Pinhas Z. Bar-Yoseph Computational Mechanics Lab. Mechanical Engineering, Technion ISCM-20 Copyright by PZ Bar-Yoseph ©
Bar-Yoseph, Appl. Num. Math. 33, , 2000
DSM for Dynamic systems Aharoni & Bar-Yoseph, Comp. Mech. 9, , 1992
Discontinuous element
Plat & Bar-Yoseph, 27 th Israel Conf. Mech. Eng , 1998 Nonlinear Spatio-Temporal Dynamics of a Flexible Rod
Bar-Yoseph, Appl. Num. Math. 33, , 2000
Nave, Bar-Yoseph & Halevi, Dynamics. & Control. 9, , 1999 The unicycle system, presents an example of inherently unstable system which can be autonomously controlled and stabilized by a skilled rider -required to maintain the unicylce’s upright position -required to maintain lateral stability -the friction torque is assumed to be dependent on the yew rate only
The adaptive technique performed very well for all stiff systems that we have experienced with (convection, radiation and chemical reactions), and is competitive with the best Gear-type routines
Space-Time Discontinuous Approximations
Bar-Yoseph & Elata, IJNME, 29, , 1990
Bar-Yoseph & Elata & Israeli, IJNME, 36, , 1993; Golzman & Bar-Yoseph (Project)
Bar-Yoseph & Elata & Israeli, IJNME, 36, , 1993; Golzman & Bar-Yoseph (Project)
Bar-Yoseph & Elata, IJNME, 29, , 1990
Fischer & Bar-Yoseph, IJNME, 48, , 2000
Adaptive Level of Details Technique for Meshing Advanced CAD Visualization Methods
Morphing between Meshes at Different Times
DGM Elements are discontinuous. CGM Conforming elements.
Space-Time Discontinuous Approximations
Gauss-Lobatto nodes are clustered near element boundaries and are chosen because of their interpolation and quadrature properties. Mass lumping by nodal quadrature. Exponential rate of convergence. The increase in the due to the discontinuity at the interelement boundaries is balanced in high order elements. Discontinuous SPECTRAL ELEMENTS
Flux Splitting Bar-Yoseph,Comput. Mech., 5, , 1989
Nonlinear Wave Eq. Miles Rubin (2005)
Flux splitting for non homogeneous
where: The effective wave speed: In a matrix form: Traper & Bar-Yoseph (Project)
The Jacobian matrix: The eigenvalues: The corresponding eigenvectors:
Displacement Traper & Bar-Yoseph (Project)
Velocity
Strain
-Time for breakdown [Lax (1964)]:
Velocity at t = 3 sec x bilinear biquadratic
Strain at t = 3 sec x bilinear biquadratic
Bar-Yoseph et al., JCP, 119, 62-74, 1995
Bar-Yoseph & Moses, IJNMHFF, 7, , 1997
Cockburn& Shu, JCP, 84, 90, 1989; Basi & Rebay, JCP, 131, , 1997