this technique. By specifying the rotation of the core, all the grid cells are given an additional source term to account for the local acceleration. This is known as using a moving reference frame. 2012 ANSYS, Inc. September 19, 2013 13 Release 14.5

Cell Zone Conditions [3] Select "fluid blade xneg" and click Edit. Observe air is already selected. Click Frame Motion, to activate the Moving Reference Frame model. Set the Rotational Axis Origin to ( 1,0). Set the Rotational Velocity to 2 rad/s (note negative). Select "fluid rotating core"as Relative Specification and click OK. This zone is rotating about its own axis, which is 1m away from the global (hub) axis. The rotation speed is half that of the outer hub. 2012 ANSYS, Inc. September 19, 2013 14 Release 14.5

Cell Zone Conditions [4] Repeat the instructions on the previous Slide for the other 3 blades: Zone fluid blade xpos Zone fluid blade yneg Zone fluid blade ypos Axis [1 0] Speed 2rad/s Relative fluid rotating core Axis [0 1] Speed 2rad/s Relative fluid rotating core Axis [0 1] Speed 2rad/s Relative fluid rotating core Axis is different for each zone It is worth taking a moment to check back through all the cell zones just defined to make sure the settings are correct. 2012 ANSYS, Inc. September 19, 2013 15 Release 14.5

Boundary Conditions [1] Under Problem Setup>Boundary Conditions. "Vel Inlet Wind". Select "vel inlet wind", click Edit and set 10 (m/s) as Velocity Magnitude. Choose Intensity and Length Scale under Turbulence. Set Turbulence Intensity to 5 % and Turbulent Length Scale to 1 (m) and click OK. "Pressure Outlet Wind". Select "pressure outlet wind", click Edit and set 0 (Pa) as Gauge Pressure. Choose Intensity and Length Scale under Turbulence. Set Turbulence Intensity to 5 % and Turbulent Length Scale to 1 m and click OK. 2012 ANSYS, Inc. September 19, 2013 16 Release 14.5

Boundary Conditions [2] Under Problem Setup>Boundary Conditions. Rotating wall. Select "wall blade xneg" then Edit. Select Moving Wall under Wall Motion. Select Rotational under Motion and retain 0 (rad/s) as Speed relative to cell zone. The solver needs to know the speed of the wall so as to properly account for wall shear. Since the motion has been set in the cell zone, we will simply tell the boundary condition to use the same conditions (that is, zero velocity with respect to the cell zone). Note that this panel will tell you which cell zone is adjacent to this wall look at the greyed out box on the second line. 2012 ANSYS, Inc. September 19, 2013 17 Release 14.5

Boundary Conditions [3] Copy the boundary conditions to other zones. 1. Press button Copy... To save time, when boundaries have identical parameters, we can copy from one to (many) others. 2. Select "wall blade xneg". 3. Select the three other blades zone ("wall blade xpos", "wall blade yneg", "wall blade ypos"). 4. Click Copy, then OK. 2012 ANSYS, Inc. September 19, 2013 18 Release 14.5

Solution Methods Under Solution>Solution Methods. Select "Coupled" for Pressure Velocity Coupling. Select "Second Order Upwind" for the turbulence equations. Under Solution>Solution Controls. Retain the default settings. Under Solution>Solution Initialization. Retain Hybrid Initialization. Click Initialize. 2012 ANSYS, Inc. September 19, 2013 19 Release 14.5

Write Case and Data File The model is now ready to run. First Save the Project to your normal working directory. File>Save Project. Then Run the Calculation. Set 250 as Number of Iterations. Click Calculate to start the steady state simulation. It will reach the default convergence criteria in about 100 iterations. Generally you should always do further checks to determine convergence. However to save time in this example we will simply assume the default convergence criteria are sufficient. 2012 ANSYS, Inc. September 19, 2013 20 Release 14.5

Post Processing [1] Post process the results in Fluent. Results>Graphics and Animations. Select Contours and click Set Up. Select Velocity under Contours of and Velocity Magnitude below that. Tick the box "Filled", but do not select any surfaces, then Display. Zoom in on the hub using the middle mouse button, by drawing a box from top left to bottom right. It is not necessary to select a plotting surface when using Fluent in 2D. By default the plot value is shown on all cells. Drag zoom box with middle mouse button. Opposite direction (right to left) will zoom out. Use "Fit To Window" to reset if necessary. 2012 ANSYS, Inc. September 19, 2013 21 Release 14.5

