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CIS 487/587 Bruce R. Maxim UM-Dearborn

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1 CIS 487/587 Bruce R. Maxim UM-Dearborn
Computer Game Physics CIS 487/587 Bruce R. Maxim UM-Dearborn

2 Game Physics Not trying to build a perfect physical model
Most things can be approximated assuming Newtonian physics and rigid bodies Use discrete simulation (constant step) techniques Just worry about center of mass for most things

3 The next 6 slides come from the Rabin text

4 Why Physics? The Human Experience Emergent Behavior
Real-world motions are physically-based Physics can make simulated game worlds appear more natural Makes sense to strive for physically-realistic motion for some types of games Emergent Behavior Physics simulation can enable a richer gaming experience

5 Why Physics? Developer/Publisher Cost Savings
Classic approaches to creating realistic motion: Artist-created keyframe animations Motion capture Both are labor intensive and expensive Physics simulation: Motion generated by algorithm Theoretically requires only minimal artist input Potential to substantially reduce content development cost At the present time, asset creation tools are not mature enough for physics to be as automatic as we would like. It currently requires quite a bit of work to get physics “right.” And so the cost of putting physics into a game may not be significantly cheaper than traditional animation approaches at this time. This should change as the physics tools improve. Artists should not worry that physics simulations will soon take over their jobs. This is particularly true for character and character-like animation. Physics and AI engines aren’t to the level yet where they can properly simulate the personality of characters that shows through in their motions!

6 High-level Decisions Physics in Digital Content Creation Software:
Many DCC modeling tools provide physics Export physics-engine-generated animation as keyframe data Enables incorporation of physics into game engines that do not support real-time physics Straightforward update of existing asset creation pipelines Does not provide player with the same emergent-behavior-rich game experience Does not provide full cost savings to developer/publisher

7 High-level Decisions Real-time Physics in Game at Runtime:
Enables the emergent behavior that provides player a richer game experience Potential to provide full cost savings to developer/publisher May require significant upgrade of game engine May require significant update of asset creation pipelines May require special training for modelers, animators, and level designers Licensing an existing engine may significantly increase third party middleware costs

8 High-level Decisions License vs. Build Physics Engine:
License middleware physics engine Complete solution from day 1 Proven, robust code base (in theory) Most offer some integration with DCC tools Features are always a tradeoff

9 High-level Decisions License vs. Build Physics Engine:
Build physics engine in-house Choose only the features you need Opportunity for more game-specific optimizations Greater opportunity to innovate Cost can be easily be much greater No asset pipeline at start of development

10 Position and Velocity Where is object at time t (using pixels)?
Equations player_x(t) = t * x_velocity + x_initial player_y(t) = t * y_velocity + y_initial Computation player_x = player_x + x_velocity player_y = player_y + y_velocity

11 Acceleration Computation
x_velocity = x_velocity + x_acceleration y_velocity = y_velocity + y_acceleration Use piecewise linear approximation to continuous functions

12 Gravity Force of attraction between objects F = G * (M1 * M2) / D2
G = gravitational constant D = distance between objects Free falling objects on Earth Equation V(t) = 1/2 * g * t2 g = 9.8 m/sec2 Computation x_velocity = x_velocity + 0 y_velocity = y_velocity + gravity

13 Projectile Motion X = x + Vx + W Y = y + Vy Vxi = cos(A) * Vi
Vyi = sin(A) * Vi Vx = Vx - WR(Vx) Vy - WR(Vy) + G W = wind A = inclination angle Vi = initial velocity WR = wind resistance G = gravity

14 Friction Conversion of kinetic energy into heat Equation Computation
Frictional Force = C * G * M C = force required to maintain constant speed G = gravity M = mass Computation while (velocity > 0) velocity = velocity - friction

15 The next 21 slides come from the Rabin text

16 Collision Detection Complicated for two reasons
1. Geometry is typically very complex, potentially requiring expensive testing 2. Naïve solution is O(n2) time complexity, since every object can potentially collide with every other object

17 Collision Detection Two basic techniques 1. Overlap testing
Detects whether a collision has already occurred 2. Intersection testing Predicts whether a collision will occur in the future

18 Overlap Testing Facts Concept Most common technique used in games
Exhibits more error than intersection testing Concept For every simulation step, test every pair of objects to see if they overlap Easy for simple volumes like spheres, harder for polygonal models

19 Overlap Testing: Useful Results
Useful results of detected collision Time collision took place Collision normal vector

20 Overlap Testing: Collision Time
Collision time calculated by moving object back in time until right before collision Bisection is an effective technique

21 Overlap Testing: Limitations
Fails with objects that move too fast Unlikely to catch time slice during overlap Possible solutions Design constraint on speed of objects Reduce simulation step size

22 Intersection Testing Predict future collisions When predicted:
Move simulation to time of collision Resolve collision Simulate remaining time step

23 Intersection Testing: Swept Geometry
Extrude geometry in direction of movement Swept sphere turns into a “capsule” shape

24 Intersection Testing: Sphere-Sphere Collision

25 Intersection Testing: Sphere-Sphere Collision
Smallest distance ever separating two spheres: If there is a collision

26 Intersection Testing: Limitations
Issue with networked games Future predictions rely on exact state of world at present time Due to packet latency, current state not always coherent Assumes constant velocity and zero acceleration over simulation step Has implications for physics model and choice of integrator

