1 e. angel and d. shreiner: interactive computer graphics 6e © addison-wesley 2012. geometry...
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1E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Geometry
Sai-Keung Wong (黃世強 )
Computer Science
National Chiao Tung University, Taiwan
2E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Objectives
• Introduce the elements of geometry Scalars
Vectors
Points
•Develop mathematical operations among them in a coordinate-free manner
•Define basic primitives Line segments
Polygons
3E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Basic Elements
• Geometry is the study of the relationships among objects in an n-dimensional space
In computer graphics, we are interested in objects that exist in three dimensions
• Want a minimum set of primitives from which we can build more sophisticated objects
• We will need three basic elements Scalars
Vectors
Points
4E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Coordinate-Free Geometry
• When we learned simple geometry, most of us started with a Cartesian approach
Points were at locations in space p=(x,y,z) We derived results by algebraic manipulations
involving these coordinates• This approach was nonphysical
Physically, points exist regardless of the location of an arbitrary coordinate system
Most geometric results are independent of the coordinate system
Example Euclidean geometry: two triangles are identical if two corresponding sides and the angle between them are identical
5E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Scalars
• Need three basic elements in geometry Scalars, Vectors, Points
• Scalars can be defined as members of sets which can be combined by two operations (addition and multiplication) obeying some fundamental axioms (associativity, commutivity, inverses)
• Examples include the real and complex number systems under the ordinary rules with which we are familiar
• Scalars alone have no geometric properties
6E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Vectors
•Physical definition: a vector is a quantity with two attributes
Direction Magnitude
•Examples include Force Velocity Directed line segments
• Most important example for graphics• Can map to other types
v
7E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Vector Operations
• Every vector has an inverse Same magnitude but points in opposite direction
• Every vector can be multiplied by a scalar
• There is a zero vector Zero magnitude, undefined orientation
• The sum of any two vectors is a vector Use head-to-tail axiom
v -v vv
u
w
8E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Linear Vector Spaces
•Mathematical system for manipulating vectors•Operations
Scalar-vector multiplication u=v Vector-vector addition: w=u+v
•Expressions such as v=u+2w-3r
Make sense in a vector space
9E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Vectors Lack Position
• These vectors are identical Same length and magnitude
• Vectors spaces insufficient for geometry Need points
10E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Points
•Location in space•Operations allowed between points and vectors
Point-point subtraction yields a vector
Equivalent to point-vector addition
P=v+Q
v=P-Q
11E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Affine Spaces
•Point + a vector space•Operations
Vector-vector addition
Scalar-vector multiplication
Point-vector addition
Scalar-scalar operations
• For any point define 1 • P = P
0 • P = 0 (zero vector)
12E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Lines
•Consider all points of the form P()=P0 + d
Set of all points that pass through P0 in the direction of the vector d
13E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Parametric Form
•This form is known as the parametric form of the line
More robust and general than other forms Extends to curves and surfaces
•Two-dimensional forms Explicit: y = mx +h Implicit: ax + by +c =0 Parametric:
x() = x0 + (1-)x1
y() = y0 + (1-)y1
14E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Rays and Line Segments
• If >= 0, then P() is the ray leaving P0 in the direction d
If we use two points to define v, then
P( ) = Q + (R-Q)=Q+v
=R + (1-)Q
For 0<=<=1 we get all the
points on the line segment
joining R and Q
15E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Convexity
•An object is convex iff for any two points in the object all points on the line segment between these points are also in the object
P
Q Q
P
convex not convex
16E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Affine Sums
•Consider the “sum”
P=1P1+2P2+…..+nPn
Can show by induction that this sum makes sense iff
1+2+…..n=1in which case we have the affine sum of the points P1P2,…..Pn
• If, in addition, i>=0, we have the convex hull of P1P2,…..Pn
17E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Convex Hull
•Smallest convex object containing P1P2,…..Pn
•Formed by “shrink wrapping” points
18E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Curves and Surfaces
•Curves are one parameter entities of the form P() where the function is nonlinear
•Surfaces are formed from two-parameter functions P(, )
Linear functions give planes and polygons
P() P(, )
19E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Planes
•A plane can be defined by a point and two vectors or by three points
P(,)=R+u+v P(,)=R+(Q-R)+(P-Q)
u
v
R
P
R
Q
20E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Triangles
convex sum of P and Q
convex sum of S() and R
for 0<=,<=1, we get all points in triangle
Barycentric Coordinates
Triangle is convex so any point inside can be represented as an affine sum
P(1, 2, 3)=1P+2Q+3R
where
1 +2 +3 = 1
i>=0
The representation is called the barycentric coordinate representation of P
21E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
22E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012.
