Animation. Computer Graphics COMP 770 (236) Spring Instructor: Brandon Lloyd 4/23/07 1
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1 Animation Computer Graphics COMP 770 (236) Spring 2007 Instructor: Brandon Lloyd 4/23/07 1
2 Today s Topics Interpolation Forward and inverse kinematics Rigid body simulation Fluids Particle systems Behavioral modeling Motion capture 4/23/07 2
3 Interpolation Interpolation is at the heart of animation gives control and continuity Keyframing animator specifies parameters at a few time instances interpolate for other times 4/23/07 3
4 Interpolating positions Can interpolate positions using splines Velocity on the curve also matters uniform changes in parameter don t necessarily translate to uniform changes in position faster slower 4/23/07 4
5 Arc length reparameterization Define s(u) as distance along a curve P(u): su ( ) = How to compute s(u) Analytically - not possible with some curves Numerically u 0 dp dµ dµ dp dx( u) dy( u) dz( u) = du du du du 4/23/07 5
6 Arc length reparameterization Compute inverse to get parameter as a function of distance u(s) s Arc length reparameterization: ( ) u Pus () s [0,( su end )] 4/23/07 6
7 Speed curves Arc-length parameterization gives uniform velocity on the curve provides a base for arbitrary velocity Ease-in / ease-out smooth start and stop motion at endpoints Can directly specify speed and integrate over time to get a distance-time function s(t): ds dt s t 4/23/07 7 t
8 Distance-time functions s s s t t t s s s t t 4/23/07 8 t
9 Interpolating orientation Fixed-axis angles Rotate about fixed global axes in some order e.g. x - y - z Euler angles Rotate about local axis in some order Problems does not always interpolate along a direct path Gimbal lock loss of a degree of freedom 4/23/07 9
10 Interpolating orientation Axis-angle interpolate axis and angle separately difficult to concatenate two axis-angle rotations Quaternions essentially the same information as axis-angle easy to concatenate rotations 4/23/07 10
11 Quaternions Represented by 4-tuple A vector in space Addition Multiplication associative but not commutative qq = ss v v sv + sv + v v Inverse [ ] ( ) 2 1 [ ] q= [ s x y z] = [ s v] [ 0 v ] q + q = [ s + s v + v ] q = q s v q = s + x + y + z 1 qq = [ ] 4/23/07 11
12 Rotations with Quaternions Representing axis-angle rotations q = [ cos( θ / 2) sin( θ / 2) a] Concatenate rotations by multiplication q = qq 1 2 Rotating a vector v' = qvq 1 inverse rotates in opposite direction magnitude cancels out. Thus q and q represent the same orientation 4/23/07 12
13 Interpolating Quaternions Since q = -q we can interpolate from q 1 to q 2 or q 1 to -q 2 desirable rotation is usually the shorter one q1 q2 = cosθ check with 4D dot product which gives the cosine of the angle between the two orientations Linear interpolation doesn t give correct results Spherical linear interpolation: ( u θ ) sin (1 ) sin( uθ ) slerp( q, q, t) = q + q sin( θ) sin( θ) /23/07 13 q 1 q 2
14 Kinematics and Dynamics Kinematics Considers only motion Deals mostly with geometric constraints Dynamics Considers underlying forces Compute configurations from initial conditions and law of physics 4/23/07 14
15 Kinematics Forward Kinematics Specify conditions (joint angles) Compute positions of end effectors Inverse Kinematics Specify goal positions of end effectors Compute conditions required to achieve goals θ 2 end effector θ 1 θ 3 4/23/07 15
16 Inverse kinematics Problem is typically underconstrained multiple solutions can choose minimum energy solution At each step: Compute difference between goal and current state Compute Jacobian of state vector Solve for change in state that moves closer to goal Integrate Easier specification for many animation tasks, but more expensive to compute 4/23/07 16
17 Inverse Kinematics θ 2 ( xv, ) θ 1 θ 3 ( x, v ) end end dθ1 dx dx dx dt dθ 1 dθ2 dθ 3 dθ x 2 end x dv dv dv dt = dθ1 dθ2 dθ3 dθ3 vend v dt i+ 1 i θ 1 θ 1 θ θ θ θ dθ1 dt i+ 1 i dθ2 2 = 2 + dt i+ 1 i dθ dt t 4/23/07 17
18 Rigid body dynamics Uses laws of physics to provide motion Basic steps Compute forces Compute accelerations from forces Integrate to find positions and velocities 4/23/07 18
19 An example Cannon ball f f gravity drag = mgy = mµ v f = f = ma p= mv j ( i+ 1) ( i) p p f x = + t p = x + m ( i+ 1) ( i) () i Euler Midpoint RK4 4/23/07 19
20 Rigid body dynamics For 3D bodies add orientation angular momentum Constraints Add hard constraints by modifying equations Add soft-constraints with springs and dampers 4/23/07 20
21 Collisions Collision detection - expensive Accelerate with hierarchies (e.g. bounding volumes) Exploint coherence Collision response kinematic penalty methods impulse methods 4/23/07 21
22 Fluids Very difficult to model by hand Use computational fluid dynamics more emphasis on speed and visual plausibility than accuracy 4/23/07 22
23 Particle systems Good for simulating smoke, fire, explosions, water, rain, snow, etc. 4/23/07 23
24 Particle systems Steps in computing a frame for a particle system New particles are born New particles assigned attributes Particles removed that exceed life span Particles are animated and shading parameters changed Render particles 4/23/07 24
25 Behavioral modeling Flocking Autonomous agents add AI to the animation process snake learns how to move crowds in train station 4/23/07 25
26 Motion capture Track actor s motion optical magnetic exoskeleton Recover joint angles from captured data Retarget motion to CG character Images copyright New Line Productions 4/23/07 26
27 Motion capture Issues noise slippage occluded markers limited capture space people aren t really rigid bodies dynamics of character aren t the same due to different proportions and mass distribution 4/23/07 27
A simple example. Assume we want to find the change in the rotation angles to get the end effector to G. Effect of changing s
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