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Wind Turbine Blade FSI (Part 2)

Info

This module is from our free online simulations course at edX.org (sign up here). The edX interface provides a better user experience and the content has been updated, so we recommend that you go through the module there rather than here. Also, you will be able to see answers to the questions embedded within the module there. 

Created using ANSYS 15.0

Note

This tutorial has videos. If you are in a computer lab, make sure to have head phones. 

Info

To access Part 1 of the tutorial, click here

Problem Specification

Overview

This tutorial considers the deformation due to aerodynamic loading of a wind turbine blade by performing a steady-state 1-way FSI (Fluid-Structure Interaction) analysis. Part 1 of the tutorial uses ANSYS Fluent to develop the aerodynamics loading on the blade. In part 2, the pressures on the wetted areas of the blade are passed as pressure load loads to ANSYS Mechanical to determine stresses and deformations on the blade. 

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The blade is made out of an orthotropic composite material, it has a varying thickness and it also has a spar inside the blade for structural rigidity. These specs, which are important for the FEA simulation, are described in  more more details in Part 2 of the tutorial.

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The turbulent wind is coming from flows towards the negative z-direction at (into the page on the above diagram) at 12 m/s which is a typical rated wind speed for a turbine this size. This incoming flow makes the blade rotate at an angular velocity of -2.22 rad/s about the z-axis (the blade is thus spinning clockwise when looking at it from the front, like most real wind turbines). The blade root is offset from the axis of rotation by 1 meter to make it more represenetative of an actual turbine where the blades would connect to the hub. Note that the  Note that to represent the blade being connected to a hub, the blade root is offset from the axis of rotation by 1 meter to represent the blade being connected to a hub. 

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Part 2

This section involves the solid mechanics aspects of this wind turbine blade tutorial. The pressures pressure load found using Fluent in Part 1 are imported in Mechanical and the stresses and deformations on the blade are subsequently determined. 

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The blade is composed of an outer surface and an inner spar. The thickness of the outside surface linearly decreases from 0.1 m at the root to 0.005 m at the tip. The spar has a similar thickness behavior with 0.1 m at its closest point to the root and 0.03 m at the tip. To sum up, here are the thickness specifications needed along with their location with respect to the global coordinate system (which represents the center of an imaginary hub and thus the center of rotation).

Surface

X (m)Thickness (m)
-10.1
-44.20.005

Spar

X (m)Thickness (m)
-30.1
-44.20.03

These thicknesses are actually very close to what you would encounter on a real turbine.  

Wind turbine blades are now made of composite materials to reduce the weight of these massive machines. Here we simplify the structural analysis by assuming that the composite material can be approximated by the following orthotropic material properties. made out of an orthotropic composite material with the following properties: (Should we include all this info here or only in Part 2?) 

Density (kg/m^3)

1550

Young's Modulus-X (Pa)

1.1375E+11

Young's Modulus-Y (Pa)

7.583E+09

Young's Modulus-Z (Pa)

7.583E+09

Poisson's Ratio-XY

0.32

Poisson's Ratio-YZ

0.37

Poisson's Ratio-XZ

0.35

Shear Modulus-XY (Pa)

5.446E+09

Shear Modulus-YZ (Pa)

2.964E+09

Shear Modulus-XZ (Pa)

2.964E+09

 

 

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These values are representative of composite properties found in real wind turbine blades.

Let's get started!

 

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Go to Step 1: Pre-Analysis & Start-Up

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