Normals
• Every plane has a vector n normal (perpendicular, orthogonal) to it
• From point-two vector form P(,)=R+u+v, we know we can use the cross product to find n = u v and the equivalent form
(P()-P) n=0
u
v
P
23E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Representation
Sai-Keung Wong (黃世強 )
Computer Science
National Chiao Tung University, Taiwan
24E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Objectives
• Introduce concepts such as dimension and basis
• Introduce coordinate systems for representing vectors spaces and frames for representing affine spaces
•Discuss change of frames and bases• Introduce homogeneous coordinates
25E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Linear Independence
•A set of vectors v1, v2, …, vn is linearly independent if
1v1+2v2+.. nvn=0 iff 1=2=…=0
• If a set of vectors is linearly independent, we cannot represent one in terms of the others
• If a set of vectors is linearly dependent, at least one can be written in terms of the others
26E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Dimension
• In a vector space, the maximum number of linearly independent vectors is fixed and is called the dimension of the space
• In an n-dimensional space, any set of n linearly independent vectors form a basis for the space
• Given a basis v1, v2,…., vn, any vector v can be written as
v=1v1+ 2v2 +….+nvn
where the {i} are unique
27E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Representation
•Until now we have been able to work with geometric entities without using any frame of reference, such as a coordinate system
•Need a frame of reference to relate points and objects to our physical world.
For example, where is a point? Can’t answer without a reference system
World coordinates
Camera coordinates
28E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Coordinate Systems
• Consider a basis v1, v2,…., vn
• A vector is written v=1v1+ 2v2 +….+nvn
• The list of scalars {1, 2, …. n}is the representation of v with respect to the given basis
• We can write the representation as a row or column array of scalars
a=[1 2 …. n]T=
n
2
1
.
29E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Example
• v=2v1+3v2-4v3
• a=[2 3 –4]T
•Note that this representation is with respect to a particular basis
•For example, in OpenGL we start by representing vectors using the object basis but later the system needs a representation in terms of the camera or eye basis
30E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Coordinate Systems
•Which is correct?
•Both are because vectors have no fixed location
v
v
31E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Frames
•A coordinate system is insufficient to represent points
• If we work in an affine space we can add a single point, the origin, to the basis vectors to form a frame
P0
v1
v2
v3
32E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Representation in a Frame
•Frame determined by (P0, v1, v2, v3)
•Within this frame, every vector can be written as
v=1v1+ 2v2 +….+nvn
•Every point can be written as
P = P0 + 1v1+ 2v2 +….+nvn
33E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Confusing Points and Vectors
Consider the point and the vector
P = P0 + 1v1+ 2v2 +….+nvn
v=1v1+ 2v2 +….+nvn
They appear to have the similar representations
p=[1 2 3] v=[1 2 3]
which confuses the point with the vector
A vector has no position v
pv
Vector can be placed anywhere
point: fixed
34E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
A Single Representation
If we define 0•P = 0 and 1•P =P then we can write
v=1v1+ 2v2 +3v3 = [1 2 3 0 ] [v1 v2 v3 P0]
T
P = P0 + 1v1+ 2v2 +3v3= [1 2 3 1 ] [v1 v2 v3 P0]
T
Thus we obtain the four-dimensional homogeneous coordinate representation
v = [1 2 3 0 ] T
p = [1 2 3 1 ] T
35E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Homogeneous Coordinates
The homogeneous coordinates form for a three dimensional point [x y z] is given as
p =[x’ y’ z’ w] T =[wx wy wz w] T
We return to a three dimensional point (for w0) byxx’/wyy’/wzz’/wIf w=0, the representation is that of a vectorNote that homogeneous coordinates replaces points in
three dimensions by lines through the origin in four dimensions
For w=1, the representation of a point is [x y z 1]
36E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Homogeneous Coordinates and Computer Graphics
•Homogeneous coordinates are key to all computer graphics systems
All standard transformations (rotation, translation, scaling) can be implemented with matrix multiplications using 4 x 4 matrices
Hardware pipeline works with 4 dimensional representations
For orthographic viewing, we can maintain w=0 for vectors and w=1 for points
