SlideShare una empresa de Scribd logo
1 de 15
Descargar para leer sin conexión
DEFLECTION CONTROL OF HYBRID
PIEZOELECTRIC FUNCTIONALLY
GRADED PLATE
S. A. Patare & K. M. Bajoria
Department of Civil Engineering,
IIT Bombay
Introduction
● Shape control of FGM plate coupled with
Piezoelectric material
● Four variable plate theory for simple formulation
● Constant displacement feedback control algorithm
● Approximate analytical solution for simply supported
and clamped plate
● Static deflection control
Piezoelectric FGM Plate Model
Displacement Field [03]
u=uo−z
∂wb
∂ x
−
(4 z3
3ht
2
)
∂ws
∂x
v=vo−z
∂wb
∂ y
−
(4z3
3ht
2
)
∂ws
∂ y
w=wb+ws
{
σx
σ y
σxy
σxz
σ yz
}=
[
C11 C12 0 0 0
C12 C22 0 0 0
0 0 C66 0 0
0 0 0 C44 0
0 0 0 0 C55
]{
ϵx
ϵy
γxy
γxz
γ yz
}−
[
0 0 ¯e31
0 0 ¯e31
0 0 0
e15 0 0
0 e15 0
]{
Ex
Ey
Ez
}
{
Dx
Dy
Dz
}=
[
0 0 0 e15 0
0 0 0 0 e15
¯e31 ¯e31 0 0 0 ]{
ϵx
ϵy
γxy
γxz
γ yz
}+
[
Ω11 0 0
0 Ω11 0
0 0 Ω33
]{
Ex
Ey
Ez
}
Constitutive
Law[05]►
Electric
Displacement[05]►
Electric Potential Function
Φ=
{ Π T
[1−
(z−h/2−hp/2
hp/2 )
2
]+AT z+BT ;for⟨h
2
z⩽⩽
h
2
+hp ⟩
Π B
[1−
(− z−h/2−hp/2
hp/2 )
2
]+AB z+BB ;for⟨−
h
2
−hp z⩽⩽−
h
2 ⟩}
Φ(z=±
h
2 )=0, Dz
(z=±(h
2
+hp))=0Boundary Conditions for Open Circuit ►
BT =−(h
2)AT ;BB=(h
2)AB
Φ=
{ΠT
[1−
(z −h/2−hp /2
hp/2 )
2
]+ AT (z−
h
2) for⟨h
2
⩽z⩽
h
2
+hp ⟩
ΠB
[1−
(− z−h/2−hp/2
hp/2 )
2
]+ AB(z+
h
2) for ⟨−
h
2
−hp ⩽z ⩽−
h
2 ⟩
Hamilton’s Principle
0=∫
0
T
(δU+δV−δK)δt
δU=∫
A
∫
−
h
2
− hp
h
2
+hp
(σx δϵx +σy δϵy +σxy δγxy +σyz δγyz +σxz δγxz)dzdA
δV =−∫
A
q δ (wb+ws)dA
◄Strain Energy
Variation
Work Done Variation►
Governing Formulation
δu0 :
∂Nx
∂x
+
∂ Nxy
∂ y
=0 δv0:
∂ N y
∂ y
+
∂ Nxy
∂ x
=0
δ wb :
∂
2
Mx
b
∂ x
2
+
∂
2
M y
b
∂ y
2
+2
∂
2
M xy
b
∂ x ∂ y
+qw=0
δ ws:
∂
2
M x
s
∂ x
2
+
∂
2
M y
s
∂ y
2
+2
∂
2
M xy
s
∂ x ∂ y
+
∂Qxz
∂ x
+
∂Q yz
∂ y
+qw=0
∫
h
2
h
2
+hp
(∂ Dx
∂x
+
∂Dy
∂ y
+
∂Dz
∂z )dz+ ∫
−
h
2
−hp
−
h
2
(∂Dx
∂ x
+
∂ Dy
∂ y
+
∂Dz
∂z )dz=0
λ1(∂2
ws
∂ x
2
+
∂2
ws
∂ y
2 )− λ2(∂2
wb
∂ x
2
+
∂2
wb
∂ y
2 )−λ3(∂2
ΠT
∂ x
2
+
∂2
ΠT
∂ y
2 )
− λ4(∂
2
ΠB
∂ x2
+
∂
2
ΠB
∂ y2 )− λ5 ΠT − λ6 ΠB }=0
Fifth Governing Equation►
Fifth Equation & Maxwell’s Law
