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Geometric Transformations

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Presentation on theme: "Geometric Transformations"— Presentation transcript:

1 Geometric Transformations
CENG 477 Introduction to Computer Graphics Fall Computer Engineering METU

2 2D Geometric Transformations

3 Basic Geometric Transformations
Geometric transformations are used to transform the objects and the camera in a scene (for animation or modelling) and are also used to transform World Coordinates to View Coordinates Given the shape, transform all the points of the shape? Transform the points and/or vectors describing it. For example: Polygon: corner points Circle, Ellipse: center point(s), point at angle 0 Some transformations preserves some of the attributes like sizes, angles, ratios of the shape.

4 Translation Simply move the object to a relative position. P' T P

5 Rotation A rotation is defined by a rotation axis and a rotation angle. For 2D rotation, the parameters are rotation angle (θ) and the rotation point (xr,yr). We reposition the object in a circular path arround the rotation point (pivot point) θ xr yr

6 Rotation When (xr,yr)=(0,0) we have r The original coordinates are:
P P' The original coordinates are: Substituting them in the first equation we get: In the matrix form we have: where

7 Rotation Rotation around an arbitrary point (xr,yr)
This equations can be written as matrix operations (we will see when we discuss homogeneous coordinates). P' r P (xr,yr)

8 Scaling Change the size of an object. Input: scaling factors (sx,sy)
non-uniform vs. uniform scaling

9 Homogenous Coordinates
All transformations can be represented by matrix operations. Translation is additive, rotation and scaling is multiplicative (+ additive if you rotate around an arbitrary point or scale around a fixed point); making the operations complicated. Adding another dimension to transformations make translation also representable by multiplication. Cartesian coordinates vs homogenous coordinates.

10 Many points in homogenous coordinates can represent the same point in Cartesian coordinates.
In homogenous coordinates, all transformations can be written as matrix multiplications.

11 Transformations in Homogenous C.
Translation Rotation Scaling

12 Composite Transformations
Application of a sequence of transformations to a point:

13 Composite Transformations
First: composition of similar type transformations If we apply to successive translations to a point:

14 Composite Transformations

15 Rotation around a pivot point
Translate the object so that the pivot point moves to the origin Rotate around origin Translate the object so that the pivot point is back to its original position

16 Scaling with respect to a fixed point
Translate to origin Scale Translate back

17 Order of matrix compositions
Matrix composition is not commutative. So, be careful when applying a sequence of transformations. pivot same pivot

18 Other Transformations
Reflection

19 Shear: Deform the shape like shifted slices.
(2,1) (0,1) (1,1) (3,1)

20 Transformations Between the Coordinate Systems
Between different systems: Polar coordinates to cartesian coordinates Between two cartesian coordinate systems. For example, relative coordinates or window to viewport transformation.

21 How to transform from x,y to x',y' ?
Superimpose x',y' to x,y Transformation: Translate so that (x0,y0) moves to (0,0) of x,y Rotate x' axis onto x axis y y' x' x x y y' x' x x

22 y Alternate method for rotation: Specify a vector V for positive y' axis: y' x' V x x

23 Elements of any rotation matrix can be expressed as elements of a set of orthogonal unit vectors:

24 Let triangle T be defined as three column vectors:
Example: y' y M T T x x' Let triangle T be defined as three column vectors:

25 Affine Transformations
Coordinate transformations of the form: Translation, rotation, scaling, reflection, shear. Any affine transformation can be expressed as the combination of these. Rotation, translation, reflection: preserve angles, lengths, parallel lines

26 3 DIMENSIONAL TRANSFORMATIONS

27 3D Transformations z x,y,z coordinates. Usual notation: Right handed coordinate system Analogous to 2D we have 4 dimensions in homogenous coordinates. Basic transformations: Translation Rotation Scaling y x y x x z z y

28 Translation move the object to a relative position. y x z y x z

29 Rotation Rotation arround the coordinate axes x axis y axis z axis z x
Counterclockwise when looking along the positive half towards origin

30 Rotation around coordinate axes
Arround x Arround y Arround z

31 Rotation Arround a Parallel Axis
Rotating the object around a line parallel to one of the axes: Translate to axis, rotate, translate back. y y y y x x x x z z z z Translate Rotate Translate back

32 Figure from the textbook

33 Rotation Around an Arbitrary Axis
Translate the object so that the rotation axis passes though the origin Rotate the object so that the rotation axis is aligned with one of the coordinate axes Make the specified rotation Reverse the axis rotation Translate back x z

34 Rotation Around an Arbitrary Axis

35 Rotation Around an Arbitrary Axis
u is the unit vector along V: First step: Translate P1 to origin: Next step: Align u with the z axis we need two rotations: rotate around x axis to get u onto the xz plane, rotate around y axis to get u aligned with z axis.

36 Rotation Around an Arbitrary Axis
Align u with the z axis 1) rotate around x axis to get u into the xz plane, 2) rotate around y axis to get u aligned with the z axis y y y u u u' α α x x x u uz β z z z

37 Dot product and Cross Product
v dot u = vx * ux + vy * uy + vz * uz. That equals also to |v|*|u|*cos(a) if a is the angle between v and u vectors. Dot product is zero if vectors are perpendicular. v x u is a vector that is perpendicular to both vectors you multiply. Its length is |v|*|u|*sin(a), that is an area of parallelogram built on them. If v and u are parallel then the product is the null vector.

38 Rotation Around an Arbitrary Axis
Align u with the z axis 1) rotate around x axis to get u into the xz plane, 2) rotate around y axis to get u aligned with the z axis We need cosine and sine of α for rotation u u' α x uz z Projection of u on yz plane

39 Rotation Around an Arbitrary Axis
Align u with the z axis 1) rotate around x axis to get u into the xz plane, 2) rotate around y axis to get u aligned with the z axis u β x u''= (a,0,d) z

40 Rotation, ... Alternative Method
Any rotation around origin can be represented by 3 orthogonal unit vectors: This matrix can be thought of as rotating the unit r1*, r2*, and r3* vectors onto x, y, and z axes. So, to align a given rotation axis u onto the z axis, we can define an (orthogonal) coordinate system and form this R matrix Define a new coordinate system with the given rotation axis u using:

41 Rotation, ... Alternative Method
Check if this is equal to

42 Scaling Change the coordinates of the object by scaling factors. y x z

43 Scaling with respect to a Fixed Point
Translate to origin, scale, translate back y x y y y x x x z z z z Translate Scale Translate back

44 Scaling with respect to a Fixed Point

45 Reflection Reflection over planes, lines or points y y y y x x x x z z

46 Shear Deform the shape depending on another dimension


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