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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6800
ANALYSIS OF LINEAR AND NON-LINEAR VIBRATIONS BY AL PIEZO-
LAMINATED PLATES
Umesh Bharambe1, K.K.Chaudhari2
1 M.Tech (Machine design) J T Mahajan College of Engg. Faizpur Maharashtra, India.
2 Asst.Professor(Mechanical) J T Mahajan College of Engg.Faizpur, Maharashtra, India.
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract - Active vibration control is
defined as a technique in which the vibration of a
structure is reduced or controlled by applying
counter force to the structure that isappropriately
out of phase but equal in amplitude to the original
vibration. As a result, two opposite force cancel
each other and structure stops vibrating.
In thisStudy, linearandnonlinearvibration
analyses are to be carried out on flax fiber
reinforced composites with and without an
interleaved natural viscoelastic layer.
Experimental and FE analysis is to be done in a
clamped-free configuration non two stacking
sequences of composites, 00and900 the procedure
consists on exciting the specimens with
piezoelectric patches with known frequency
Vibration control reduction can significantly
improve the performance and operation of
systems and machines in various industries. As
technology advances, the methods of vibration
control also become more involved and therefore
allow for control of more complex structures. This
paper focuses on vibration control of a flexible
plate system having viscoelastic layer.
Key Words: Stress concentration, stress Analysis,
Complex structure.
1. INTRODUCTION
As piezoelectric technology advances,
dynamic systems present more complexproblems
with less obvious solutions. One common
application for these advanced controllers is
vibration reduction. In high precision systems,
vibrations can decrease accuracies and
efficiencies, and cause potentially disastrous
damage. The abilitytocontrolthese vibrationsand
minimize amplitude response to disturbances is
valuable to many different industries across the
board. This paper focuses on vibration controlofa
flexible plate system.
Adaptive structures using piezoelectric
materials usually employ lead zirconium titanate
(PZT) ceramic sensors and actuators todetect and
mechanically deform a structure. Piezo polymer
films are not usually preferred because they lack
the stiffness requirements to achieve high
actuation authority. The addition of the PZT
material allows the structure to sense and react to
its environment. Conventionaladaptive structures
require a network of these actuators and sensors
to be bonded to the surfaces or embedded within
the structure. The actuators and sensors are
coupled together to form a closed-loop network.
This enables the sensors to detect a change in
structural deformation, and then feed the
actuators with a signal to produce the desired
response to the external stimulus. Advanced
piezo-controllersmake up a broadcategorywithin
the controls field. These controllers are capable of
achieving control as well as being robust and
adaptive to variances in system parameters.
Advanced controllers can be made effective when
the system is modeled accurately. With the goal of
more effective controllers, the dynamic system
model pays an important role in the controller
design.
2. MATHEMATICAL MODELING
Mechanical vibrations span amplitudes from
meters to nanometers. Their detrimentaleffect on
systems may be of various natures:
Failure: vibration-induced structural failure may
occur by excessive strain during transient events
(e.g. building response to earthquake)
Comfort: where vibrations are detrimental to
comfort are numerous: noise and vibration in
helicopters, car suspensions, and wind induced
sway of buildings.
Vibration reduction can be achieved in many
different ways, depending on the problem; the
most common are stiffening, damping and
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6801
isolation. Stiffening consists of shifting the
resonance frequency of the structure beyond the
frequency band of excitation. Damping consists of
reducing the resonance peaks by dissipating the
vibration energy. Isolation consists of preventing
the propagation of disturbances to sensitive parts
of the systems. The objective of active damping is
to reduce the effect of the resonant peaks on the
response of the structure. From
Consider a rectangular sandwich or laminated
composite plates the plane dimensionsofthe plate
are denoted by a, b whereas the thickness of its
top face sheet, core, and bottom face sheet are
denoted by h1, h2, and h3, respectively. The plane
displacement components are assumed to be as
the results of superposition of local and global
displacement fields
Where uG, vG, and wG denote the global
components of the displacement field
While uL and vL are of the two-term local
displacement components.
Components are assumed to be linear and
the local components are considered to be
piecewise linear. Imposing the continuity
conditions of the displacement components at the
interfaces between the layers.
Figure2.1GeometryandCoordinateSystemofthePlate
Therefore, independent displacement parameters
left to be determined based on the next stages.