◄Displacement Feedback
Control Law [02]
ΠT =Gd Π B+Gv ˙Π B
Approximate Analytical Solution [04]
u0=∑
m=1
∞
∑
n=1
∞
U eiwt ∂ XM (x)
∂x
YN ( y ) v0=∑
m=1
∞
∑
n=1
∞
V eiwt
XM (x)
∂YN ( y)
∂ y
wb=∑
m=1
∞
∑
n=1
∞
W b eiwt
XM (x)YN ( y) ws=∑
m=1
∞
∑
n=1
∞
W s eiwt
XM (x)YN ( y )
Π=∑
m=1
∞
∑
n=1
∞
Π eiwt
XM (x)YN ( y)
Numerical
● A square plate of 200mm size
● Thickness of FGM plate is 1 mm while Piezo layers
is 0.1 mm
● Uniform load of 100 N/m2
● FGM core of Ti-6Al-4V and Aluminium Oxide
● Power law is taken 2 (constant)
Shape control for simpy supported plate
Shape control for clamped Plate
Conclusion
● It is possible to consider simple four variable plate theory for
analysis of hybrid piezoelectric FGM plate
● Open circuit potential function for four variable plate theory
is proposed and validated
● Good results are obtained for static bending of plate
● Approximate analytical solution further simplies the analysis
for other boundary condition
● Smart hybrid piezoelectric FGM plate model is developed with
minimum computational efforts
● Change in power law, aspect ratio and FGM materials can be
considered for further study
References
1) P. A. Jadhav and K. M. Bajoria: Stability analysis of thick piezoelectric metal
based FGM plate using first order and higher order shear deformation theory,
Int. J. Mech. Mater. Des., 11, 2015, pp. 387-403
2) T. Nguyen-Thoi, K. Nguyen-Quang, H. Dang-Trung, V. Ho-Huu and H.
Luong-Van: Analysis and control of FGM plates integrated with piezoelectric
sensors and actuators using cell-based smoothed discrete shear gap method,
Compos. Struct., 165, 2016, pp. 115-129.
3) Seung-Eock Kim and Huu-Tai Thai: A simple higher-order shear deformation
theory for bending and free vibration analysis of functionally graded plates,
Compos. Struct., 96, 2013,pp. 165-173.
4) M. R. Barati, H. Shahverdi and A. M. Zenkour: Electro-mechanical vibration
of smart piezoelectric FG plates with porosities according to a refined four-
variable theory, Mech. Adv. Mater. Struct., 24 (12), 2017, pp. 987-998.
5) H. F. Tiersten: Linear piezoelectric plate vibrations, Plenum Press, New York,
1969.
Thank You

