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Matrix Methods in Kinematics

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Presentation on theme: "Matrix Methods in Kinematics"— Presentation transcript:

1 Matrix Methods in Kinematics
Vector Methods with Matrix Notation Rigid Body Rotation Matrices Rigid Body – points have same relative position Displacement = Rotation and Translation Angular rotations described about 1. Right hand Cartesian axes (x,y,z) 2. Arbitrary Axis 3. Euler Angles

2 Matrix Methods in Kinematics
Holonomic Systems Holonomic Constraints Relations between co-ordinates and possibly time) Rigid body xyz displacement is not order dependent

3 Matrix Methods in Kinematics
Rigid body rotations Rotations not commutative (order dependent)

4 Matrix Methods in Kinematics
1. Rotate about Z (α) Components in the fixed system x-y Rotation matrix

5 Matrix Methods in Kinematics
Rotation about three Cartesian axes y x z X,Y,Z axes fixed in space

6 Matrix Methods in Kinematics
Plane rotation (2D) (rotation about z) Spatial Rotation – sequence z,y,x

7 Matrix Methods in Kinematics

8 Matrix Methods in Kinematics
y u 2. Rotation about axis u (φ) Decompose to rotations about x, y, z Rotate u about z and then back again +/- show directions x z

9 Matrix Methods in Kinematics
y x z u

10 Matrix Methods in Kinematics

11 Matrix Methods in Kinematics
3. Euler Angles Displacement of a rigid body in terms of three relative displacement angles Each rotation about an axis whose location depends on preceding rotation 1 2 3 4 sets of axes initially coincident xyz fixed in the body

12 Matrix Methods in Kinematics

13 Matrix Methods in Kinematics

14 Matrix Methods in Kinematics
12 different possible rotation sets z-x-z x-y-x y-z-y z-y-z x-z-x y-x-y x-y-z y-z-x z-x-y x-z-y z-y-x y-x-z

15 Matrix Methods in Kinematics

16 Matrix Methods in Kinematics

17 Matrix Methods in Kinematics
Euler Angles Angular Velocity Vectors 3 1 Rigid body 3 1 2 2

18 Matrix Methods in Kinematics
Rotation of Rigid Body in 2d Cartesian Space p1 q1 Fixed x-y Vector form

19 Matrix Methods in Kinematics
2 1

20 Matrix Methods in Kinematics
3x3 D = plane displacement matrix

21 Matrix Methods in Kinematics
Spatial (3D) Rigid Body Displacement Replace Cartesian u Axis Euler Using Cartesian new original 4x4 matrix (3D)

22 Matrix Methods in Kinematics
Screw displacement matrix y q u q1 p=p1+su s p1 z x Screw displacement matrix

23 Matrix Methods in Kinematics
12 non constant elements 3D space= 6 DOF, 6 elements are dependent To Define D: euler angles, dir cos, points on body, etc…

24 Matrix Methods in Kinematics
Example Displacement of a point Moving with a rigid body

25 Matrix Methods in Kinematics
3x3 Displacement matrix

26 Matrix Methods in Kinematics
Finite Rotation Pole – plane rotation about p0 po With new position vectors p1=p2=p0

27 Original displacement matrix
Matrix Methods in Kinematics Previously p1 and p2 in Displacement matrix D now written as: q2 is the same point Original displacement matrix

28 Matrix Methods in Kinematics

29 Matrix Methods in Kinematics
HW #5 Salute Y X q shoulder 30◦ p Z p1=elbow q1=tip of finger Use Cartesian angles to find [D] Treat as 3 independent rotations

30 Matrix Methods in Kinematics
HW #5 Salute Y Y Changed axes notation X X shoulder 2 Z p 1 Z q p1=elbow move origins for 2,3 rotations Y q1=tip of finger X 30◦ z-y-z rotation 3 Z

31 Matrix Methods in Kinematics
Finding the Displacement Matrix by Inversion y B1 Known points C1 C2 A1 A2 B2 x

32 Matrix Methods in Kinematics
Displacement Matrix by Inversion

33 Matrix Methods in Kinematics
q q1 d a x y 2D Planar motion z D=d*a-1

34 Matrix Methods in Kinematics
Finding the inverse of A (by hand – the long way) adj - adjoint ith row=ith column α=co factor Mij= minor of A

35 Matrix Methods in Kinematics
Using MATLAB inv(a) ans = d = a = D=d*a-1 Displacement matrix

36 Matrix Methods in Kinematics
HW 5 by Inversion Using My arm

37 Matrix Methods in Kinematics
By Inverse method – position D =

38 Matrix Methods in Kinematics
By Inverse method – position

39 Matrix Methods in Kinematics


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