2.2 The Governing Equations of the Laminated
Composite or Sandwich Plate
The governing equations are derived basedon the
principle of minimum total potential energy
Where U and V are the strain energy and work of
the externally applied loads, respectively
Where q is the transversely distributed load and
the strain andstressquantitiesmaybe determined
based on the unknown displacement parameters
through the following relations for the ith layer.
3. EXPERIMENTAL SETUP
The first step of the experimental system is to
manufacture the Glass Fiber Plate, the Glass Fiber
platesare manufacturedbyHandLayup technique.
The araldite is used as the Viscoelastic material to
fill the core.
The experimentation involves the Preparation of
Aluminum plate with the piezoelectric patches.
This section discusses the process of
manufacturing the composites as well as the
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6802
components of the experimentalsystems, the type
of actuation signal employed, and post processing
of the actively monitored signal, development of
the new damage signature, and test results Teflon
slice having dimensions (50 x 50) mm are
embedded in composite plate at the time of
manufacturing the specimens this embedded
Teflon sheet considered as a type of delamination
or damage in composite plate.
Figure 3.1: Schematic Diagram of Experimental
Setup
3.2 Procedure for Experimental setup byusing
FFT analyzer
 Plate of required length is taken.
 By the use of screw gauge the depth and width
of plate section were measured.
 The connections of the FFT analyzer, laptop,
transducers, and model hammer along with
the requisite power connections were made.
 The accelerometerwasfixedbybeeswaxtothe
plate at one of the nodal points.
 The function generator is used to excite the
piezo patch connected to piezo by thin wires.
 Then the voltage is provided by using the
function generator to the different piezo
patches and the amplitude Vs frequency graph
was obtained from graphical user interface.
 The FFT analyzer and the accelerometer are
the interface to convert the time domain
response to frequency domain. Hence the
frequency response spectrumH1 (response,
force) was obtained.
 By moving the cursor to the peaks of the FFT
graph, the cursor values and the resonant
frequencies were recorded.
 The above procedure is repeated for all the
nodal points and all materials plates and all
structures.
 The values (i.e., natural frequencies and
resonant frequencies) obtained from the FRF
spectrums were compared with respect to the
FEM analysis.
Figure 3.2: AL Plates with piezo patch
3.3 Experimental Results:
For AL Plate:
a) Frequency Plot for position 1 without
Control:
b) Frequency Plot for Position 1 with Control:
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6803
Frequency for Position 1
Frequency
No
Without
Control
With Control
1 313 309
2 1012 991
3 2105 2089.01
4. FEM STRUCTURAL ANALYSIS
In the Numerical analysis we used ANSYS
APDL software to derive the finite element model
of the smart plate containing piezo patches. From
this analysis we can determine the Frequencies of
the natural vibrations without actuating &
actuatingthe piezopatches. We alsodetermine the
maximum admissible actuation voltage and the
maximum deflection the plate. Based on this
model the smart plate is produced and result of
the smart plate.
At the initial stage of design, the finite
element model is sufficient which allows
determining the location, size of an actuator and
its power requirement. In the modeling and
analysis of piezoelectric crystal typical finite
element used was (SOLID5), which has
piezoelectric capacityin three-dimensionalcouple
field problem. Like otherstructuralsolidelements,
this element has three displacement degrees of
freedom per node. In addition to this degree of
freedom the element has also potential degree for
the analysis of the electromechanical coupling
problems. Piezoelectric actuator inherently
exhibits anisotropic and yield three-dimensional
spatial vibration in their response to the
piezoelectric actuation.
Figure 4.1: Line Model of Plate
Figure 4.2: Meshed Model
Figure 4.3 : Boundary Conditions
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6804
4.1ANSYS Results for Aluminium Plate:
a) Frequencyplot position1without controller
b) Frequency plot position 1 with controller
Frequency for Position 1
Frequency
Number
Without
Control
With Control
1 309.026 303.212
2 1005 987.376
3 2067 2099
5. RESULT AND DISCUSSION
For Aluminum Plate:
The positions are specified in the experimental &
Finite Element Setup is considered for the
Results & Discussions. The Modal Frequencies
Obtained Experimentally is shown in Following
Table.