Más contenido relacionado

La actualidad más candente

Load distribution of soil mechanics
Load distribution of soil mechanics Load distribution of soil mechanics
Load distribution of soil mechanics Karan Patel
 
Fixed point and weak commuting mapping
Fixed point and weak commuting mappingFixed point and weak commuting mapping
Fixed point and weak commuting mappingeSAT Publishing House
 
Cubic Spline Interpolation
Cubic Spline InterpolationCubic Spline Interpolation
Cubic Spline InterpolationVARUN KUMAR
 
On Optimization of Manufacturing of a Two-level Current-mode Logic Gates in a...
On Optimization of Manufacturing of a Two-level Current-mode Logic Gates in a...On Optimization of Manufacturing of a Two-level Current-mode Logic Gates in a...
On Optimization of Manufacturing of a Two-level Current-mode Logic Gates in a...BRNSS Publication Hub
 
Numerical simulation on laminar convection flow and heat transfer over a non ...
Numerical simulation on laminar convection flow and heat transfer over a non ...Numerical simulation on laminar convection flow and heat transfer over a non ...
Numerical simulation on laminar convection flow and heat transfer over a non ...eSAT Journals
 
(PART1/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
(PART1/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981(PART1/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
(PART1/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981Ali Faizan Wattoo
 
09-Strength of Gusset Plate (Steel Structural Design & Prof. Shehab Mourad)
09-Strength of Gusset Plate (Steel Structural Design & Prof. Shehab Mourad)09-Strength of Gusset Plate (Steel Structural Design & Prof. Shehab Mourad)
09-Strength of Gusset Plate (Steel Structural Design & Prof. Shehab Mourad)Hossam Shafiq II
 
(Part 2/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
(Part 2/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981(Part 2/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
(Part 2/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981Ali Faizan Wattoo
 
Navier-Stokes Equation of Motion
 Navier-Stokes Equation of Motion  Navier-Stokes Equation of Motion
Navier-Stokes Equation of Motion Sukhvinder Singh
 
Applied numerical methods lec14
Applied numerical methods lec14Applied numerical methods lec14
Applied numerical methods lec14Yasser Ahmed
 
Sweeping discussion on_dirac_fields_update1
Sweeping discussion on_dirac_fields_update1Sweeping discussion on_dirac_fields_update1
Sweeping discussion on_dirac_fields_update1foxtrot jp R
 
07 3 d_elasticity_02_3d_stressstrain
07 3 d_elasticity_02_3d_stressstrain07 3 d_elasticity_02_3d_stressstrain
07 3 d_elasticity_02_3d_stressstrainVijay Kumar
 
navier stokes equation
navier stokes equationnavier stokes equation
navier stokes equationKaran Patel
 
Sachpazis_Foundation Analysis & Design. Calculation according to EN 1997-1-2008
Sachpazis_Foundation Analysis & Design. Calculation according to EN 1997-1-2008Sachpazis_Foundation Analysis & Design. Calculation according to EN 1997-1-2008
Sachpazis_Foundation Analysis & Design. Calculation according to EN 1997-1-2008Dr.Costas Sachpazis
 
12-Examples on Compression Members (Steel Structural Design & Prof. Shehab Mo...
12-Examples on Compression Members (Steel Structural Design & Prof. Shehab Mo...12-Examples on Compression Members (Steel Structural Design & Prof. Shehab Mo...
12-Examples on Compression Members (Steel Structural Design & Prof. Shehab Mo...Hossam Shafiq II
 
Controllability observability-pole-zero-cancellation
Controllability observability-pole-zero-cancellationControllability observability-pole-zero-cancellation
Controllability observability-pole-zero-cancellationcairo university
 
05-Strength of Double Angle Bolted Tension Members (Steel Structural Design &...
05-Strength of Double Angle Bolted Tension Members (Steel Structural Design &...05-Strength of Double Angle Bolted Tension Members (Steel Structural Design &...
05-Strength of Double Angle Bolted Tension Members (Steel Structural Design &...Hossam Shafiq II
 
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...SEENET-MTP
 

La actualidad más candente (20)

Load distribution of soil mechanics
Load distribution of soil mechanics Load distribution of soil mechanics
Load distribution of soil mechanics
 
Footing Design
Footing DesignFooting Design
Footing Design
 
Fixed point and weak commuting mapping
Fixed point and weak commuting mappingFixed point and weak commuting mapping
Fixed point and weak commuting mapping
 
Cubic Spline Interpolation
Cubic Spline InterpolationCubic Spline Interpolation
Cubic Spline Interpolation
 
On Optimization of Manufacturing of a Two-level Current-mode Logic Gates in a...
On Optimization of Manufacturing of a Two-level Current-mode Logic Gates in a...On Optimization of Manufacturing of a Two-level Current-mode Logic Gates in a...
On Optimization of Manufacturing of a Two-level Current-mode Logic Gates in a...
 
