2
Matrices
������
�
�
������
�
�
��
nmnn
m
m
m
mn
aaa
aaa
aaa
aaa
A
�
���
21
33231
22221
11211
mnmnmn BAC ��� � Sum:Sum:
ijijij bac ��
A and B must have the same A and B must have the same dimensionsdimensions
3
Matrices
pmmnpn BAC ��� �Product:Product:
��
m
kkjikij bac
1
A and B must have A and B must have compatible dimensionscompatible dimensions
nnnnnnnn ABBA �����
Identity Matrix:
AAIIAI �������
�
�
�����
�
�
�
100
010
001
5
Matrices
mnT
nm AC �� �Transpose:Transpose:
jiij ac � TTT ABAB �)(
TTT BABA � � )(
IfIf AAT � A is symmetricA is symmetric
6
Matrices
Determinant:Determinant: A must be squareA must be square
3231
222113
3331
232112
3332
232211
333231
232221
131211
detaa
aaa
aa
aaa
aa
aaa
aaa
aaa
aaa ���
���
�
�
���
�
�
122122112221
1211
2221
1211det aaaaaa
aa
aa
aa ������
���
7
Matrices
IAAAA nnnnnnnn�� �����
� 11
Inverse:Inverse: A must be squareA must be square
���
���
�
�
���
��
���
�
1121
1222
12212211
1
2221
1211 1aa
aa
aaaaaa
aa
11
2D Translation using Matrices
PP
xxyy
ttxx
ttyyPP !!tt
),(
),(
yx tt
yx�
�
t
P
���
�
�
���
�
�
���
���
�
���
���
�
�
�
11
0
0
1' y
x
t
t
ty
tx
y
x
y
xP
tt PP
13
Scaling Equation
PP
xxyy
s.xs.x
PP !!s.ys.y
),('
),(
sysx
yx�
�
P
P
PP �� s'
��
���
����
���
����
���
�
y
x
s
s
sy
sx
0
0'P
SPSP ��'
15
Rotation Equations
CounterCounter--clockwise rotation by an angle clockwise rotation by an angle ��
���
������
��� �
����
���
y
x
y
x
cossin
sincos
'
'
PPxx
YY !!PP !! ��
XX !!yy R.PP'
16
Why does multiplying points by R rotate them?
• Think of the rows of R as a new coordinate system. Taking inner products of each points with these expresses that point in that coordinate system.
• This means rows of R must be orthonormal vectors (orthogonal unit vectors).
• Think of what happens to the points (1,0) and (0,1). They go to (cos theta, -sin theta), and (sin theta, cos theta). They remain orthonormal, and rotate clockwise by theta.
• Any other point, (a,b) can be thought of as a(1,0) + b(0,1). R(a(1,0)+b(0,1) = Ra(1,0) + Ra(0,1) = aR(1,0) + bR(0,1). So it’s in the same position relative to the rotated coordinates that it was in before rotation relative to the x, y coordinates. That is, it’s rotated.
17
Degrees of Freedom
R is 2x2 R is 2x2 4 elements4 elementsBUT! There is only 1 degree of freedom: BUT! There is only 1 degree of freedom: ��
1)det( �
��
��
R
IRRRR TT
The 4 elements must satisfy the fol lowing constraints:The 4 elements must satisfy the fol lowing constraints:
���
������
��� �
����
���
y
x
y
x
cossin
sincos
'
'
18
Transformations can be composed
• Matrix multiplication is associative.• Combine series of transformations into
one matrix. (example, whiteboard).• In general, the order matters. (example,
whiteboard).• 2D Rotations can be interchanged.
Why?
19
Rotation and Translation
100
tycos�
sin �
tx-sin �
cos�
( )(1
y
x )
100
tyab
tx-ba( )(1
y
x )Rotation, Scaling and Translation
20
Rotation about an arbitrary point
• Can translate to origin, rotate, translate back. (example, whiteboard).
• This is also rotation with one translation.– Intuitively, amount of rotation is same
either way.– But a translation is added.
21
Inverse of a rotation
• If R is a rotation, RRT = I.– This is because the diagonals of RRT are the
magnitudes of the rows, which are all 1, because the rows are unit vectors giving directions.
– The off-diagonals are the inner product of orthogonal unit vectors, which are zero.
• So the transpose of R is its inverse, a rotation of equal magnitude in the opposite direction.
22
Stretching Equation
PP
xxyy
SSxx.x.x
PP !!SSyy.y.y��
���
����
���
�
���
���
��
y
xs
s
ys
xs
y
x
y
x
0
0'P
),('
),(
ysxs
yx
yx
P
P
S
PSP �'
23
Stretching = tilting and projecting(with weak perspective)
��
���
�����
�
�
���
�
�
���
���
����
���
�
���
���
��
y
xs
s
sy
xs
s
ys
xsy
x
yy
x
y
x
10
00
0'P
24
Linear Transformation
��
���
���
���
�
�����
�
�
���
�
�
��
���
�
��
��
���
����
���
�
���
���
���
���
�
��
��
���
����
���
�
y
xs
s
s
y
xs
s
y
x
dc
ba
y
x
y
y
x
��
��
��
��
sincos
cossin
10
0
sincos
cossin
sincos
cossin0
0
sincos
cossin
'PSVD
26
Viewing Position
• Express world in new coordinate system.
• If origins same, this is done by taking inner product with new coordinates.
• Otherwise, we must translate.
27
Suppose, for example, we want to have the y axis show how we are facing. We want to be at (7,3), facing in direction (ct,st). The x axis must be orthogonal, (-st,ct). If we want to express (x,y) in this coordinate frame, we need to take: (ct,st)*(x-7,y-3), and (-st,ct)*(x-7,y-3). This is done by multiplying by matrix with rows (-st,ct) and (ct,st)
28
Simple 3D Rotation
���
�
�
���
�
�
���
�
�
���
�
��
n
n
n
zzz
yyy
xxx
21
21
21...
100
0cossin
0sincos ����
Rotation about z axis.
Rotates x,y coordinates. Leaves z coordinates fixed.
29
Full 3D Rotation
���
�
�
���
�
�
����
�
�
���
�
�
����
�
�
���
�
�
������
cossin0
sincos0
001
cos0sin
010
sin0cos
100
0cossin
0sincos
R
• Any rotation can be expressed as combination of three rotations about three axes.
���
�
���
�
�
�
100
010
001TRR
• Rows (and columns) of R are orthonormal vectors.
• R has determinant 1 (not -1).
30
• Intuitively, it makes sense that 3D rotations can be expressed as 3 separate rotations about fixed axes. Rotations have 3 degrees of freedom; two describe an axis of rotation, and one the amount.
• Rotations preserve the length of a vector, and the angle between two vectors. Therefore, (1,0,0), (0,1,0), (0,0,1) must be orthonormal after rotation. After rotation, they are the three columns of R. So these columns must be orthonormal vectors for R to be a rotation. Similarly, if they are orthonormal vectors (with determinant 1) R will have the effect of rotating (1,0,0), (0,1,0), (0,0,1). Same reasoning as 2D tells us all other points rotate too.
• Note if R has determinant -1, then R is a rotation plus a reflection.
32
Transformation of lines/normals
• 2D. Line is set of points (x,y) for which (x,y).(ab)T=0. Suppose we rotate points by R. We want a matrix, T, so that:
R*(x,y) .T