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Mechanical Vibrations-1 PDF

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The key takeaways are about modeling vibration systems using different elements like springs, masses and dampers and discussing different types of vibration systems and damping.

Discrete and continuous systems are discussed as well as single, two and infinite degree of freedom systems.

Viscous, dry friction, hysteretic and structural damping are discussed.

Jiraphon Srisertpol, Ph.

D
School of Mechanical Engineering

Recommended reading :

...  : !"#, Pearson Education
Indochina 2545

Singiresu S.Rao : Mechanical Vibration (Fourth Edition) ,Prentice Hall
2004. SI Edition

Leonard Meirovitch : Fundamentals of Vibrations , Mc-Graw Hill 2001.

Kelly S. Graham : Fundamentals of Mechanical Vibrations,
Mc-Graw Hill 2000.

Introduction to Vibration and The


Free Response





The Spring-Mass model


Single degree of freedom
Simple harmonic motion
Relationship between Displacement, Velocity
and Acceleration
Representations of harmonic motion

School of Mechanical Engineering

The Vibration of a Fixed-Fixed String

School of Mechanical Engineering

The main mass and dynamic absorber at three


frequencies.

Vibration Characteristics of a
Spring

Fundamental Torsional Mode of a


Valve Support Stand

Deflected Elastomer Shock


Isolation

Structural Vibration

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!"#$%&')*+,!)-.&'%&')/0.$1'2*))





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 ! "" #$% &'()*+#+
,)-.."""  .
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#BCDEFGHI (Degree of Freedom, DOF) - LF


M(Coordinate) !OPQ!OR!OSGTCUDTVU"LHIP"WP
BQXYT"T"Z C"!RTFWBB!OC[HF#YU"

Single degree of freedom system

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14

Three degree of freedom system

Two degree of freedom system

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Infinite number of degree of freedom


system


  


Discrete System (Lumped System)-""*'#/



$(#(//+
'/ " 2*' /#
Continuous System (Distributed System)- ""* *
'/ " 2)-
(' /

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  (Free Vibration)

 









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 ."" (Free Vibration)


 ."""  " (Forced Vibration)
 .""(*# (Undamped Vibration)
 .""*# (Damped Vibration)
 ."", (Linear Vibration)
 .""(, (Nonlinear Vibration)
 .""'#/(/ (Deterministic Vibration)
 ."" (Random Vibration)

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$ ""
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+*//
 2. $'#/ 2.
   2/'
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20

XBBSGTGOEFGYTF"
(Undamped Vibration)

XBBB"EB (Forced Vibration)




$ ""3+.'3+ &.'3+*2


)-.
&2'#$(&2' 4(/
 
*2 ,  $(/
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#
*
.""*2()   "*5,""  *2*

**, (amplitude)  *  *+ 


*2
   (Resonance)




#+ *(*1*+
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).*+/ #$.$/
$""
$*.""(*#'#
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$**2**
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 .""*""*+
*5, (Natural Frequency)

21

22

    (Linear Vibration)

XBBGOEFGYTF" (Damped Vibration)




#+  ** 1*+


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23

"" &)"/+ 
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(Principle of Superposition)

24

XBBSGTHIH"HP (Nonlinear Vibration)




XBBYSP (Deterministic Vibration)

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25

CDFHEY!"FFG
(Vibration Analysis Procedure)

XBBRTG (Random Vibration)




26

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/4 .*'""('#//
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27

.""'
 6 (Mathematical Modeling)
#
$* (Derivation of Governing Equations)
#8
9
+
$* (Solution of Governing Equations)
#68
*(/ (Interpretation of the Results)

28

P"XBBL#"!"E[
(Mathematical Modeling)






YGHE#`!O
(Derivation of Governing Equations)

:"$2""*/  %/+.**
/+.""'
+3 ,
..#

 +6 .""""/+)(spring )
.*'#/1*+
/+ #(damped)
.*)-.#


6 /+ 
(mass) , 9$+





. 56
)
*+)
)
& (Laplace)s transform)
5*, 
 (Numerical method)

Dynamic System Modeling and Analysis, Hung V Vu and Ramin S. Esfandiari,


McGraw-Hill 1998

29

30

FHEYb#!OSP
(Interpretation of the Results)