Numerical simulation on laminar convection flow and heat transfer over a non ...
Numerical simulation on laminar convection flow and heat transfer over a non ...Numerical simulation on laminar convection flow and heat transfer over a non ...
Numerical simulation on laminar convection flow and heat transfer over a non ...
 
(PART1/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
(PART1/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981(PART1/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
(PART1/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
 
09-Strength of Gusset Plate (Steel Structural Design & Prof. Shehab Mourad)
09-Strength of Gusset Plate (Steel Structural Design & Prof. Shehab Mourad)09-Strength of Gusset Plate (Steel Structural Design & Prof. Shehab Mourad)
09-Strength of Gusset Plate (Steel Structural Design & Prof. Shehab Mourad)
 
(Part 2/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
(Part 2/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981(Part 2/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
(Part 2/2)COLLAPSE OF THE HYATT REGENCY WALKWAYS 1981
 
Navier-Stokes Equation of Motion
 Navier-Stokes Equation of Motion  Navier-Stokes Equation of Motion
Navier-Stokes Equation of Motion
 
Applied numerical methods lec14
Applied numerical methods lec14Applied numerical methods lec14
Applied numerical methods lec14
 
Sweeping discussion on_dirac_fields_update1
Sweeping discussion on_dirac_fields_update1Sweeping discussion on_dirac_fields_update1
Sweeping discussion on_dirac_fields_update1
 
07 3 d_elasticity_02_3d_stressstrain
07 3 d_elasticity_02_3d_stressstrain07 3 d_elasticity_02_3d_stressstrain
07 3 d_elasticity_02_3d_stressstrain
 
Ijtra1501104
Ijtra1501104Ijtra1501104
Ijtra1501104
 
navier stokes equation
navier stokes equationnavier stokes equation
navier stokes equation
 
Sachpazis_Foundation Analysis & Design. Calculation according to EN 1997-1-2008
Sachpazis_Foundation Analysis & Design. Calculation according to EN 1997-1-2008Sachpazis_Foundation Analysis & Design. Calculation according to EN 1997-1-2008
Sachpazis_Foundation Analysis & Design. Calculation according to EN 1997-1-2008
 
12-Examples on Compression Members (Steel Structural Design & Prof. Shehab Mo...
12-Examples on Compression Members (Steel Structural Design & Prof. Shehab Mo...12-Examples on Compression Members (Steel Structural Design & Prof. Shehab Mo...
12-Examples on Compression Members (Steel Structural Design & Prof. Shehab Mo...
 
Controllability observability-pole-zero-cancellation
Controllability observability-pole-zero-cancellationControllability observability-pole-zero-cancellation
Controllability observability-pole-zero-cancellation
 
05-Strength of Double Angle Bolted Tension Members (Steel Structural Design &...
05-Strength of Double Angle Bolted Tension Members (Steel Structural Design &...05-Strength of Double Angle Bolted Tension Members (Steel Structural Design &...
05-Strength of Double Angle Bolted Tension Members (Steel Structural Design &...
 
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
Yurri Sitenko "Boundary effects for magnetized quantum matter in particle and...
 

Similar a Hybrid Piezoelectric FGM plate shape control

Topological flat bands without magic angles in massive twisted bilayer graphe...
Topological flat bands without magic angles in massive twisted bilayer graphe...Topological flat bands without magic angles in massive twisted bilayer graphe...
Topological flat bands without magic angles in massive twisted bilayer graphe...JAVVAJI SRIVANI
 
The response of a rectangular micro-plate to me-chanical shocks considering m...
The response of a rectangular micro-plate to me-chanical shocks considering m...The response of a rectangular micro-plate to me-chanical shocks considering m...
The response of a rectangular micro-plate to me-chanical shocks considering m...Kaveh Rashvand
 
