Title: Robot Dynamics (1)
1ROBOT DYNAMICS
DYNAMIC ANALYSIS AND FORCES
Prof. Charlton S. Inao Defence University Debre
Zeit , Ethiopia
2Introduction
- 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.
3Newtonian Mechanics
- Easier for simpler systems.
- Familiar to users
4Lagrangian Mechanics
- Easier for more complicated systems
- Based on systems energies
- Systematic
- Lagrangian is the difference between kinetic and
potential energies of the system
5Lagrangian Relationships
- Lagrangian relationships are
6Review 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
7Illustration
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9Lagrangian 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.
11Lagrangian mechanics
- Please see examples in the book for the
application of Lagrangian mechanics. For the
following system we can derive equations of
motion as
12Example 1
13Kinematics Solution
Wangular velocity of the wheel 2rdiameter X
dot linear velocity
14Dynamics Solution
15Notes
16Notes
velocity
distance
17Example 2
Newtonian mechanics VS Lagrangian mechanics
18Solution
a) Lagrangian Mechanics
19b) Newtonian Mechanics
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21Example 3
22Solution 3
23a) KEKE cart KE pendulum
1
24b) PEPE spring PE pendulum
Pendulum
Spring
25b.1) PE pendulum
26LK-P
27Solution 3 continued
28Review/Reference
29Solution 3 continued
30Example 4 (For home study or work out exercise)
31Solution 4
32Solution 4 contd..
33Solution 4 contd..
34Solution 4 contd..
35Solution 4 contd..
36Taking the derivatives of the Langrangian and
substituting into Equation 4.4 yields to the ffg.
Equation of Motion
37Equation of motion in Matrix Form
Solution 4 contd..
38Example 5 (Class Discussion)
39Solution 5
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41Solution 5 .. In matrix form
42DETAILED SOLUTION No. 5
Solve for Kinetic Energy for each link
Solve for K1
43RECALL
44Reference Moment of InertiaThin rod about axis
through end perpendicular to length
45Solve for the X and Y component of M2
Horizontal component up to point m2
vertical component up to point m2
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47Comcenter of mass
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49Differentiate XD and YD to get the velocity and
the velocity of the arm distance up to point m2
U r
Vcos?
U V
Recall
50Calculate the VD ,up to Mass2and square it, for
linear an d angular component of momentum
expression, V2D
51Solve for K2
K1
K2
52Solve for K2
Angular momentum
linear momentum
Recall
53Solve for Lagrangian,L K-P
54Differentiation with respect to time, in terms of
both variables, i. e. r,?
1st
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56Differentiation of L with respect to ?
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58Solve for Lagrangian, K-P
59Detailed calculation for VD2
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