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Variational integration for articulated body dynamics

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Path of system minimizes 'action' = L(q,v) dt. where L(q,v) = T(v) U(q) ... L. Kharevych, Weiwei, Y. Tong, E. Kanso, J. E. Marsden, P. Schr der, and M. Desbrun. ... – PowerPoint PPT presentation

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Title: Variational integration for articulated body dynamics


1
Variational integration for articulated body
dynamics
  • Rahul Narain
  • COMP790 project progress report
  • Nov. 16, 2006

2
Background
  • Variational principles in classical mechanics
  • e.g. Principle of least action
  • Path of system minimizes action ? L(q,v) dt
  • where L(q,v) T(v) - U(q)
  • Discretize integral ? time-stepping scheme

Kinetic energy
Potential energy
3
The discrete equations
  • qk1 - qk hkvk1
  • pk1 - pk ?Ld(qk,vk1)/?vk1 Fd(qk,vk1)
    hk?k?g(qk)
  • hkpk1 ?Ld(qk,vk1)/?qk
  • g(qk1) 0
  • Need to plug in external forces,derivatives of
    Lagrangian

4
Current status
  • Worked out the derivatives of the Lagrangian
  • for both reduced coordinate and maximal
    coordinate formulations
  • Ready to put into code

5
Remaining work
  • Implement!
  • I might need (constrained?) non-linear
    optimization code
  • Practical comparison of speed, accuracy, etc.
    with other integration methods

6
Long-term goals
  • More general animation scenarios
  • Contact handling
  • Collision response
  • Adaptive dynamics
  • in the context of variational integration

7
References
  • L. Kharevych, Weiwei, Y. Tong, E. Kanso, J. E.
    Marsden, P. Schröder, and M. Desbrun. Geometric,
    Variational Integrators for Computer Animation.
    Eurographics/ACM SIGGRAPH Symposium on Computer
    Animation, 2006.
  • A. Stern and M. Desbrun. Discrete Geometric
    Mechanics for Variational Time Integrators. In
    course notes of Discrete Differential Geometry
    An Applied Introduction, course at ACM SIGGRAPH
    2006.
  • J.E. Marsden and M. West. Discrete mechanics and
    variational integrators. Acta Numerica 10, 2001.
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