Frequency for Position 1
Frequency
No
Without
Control
With
Control
%
Control
Obtained
1 313 309 1.2
2 1012 991 2.07
3 2105 2089.01 0.759
Table No.5.1 Results Obtained From
Experimental Analysis for Al Plate.
Frequency for Position 1
Frequency
Number
Without
Control
With
Control
% Control
Obtained
1 309.026 303.212 2
2 1005 987.376 1.75
3 2099 2067 1.52
Table No.5.2Results Obtained From
Experimental Analysis for Al Plate
6. CONCLUSION
From the Finite Element & Experimental
Results It is seen that the piezoelectric material is
an effective tool for control of vibration. The size
of piezoelectric patch also plays an important role
to control the vibrations. Here we have used small
patch but the actuations produced are good as
compared.
The position of sensor is also an important
factor to detect the vibrations in the plate
structures. It is observed from results that the
control obtained near to free end is less as
compared to other locations.
It is also observed that Viscoelastic core has a
great impact over the vibrations, it can be used to
produce the damping effect.
The control obtained islessin composite plate,
but satisfactory as compared to amplitude of
vibrations.
It is can be concluded that the vibrations
response in laminated plates are less as compared
to isometric plates.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6805
REFERENCES
1. Dr. Kishor B. Waghulde, Dr. Bimlesh Kumar,
“Active Vibration Analysis of Piezo-
Laminated Cantilever Beam”,International
Journal of Scientific & Engineering Research,
Volume 5, Issue 12, December-2014, ISSN
2229-5518,PP 624-628.
2. H Karagulle, L Malgaca and H F Oktem,
“Analysis of active vibration control in smart
structures by ANSYS”, Institute of Physics
Publishing,PII:S0964-1726(04)77278-X,
(2004) 661–667.
3. Yavuz Yaman, Tarkan Caliskan, Volkan
Nalbantoglu, Eswar Prasad, David Waechter,
“ACTIVE VIBRATION CONTROL OF ASMART
PLATE”, ICAS2002 CONGRESS.
4. M. Kozupa, and J. Wiciak, “Active Vibration
Control ofRectangularPlate withDistributed
Piezoelements Excited Acoustically and
Mechanically”, ACTA PHYSICA POLONICA,
Acoustic and Biomedical Engineering.
5. S. K. Sarangi, M. C. Ray, “Active damping of
geometrically nonlinear vibrations of
laminated composite plates using vertically
reinforced 1-3 piezoelectric composites”,
Acta Mech 222, 363–380 (2011) DOI
10.1007/s00707-011-0531.

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IRJET- Analysis of Linear and Non-Linear Vibrations by Al Piezo-Laminated Plates

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6800 ANALYSIS OF LINEAR AND NON-LINEAR VIBRATIONS BY AL PIEZO- LAMINATED PLATES Umesh Bharambe1, K.K.Chaudhari2 1 M.Tech (Machine design) J T Mahajan College of Engg. Faizpur Maharashtra, India. 2 Asst.Professor(Mechanical) J T Mahajan College of Engg.Faizpur, Maharashtra, India. ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Active vibration control is defined as a technique in which the vibration of a structure is reduced or controlled by applying counter force to the structure that isappropriately out of phase but equal in amplitude to the original vibration. As a result, two opposite force cancel each other and structure stops vibrating. In thisStudy, linearandnonlinearvibration analyses are to be carried out on flax fiber reinforced composites with and without an interleaved natural viscoelastic layer. Experimental and FE analysis is to be done in a clamped-free configuration non two stacking sequences of composites, 00and900 the procedure consists on exciting the specimens with piezoelectric patches with known frequency Vibration control reduction can significantly improve the performance and operation of systems and machines in various industries. As technology advances, the methods of vibration control also become more involved and therefore allow for control of more complex structures. This paper focuses on vibration control of a flexible plate system having viscoelastic layer. Key Words: Stress concentration, stress Analysis, Complex structure. 1. INTRODUCTION As piezoelectric technology advances, dynamic systems present more complexproblems with less obvious solutions. One common application for these advanced controllers is vibration reduction. In high precision systems, vibrations can decrease accuracies and efficiencies, and cause potentially disastrous damage. The abilitytocontrolthese vibrationsand minimize amplitude response to disturbances is valuable to many different industries across the board. This paper focuses on vibration controlofa flexible plate system. Adaptive structures using piezoelectric materials usually employ lead zirconium titanate (PZT) ceramic sensors and actuators todetect and mechanically deform a structure. Piezo polymer films are not usually preferred because they lack the stiffness requirements to achieve high actuation authority. The addition of the PZT material allows the structure to sense