Post Processing [2] The Velocity contours should look like this: Without the cell zone motion (MRF) this would have looked much more symmetrical between top and bottom. 10 m/s wind Save the project File>Save Project. 4 rad/s Hub Rotation You can save this image from Fluent for use in a report: File>Save Picture. TIFF, and Colour. Resolution 1200 x 1200. "Save". Close Fluent, and return to the ANSYS Workbench window. 2012 ANSYS, Inc. September 19, 2013 22 Release 14.5

Part 2: Using Sliding Meshes 2012 ANSYS, Inc. September 19, 2013 23 Release 14.5

Sliding Meshes Introduction There are times when the MRF assumption used in Part 1 is an over simplification of the problem. Only one position of the hub relative to the incoming wind was simulated. There will also be some vortices that affect each blade from other blades that have just passed upwind. In this next part, we will actually move the relative positions of all the components within Fluent, and solve this in a transient (time dependant) manner. 2012 ANSYS, Inc. September 19, 2013 24 Release 14.5

Preparing Workbench On the Workbench Project Page, right click on the arrow at the top of the Fluent model, and select "Duplicate". Name the newly created copy "Sliding Mesh Model". Drag the results over from the MRF model (drag a line from cell A3 to B3). This is so we can use the steady state solution as a starting point for the new Sliding Mesh computation. Launch Fluent by double clicking on the new Solution cell (B3). The message "Note: zone surface: cannot create surface from sliding interface zone" appears when Fluent opens and reads the case and data files. It simply means the boundaries of the non conformal interfaces match exactly, such that there are no non overlapping sections on either side of the interface. 2012 ANSYS, Inc. September 19, 2013 25 Release 14.5

Model Setup General Comments All the model setup values (boundary conditions, etc.) are available in the new Fluent session. You may want to have a look (boundary conditions, plot velocity contours etc.) to observe this for yourself. The following slides will show how to change this model to a sliding mesh case. 2012 ANSYS, Inc. September 19, 2013 26 Release 14.5

Solver Setup Select Transient solver. Problem Setup>General>Solver. Under Problem Setup>Cell Zone Conditions Select "fluid rotating core" and click Edit. Click Copy to Mesh Motion in the Reference Frame Tab to activate the Sliding Mesh model. The motion type is changed from "Frame Motion" to "Mesh Motion". Move to the Mesh Motion Tab and observe the rotation speed has been transferred. click OK. 2012 ANSYS, Inc. September 19, 2013 27 Release 14.5

Setting up Cell Zones Repeat this process for the 4 blade regions: fluid blade xneg fluid blade xpos fluid blade yneg fluid blade ypos For each zone, on the Reference Frame tab, click "Copy to Mesh Motion". On the Mesh Motion tab, verify the axis, rotation speed, and "relative to cell zone" fields are correct. For all four blades, their motion should be relative to zone "fluid rotating core". Therefore not only will each blade rotate about its own axis, but in addition its axis will translate to follow the motion of the hub region ("fluid rotating core"). 2012 ANSYS, Inc. September 19, 2013 28 Release 14.5

Setting up an Animation [1] Solution>Calculation Activities>Solution Animations>Create/Edit. In the Solution Animation Panel increase the Animation Sequences to 1. Select Time Step under When and click Define. In Animation Sequence Panel select Window 2, SET, then Contours. It is very useful with transient simulations to record key frames of the solution progress. Not only does this help understand the result, but also aids de bugging if the settings are not as intended. 2012 ANSYS, Inc. September 19, 2013 29 Release 14.5

Setting up an Animation [2] On the Contour Panel: Set Contours of Velocity>Velocity Magnitude. Select "Filled". Deselect Global Range, Auto Range and Clip to Range. Enter Min=0, Max=15. Deselect all surfaces. Click "Display". Close the Contour Panel. OK the Animation Sequence Panel. OK the Solution Animation Panel. Graphic layout: Enable 2 window display. Use the middle mouse button to zoom in on the blades in graphic window 2. Forcing a Max and Min value will ensure all frames in the animation are consistent. 2012 ANSYS, Inc. September 19, 2013 30 Release 14.5

