Download presentation
Presentation is loading. Please wait.
1
UNC Chapel Hill M. C. Lin Review Particle Dynamics (see transparencies in class)
2
UNC Chapel Hill M. C. Lin Disclaimer The following slides reuse materials from SIGGRAPH 2001 Course Notes on Physically-based Modeling (copyright 2001 by Andrew Witkin at Pixar).
3
UNC Chapel Hill M. C. Lin A Newtonian Particle
4
UNC Chapel Hill M. C. Lin Second Order Equations As discussed in the last lecture, we can transform a second order equation into a couple of first order equations. as shown here.
5
UNC Chapel Hill M. C. Lin Phase (State) Space
6
UNC Chapel Hill M. C. Lin Particle Structure
7
UNC Chapel Hill M. C. Lin Solver Interface
8
UNC Chapel Hill M. C. Lin Particle Systems
9
UNC Chapel Hill M. C. Lin Overall Setup
10
UNC Chapel Hill M. C. Lin Derivatives Evaluation Loop
11
UNC Chapel Hill M. C. Lin Particle Systems with Forces
12
UNC Chapel Hill M. C. Lin Solving Particle System Dynamics
13
UNC Chapel Hill M. C. Lin Type of Forces
14
UNC Chapel Hill M. C. Lin Gravity
15
UNC Chapel Hill M. C. Lin Force Fields Magnetic Fields –the direction of the velocity, the direction of the magnetic field, and the resulting force are all perpendicular to each other. The charge of the particle determines the direction of the resulting force. Vortex (an approximation) –rotate around an axis of rotation = magnitude/R tightness –need to specify center, magnitude, tightness –R is the distance from center of rotation Tornado –try a translation along the vortex axis that is also dependent on R, e.g. if Y is the axis of rotation, then
16
UNC Chapel Hill M. C. Lin Viscous Drag
17
UNC Chapel Hill M. C. Lin Spring Forces
18
UNC Chapel Hill M. C. Lin Collision and Response After applying forces, check for collisions or penetration If one has occurred, move particle to surface Apply resulting contact force (such as a bounce or dampened spring forces)
19
UNC Chapel Hill M. C. Lin Bouncing off the Wall
20
UNC Chapel Hill M. C. Lin Normal & Tangential Forces
21
UNC Chapel Hill M. C. Lin Collision Detection Collision!
22
UNC Chapel Hill M. C. Lin Collision Response (k r is the coefficient of restitution, 0 k r 1)
23
UNC Chapel Hill M. C. Lin Condition for Contact
24
UNC Chapel Hill M. C. Lin Contact Forces Friction: F f = -k f (-NF) v t F c = - F N = - (N F)F
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.