For perspective we need a perspective division
37E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Change of Coordinate Systems
•Consider two representations of a the same vector with respect to two different bases. The representations are
v=1v1+ 2v2 +3v3 = [1 2 3] [v1 v2 v3]
T
=1u1+ 2u2 +3u3 = [1 2 3] [u1 u2 u3]
T
a=[1 2 3 ]b=[1 2 3]
where
38E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Representing second basis in terms of first
Each of the basis vectors, u1,u2, u3, are vectors that can be represented in terms of the first basis
u1 = 11v1+12v2+13v3
u2 = 21v1+22v2+23v3
u3 = 31v1+32v2+33v3
v
39E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Matrix Form
The coefficients define a 3 x 3 matrix
and the bases can be related by
see text for numerical examples
a=MTb
33
M =
40E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Change of Frames
• We can apply a similar process in homogeneous coordinates to the representations of both points and vectors
• Any point or vector can be represented in either frame
• We can represent Q0, u1, u2, u3 in terms of P0, v1, v2, v3
Consider two frames:(P0, v1, v2, v3)(Q0, u1, u2, u3) P0 v1
v2
v3
Q0
u1u2
u3
41E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Representing One Frame in Terms of the Other
u1 = 11v1+12v2+13v3
u2 = 21v1+22v2+23v3
u3 = 31v1+32v2+33v3
Q0 = 41v1+42v2+43v3 +44P0
Extending what we did with change of bases
defining a 4 x 4 matrix
M =
42E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Working with Representations
Within the two frames any point or vector has a representation of the same form
a=[1 2 3 4 ] in the first frameb=[1 2 3 4 ] in the second frame
where 4 4 for points and 4 4 for vectors and
The matrix M is 4 x 4 and specifies an affine transformation in homogeneous coordinates
a=MTb
43E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Affine Transformations
•Every linear transformation is equivalent to a change in frames
•Every affine transformation preserves lines
•However, an affine transformation has only 12 degrees of freedom because 4 of the elements in the matrix are fixed and are a subset of all possible 4 x 4 linear transformations
44E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
The World and Camera Frames
• When we work with representations, we work with n-tuples or arrays of scalars
• Changes in frame are then defined by 4 x 4 matrices
• In OpenGL, the base frame that we start with is the world frame
• Eventually we represent entities in the camera frame by changing the world representation using the model-view matrix
• Initially these frames are the same (M=I)
45E. Angel and D. Shriener: Interactive Computer Graphics 6E © Addison-Wesley 2012
Moving the Camera
If objects are on both sides of z=0, we must move camera frame
1000
d100
0010
0001
M =
46E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Transformations
Sai-Keung Wong (黃世強 )
Computer Science
National Chiao Tung University, Taiwan
47E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Objectives
• Introduce standard transformations Rotation
Translation
Scaling
Shear
•Derive homogeneous coordinate transformation matrices
•Learn to build arbitrary transformation matrices from simple transformations
48E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
General Transformations
A transformation maps points to other points and/or vectors to other vectors
Q=T(P)
v=T(u)
49E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Affine Transformations
•Line preserving•Characteristic of many physically important transformations
Rigid body transformations: rotation, translation
Scaling, shear
• Importance in graphics is that we need only transform endpoints of line segments and let implementation draw line segment between the transformed endpoints
50E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Pipeline Implementation
transformation rasterizer
u
v
u
v
T
T(u)
T(v)
T(u)T(u)
T(v)
T(v)
vertices vertices pixels
framebuffer
(from application program)
51E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Notation
We will be working with both coordinate-free representations of transformations and representations within a particular frame
P,Q, R: points in an affine space u, v, w: vectors in an affine space , , : scalars p, q, r: representations of points
-array of 4 scalars in homogeneous coordinates u, v, w: representations of points
-array of 4 scalars in homogeneous coordinates
52E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Translation
•Move (translate, displace) a point to a new location
•Displacement determined by a vector d Three degrees of freedom P’=P+d
P
P’
d
53E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
How many ways?