and react to its environment. Conventionaladaptive structures require a network of these actuators and sensors to be bonded to the surfaces or embedded within the structure. The actuators and sensors are coupled together to form a closed-loop network. This enables the sensors to detect a change in structural deformation, and then feed the actuators with a signal to produce the desired response to the external stimulus. Advanced piezo-controllersmake up a broadcategorywithin the controls field. These controllers are capable of achieving control as well as being robust and adaptive to variances in system parameters. Advanced controllers can be made effective when the system is modeled accurately. With the goal of more effective controllers, the dynamic system model pays an important role in the controller design. 2. MATHEMATICAL MODELING Mechanical vibrations span amplitudes from meters to nanometers. Their detrimentaleffect on systems may be of various natures: Failure: vibration-induced structural failure may occur by excessive strain during transient events (e.g. building response to earthquake) Comfort: where vibrations are detrimental to comfort are numerous: noise and vibration in helicopters, car suspensions, and wind induced sway of buildings. Vibration reduction can be achieved in many different ways, depending on the problem; the most common are stiffening, damping and
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6801 isolation. Stiffening consists of shifting the resonance frequency of the structure beyond the frequency band of excitation. Damping consists of reducing the resonance peaks by dissipating the vibration energy. Isolation consists of preventing the propagation of disturbances to sensitive parts of the systems. The objective of active damping is to reduce the effect of the resonant peaks on the response of the structure. From Consider a rectangular sandwich or laminated composite plates the plane dimensionsofthe plate are denoted by a, b whereas the thickness of its top face sheet, core, and bottom face sheet are denoted by h1, h2, and h3, respectively. The plane displacement components are assumed to be as the results of superposition of local and global displacement fields Where uG, vG, and wG denote the global components of the displacement field While uL and vL are of the two-term local displacement components. Components are assumed to be linear and the local components are considered to be piecewise linear. Imposing the continuity conditions of the displacement components at the interfaces between the layers. Figure2.1GeometryandCoordinateSystemofthePlate Therefore, independent displacement parameters left to be determined based on the next stages. 2.2 The Governing Equations of the Laminated Composite or Sandwich Plate The governing equations are derived basedon the principle of minimum total potential energy Where U and V are the strain energy and work of the externally applied loads, respectively Where q is the transversely distributed load and the strain andstressquantitiesmaybe determined based on the unknown displacement parameters through the following relations for the ith layer. 3. EXPERIMENTAL SETUP The first step of the experimental system is to manufacture the Glass Fiber Plate, the Glass Fiber platesare manufacturedbyHandLayup technique. The araldite is used as the Viscoelastic material to fill the core. The experimentation involves the Preparation of Aluminum plate with the piezoelectric patches. This section discusses the process of manufacturing the composites as well as the
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6802 components of the experimentalsystems, the type of actuation signal employed, and post processing of the actively monitored signal, development of the new damage signature, and test results Teflon slice having dimensions (50 x 50) mm are embedded in composite plate at the time of manufacturing the specimens this embedded Teflon sheet considered as a type of delamination or damage in composite plate. Figure 3.1: Schematic Diagram of Experimental Setup 3.2 Procedure for Experimental setup byusing FFT analyzer  Plate of required length is taken.  By the use of screw gauge the depth and width of plate section were measured.  The connections of the FFT analyzer, laptop, transducers, and model hammer along with the requisite power connections were made.  The accelerometerwasfixedbybeeswaxtothe plate at one of the nodal points.  The function generator is used to excite the piezo patch connected to piezo by thin wires.  Then the voltage is provided by using the function generator to the different piezo patches and the amplitude Vs frequency graph was obtained from graphical user interface.  The FFT analyzer and the accelerometer are the interface to convert the time domain response to frequency domain. Hence the frequency response spectrumH1 (response, force) was obtained.  By moving the cursor to the peaks of the FFT graph, the cursor values and the resonant frequencies were recorded.  The above procedure is repeated for all the nodal points and all materials plates and all structures.  The values (i.e., natural frequencies and resonant frequencies) obtained from the FRF spectrums were compared with respect to the FEM analysis. Figure 3.2: AL Plates with piezo patch 3.3 Experimental Results: For AL Plate: a) Frequency Plot for position 1 without Control: b) Frequency Plot for Position 1 with Control:
