'Euler equations' diaporamas de présentation

Accurate numerical solution of Euler equations by optimal control of dissipation

Accurate numerical solution of Euler equations by optimal control of dissipation. SM Deshpande EMU, JNCASR, Bangalore smd@jncasr.ac.in. Omesh Reshi L & T, Mumbai. N Anil Dept. of Aerospace Engg. IISc, Bangalore.

596 views • 59 slides

The equations of motion and their numerical solutions II

799 views • 48 slides

Manipulator Dynamics 2

Manipulator Dynamics 2. Instructor: Jacob Rosen Advanced Robotic - MAE 263D - Department of Mechanical & Aerospace Engineering - UCLA. Forward Dynamics. Problem Given: Joint torques and links geometry, mass, inertia, friction

503 views • 48 slides

Time reversed algorithm for pure convection

Time reversed algorithm for pure convection. V .?. Goloviznin. Mathematical modeling transport phenomena on computational grid is one of the fundamental problems of the modern computational mathematics. Simplest transport equation is time reversed. is led to the same equation. Substitution.

512 views • 38 slides

Manipulator Dynamics 2

Manipulator Dynamics 2. Instructor: Jacob Rosen Advanced Robotic - MAE 263D - Department of Mechanical & Aerospace Engineering - UCLA. Forward Dynamics. Problem Given: Joint torques and links geometry, mass, inertia, friction

421 views • 37 slides

Fin500J: Mathematical Foundations in Finance Topic 6: Ordinary Differential Equations

Fin500J: Mathematical Foundations in Finance Topic 6: Ordinary Differential Equations Philip H. Dybvig Reference: Lecture Notes by Paul Dawkins, 2007, page 20-33, page 102-121, page 137-155 and page 340-344 http://tutorial.math.lamar.edu/terms.aspx Slides designed by Yajun Wang.

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Draft Tube Flow

Draft Tube Flow. u 1. c 1. w 1. u 2. w 2. c 2. Swirl at the outlet from Francis runners. u 2. b 2. c 2. w 2. c 2u. u 2. b 2. c 2. c 2m. w 2. c 2u. u 2. b 2. c 2m. w 2. c 2. Phenomenon in the draft tube flow Swirl flow Flow in bend

478 views • 31 slides

Modelling of interfaces separating compressible fluids and mixtures of materials

Modelling of interfaces separating compressible fluids and mixtures of materials. Multiphase shock relations and extra physics. Erwin FRANQUET and Richard SAUREL Polytech Marseille, UMR CNRS 6595 - IUSTI. Baer & Nunziato (1986). and. Saurel & al. (2003) Chinnayya & al (2004).

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Fiscal policies in the nonstohastic growth models

336 views • 22 slides

Towards simulation of detonation-induced shell dynamics with the Virtual Test Facility

Towards simulation of detonation-induced shell dynamics with the Virtual Test Facility. Ralf Deiterding, Fehmi Cirak, Dan Meiron Caltech Comref 2005, Heidelberg Jan. 27, 2005. Outline of presentation. Detonation simulation Governing equations A reliable Roe-type upwind scheme

224 views • 22 slides

AMS 599 Special Topics in Applied Mathematics Lecture 3

AMS 599 Special Topics in Applied Mathematics Lecture 3. James Glimm Department of Applied Mathematics and Statistics, Stony Brook University Brookhaven National Laboratory. Fluid Transport. The Euler equations neglect dissipative mechanisms

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Euler Rotation

Euler Rotation. Angular Momentum. The angular momentum J is defined in terms of the inertia tensor and angular velocity. All rotations included The angular momentum need not be collinear with the angular velocity. Not along principal axis Not at center of mass . p. J. r.

448 views • 8 slides

Physics 430: Lecture 24 Euler Equations

Physics 430: Lecture 24 Euler Equations. Dale E. Gary NJIT Physics Department. 10.7 Euler Equations.

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thickness

For spherical winds set: angle=pi/2 base=0 radius= r_outer thickness < r_outer For collimated winds set: angle=0 base=cylindrical radius radius=cylinder height thickness < radius For conical jets set: angle < Pi/2 base >= 0 radius = r_outer thickness < r_outer.

204 views • 1 slides