Although we can move a point to a new location in infinite ways, when we move many points there is usually only one way
object translation: every point displaced by same vector
54E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Translation Using Representations
Using the homogeneous coordinate representation in some frame
p=[ x y z 1]T
p’=[x’ y’ z’ 1]T
d=[dx dy dz 0]T
Hence p’ = p + d or
x’=x+dx
y’=y+dy
z’=z+dz
note that this expression is in four dimensions and expressespoint = vector + point
55E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Translation Matrix
We can also express translation using a 4 x 4 matrix T in homogeneous coordinatesp’=Tp where
T = T(dx, dy, dz) =
This form is better for implementation because all affine transformations can be expressed this way and multiple transformations can be concatenated together
1000
d100
d010
d001
z
y
x
56E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Rotation (2D)
Consider rotation about the origin by degrees radius stays the same, angle increases by
x’=x cos –y sin y’ = x sin + y cos
x = r cos y = r sin
x = r cos (y = r sin (
57E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Rotation about the z axis
• Rotation about z axis in three dimensions leaves all points with the same z
Equivalent to rotation in two dimensions in planes of constant z
or in homogeneous coordinates
p’=Rz()p
x’=x cos –y sin y’ = x sin + y cos z’ =z
58E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Rotation Matrix
1000
0100
00 cossin
00sin cos
R = Rz() =
59E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Rotation about x and y axes
• Same argument as for rotation about z axis For rotation about x axis, x is unchanged
For rotation about y axis, y is unchanged
R = Rx() =
R = Ry() =
1000
0 cos sin0
0 sin- cos0
0001
1000
0 cos0 sin-
0010
0 sin0 cos
60E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Scaling
1000
000
000
000
z
y
x
s
s
s
S = S(sx, sy, sz) =
x’=sxxy’=syxz’=szx
p’=Sp
Expand or contract along each axis (fixed point of origin)
61E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Reflection
corresponds to negative scale factors
originalsx = -1 sy = 1
sx = -1 sy = -1 sx = 1 sy = -1
62E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Inverses
• Although we could compute inverse matrices by general formulas, we can use simple geometric observations
Translation: T-1(dx, dy, dz) = T(-dx, -dy, -dz)
Rotation: R -1() = R(-)• Holds for any rotation matrix• Note that since cos(-) = cos() and sin(-)=-sin()
R -1() = R T()
Scaling: S-1(sx, sy, sz) = S(1/sx, 1/sy, 1/sz)
63E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Concatenation
• We can form arbitrary affine transformation matrices by multiplying together rotation, translation, and scaling matrices
• Because the same transformation is applied to many vertices, the cost of forming a matrix M=ABCD is not significant compared to the cost of computing Mp for many vertices p
• The difficult part is how to form a desired transformation from the specifications in the application
64E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Order of Transformations
•Note that matrix on the right is the first applied
•Mathematically, the following are equivalent
p’ = ABCp = A(B(Cp))•Note many references use column matrices to represent points. In terms of column matrices
p’T = pTCTBTAT
65E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
General Rotation About the Origin
x
z
yv
A rotation by about an arbitrary axiscan be decomposed into the concatenationof rotations about the x, y, and z axes
R() = Rz(z) Ry(y) Rx(x)
x y z are called the Euler angles
Note that rotations do not commuteWe can use rotations in another order butwith different angles
66E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Rotation About a Fixed Point other than the Origin
Move fixed point to origin
Rotate
Move fixed point back
M = T(pf) R() T(-pf)
67E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Instancing
• In modeling, we often start with a simple object centered at the origin, oriented with the axis, and at a standard size
•We apply an instance transformation to its vertices to
Scale
Orient
Locate
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Shear
• Helpful to add one more basic transformation
• Equivalent to pulling faces in opposite directions
69E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Shear Matrix
Consider simple shear along x axis
x’ = x + y cot y’ = yz’ = z
1000
0100
0010
00cot 1
H() =
70E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
OpenGL Transformations
Sai-Keung Wong (黃世強 )
Computer Science
National Chiao Tung University, Taiwan
71E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Objectives
•Learn how to carry out transformations in OpenGL
Rotation
Translation
Scaling
• Introduce mat,h and vec.h transformations Model-view
Projection
72E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Pre 3.1OpenGL Matrices
• In OpenGL matrices were part of the state•Multiple types
Model-View (GL_MODELVIEW) Projection (GL_PROJECTION) Texture (GL_TEXTURE) Color(GL_COLOR)
•Single set of functions for manipulation•Select which to manipulated byglMatrixMode(GL_MODELVIEW);glMatrixMode(GL_PROJECTION);
73E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Current Transformation Matrix (CTM)
• Conceptually there is a 4 x 4 homogeneous coordinate matrix, the current transformation matrix (CTM) that is part of the state and is applied to all vertices that pass down the pipeline
• The CTM is defined in the user program and loaded into a transformation unit
CTMvertices vertices
p p’=CpC
74E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
CTM operations
• The CTM can be altered either by loading a new CTM or by postmutiplication
Load an identity matrix: C ILoad an arbitrary matrix: C M
Load a translation matrix: C TLoad a rotation matrix: C RLoad a scaling matrix: C S
Postmultiply by an arbitrary matrix: C CMPostmultiply by a translation matrix: C CTPostmultiply by a rotation matrix: C C RPostmultiply by a scaling matrix: C C S
75E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Rotation about a Fixed Point
Start with identity matrix: C IMove fixed point to origin: C CTRotate: C CRMove fixed point back: C CT -1
Result: C = TR T –1 which is backwards.