2d beam element with combined loading bending axial and torsion
2d beam element with combined loading bending axial and torsion2d beam element with combined loading bending axial and torsion
2d beam element with combined loading bending axial and torsionrro7560
 
Spectral properties of the Goldstino in supersymmetric Bose-Fermi mixtures
Spectral properties of the Goldstino in supersymmetric Bose-Fermi mixturesSpectral properties of the Goldstino in supersymmetric Bose-Fermi mixtures
Spectral properties of the Goldstino in supersymmetric Bose-Fermi mixturesDaisuke Satow
 
Heterogeneous relaxation dynamics in amorphous materials under cyclic loading
Heterogeneous relaxation dynamics in amorphous materials under cyclic loadingHeterogeneous relaxation dynamics in amorphous materials under cyclic loading
Heterogeneous relaxation dynamics in amorphous materials under cyclic loadingNikolai Priezjev
 
stress strain dispalcement.pdf
stress strain dispalcement.pdfstress strain dispalcement.pdf
stress strain dispalcement.pdfShikhaSingla15
 
Second-Order Phase Transition in Heisenberg Model on Triangular Lattice with ...
Second-Order Phase Transition in Heisenberg Model on Triangular Lattice with ...Second-Order Phase Transition in Heisenberg Model on Triangular Lattice with ...
Second-Order Phase Transition in Heisenberg Model on Triangular Lattice with ...Shu Tanaka
 
A study on mhd boundary layer flow over a nonlinear
A study on mhd boundary layer flow over a nonlinearA study on mhd boundary layer flow over a nonlinear
A study on mhd boundary layer flow over a nonlineareSAT Publishing House
 
MODELING OF MANUFACTURING OF A FIELDEFFECT TRANSISTOR TO DETERMINE CONDITIONS...
MODELING OF MANUFACTURING OF A FIELDEFFECT TRANSISTOR TO DETERMINE CONDITIONS...MODELING OF MANUFACTURING OF A FIELDEFFECT TRANSISTOR TO DETERMINE CONDITIONS...
MODELING OF MANUFACTURING OF A FIELDEFFECT TRANSISTOR TO DETERMINE CONDITIONS...antjjournal
 
Dynamic stiffness and eigenvalues of nonlocal nano beams
Dynamic stiffness and eigenvalues of nonlocal nano beamsDynamic stiffness and eigenvalues of nonlocal nano beams
Dynamic stiffness and eigenvalues of nonlocal nano beamsUniversity of Glasgow
 
Mhd and heat transfer in a thin film over an unsteady stretching surface with
Mhd and heat transfer in a thin film over an unsteady stretching surface withMhd and heat transfer in a thin film over an unsteady stretching surface with
Mhd and heat transfer in a thin film over an unsteady stretching surface withIAEME Publication
 
2018SOE07-Kim-Computation of Added resistance of ships by using a frequency-d...
2018SOE07-Kim-Computation of Added resistance of ships by using a frequency-d...2018SOE07-Kim-Computation of Added resistance of ships by using a frequency-d...
2018SOE07-Kim-Computation of Added resistance of ships by using a frequency-d...SahilJawa3
 
Phase diagram at finite T & Mu in strong coupling limit of lattice QCD
Phase diagram at finite T & Mu in strong coupling limit of lattice QCDPhase diagram at finite T & Mu in strong coupling limit of lattice QCD
Phase diagram at finite T & Mu in strong coupling limit of lattice QCDBenjamin Jaedon Choi
 
Direct method for soliton solution
Direct method for soliton solutionDirect method for soliton solution
Direct method for soliton solutionMOHANRAJ PHYSICS
 
Measurement-induced long-distance entanglement with optomechanical transducers
Measurement-induced long-distance entanglement with optomechanical transducersMeasurement-induced long-distance entanglement with optomechanical transducers
Measurement-induced long-distance entanglement with optomechanical transducersOndrej Cernotik
 

Similar a Hybrid Piezoelectric FGM plate shape control (20)

Beam buckling
Beam bucklingBeam buckling
Beam buckling
 
Topological flat bands without magic angles in massive twisted bilayer graphe...
Topological flat bands without magic angles in massive twisted bilayer graphe...Topological flat bands without magic angles in massive twisted bilayer graphe...
Topological flat bands without magic angles in massive twisted bilayer graphe...
 
