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    Evan Greer,Mentor: Dr. Marcelo Kobayashi,HARP REU ProgramAugust 2, 2012Contact: [email protected]

    globalwindgroup.com

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    Introduction and Motivations Creating the geometry

    Stationary study of turbine geometry Rotating study of turbine geometry Future Plans Acknowledgements

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    Energy Security

    High reliability of fossil fuels leads to widespread use

    Set amount of fossil fuel outputs a setamount of energy

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    Introduction of reliability to renewableresources, wind energy in particular

    Wind energy is subject to low reliability dueto changing weather conditions

    Scale predictions of large scale weatherpatterns to make predictions about theenvironment around the turbine

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    The effects of local topography on efficiencywill be studied

    WRF (weather research and forecasting)model coupled with CFD models

    This is the future goal of this research but firsta working model of the turbine must becreated and studied

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    Used a sample geometry fromComsol Multiphysics

    Played with initial conditions

    and mesh sizes Learned how to use the Comsol

    Multiphysics software

    Studied introductory tutorialbuilding a busbar geometry

    Learned how to set up fluid flowand thermoelectric physics

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    Approximated the geometry of atypical wind turbine

    Height of the tower set at 300 ft

    Length of the rotors set at 200 ft

    Length of the nacelle set at 40 ft

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    Front View Side View

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    Created for theimplementation of the slidingmesh

    Cylindrical region with aheight of 80 ft encompassingthe blades

    Domain to move with the

    blades

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    Region where boundaryand initial conditions are tobe defined

    Created a cylindricalregion behind the slidingregion to study wake

    Material for the flow setas air and material forturbine set as aluminum

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    Generated mesh usingtetrahedral elements

    Mesh had to be refinedaround blades

    Mesh consisted of 93349elements

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    Ran a stationary turbulent flow study using ak-model

    This model has the purpose of understandinghow fluid flow is affected by geometry

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    Used a simple turbulent flow physical model

    Stationary study step with no timedependence

    Inlet velocity of 3.219 m/s, this is the averageannual wind speed of Honolulu reported byNOAA [1]

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    Outlet condition was also set to atmosphericpressure

    Also, a volume force was introduced on theflow domain

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    Used Rotating Machinery,Turbulent Flow physical model

    Moving domains are coupledwith stationary domains by

    identity pairs

    At these identity pairs, a fluxcontinuity boundary conditionis applied

    Navier-Stokes equations areformulated based on rotatingand stationary coordinatesystems

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    Convergence of time stepped solution

    Solution would get stuck on calculation oftime step

    Many issues with script files and runs onsupercomputer

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    Issues with licensing Jobs would terminate because of lack of licensing on

    multiple nodes

    Solved with batch and cluster computing add-on tojob configurations within Comsol

    Issues with node communication Comsol would get kicked nodes

    Solved using MPD (Multi processing Daemon) used byComsol to communicate between nodes

    Accomplished through modification of script files withthe help of Andrew Yukitomo

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    Isolated rotatinggeometry

    Try to get rotatingblade workingwithout pairing

    Added input andoutput condition

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    Added pairing and flowcontinuity conditionbetween stationary and

    rotating domains

    Used overlapping domainsand input and outputconditions

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    Used non-overlappingdomains

    Got rid of input and outputconditions, instead used apressure point constraint

    Increased number of

    iterations used by the solver

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    Complete the set up of the full rotatinggeometry

    Get the blade study to run for larger time scales Further work needs to be done to understand where

    and why the convergence errors are occurring

    Understanding how to make a more accurate mesh

    Introduce the stationary wake region and a twodimensional pairing region

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    Introduce the flow domain and threedimensional pairing and get the complete

    model to run

    Get the rotation of the turbine to be dictatedby inlet velocity conditions

    This will involve delving deeper into the interfaceto understand how to program physical models

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    Project benchmarks:

    Creating geometry

    Modeling stationary case Implementation of sliding mesh

    Implementation of Large Eddy Simulation

    Implementation of WRF data This research will be continued under a NASA

    space grant in the fall

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    I would like to thank Dr. Susan Brown for giving methe opportunity to be a part of this program and Dr.Marcelo Kobayashi for his continued support andallowing me to share in his research. I also want to

    acknowledge Andrew Yukitomo for his continued helpwith script files and supercomputing issues and HOSCfor allowing us to use the supercomputing facilities forour work.

    "This material is based upon work supported by the National ScienceFoundation under Grant No. 0852082. Any opinions, findings, andconclusions or recommendations expressed in this material are those of theauthor(s) and do not necessarily reflect the views of the National ScienceFoundation."

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    [1] Delliger, Dan, 2008, Average Wind Speed, Comparative Climate Data,http://lwf.ncdc.noaa.gov/oa/climate/online/ccd/avgwind.html(July 5, 2012)

    [2] Laminar Flow in a Baffled Stirred Mixer. Comsol Multiphysics 4.3 sampleprogram documentation, 2012

    http://lwf.ncdc.noaa.gov/oa/climate/online/ccd/avgwind.htmlhttp://lwf.ncdc.noaa.gov/oa/climate/online/ccd/avgwind.html