'Lagrangian' presentation slideshows

Inexact Methods for PDE-Constrained Optimization

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AOE 5104 Class 6

550 views • 37 slides

TinyOS: Radio, Concurrent Execution, and P ower control

TinyOS: Radio, Concurrent Execution, and P ower control. Class 7. Announcements. Please email TA with group members It is necessary to distribute sensors to the groups Phase 1 for your group projects due on October 12 th . Requirements posted on the course webpage. Agenda. Review Quiz

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Ch. 7: Dynamics

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NLO QCD corrections to FCNC single top production at hadron colliders

NLO QCD corrections to FCNC single top production at hadron colliders. Jun Gao, in collaboration with Chong Sheng Li, Hua Xing Zhu and Jia Jun Zhang. ITP of Peking University Aug 25, 2009 . Outline. 1, Introduction 2, FCNC single top production 3, Numerical results 4, Conclusion.

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The Quasiharmonic Approximation

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Quantum measurements and chiral magnetic effect

Quantum measurements and chiral magnetic effect. V.Shevchenko Kurchatov Institute, Moscow. based on arXiv : 1008.4977 (with V.Orlovsky ); 1208.0777 . Workshop on QCD in strong magnetic field Trento, Italy, 15 November 2012. Vacuum of any QFT (and the SM in particular) is

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The Maximum Principle of Optimal Control: A History of Ingenious Idea and Missed Opportunities

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SVM QP & Midterm Review

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Efficient Inference for Fully-Connected CRFs with Stationarity

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Separating Hyperplanes

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Quadratic Programming and Duality

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An elastic Lagrangian for space-time

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Parity

Let us examine the parity operator (P) and its eigenvalues. The parity operator acting on a wavefunction is defined by: P Y (x, y, z) = Y (-x, -y, -z) P 2 Y (x, y, z) = P Y (-x, -y, -z) = Y (x, y, z) Therefore P 2 = I and the parity operator is unitary.

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Optimality criterion methods

Optimality criterion methods. Methods that use directly an optimality criterion in order to resize the structure. Fully stress design and stress ratio resizing. Dual methods. Simple resizing rule based on Lagrange multiplier for single constraint. Fully stressed design.

458 views • 10 slides

Dissipative Force

Dissipative Force. Generalized force came from a transformation. Jacobian transformation Not a constraint Conservative forces were separated in the Lagrangian. Non-Potential Force. Velocity Dependent. A function M may exist that still permits a Lagrangian.

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Double Pendulum

Double Pendulum. Coupled Motion. Two plane pendulums of the same mass and length. Coupled potentials The displacement of one influences the other Coupling is small Define two angles q 1 , q 2 as generalized variables. k. l. l. q 1. q 2. m. m. Coupled Equations.

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Lagrangian

394 views • 8 slides