Control of Vibration
Control of vibration or vibration suppression is possible using various passive and active methods
Passive action is independent of the resulting vibration – Open Loop System.
Active method is dependent on the resulting vibration – Closed Loop System.
Various Active and Passive Control Strategies
Reduction of excitation at the source
Examples:
Source provides the energy to maintain vibration. sources of vibration could be of several types:
Transient – for e.g. shock loading
Forced excitation – Source (continuous) independent of Response
Self-excited – Source generated by the Response for e.g. vortex induced vibration.
Parametric excitation – System parameters (m,c or k ) change with respect to time.
(ii) Isolation of the source
Modify the transmission path of vibration between source and the system to protect the system.
Example - Insertion of resilient elements – Springs, Dampers, Viscoelastic Materials, Pneumatic
Suspension etc. between the source and the system.
Very often vibration isolators are developed using a combination of springs and dampers. For example, viscoelastic materials are bonded to metal fasteners and used as anti-vibration mounts or isolators. The construction of a typical bonded rubber spring for use under compressive loading is shown below.
(iii) System modification
A large number of methods exist in this group including detuning, decoupling, using additive damping treatments ( constrained and unconstrained ), stiffeners and massive blocks (as foundation)
Consider the motion of the following single degree of freedom (SDOF) system:
Stiffness controlled
(II) Near resonance, the vibration is
Damping Controlled
(III) Aat high frequency, the vibration is
Inertia Controlled
Redesign of a Vibrating System
Redesign of a vibrating system involves modelling of materials - generally
For metals and alloys:
Stiffness is a function of elastic moduli ( E, G, K ) and the geometric dimensions depending on the type of loading and deformation (bending, twisting etc.) Damping and Loss Factor are generally constant.
Inertia depends on Density and Geometry.
Viscoelastic Materials
Viscoelastic materials: butyl rubber, plasticized polyvinyl acetate, silicon rubber, polyurethane, thiokol RD etc. S
tiffness and Damping properties for viscoelastic materials are frequency and temperature dependent due to transition from Glassy to Rubbery Phase.
Thiokol RD:
The loss factor is 2 corresponding to a critical frequency of 7 Hz at 50C and around 800 Hz at 200C.
Viscoelastic Materials
A qualitative plot of loss coefficient vs, Young's modulus for different classes of materials is shown here for comparison.
(iv) Use of Additive Layers
This involves addition of a secondary vibratory system to the original (primary) vibratory system which is under excitation. Some secondary systems are vibration neutralizer, vibration absorber, tuned, selftuned, impact absorbers. This strategy has been successfully used for suppressing vibration in very small to very large systems.
Examples: electric hair clippers, DC-9 aircraft, tractors, foot bridges, pipelines etc. Viscoelastic materials are used as additive damping treatments: constrained and unconstrained layers
Extensional and shear deformation of the damping layer
Steps in Vibration Control: A. Identification and characterization of the source of vibration. B. Specify the level to which the vibration should be reduced. C. Select the method appropriate for realizing the vibration reduction level identified in step B. D. Prepare an analytical design based on the method chosen in step C. E. Realize in practice (i.e. hardware mechanization of) the analytical design constructed in step D.
Often spacers are designed to enhance extensional damping
Steps in Vibration Control:
A. Identification and characterization of the source of vibration.
B. Specify the level to which the vibration should be reduced.
C. Select the method appropriate for realizing the vibration reduction level identified in step B.
D. Prepare an analytical design based on the method chosen in step C.
E. Realize in practice (i.e. hardware mechanization of) the analytical design constructed in step D.
Step A: Identification and characterization of the source of vibration
Note: Often for a linear system, the analysis of the response helps in determining the nature of the excitation. As shown here, the response can be analysed either in time domain or in frequency domain.
Step B - Identify suitable response variable and decide on the accepted level of vibration
Different design manuals/handbooks are available which corresponds to acceptable level of vibration for specified field of applications. The table below is an excerpt of some of the frequently encountered applications and corresponding accepted level of vibration.
Step C: Choice of a Method of Vibration Control
To control vibration effectively one can choose any of the five methods as discussed earlier or a combination of these methods
Steps D and E will be discussed from Module 2 onwards. In the next lecture, we will discuss method (iv) and (v) of vibration control.
1. What is vibration control in mechanical engineering? |
2. What are the common sources of vibrations in mechanical systems? |
3. What are the key strategies for vibration control in mechanical engineering? |
4. How can vibration control improve the performance of mechanical systems? |
5. What are the challenges faced in vibration control in mechanical engineering? |
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