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6803 Frequency for Position 1 Frequency No Without Control With Control 1 313 309 2 1012 991 3 2105 2089.01 4. FEM STRUCTURAL ANALYSIS In the Numerical analysis we used ANSYS APDL software to derive the finite element model of the smart plate containing piezo patches. From this analysis we can determine the Frequencies of the natural vibrations without actuating & actuatingthe piezopatches. We alsodetermine the maximum admissible actuation voltage and the maximum deflection the plate. Based on this model the smart plate is produced and result of the smart plate. At the initial stage of design, the finite element model is sufficient which allows determining the location, size of an actuator and its power requirement. In the modeling and analysis of piezoelectric crystal typical finite element used was (SOLID5), which has piezoelectric capacityin three-dimensionalcouple field problem. Like otherstructuralsolidelements, this element has three displacement degrees of freedom per node. In addition to this degree of freedom the element has also potential degree for the analysis of the electromechanical coupling problems. Piezoelectric actuator inherently exhibits anisotropic and yield three-dimensional spatial vibration in their response to the piezoelectric actuation. Figure 4.1: Line Model of Plate Figure 4.2: Meshed Model Figure 4.3 : Boundary Conditions
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6804 4.1ANSYS Results for Aluminium Plate: a) Frequencyplot position1without controller b) Frequency plot position 1 with controller Frequency for Position 1 Frequency Number Without Control With Control 1 309.026 303.212 2 1005 987.376 3 2067 2099 5. RESULT AND DISCUSSION For Aluminum Plate: The positions are specified in the experimental & Finite Element Setup is considered for the Results & Discussions. The Modal Frequencies Obtained Experimentally is shown in Following Table. Frequency for Position 1 Frequency No Without Control With Control % Control Obtained 1 313 309 1.2 2 1012 991 2.07 3 2105 2089.01 0.759 Table No.5.1 Results Obtained From Experimental Analysis for Al Plate. Frequency for Position 1 Frequency Number Without Control With Control % Control Obtained 1 309.026 303.212 2 2 1005 987.376 1.75 3 2099 2067 1.52 Table No.5.2Results Obtained From Experimental Analysis for Al Plate 6. CONCLUSION From the Finite Element & Experimental Results It is seen that the piezoelectric material is an effective tool for control of vibration. The size of piezoelectric patch also plays an important role to control the vibrations. Here we have used small patch but the actuations produced are good as compared. The position of sensor is also an important factor to detect the vibrations in the plate structures. It is observed from results that the control obtained near to free end is less as compared to other locations. It is also observed that Viscoelastic core has a great impact over the vibrations, it can be used to produce the damping effect. The control obtained islessin composite plate, but satisfactory as compared to amplitude of vibrations. It is can be concluded that the vibrations response in laminated plates are less as compared to isometric plates.
  • 6. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 | May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 6805 REFERENCES 1. Dr. Kishor B. Waghulde, Dr. Bimlesh Kumar, “Active Vibration Analysis of Piezo- Laminated Cantilever Beam”,International Journal of Scientific & Engineering Research, Volume 5, Issue 12, December-2014, ISSN 2229-5518,PP 624-628. 2. H Karagulle, L Malgaca and H F Oktem, “Analysis of active vibration control in smart structures by ANSYS”, Institute of Physics Publishing,PII:S0964-1726(04)77278-X, (2004) 661–667. 3. Yavuz Yaman, Tarkan Caliskan, Volkan Nalbantoglu, Eswar Prasad, David Waechter, “ACTIVE VIBRATION CONTROL OF ASMART PLATE”, ICAS2002 CONGRESS. 4. M. Kozupa, and J. Wiciak, “Active Vibration Control ofRectangularPlate withDistributed Piezoelements Excited Acoustically and Mechanically”, ACTA PHYSICA POLONICA, Acoustic and Biomedical Engineering. 5. S. K. Sarangi, M. C. Ray, “Active damping of geometrically nonlinear vibrations of laminated composite plates using vertically reinforced 1-3 piezoelectric composites”, Acta Mech 222, 363–380 (2011) DOI 10.1007/s00707-011-0531.