2.2. dynamics of rigid bodies - ux.uis.nohirpa/dms6021/2017/2.2 dynamics of rigid bodies.pdf ·...

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Dynamics and control of mechanical systemsDate ContentDay 1(01/08)

• Review of the basics of mechanics. • Kinematics of rigid bodies - coordinate transformation, angular velocity

vector, description of velocity and acceleration in relatively moving frames. Day 2(03/08)

§ Euler angles, Review of methods of momentum and angular momentum of system of particles, inertia tensor of rigid body.

• Dynamics of rigid bodies - Euler equations, application to motion of symmetric tops and gyroscopes and problems of system of bodies.

Day 3(05/08)

• Kinetic energy of a rigid body, virtual displacement and classification of constraints.

• D’ Alembert’s principle. Day 4(07/08)

• Introduction to generalized coordinates, derivation of Lagrange's equation from D’ Alembert’s principle.

• Small oscillations, matrix formulation, Eigen value problem and numerical solutions.

Day 5(09/08)

• Modelling mechanical systems, Introduction to MATLAB®, computer generation and solution of equations of motion.

• Introduction to complex analytic functions, Laplace and Fourier transform.Day 6(11/08)

• PID controllers, Phase lag and Phase lead compensation. • Analysis of Control systems in state space, pole placement, computer

simulation through MATLAB.

DMS6021 - Dynamics and Control of Mechanical Systems

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ContentPurpose:

Focus on4 Preview of dynamics of rigid bodies4 Euler equations,4 Application to motion of symmetric tops and

gyroscopes and problems of system of bodies.


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IntroductionThe dynamics of rigid bodies can be analyzed as4 Rotation about a fixed point*

OR4 General 3D motion (about center of mass of the body)


å

å

=

W+=

=

)(fixed)body (not coordinate

secondary aabout rotating If

iiiO

OO

OO

rxmxrwhere

xdtddtd

wH

HH

HM

å

å

=

W+=

=

)( iii RxmxRwhere

xdtddtd

wH

HH

HM

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Dynamics of rigid body4 For a moving coordinate system x-y-z with angular

velocity Ω, the moment relation becomes:


( )( ) !"#$$$ !$$$ "#

%%%

%

HH

HHHH

HHM

ofdirectioninChange

ofmagnitudeinChange

zyx

xyz

xkji

x

W+++=

W+=å

where

Show that this is correct!

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Dynamics of rigid body4 For reference axes attached to the body, moments and

products of inertia will become invariant with time, 4 And Ω = ω

4 In general (rotation about a fixed axis)


( ) ( ) torqueappliedexternalMxCCaxis

bodyCaxisfixedCC

=+== åå ;HHHM w!!

( )( )( )( )k

ji

H

33

22

11

)(

wwww

w

!

!

!!

!

IIIIdtId

axisbodyC

++==

÷øö

çèæ=

( )( )( )( )( )( )k

jiH

2121

1313

3232

IIIIIIx

------=

wwwwwww

( )( )( )

EquationssEulerMIIIMIIIMIII

z

y

x

'

212133

131322

323211

ïþ

ïý

ü

=--

=--=--

www

wwwwww

!

!

!

Ang. velocity of rotating frame attached to body

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Euler’s Equations


4 For a reference axes coinciding with the principal axesof inertia

The origin can be either at the mass center (C) or at a point Ofixed to the body and fixed in spaceThe products of inertia: Ixy = Iyz = Ixz = 0Thus, the moment equation becomes

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Dynamics of rigid body4 When no external torque is applied on a rigid body,

angular momentum is conserved

Where the subscripts are simplified as follows: xx = 1, yy = 2 and zz = 3

The Euler equations for this case (principal axis, noexternal torque)*


[ ] [ ]TT IIIHHHIwheredtd

3322113210 wwww =Þ== HH

( )( )( )212133

131322

323211

IIIIIIIII

-=-=-=

wwwwwwwww

!

!

! Show that these are correct!

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Dynamics of rigid body… Euler Equations4 Euler’s equations are the 3D equations of motion for a rigid

body - used to analyze the motion of a rigid body4 Using the three components of Newton’s 2nd law and Euler

equations, motion of a rigid body in 3D is completely defined


4 Three steps of rigid body analysis using Euler equations:1. Choose a coordinate system (that rotates about a fixed point O or

that has its origin at the center of mass)2. Draw the free body diagram3. Apply the equations of motion (Newton’s second law and equations

of angular motion)

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Dynamics of rigid body… Euler Equations4 Please read and try to understand about (Not pensum)Application of the relations of rigid body motion to

motion of symmetric tops andgyroscopes


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Summary and Questions


Next: Kinetic energy of a rigid body, virtual displacement and classification of constraints

4 Considered dynamics of rigid bodyRotation about a fixed axisRotation about the center of massMoment equation for a moving coordinate system

4 Derived Euler´s Equations formotion with moving coordinate systema coordinate system attached to the rotating bodycases when no external torque is applied andcases when the axis of rotation coincides with axis principal axes ofinertia

?

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Exercise 14 A small particle of mass m and its restraining cord are spinning with an

angular velocity ω on the horizontal surface of a smooth disk, shown in section view below. As the force Fs is slowly increased, r decreases and ω changes. Initially, the mass is spinning with ω0 and r0.

Determine: i) an expression for ω as a function of r, and ii) the work done on the particle by Fs between r0 and an arbitrary r.

Verify the principle of work and energy.


Solution

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Exercise 24 A pendulum consisting of a mass, M, is suspended by a rigid rod of

length L. The pendulum is initially at rest and the mass of the rod can be neglected. A bullet of mass m and velocity v0 impacts M and stays embedded in it. The angle that the velocity vector v0 forms with the horizontal is α.

Find out the angle θmax reached by the pendulum.


Solution

2.2. dynamics of rigid bodies - ux.uis.nohirpa/dms6021/2017/2.2 dynamics of rigid bodies.pdf ·...

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