This result is a consequence of doing postmultiplications.Let’s try again.
76E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Reversing the Order
We want C = T –1 R T so we must do the operations in the following order
C IC CT -1
C CRC CT
Each operation corresponds to one function call in the program.
Note that the last operation specified is the first executed in the program
77E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
CTM in OpenGL
•OpenGL had a model-view and a projection matrix in the pipeline which were concatenated together to form the CTM
•We will emulate this process
78E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Rotation, Translation, Scaling
mat4 r = Rotate(theta, vx, vy, vz)m = m*r;
mat4 s = Scale( sx, sy, sz)mat4 t = Transalate(dx, dy, dz);m = m*s*t;
mat4 m = Identity();
Create an identity matrix:
Multiply on right by rotation matrix of theta in degrees where (vx, vy, vz) define axis of rotation
Do same with translation and scaling:
79E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Example
• Rotation about z axis by 30 degrees with a fixed point of (1.0, 2.0, 3.0)
• Remember that last matrix specified in the program is the first applied
mat 4 m = Identity();m = Translate(1.0, 2.0, 3.0)* Rotate(30.0, 0.0, 0.0, 1.0)* Translate(-1.0, -2.0, -3.0);
80E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Arbitrary Matrices
•Can load and multiply by matrices defined in the application program
•Matrices are stored as one dimensional array of 16 elements which are the components of the desired 4 x 4 matrix stored by columns
•OpenGL functions that have matrices as parameters allow the application to send the matrix or its transpose
81E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Matrix Stacks
• In many situations we want to save transformation matrices for use later
Traversing hierarchical data structures (Chapter 8)
Avoiding state changes when executing display lists
•Pre 3.1 OpenGL maintained stacks for each type of matrix
•Easy to create the same functionality with a simple stack class
82E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Reading Back State
• Can also access OpenGL variables (and other parts of the state) by query functions
glGetIntegervglGetFloatvglGetBooleanvglGetDoublevglIsEnabled
83E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Using Transformations
• Example: use idle function to rotate a cube and mouse function to change direction of rotation
• Start with a program that draws a cube in a standard way
Centered at origin
Sides aligned with axes
Will discuss modeling in next lecture
84E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
main.c
void main(int argc, char **argv) { glutInit(&argc, argv); glutInitDisplayMode(GLUT_DOUBLE | GLUT_RGB | GLUT_DEPTH); glutInitWindowSize(500, 500); glutCreateWindow("colorcube"); glutReshapeFunc(myReshape); glutDisplayFunc(display); glutIdleFunc(spinCube); glutMouseFunc(mouse); glEnable(GL_DEPTH_TEST); glutMainLoop();}
85E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Idle and Mouse callbacks
void spinCube() {theta[axis] += 2.0;if( theta[axis] > 360.0 ) theta[axis] -= 360.0;glutPostRedisplay();
}
void mouse(int btn, int state, int x, int y){ if(btn==GLUT_LEFT_BUTTON && state == GLUT_DOWN) axis = 0; if(btn==GLUT_MIDDLE_BUTTON && state == GLUT_DOWN) axis = 1; if(btn==GLUT_RIGHT_BUTTON && state == GLUT_DOWN) axis = 2;}
86E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Display callback
void display(){ glClear(GL_COLOR_BUFFER_BIT | GL_DEPTH_BUFFER_BIT); glUniform(…); //or glUniformMatrix glDrawArrays(…);
glutSwapBuffers();}
We can form matrix in application and send to shader and let shader do the rotation or we can send the angle and axis to the shader and let the shader form the transformation matrix and then do the rotation
More efficient than transforming data in application and resending the data
87E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Using the Model-view Matrix
• In OpenGL the model-view matrix is used to Position the camera
• Can be done by rotations and translations but is often easier to use a LookAt function
