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Robot Dynamics (1)

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Title: Robot Dynamics (1)


1
ROBOT DYNAMICS
DYNAMIC ANALYSIS AND FORCES
Prof. Charlton S. Inao Defence University Debre
Zeit , Ethiopia
2
Introduction
  • Analysis of forces, torques, inertias, loads, and
    accelerations.
  • Derivation of dynamic equations of motion.
  • Allows determination of important loads for
    design.
  • Assists in the selection of actuators.

3
Newtonian Mechanics
  • Easier for simpler systems.
  • Familiar to users

4
Lagrangian Mechanics
  • Easier for more complicated systems
  • Based on systems energies
  • Systematic
  • Lagrangian is the difference between kinetic and
    potential energies of the system

5
Lagrangian Relationships
  • Lagrangian relationships are

6
Review of Basics
  • Potential energy is energy stored in an object
    due to its position or arrangement.
  • Kinetic energy is energy of an object due to its
    movement - its motion

7
Illustration
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Lagrangian Mechanics
  • Lagrangian field theory is a formalism in
    classical field theory. It is the field-theoretic
    analogue of Lagrangian mechanics
  • Lagrangian mechanics is used for discrete
    particles each with a finite number of degrees of
    freedom. Lagrangian field theory applies to
    continua and fields, which have an infinite
    number of degrees of freedom.
  • Deals with energy.. The difference between
    Kinetic and Potential energy.

10
  • In this chapter, were going to learn about a
    whole new way of looking at things.
  • Consider the system of a mass on the end of a
    spring. We can analyze this, of course, by using
    F ma to write downm mx -kx.
  • The solutions to this equation are sinusoidal
    functions, as we well know.
  • We can, however, ?gure things out by using
    another method which doesnt explicitly use
  • F ma.
  • In many (in fact, probably most) physical
    situations, this new method is far superior to
    using F ma.

11
Lagrangian mechanics
  • Please see examples in the book for the
    application of Lagrangian mechanics. For the
    following system we can derive equations of
    motion as

12
Example 1
13
Kinematics Solution
Wangular velocity of the wheel 2rdiameter X
dot linear velocity
14
Dynamics Solution
15
Notes
16
Notes
velocity
distance
17
Example 2
Newtonian mechanics VS Lagrangian mechanics
18
Solution
a) Lagrangian Mechanics
19
b) Newtonian Mechanics
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Example 3
22
Solution 3
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a) KEKE cart KE pendulum
1
24
b) PEPE spring PE pendulum
Pendulum
Spring
25
b.1) PE pendulum
26
LK-P
27
Solution 3 continued
28
Review/Reference
29
Solution 3 continued
30
Example 4 (For home study or work out exercise)
31
Solution 4
32
Solution 4 contd..
33
Solution 4 contd..
34
Solution 4 contd..
35
Solution 4 contd..
36
Taking the derivatives of the Langrangian and
substituting into Equation 4.4 yields to the ffg.
Equation of Motion
37
Equation of motion in Matrix Form
Solution 4 contd..
38
Example 5 (Class Discussion)
39
Solution 5
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Solution 5 .. In matrix form
42
DETAILED SOLUTION No. 5
Solve for Kinetic Energy for each link
Solve for K1
43
RECALL
44
Reference Moment of InertiaThin rod about axis
through end perpendicular to length
45
Solve for the X and Y component of M2
Horizontal component up to point m2
vertical component up to point m2
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Comcenter of mass
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Differentiate XD and YD to get the velocity and
the velocity of the arm distance up to point m2
U r
Vcos?
U V

Recall
50
Calculate the VD ,up to Mass2and square it, for
linear an d angular component of momentum
expression, V2D
51
Solve for K2
K1
K2
52
Solve for K2
Angular momentum
linear momentum
Recall
53
Solve for Lagrangian,L K-P
54
Differentiation with respect to time, in terms of
both variables, i. e. r,?
1st
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Differentiation of L with respect to ?
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Solve for Lagrangian, K-P
59
Detailed calculation for VD2
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  • THE END
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