Yb#Hc#QGHE#`!O
(Solution of Governing Equations)

.
$* "" ".""'
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5"+.
)8

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+
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Mathematical Model of
Motorcycle

Vibration Analysis Procedure

."'
*+*/

Single-degree of freedom model *./) b.

keq {kt , kr , ks } equivalentstiffness.


ceq {cs , cr } equivalentdamping constant.
meq {mr , mv , mw } equivalent mass
r rider ,t tires, s struts , v vehicle body, w wheels,

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Mathematical Model of
Motorcycle

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Mathematical Model of
Motorcycle

r rider ,t tires, s struts ,v vehicle body, w wheels,

r rider ,t tires, s struts ,v vehicle body, w wheels,

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36

Mathematical Model of
Motorcycle

    !"# $


Springs Elements
 Mass or Inertia Elements
 Damping Elements


r rider ,t tires, s struts ,v vehicle body, w wheels,

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Spring Elements







Stiffness (N/m)
Youngs modulus (N/m)
Density (kg/m)
Shear modulus G(N/m)
Springs in series
Springs in parallel

).) 6/ ""**/#+*, $



 +6""
Spring force

F = kx

k spring contant or spring stiffness


x displacement(deformation)

Potential energy in the spring :

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U=

1 2
kx
2

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Springs in Parallel

Springs in Series
1. Static of the system ( st )

Equilibrium equation

W = k1 st + k 2 st

st = 1 + 2

2. Equilibrium equation W = k11

W = keq st

W = k2 2

where keq = k1 + k 2

3. keq for the same static deflection

W = keq st

k11 = k 2 2 = keq st
or

Equivalent spring constant (keq ) in parallel

Equivalent spring constant (keq ) in series

keq = k1 + k 2 + k3 + + k n

1
1 1 1
1
= + + ++
keq k1 k 2 k3
kn

1 =

that is,

keq st
k1

, 2 =

keq st
k2

1
1 1
= +
keq k1 k 2

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Damping Elements

EX: Springs in Parallel

shear modulus G = 80 109 N m 2

mean coil diameter D = 20 cm


wire diameter d = 2 cm


The stiffness of helical spring is given by

 #$#$/ (Viscous Damping)


 #$.*+/#.4 ".4 (Dry
Friction or Coulomb Damping)
 #$(+/$ #+ / (Hysteretic Damping or
Structural Damping)

d 4G (0.02 ) 80 109
=
40,000 N m
k=
3
8D 3n
8(0.2 ) 5
4

The equivalent spring constant of the suspension system is given by

keq = 3k = 3 40,000 = 120,000 N m


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Viscous Damping

Damping

All real systems dissipate energy when they vibrate. To


account for this we must consider damping. The most simple
form of damping (from a mathematical point of view) is called
viscous damping. A viscous damper (or dashpot) produces a
force that is proportional to velocity.
Mostly a mathematically motivated form, allowing
a solution to the resulting equations of motion that predicts
reasonable (observed) amounts of energy dissipation.

Damper (c)
x

f c = cv(t ) = cx (t )

fc
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Viscous Damping


Equivalentdampingconstant (ceq ) in series

1 1 1
1
= + +
ceq c1 c2
cn




Damper
Damping coefficient
Critical damping coefficient
Damping ratio

Equivalentdampingconstant (ceq ) in parallel


ceq = c1 + c2 + + c3

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Ex: Horizontal milling machine






Underdamped Motion
Overdamped Motion
Critically Damped Motion

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Ex: Horizontal milling machine

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Ex: Horizontal milling machine


Fs = keq x

Fsi = ki x ; i = 1,2,3,4
Fdi = ci x ; i = 1,2,3,4

Fd = ceq x

Fs = Fs1 + Fs 2 + Fs 3 + Fs 4
Fd = Fd1 + Fd 2 + Fd 3 + Fd 4

where

keq = k1 + k2 + k3 + k4
ceq = c1 + c2 + c3 + c4

Fs + Fd = W total vertical force

G center of mass , Fsi forces acting on the springs , Fdi forces acting on the dampers
Fs forces acting on all the springs , Fd forces acting on all the dampers

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Newtons second law


Conservation of Energy
Potential Energy
Kinetic Energy
Natural frequency

53

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