Build models of objects
• The projection matrix is used to define the view volume and to select a camera lens
• Although these matrices are no longer part of the OpenGL state, it is usually a good strategy to create them in our own applications
88E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Smooth Rotation
• From a practical standpoint, we are often want to use transformations to move and reorient an object smoothly
Problem: find a sequence of model-view matrices M0,M1,…..,Mn so that when they are applied successively to one or more objects we see a smooth transition
• For orientating an object, we can use the fact that every rotation corresponds to part of a great circle on a sphere
Find the axis of rotation and angle Virtual trackball (see text)
89E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Incremental Rotation
• Consider the two approaches
For a sequence of rotation matrices R0,R1,
…..,Rn , find the Euler angles for each and use Ri= Riz Riy Rix
• Not very efficient
Use the final positions to determine the axis and angle of rotation, then increment only the angle
• Quaternions can be more efficient than either
90E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Quaternions
• Extension of imaginary numbers from two to three dimensions
• Requires one real and three imaginary components i, j, k
• Quaternions can express rotations on sphere smoothly and efficiently. Process:
Model-view matrix quaternion Carry out operations with quaternions Quaternion Model-view matrix
q=q0+q1i+q2j+q3k
91E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Interfaces
• One of the major problems in interactive computer graphics is how to use two-dimensional devices such as a mouse to interface with three dimensional obejcts
• Example: how to form an instance matrix?• Some alternatives
Virtual trackball 3D input devices such as the spaceball Use areas of the screen
• Distance from center controls angle, position, scale depending on mouse button depressed
92E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Building Models
Sai-Keung Wong (黃世強 )
Computer Science
National Chiao Tung University, Taiwan
93E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Objectives
• Introduce simple data structures for building polygonal models
Vertex lists
Edge lists
•Deprecated OpenGL vertex arrays
94E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Representing a Mesh
• Consider a mesh
• There are 8 nodes and 12 edges 5 interior polygons
6 interior (shared) edges
• Each vertex has a location vi = (xi yi zi)
v1 v2
v7
v6
v8
v5
v4
v3
e1
e8
e3
e2
e11
e6
e7
e10
e5
e4
e9
e12
95E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Simple Representation
• Define each polygon by the geometric locations of its vertices
• Leads to OpenGL code such as
• Inefficient and unstructured Consider moving a vertex to a new location
Must search for all occurrences
vertex[i] = vec3(x1, x1, x1);vertex[i+1] = vec3(x6, x6, x6);vertex[i+2] = vec3(x7, x7, x7);i+=3;
96E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Inward and Outward Facing Polygons
• The order {v1, v6, v7} and {v6, v7, v1} are equivalent in that the same polygon will be rendered by OpenGL but the order {v1, v7, v6} is different
• The first two describe outwardly
facing polygons• Use the right-hand rule =
counter-clockwise encirclement
of outward-pointing normal • OpenGL can treat inward and
outward facing polygons differently
97E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Geometry vs Topology
•Generally it is a good idea to look for data structures that separate the geometry from the topology
Geometry: locations of the vertices
Topology: organization of the vertices and edges
Example: a polygon is an ordered list of vertices with an edge connecting successive pairs of vertices and the last to the first
Topology holds even if geometry changes
98E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Vertex Lists
• Put the geometry in an array
• Use pointers from the vertices into this array
• Introduce a polygon listx1 y1 z1
x2 y2 z2
x3 y3 z3
x4 y4 z4
x5 y5 z5.
