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24
1 Damped Vibration Topics: Introduction to Damped Vibration Damping Models Viscous Damping Energy Dissipation Damping Parameters Structural Damping Coulomb Damping Solution of Equations of Motion Logarithmic Decrement Practical Applications

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Page 1: Damped Vibration - WPMU DEV

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Damped VibrationTopics:• Introduction to Damped Vibration• Damping Models• Viscous Damping• Energy Dissipation• Damping Parameters• Structural Damping• Coulomb Damping• Solution of Equations of Motion• Logarithmic Decrement• Practical Applications

Page 2: Damped Vibration - WPMU DEV

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1. Vibrating systems can encounter damping in various ways like

• Intermolecular friction

• Sliding friction

• Fluid resistance

2. Damping estimation of any system is the most difficult process in any vibration analysis

3. The damping is generally complex and generally for mechanical systems it is so small to compute

Fluid resistant damper

x

Introduction Damped Vibrations

Page 3: Damped Vibration - WPMU DEV

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Structural

Coulomb

Viscous

Inherent Intermolecular friction

Rubbing between surfaces

Fluid friction (viscosity)

Damping Models

Cause of Damping

StructuralDamping

CoulombDamping

ViscousDamping

Page 4: Damped Vibration - WPMU DEV

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Damped VibrationTopics:• Introduction to Damped Vibration• Damping Models• Viscous Damping• Energy Dissipation• Damping Parameters• Structural Damping• Coulomb Damping• Solution of Equations of Motion• Logarithmic Decrement• Practical Applications

Page 5: Damped Vibration - WPMU DEV

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Occurs when system vibrates in a viscous medium

Obeys Newton's law of viscosity

The damping force is given by

dvdz

τ μ=

For the given viscous dashpot..

c – damping constant

Viscous Damping

Page 6: Damped Vibration - WPMU DEV

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Energy dissipation in case of of damping is extremely important because it gives the configuration of the damper

Damping energy dissipated in viscous damping

2dW cwXπ=Which comes out to be

So if we have any system and if we can calculate the energy dissipated by the system

The system can be modeled by the

equivalent viscous damping as 2dnv

eqWC

Xπω=

dW cxdx= ∫ &

Wdnv is the energy dissipated due to non viscous damping

X – amplitude of vibration

Energy Dissipation

Page 7: Damped Vibration - WPMU DEV

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Damped VibrationTopics:• Introduction to Damped Vibration• Damping Models• Viscous Damping• Energy Dissipation• Damping Parameters• Structural Damping• Coulomb Damping• Solution of Equations of Motion• Logarithmic Decrement• Practical Applications

Page 8: Damped Vibration - WPMU DEV

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dWV

β =

2dW cwV k

ηπ

= =

Specific damping capacity

Loss coefficient

The damping properties of the system can be compared using parameters like β and η

Specific damping capacity: Ratio of Energy loss per cycle to the max PE of system

Loss coefficient: Ratio of energy loss per radian to max PE of system

Hence using parameters like β and η we can compare two systems for which we don’t know the value of c

Damping parameters

Page 9: Damped Vibration - WPMU DEV

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Energy dissipation due to Inter Molecular Friction comes under structural damping category

Here energy dissipated is 2dW Xα=

eqCwαπ

=Hence equivalent damping is

α Constant

kαπ

Γ =Structural damping loss coefficient is given by

Structural Damping

Page 10: Damped Vibration - WPMU DEV

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Equation of motion for coulomb damping is

N Kμ = ΔAlso

Opposite sign to be used for + and – ve velocity

Free body diagram

Coulomb Damping

Page 11: Damped Vibration - WPMU DEV

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Solution is given by

The decrease of is very important is important characteristics of coulomb damping

For initial condition of xo displacement and zero input velocity

Coulomb Damping

Page 12: Damped Vibration - WPMU DEV

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Damped VibrationTopics:• Introduction to Damped Vibration• Damping Models• Viscous Damping• Energy Dissipation• Damping Parameters• Structural Damping• Coulomb Damping• Solution of Equations of Motion• Logarithmic Decrement• Practical Applications

Page 13: Damped Vibration - WPMU DEV

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Now let us know how the solution of the equations of motion are effected by the introduction of damping parameters.

The generalized equation of motion is 0Mx cx kx+ + =&& &

The viscous damping is more common or in other terms equivalent viscous damping is more commonly used in place.

Hence using that in the analysis…

Solution of Equations of Motion

Page 14: Damped Vibration - WPMU DEV

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SDF viscous damping solutions

Damped SDF and free body diagram

The eqn of motion is given by

x(t)

A particular solution is given by

Hence

Solution of Equations of Motion

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A general solution is given by

To make the solution more general the critical damping coefficient is defined as

which gives the criteria for various damping properties

So the solution now becomes in terms of asξ

This gives rise to four cases as discussed next

c

cc

ξ =where

The two roots of the above equation are given by

Solution of Equations of Motion

Page 16: Damped Vibration - WPMU DEV

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1. Under damped

2. Undamped

3. Over damped

4. Critically damped

ξξξ <1

=0

>1

=1ξOver damped

The general solution becomes

The solution will be non oscillatory and gradually comes to rest

Type of System depends on Damping Factor

Solution of Equations of Motion

Page 17: Damped Vibration - WPMU DEV

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Critically damped

The general solution becomes

For zero initial conditions

Solution of Equations of Motion

Door Damper

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Under damped

The general solution becomes

The damped time period is given by

2

21

dTp

πξ

=−

The envelope for the under damped curve is given by as shownnte ξω−

Solution of Equations of Motion

Page 19: Damped Vibration - WPMU DEV

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Damped VibrationTopics:• Introduction to Damped Vibration• Damping Models• Viscous Damping• Energy Dissipation• Damping Parameters• Structural Damping• Coulomb Damping• Solution of Equations of Motion• Logarithmic Decrement• Practical Applications

Page 20: Damped Vibration - WPMU DEV

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The logarithmic decrement is the Natural log of Ratio of the Successive Drops in the Amplitude

It is used for the estimation of the value of of the system experimentally

ξ

For two points

Since the outer envelope is an exponential curve

Logarithmic Decrement

Page 21: Damped Vibration - WPMU DEV

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Logarithmic decrement is given by

That is

2

21πξδξ

=−

01 lnn

Xn X

δ =

Which gives

If we consider the drop in amplitude in n successive cycles then the log decrement is given by

Logarithmic Decrement

Page 22: Damped Vibration - WPMU DEV

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Viscous dampers:

Various types of viscous dampers are shown

Practical Applications

Gun BarrelDoor Damper

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Assignment

1

2

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Assignment

A machine of mass 2000kg mounted on isolators has a frequency of 8Hz. Loss modulus of the isolator in shear is found to be a function of the isolator strain amplitude. What will be the ratio of successive amplitudes in a free vibration rap test when peak to peak isolator strain amplitude is a) 0.001 and b) 0.05.

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