3D Transformations, Homogeneous coords

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10/5/04 © University of Wisconsin, CS559 F all 2004 Last Time • Compositing Painterly Rendering Intro to 3D Graphics Homework 3 due Oct 12 in class

Transcript of 3D Transformations, Homogeneous coords

Page 1: 3D Transformations, Homogeneous coords

10/5/04 © University of Wisconsin, CS559 Fall 2004

Last Time

• Compositing• Painterly Rendering• Intro to 3D Graphics• Homework 3 due Oct 12 in class

Page 2: 3D Transformations, Homogeneous coords

10/5/04 © University of Wisconsin, CS559 Fall 2004

Today

• Composing transformations• 3D Transformations• Homogeneous coordinates• Intro to Viewing

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10/5/04 © University of Wisconsin, CS559 Fall 2004

2D Rotation

• Rotate counter-clockwise about the origin by an angle

00

cossinsincos

yx

yx

x

y

x

y

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Rotating About An Arbitrary Point

• What happens when you apply a rotation transformation to an object that is not at the origin?

x

y

?

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Rotating About An Arbitrary Point

• What happens when you apply a rotation transformation to an object that is not at the origin?– It translates as well

x

y

x

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10/5/04 © University of Wisconsin, CS559 Fall 2004

How Do We Fix it?

• How do we rotate an about an arbitrary point?– Hint: we know how to rotate about the origin of a coordinate system

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Rotating About An Arbitrary Point

x

y

x

y

x

y

x

y

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Rotate About Arbitrary Point

• Say you wish to rotate about the point (a,b)• You know how to rotate about (0,0)• Translate so that (a,b) is at (0,0)

– x’=x–a, y’=y–b

• Rotate– x”=(x-a)cos-(y-b)sin, y”=(x-a)sin+(y-b)cos

• Translate back again– xf=x”+a, yf=y”+b

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Scaling an Object not at the Origin

• What happens if you apply the scaling transformation to an object not at the origin?

• Based on the rotating about a point composition, what should you do to resize an object about its own center?

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Back to Rotation About a Pt

• Say R is the rotation matrix to apply, and p is the point about which to rotate

• Translation to Origin:• Rotation:• Translate back:• The translation component of the composite transformation

involves the rotation matrix. What a mess!

pxx RpRxpxRxRx )(

pRpRxpxx

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Homogeneous Coordinates

• Use three numbers to represent a point• (x,y)=(wx,wy,w) for any constant w0

– Typically, (x,y) becomes (x,y,1)– To go backwards, divide by w

• Translation can now be done with matrix multiplication!

11001yx

baabaa

yx

yyyyx

xxyxx

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Basic Transformations

• Translation: Rotation:

• Scaling:

1001001

y

x

bb

1000000

y

x

ss

1000cossin0sincos

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Homogeneous Transform Advantages

• Unified view of transformation as matrix multiplication– Easier in hardware and software

• To compose transformations, simply multiply matrices– Order matters: AB is generally not the same as BA

• Allows for non-affine transformations:– Perspective projections!– Bends, tapers, many others

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Directions vs. Points

• We have been talking about transforming points• Directions are also important in graphics

– Viewing directions– Normal vectors– Ray directions

• Directions are represented by vectors, like points, and can be transformed, but not like points

(1,1)(-2,-1)

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Transforming Directions

• Say I define a direction as the difference of two points: d=a–b– This represents the direction of the line between two points

• Now I translate the points by the same amount: a’=a+t, b’=b+t

• How should I transform d?