x6 y6 z6
x7 y7 z7
x8 y8 z8
P1P2P3P4P5
v1
v7
v6
v8
v5
v6topology geometry
99E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Shared Edges
• Vertex lists will draw filled polygons correctly but if we draw the polygon by its edges, shared edges are drawn twice
• Can store mesh by edge list
100E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Edge List
v1 v2
v7
v6
v8
v5
v3
e1
e8
e3
e2
e11
e6
e7
e10
e5
e4
e9
e12
e1e2e3e4e5e6e7e8e9
x1 y1 z1
x2 y2 z2
x3 y3 z3
x4 y4 z4
x5 y5 z5.
x6 y6 z6
x7 y7 z7
x8 y8 z8
v1v6
Note polygons arenot represented
101E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Modeling a Cube
typedef vex3 point3;point3 vertices[] = {point3(-1.0,-1.0,-1.0), point3(1.0,-1.0,-1.0), point3(1.0,1.0,-1.0), point3(-1.0,1.0,-1.0), point3(-1.0,-1.0,1.0), point3(1.0,-1.0,1.0), point3(1.0,1.0,1.0), point3(-1.0,1.0,1.0)};
typedef vec3 color3;color3 colors[] = {color3(0.0,0.0,0.0), color3(1.0,0.0,0.0), color3(1.0,1.0,0.0), color(0.0,1.0,0.0), color3(0.0,0.0,1.0), color3(1.0,0.0,1.0), color3(1.0,1.0,1.0), color3(0.0,1.0,1.0});
Define global arrays for vertices and colors
102E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Drawing a triangle from a list of indices
Draw a triangle from a list of indices into the array vertices and assign a color to each index
void triangle(int a, int b, int c, int d){ vcolors[i] = colors[d]; position[i] = vertices[a]; vcolors[i+1] = colors[d]); position[i+1] = vertices[a]; vcolors[i+2] = colors[d]; position[i+2] = vertices[a]; i+=3; }
103E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Draw cube from faces
void colorcube( ){ quad(0,3,2,1); quad(2,3,7,6); quad(0,4,7,3); quad(1,2,6,5); quad(4,5,6,7); quad(0,1,5,4);}
0
5 6
2
4 7
1
3
Note that vertices are ordered so that we obtain correct outward facing normals
104E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Efficiency
•The weakness of our approach is that we are building the model in the application and must do many function calls to draw the cube
•Drawing a cube by its faces in the most straight forward way used to require
6 glBegin, 6 glEnd 6 glColor 24 glVertex More if we use texture and lighting
105E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Vertex Arrays
• OpenGL provided a facility called vertex arrays that allows us to store array data in the implementation
• Six types of arrays were supported initially Vertices
Colors
Color indices
Normals
Texture coordinates
Edge flags
• Now vertex arrays can be used for any attributes
106E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Old Style Initialization
• Using the same color and vertex data, first we enableglEnableClientState(GL_COLOR_ARRAY);
glEnableClientState(GL_VERTEX_ARRAY);
• Identify location of arraysglVertexPointer(3, GL_FLOAT, 0, vertices);
glColorPointer(3, GL_FLOAT, 0, colors);
3d arrays stored as floats data contiguousdata array
107E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Mapping indices to faces
•Form an array of face indices
•Each successive four indices describe a face of the cube
•Draw through glDrawElements which replaces all glVertex and glColor calls in the display callback
GLubyte cubeIndices[24] = {0,3,2,1,2,3,7,6 0,4,7,3,1,2,6,5,4,5,6,7,0,1,5,4};
108E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Drawing the cube
• Old Method:
• Problem is that although we avoid many function calls, data are still on client side
• Solution: no immediate mode
Vertex buffer object
Use glDrawArrays
glDrawElements(GL_QUADS, 24, GL_UNSIGNED_BYTE, cubeIndices);
Draws cube with 1 function call!!
