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FUNDAMENTALS OF VIBRATION
BY:- SHUBHAM CHAURASIYA
(DEPARTMENT OF MECHANICAL
ENGINEERING PUNJAB UNIVERSITY)
BASIC CONCEPTS OF VIBRATION?
 Vibration is a mechanical phenomena whereby
oscillation occur about an equilibrium point
 All bodies having mass and elasticity are capable of
producing vibration
 The mass is inherent of the body and elasticity
causes relative motion among its parts
 When body particles are displaced by the
application of external force the internal forces in
the form of elastic energy are present in the body
 In this way, vibratory motion is repeated indefinitely
and exchange of energy takes place
SOME BASIC DEFINITIONS
FREE AND ITS SUB TYPES
FREE VIBRATION:-
In Free vibration, the object is not under the influence of any
kind of outside force.
a)Longitudinal vibration: when the particles of the body move
parallel to the axis of the body, the vibration is known as
longitudinal vibration.
b)Transverse vibration: hen the particles of the body move
nearly perpendicular to the axis of the body, the vibration is
known as transverse vibration.
c)Torsional vibration: When the particles of the body move in
a circle about the axis of the body, the vibration is known as
torsional vibration.
LONGITUDINAL
VIBRATION
TRANSVERSE
VIBRATION
TORSIONAL
VIBRATION
FORCED VIBRATION
When a periodic disturbing force keeps the body in
vibration through out its entire period of motion,
such vibration is said to be a forced vibration. The
frequency of vibration of the body is same as the
frequency of the applied force.
DAMPED VIBRATION
 If the vibratory system has a damper the motion of
the system will be dissipated in friction.this type of
vibration is called damped vibration
UNDAMPED VIBRATION
 On the contrary,the system no damper is known as
undamped vibration
LINEAR AND NON-LINEAR VIBRATION
 If in a vibratory system mass,spring and damper
behave in a linear manner,the vibrations caused are
known as linear in nature.Linear vibrations are
governed by linear differential equations.They
follow the law of superposition.Mathematically if a1
and a2 are solution of 1 &2 then a1+a2 is solution
of 3 1
2
3
On the other hand if the amplitude of vibration is very high it
Becomes non linear in nature
RESONANCE
 When the frequency of external excitation is equal
to the natural frequency of a vibrating body,the
amplitude of a vibration becomes excessively
large.This concept is known as resonance
CONTINUOUS SYSTEM
 Most of the mechanical system include elastic
members which have infinite no. Of degree of
freedom are called continuous system
cantilever beam a typical example of continuous system
DISCRETE SYS
 System with finite number of degree of freedom are
called discrete or lumped system
System with
1 degree of freedom
System with 2 degree of freedom
SHM(SIMPLE HARMONIC MOTION)
SHM
SHM CONTINUED.....
SHM CONTINUED.....
ADDITION OF SHM
FOURIER SERIES
 J.Fourier, a French mathematician, developed this
 It is a periodic function in terms of series of sines
and cosines
 With the help of this series vibration results
obtained experimentally can be analysed
analytically
MATHEMATICAL FORM OF FOURIER
SERIES

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Fundamentals of vibration

  • 1. FUNDAMENTALS OF VIBRATION BY:- SHUBHAM CHAURASIYA (DEPARTMENT OF MECHANICAL ENGINEERING PUNJAB UNIVERSITY)
  • 2. BASIC CONCEPTS OF VIBRATION?  Vibration is a mechanical phenomena whereby oscillation occur about an equilibrium point  All bodies having mass and elasticity are capable of producing vibration  The mass is inherent of the body and elasticity causes relative motion among its parts  When body particles are displaced by the application of external force the internal forces in the form of elastic energy are present in the body  In this way, vibratory motion is repeated indefinitely and exchange of energy takes place
  • 4. FREE AND ITS SUB TYPES FREE VIBRATION:- In Free vibration, the object is not under the influence of any kind of outside force. a)Longitudinal vibration: when the particles of the body move parallel to the axis of the body, the vibration is known as longitudinal vibration. b)Transverse vibration: hen the particles of the body move nearly perpendicular to the axis of the body, the vibration is known as transverse vibration. c)Torsional vibration: When the particles of the body move in a circle about the axis of the body, the vibration is known as torsional vibration.
  • 6. FORCED VIBRATION When a periodic disturbing force keeps the body in vibration through out its entire period of motion, such vibration is said to be a forced vibration. The frequency of vibration of the body is same as the frequency of the applied force.
  • 7. DAMPED VIBRATION  If the vibratory system has a damper the motion of the system will be dissipated in friction.this type of vibration is called damped vibration
  • 8. UNDAMPED VIBRATION  On the contrary,the system no damper is known as undamped vibration
  • 9. LINEAR AND NON-LINEAR VIBRATION  If in a vibratory system mass,spring and damper behave in a linear manner,the vibrations caused are known as linear in nature.Linear vibrations are governed by linear differential equations.They follow the law of superposition.Mathematically if a1 and a2 are solution of 1 &2 then a1+a2 is solution of 3 1 2 3 On the other hand if the amplitude of vibration is very high it Becomes non linear in nature
  • 10. RESONANCE  When the frequency of external excitation is equal to the natural frequency of a vibrating body,the amplitude of a vibration becomes excessively large.This concept is known as resonance
  • 11. CONTINUOUS SYSTEM  Most of the mechanical system include elastic members which have infinite no. Of degree of freedom are called continuous system cantilever beam a typical example of continuous system
  • 12. DISCRETE SYS  System with finite number of degree of freedom are called discrete or lumped system System with 1 degree of freedom System with 2 degree of freedom
  • 14. SHM
  • 18. FOURIER SERIES  J.Fourier, a French mathematician, developed this  It is a periodic function in terms of series of sines and cosines  With the help of this series vibration results obtained experimentally can be analysed analytically
  • 19. MATHEMATICAL FORM OF FOURIER SERIES