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Homogeneous Directions

• Translation does not affect directions!• Homogeneous coordinates give us a very clean way of

handling this• The direction (x,y) becomes the homogeneous direction

(x,y,0)

• The correct thing happens for rotation and scaling also– Scaling changes the length of the vector, but not the direction– Normal vectors are slightly different – we’ll see more later

001001001

yx

yx

bb

y

x

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3D Transformations

• Homogeneous coordinates: (x,y,z)=(wx,wy,wz,w)• Transformations are now represented as 4x4 matrices• Typical graphics packages allow for specification of

translation, rotation, scaling and arbitrary matrices– OpenGL: glTranslate[fd], glRotate[fd], glScale[fd],

glMultMatrix[fd]

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3D Translation

11000100010001

1zyx

ttt

zyx

z

y

x

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3D Rotation

• Rotation in 3D is about an axis in 3D space passing through the origin

• Using a matrix representation, any matrix with an orthonormal top-left 3x3 sub-matrix is a rotation– Rows are mutually orthogonal (0 dot product)– Determinant is 1– Implies columns are also orthogonal, and that the transpose is equal

to the inverse

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3D Rotation

.,0,0,0,0 then

11000000

if and11000

000

1

113231213

2

1

etczyx

R

zyx

rrrrrrrrr

zyx

zzzyzx

yzyyyx

xzxyxx

rrrrrrrrrrr

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Problems with Rotation Matrices

• Specifying a rotation really only requires 3 numbers– Axis is a unit vector, so requires 2 numbers– Angle to rotate is third number

• Rotation matrix has a large amount of redundancy– Orthonormal constraints reduce degrees of freedom back down to 3– Keeping a matrix orthonormal is difficult when transformations are

combined

• Rotations are a very complex subject, and a detailed discussion is way beyond the scope of this course

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Alternative Representations

• Specify the axis and the angle (OpenGL method)– Hard to compose multiple rotations

• Euler angles: Specify how much to rotate about X, then how much about Y, then how much about Z– Hard to think about, and hard to compose– Any three axes will do e.g. X,Y,X

• Specify the axis, scaled by the angle– Only 3 numbers, called the exponential map

• Quaternions

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Quaternions

• 4-vector related to axis and angle, unit magnitude– Rotation about axis (nx,ny,nz) by angle :

• Reasonably easy to compose• Reasonably easy to go to/from rotation matrix• Only normalized quaternions represent rotations, but you

can normalize them just like vectors, so it isn’t a problem• Easy to perform spherical interpolation

2/sin,2/cos,2/cos,2/cos zyx nnn

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Other Rotation Issues

• Rotation is about an axis at the origin– For rotation about an arbitrary axis, use the same trick as in 2D:

Translate the axis to the origin, rotate, and translate back again

• Rotation is not commutative– Rotation order matters– Experiment to convince yourself of this

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Transformation Leftovers

• Scale, shear etc extend naturally from 2D to 3D• Rotation and Translation are the rigid-body

transformations:– Do not change lengths or angles, so a body does not deform when

transformed

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Modeling 101

• For the moment assume that all geometry consists of points, lines and faces

• Line: A segment between two endpoints• Face: A planar area bounded by line segments

– Any face can be triangulated (broken into triangles)

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Modeling and OpenGL

• In OpenGL, all geometry is specified by stating which type of object and then giving the vertices that define it

• glBegin(…) …glEnd()• glVertex[34][fdv]

– Three or four components (regular or homogeneous)– Float, double or vector (eg float[3])

• Chapter 2 of the red book

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Rendering

• Generate an image showing the contents of some region of space– The region is called the view volume, and it is defined by the user

• Determine where each object should go in the image– Viewing, Projection

• Determine which pixels should be filled– Rasterization

• Determine which object is in front at each pixel– Hidden surface elimination, Hidden surface removal, Visibility

• Determine what color it is– Lighting, Shading

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10/5/04 © University of Wisconsin, CS559 Fall 2004

Graphics Pipeline

• Graphics hardware employs a sequence of coordinate systems– The location of the geometry is expressed in each coordinate system

in turn, and modified along the way– The movement of geometry through these spaces is considered a

pipeline

Local Coordinate

Space

World Coordinate

Space

View Space

Canonical View

Volume

Display Space