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dc.contributor.advisorQiqi Wang.en_US
dc.contributor.authorBlonigan, Patrick Josephen_US
dc.contributor.otherMassachusetts Institute of Technology. Department of Aeronautics and Astronautics.en_US
dc.date.accessioned2013-11-18T20:40:26Z
dc.date.available2013-11-18T20:40:26Z
dc.date.copyright2013en_US
dc.date.issued2013en_US
dc.identifier.urihttp://hdl.handle.net/1721.1/82478
dc.descriptionThesis (S.M.)--Massachusetts Institute of Technology, Dept. of Aeronautics and Astronautics, 2013.en_US
dc.descriptionThis electronic version was submitted and approved by the author's academic department as part of an electronic thesis pilot project. The certified thesis is available in the Institute Archives and Special Collections.en_US
dc.descriptionCataloged from department-submitted PDF version of thesisen_US
dc.descriptionIncludes bibliographical references (p. 103-104).en_US
dc.description.abstractComputational methods for sensitivity analysis are invaluable tools for fluid dynamics research and engineering design. These methods are used in many applications, including aerodynamic shape optimization and adaptive grid refinement. However, traditional sensitivity analysis methods break down when applied to long-time averaged quantities in chaotic dynamical systems, such as those obtained from high-fidelity turbulence simulations. Also, a number of dynamical properties of chaotic systems, most notably the "Butterfly Effect", make the formulation of new sensitivity analysis methods difficult. This paper will discuss two chaotic sensitivity analysis methods and demonstrate them on several chaotic dynamical systems including the Lorenz equations and a chaotic Partial Differential Equation, the Kuramoto-Sivshinsky equation. The first method, the probability density adjoint method, forms a probability density function on the strange attractor associated with the system and uses its adjoint to find gradients. This was achieved using a novel numerical method in which the attractor manifold, instead of a region of phase space, is discretized. The second method, the Least Squares Sensitivity method, finds some "shadow trajectory" in phase space for which perturbations do not grow exponentially. This method is formulated as a quadratic programing problem with linear constraints. Several multigrid-in-time methods to solve the KKT system arising from this optimization problem will be discussed in depth. While the probability density adjoint method is better suited for smaller systems and reduced order models, least squares sensitivity analysis, solved with a multigrid-in-time method could be applied to higher dimensional systems such as high fidelity fluid flow simulations.en_US
dc.description.statementofresponsibilityby Patrick Joseph Blonigan.en_US
dc.format.extent104 p.en_US
dc.language.isoengen_US
dc.publisherMassachusetts Institute of Technologyen_US
dc.rightsM.I.T. theses are protected by copyright. They may be viewed from this source for any purpose, but reproduction or distribution in any format is prohibited without written permission. See provided URL for inquiries about permission.en_US
dc.rights.urihttp://dspace.mit.edu/handle/1721.1/7582en_US
dc.subjectAeronautics and Astronautics.en_US
dc.titleNew methods for sensitivity analysis of chaotic dynamical systemsen_US
dc.typeThesisen_US
dc.description.degreeS.M.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Aeronautics and Astronautics
dc.identifier.oclc862226253en_US


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