27 Dealing with Complexity
Two issues 1. Complex geometry must be simplified 2. Reduce number of object pair tests

28 Dealing with Complexity: Simplified Geometry
Approximate complex objects with simpler geometry, like this ellipsoid

29 Dealing with Complexity: Bounding Volumes
Bounding volume is a simple geometric shape Completely encapsulates object If no collision with bounding volume, no more testing is required Common bounding volumes Sphere Box

30 Dealing with Complexity: Box Bounding Volumes

31 Dealing with Complexity: Achieving O(n) Time Complexity
One solution is to partition space

32 Collision Resolution: Examples
Two billiard balls strike Calculate ball positions at time of impact Impart new velocities on balls Play “clinking” sound effect Rocket slams into wall Rocket disappears Explosion spawned and explosion sound effect Wall charred and area damage inflicted on nearby characters Character walks through wall Magical sound effect triggered No trajectories or velocities affected

33 Collision Resolution: Parts
Resolution has three parts 1. Prologue 2. Collision 3. Epilogue

34 Collision Resolution: Prologue
Collision known to have occurred Check if collision should be ignored Other events might be triggered Sound effects Send collision notification messages

35 Collision Resolution: Collision
Place objects at point of impact Assign new velocities Using physics or Using some other decision logic

36 Collision Resolution: Epilogue
Propagate post-collision effects Possible effects Destroy one or both objects Play sound effect Inflict damage Many effects can be done either in the prologue or epilogue

37 Collision Resolution: Resolving Overlap Testing
1. Extract collision normal 2. Extract penetration depth 3. Move the two objects apart 4. Compute new velocities

38 Collision Resolution: Extract Collision Normal
Find position of objects before impact Use two closest points to construct the collision normal vector

39 Collision Resolution: Extract Collision Normal
Sphere collision normal vector Difference between centers at point of collision

40 Collision Resolution: Resolving Intersection Testing
Simpler than resolving overlap testing No need to find penetration depth or move objects apart Simply 1. Extract collision normal 2. Compute new velocities

41 Simple Collision Handling
Detect that collision has occurred (bounding box) Determine the time of the collision (may need to back up to point of collision) Determine where objects are when they touch Determine the collision normal (angle of incidence = angle of reflection) Determine the velocity vectors after the collision Determine any changes in motion

42 Simple Kinematics P(x, y) Forward kinematic problem theta2 L2 L1
find position of P from theta1, theta2, L1, L2 use the 2D translation and rotation matrices (TL2*Rtheta2)* (TL1*Rtheta1) generalizes to any number of links theta2 L2 L1 theta1

43 Particle System Explosions
Start with lots of small objects (1 to 4 pixels) Initialize particles with random velocities based on velocity of exploding object Apply gravity Transform color intensity as a function of time Destroy objects when they collide or after a fixed amount of time

44 The next 7 slides come from the Rabin text

45 Generalized Rigid Bodies
Key Differences from Particles Not necessarily spherical in shape Position, p, represents object’s center-of-mass location Surface may not be perfectly smooth Friction forces may be present Experience rotational motion in addition to translational (position only) motion

46 Generalized Rigid Bodies – Simulation
Angular Kinematics Orientation, 3x3 matrix R or quaternion, q Angular velocity, w As with translational/particle kinematics, all properties are measured in world coordinates Additional Object Properties Inertia tensor, J Center-of-mass Additional State Properties for Simulation Orientation Angular momentum, L=Jw Corresponding state derivatives

47 Generalized Rigid Bodies - Simulation
Torque Analogous to a force Causes rotational acceleration Cause a change in angular momentum Torque is the result of a force (friction, collision response, spring, damper, etc.)

48 Collision Response Why? Two Basic Approaches
Performed to keep objects from interpenetrating To ensure behavior similar to real-world objects Two Basic Approaches Approach 1: Instantaneous change of velocity at time of collision Benefits: Visually the objects never interpenetrate Result is generated via closed-form equations, and is perfectly stable Difficulties: Precise detection of time and location of collision can be prohibitively expensive (frame rate killer) Logic to manage state is complex

49 Collision Response Two Basic Approaches (continued)
Approach 2: Gradual change of velocity and position over time, following collision Benefits Does not require precise detection of time and location of collision State management is easy Potential to be more realistic, if meshes are adjusted to deform according to predicted interpenetration Difficulties Object interpenetration is likely, and parameters must be tweaked to manage this Simulation can be subject to numerical instabilities, often requiring the use of implicit finite difference methods

50 Final Comments Instantaneous Collision Response
Classical approach: Impulse-momentum equations See text for full details Gradual Collision Response Classical approach: Penalty force methods Resolve interpenetration over the course of a few integration steps Penalty forces can wreak havoc on numerical integration Instabilities galore Implicit finite difference equations can handle it But more difficult to code Geometric approach: Ignore physical response equations Enforce purely geometric constraints once interpenetration has occurred

51 Final Comments Simple Games Generalized Rigid Body Simulation
Closed-form particle equations may be all you need Numerical particle simulation adds flexibility without much coding effort Collision detection is probably the most difficult part of this Generalized Rigid Body Simulation Includes rotational effects and interesting (non-constant) forces

52 Time-Based Modeling Time t is used in all kinematic equations that move objects (to avoid discontinuities caused by “slower” frame rates) This involves scaling dx and dy based on elapsed time (rather than a virtual clock) This allow constant movement regardless of processor slow downs


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