Download presentation
Presentation is loading. Please wait.
1
UNC Chapel Hill M. C. Lin Disclaimer The following slides reuse materials from SIGGRAPH 2001 Course Notes on Physically-based Modeling (copyright 2001 by David Baraff at Pixar).
2
UNC Chapel Hill M. C. Lin Determining Step Size Explicit Integration –Too big, unstable! –Too small, too slow –Adaptive, maybe –Ultimately the constants decide! Implicit Methods –Taking large steps when possible
3
UNC Chapel Hill M. C. Lin An Example
4
UNC Chapel Hill M. C. Lin Speed Limitation of Euler’s Method
5
UNC Chapel Hill M. C. Lin Stiff Equations
6
UNC Chapel Hill M. C. Lin A Stiff Energy Landscape
7
UNC Chapel Hill M. C. Lin Example: Particle-on-line
8
UNC Chapel Hill M. C. Lin Example: Particle-on-line
9
UNC Chapel Hill M. C. Lin Example: Particle-on-line
10
UNC Chapel Hill M. C. Lin Example: Particle-on-line
11
UNC Chapel Hill M. C. Lin Explicit Integration
12
UNC Chapel Hill M. C. Lin Problems
13
UNC Chapel Hill M. C. Lin Explicit vs. Implicit Euler Method vs.
14
UNC Chapel Hill M. C. Lin
15
UNC Chapel Hill M. C. Lin One Step: Implicit vs. Explicit
16
UNC Chapel Hill M. C. Lin Large Systems
17
UNC Chapel Hill M. C. Lin Implicit Integration
18
UNC Chapel Hill M. C. Lin Implicit Integration
19
UNC Chapel Hill M. C. Lin Implicit Integration
20
UNC Chapel Hill M. C. Lin Linearized Implicit Integration
21
UNC Chapel Hill M. C. Lin Single-Step Implicit Euler Method
22
UNC Chapel Hill M. C. Lin Solving Large Systems Matrix structure reflects force-coupling: (i, j)th entry exists iff f i depends on X j Conjugate gradient a good first choice
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.