Write Case and Data File The model is now ready to run. First Save the Project to your normal working directory. File>Save Project. Then Run the Calculation Set 0.005s as Time Step Size. An Initialization of this case is not necessary because we want to continue the simulation with "start condition" of the Moving Reference Frame calculation already performed. Set 314 as number of time steps. 4 rads/sec equates to 1.57secs/rotation. 0.005s x 314 = 1.57s. Click Calculate to start the transient simulation. At each time step, Fluent iterates until the solution has converged for the current time step (or the maximum number of iterations per time step is reached), then advances to the next time step and iterates until the solution has converged, and so on until the prescribed 314 time steps have been completed. The total number of iterations required is around 2300. If you are running short of time you can stop the simulation early and proceed to checking the results (next slide). We suggest you allow the solver to perform at least 79 timesteps (0.4secs), the device will have moved 90. 2012 ANSYS, Inc. September 19, 2013 31 Release 14.5

Residual Plots in Transient Simulations If you have time to run the transient calculation, and did not move ahead to the post processing steps, the residual plot (change the number of iterations to plot to 100 before displaying) will look like the figure below. The residuals form a sawtooth pattern, with high values at the beginning of the time step which then decrease over a number of iterations until the convergence criteria are reached. Convergence achieved solution advances to next time step. 2012 ANSYS, Inc. September 19, 2013 32 Release 14.5

Reviewing the Solution When the calculation is complete: Graphics and Animations>Solution Animation Playback>Setup. Selecting the "Play" button will let you review the animation. Alternatively you can select Write/Record Format, and select MPEG. Wait a few moments while the animation is built. The animation will appear in the folder: working directory\workbench_project_name\dp0\flu 1\Fluent\sequence 1.mpeg Save the Project. File>Save Project. 2012 ANSYS, Inc. September 19, 2013 33 Release 14.5

Comparing the Results The images below show a comparison of the result from the MRF and sliding mesh approaches. (Colour scale from 0 to 15 m/s). Although the MRF approach gave a useful early indication of the velocity field and wake behind the blades, a full Transient approach is needed to accurately predict the flow field. MRF Result (Part 1) Sliding Mesh Result (Part 2) 2012 ANSYS, Inc. September 19, 2013 34 Release 14.5

Optional Extras If you have finished early, ahead of the rest of the class, you may want to investigate reporting the torque on the blades by computing the moment about the rotational axis. Use Report>Forces>Moments (and set appropriate axes). Pick the 4 blades. Compare the result from the two cases computed. The Moment Coefficient can also be plotted as a graph during the solution process Monitors>Moment. Click the "Help" button on this panel and follow the link to "Monitoring Force and Moment Coefficients" to find out more. Note that this reports a coefficient, which uses the values set in Report>Reference Values (see help pages). Once set, if you run the solver on for further timesteps, you will see how the moment varies sinusoidally as the device rotates. 2012 ANSYS, Inc. September 19, 2013 35 Release 14.5

Summary This workshop has shown two techniques for performing a CFD simulation where objects move within the flow domain. Using MRF techniques, the flow can quickly be simulated using a steady state solver by applying appropriate acceleration terms to each grid cell. Although this works, it was not ideal for this particular scenario. In the case of this wind turbine, the underlying physics of this case require a transient simulation. Vortices break off the upwind blades, and the downwind blades pass through these. Therefore this workshop has also shown how the fluid region can be modified by the solver at every timestep. There is no need to have to go back to the pre processor to generate a fresh mesh at each step. The key feature needed in the mesh in order to do this was having different, disconnected (non conformal) cell zones. Since they are disconnected, Fluent could move them as a rigid body. If the parts actually change shape, there are further tools available in Fluent (the Dynamic Mesh Model) which allow much greater changes to be made to the mesh, adding and removing grid cells where necessary. 2012 ANSYS, Inc. September 19, 2013 36 Release 14.5