Rotating Cube
•Full example•Model Colored Cube•Use 3 button mouse to change direction of rotation
•Use idle function to increment angle of rotation
109E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
Cube Vertices
110E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
// Vertices of a unit cube centered at origin// sides aligned with axespoint4 vertices[8] = { point4( -0.5, -0.5, 0.5, 1.0 ), point4( -0.5, 0.5, 0.5, 1.0 ), point4( 0.5, 0.5, 0.5, 1.0 ), point4( 0.5, -0.5, 0.5, 1.0 ), point4( -0.5, -0.5, -0.5, 1.0 ), point4( -0.5, 0.5, -0.5, 1.0 ), point4( 0.5, 0.5, -0.5, 1.0 ), point4( 0.5, -0.5, -0.5, 1.0 )};
Colors
111E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
// RGBA colorscolor4 vertex_colors[8] = { color4( 0.0, 0.0, 0.0, 1.0 ), // black color4( 1.0, 0.0, 0.0, 1.0 ), // red color4( 1.0, 1.0, 0.0, 1.0 ), // yellow color4( 0.0, 1.0, 0.0, 1.0 ), // green color4( 0.0, 0.0, 1.0, 1.0 ), // blue color4( 1.0, 0.0, 1.0, 1.0 ), // magenta color4( 1.0, 1.0, 1.0, 1.0 ), // white color4( 0.0, 1.0, 1.0, 1.0 ) // cyan};
Quad Function
112E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
// quad generates two triangles for each face and assigns colors// to the verticesint Index = 0;void quad( int a, int b, int c, int d ){ colors[Index] = vertex_colors[a]; points[Index] = vertices[a]; Index++; colors[Index] = vertex_colors[b]; points[Index] = vertices[b]; Index++; colors[Index] = vertex_colors[c]; points[Index] = vertices[c]; Index++; colors[Index] = vertex_colors[a]; points[Index] = vertices[a]; Index++; colors[Index] = vertex_colors[c]; points[Index] = vertices[c]; Index++; colors[Index] = vertex_colors[d]; points[Index] = vertices[d]; Index++;}
Color Cube
113E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
// generate 12 triangles: 36 vertices and 36 colorsvoidcolorcube(){ quad( 1, 0, 3, 2 ); quad( 2, 3, 7, 6 ); quad( 3, 0, 4, 7 ); quad( 6, 5, 1, 2 ); quad( 4, 5, 6, 7 ); quad( 5, 4, 0, 1 );}
Initialization I
114E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
void init(){ colorcube();
// Create a vertex array object
GLuint vao; glGenVertexArrays ( 1, &vao ); glBindVertexArray ( vao );
Initialization II
115E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
// Create and initialize a buffer object GLuint buffer; glGenBuffers( 1, &buffer ); glBindBuffer( GL_ARRAY_BUFFER, buffer ); glBufferData( GL_ARRAY_BUFFER, sizeof(points) + sizeof(colors), NULL, GL_STATIC_DRAW ); glBufferSubData( GL_ARRAY_BUFFER, 0, sizeof(points), points ); glBufferSubData( GL_ARRAY_BUFFER, sizeof(points), sizeof(colors), colors );// Load shaders and use the resulting shader program GLuint program = InitShader( "vshader36.glsl", "fshader36.glsl" ); glUseProgram( program );
Initialization III
116E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
// set up vertex arrays GLuint vPosition = glGetAttribLocation( program, "vPosition" ); glEnableVertexAttribArray( vPosition ); glVertexAttribPointer( vPosition, 4, GL_FLOAT, GL_FALSE, 0, BUFFER_OFFSET(0) );
GLuint vColor = glGetAttribLocation( program, "vColor" ); glEnableVertexAttribArray( vColor ); glVertexAttribPointer( vColor, 4, GL_FLOAT, GL_FALSE, 0, BUFFER_OFFSET(sizeof(points)) );
theta = glGetUniformLocation( program, "theta" );
Display Callback
117E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
voiddisplay( void ){ glClear( GL_COLOR_BUFFER_BIT |GL_DEPTH_BUFFER_BIT );
glUniform3fv( theta, 1, theta ); glDrawArrays( GL_TRIANGLES, 0, NumVertices );
glutSwapBuffers();}
Mouse Callback
118E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
voidmouse( int button, int state, int x, int y ){ if ( state == GLUT_DOWN ) { switch( button ) { case GLUT_LEFT_BUTTON: Axis = Xaxis; break; case GLUT_MIDDLE_BUTTON: Axis = Yaxis; break; case GLUT_RIGHT_BUTTON: Axis = Zaxis; break; } }}
Idle Callback
119E. Angel and D. Shreiner: Interactive Computer Graphics 6E © Addison-Wesley 2012
voididle( void ){ theta[axis] += 0.01;
if ( theta[axis] > 360.0 ) { theta[axis] -= 360.0; }
glutPostRedisplay();}