The response of a rectangular micro-plate to me-chanical shocks considering m...
The response of a rectangular micro-plate to me-chanical shocks considering m...The response of a rectangular micro-plate to me-chanical shocks considering m...
The response of a rectangular micro-plate to me-chanical shocks considering m...
 
2d beam element with combined loading bending axial and torsion
2d beam element with combined loading bending axial and torsion2d beam element with combined loading bending axial and torsion
2d beam element with combined loading bending axial and torsion
 
Spectral properties of the Goldstino in supersymmetric Bose-Fermi mixtures
Spectral properties of the Goldstino in supersymmetric Bose-Fermi mixturesSpectral properties of the Goldstino in supersymmetric Bose-Fermi mixtures
Spectral properties of the Goldstino in supersymmetric Bose-Fermi mixtures
 
Heterogeneous relaxation dynamics in amorphous materials under cyclic loading
Heterogeneous relaxation dynamics in amorphous materials under cyclic loadingHeterogeneous relaxation dynamics in amorphous materials under cyclic loading
Heterogeneous relaxation dynamics in amorphous materials under cyclic loading
 
stress strain dispalcement.pdf
stress strain dispalcement.pdfstress strain dispalcement.pdf
stress strain dispalcement.pdf
 
Second-Order Phase Transition in Heisenberg Model on Triangular Lattice with ...
Second-Order Phase Transition in Heisenberg Model on Triangular Lattice with ...Second-Order Phase Transition in Heisenberg Model on Triangular Lattice with ...
Second-Order Phase Transition in Heisenberg Model on Triangular Lattice with ...
 
A study on mhd boundary layer flow over a nonlinear
A study on mhd boundary layer flow over a nonlinearA study on mhd boundary layer flow over a nonlinear
A study on mhd boundary layer flow over a nonlinear
 
MODELING OF MANUFACTURING OF A FIELDEFFECT TRANSISTOR TO DETERMINE CONDITIONS...
MODELING OF MANUFACTURING OF A FIELDEFFECT TRANSISTOR TO DETERMINE CONDITIONS...MODELING OF MANUFACTURING OF A FIELDEFFECT TRANSISTOR TO DETERMINE CONDITIONS...
MODELING OF MANUFACTURING OF A FIELDEFFECT TRANSISTOR TO DETERMINE CONDITIONS...
 
cheb_conf_aksenov.pdf
cheb_conf_aksenov.pdfcheb_conf_aksenov.pdf
cheb_conf_aksenov.pdf
 
Dynamic stiffness and eigenvalues of nonlocal nano beams
Dynamic stiffness and eigenvalues of nonlocal nano beamsDynamic stiffness and eigenvalues of nonlocal nano beams
Dynamic stiffness and eigenvalues of nonlocal nano beams
 
CMSI計算科学技術特論C (2015) ALPS と量子多体問題①
CMSI計算科学技術特論C (2015) ALPS と量子多体問題①CMSI計算科学技術特論C (2015) ALPS と量子多体問題①
CMSI計算科学技術特論C (2015) ALPS と量子多体問題①
 
Mhd and heat transfer in a thin film over an unsteady stretching surface with
Mhd and heat transfer in a thin film over an unsteady stretching surface withMhd and heat transfer in a thin film over an unsteady stretching surface with
Mhd and heat transfer in a thin film over an unsteady stretching surface with
 
2018SOE07-Kim-Computation of Added resistance of ships by using a frequency-d...
2018SOE07-Kim-Computation of Added resistance of ships by using a frequency-d...2018SOE07-Kim-Computation of Added resistance of ships by using a frequency-d...
2018SOE07-Kim-Computation of Added resistance of ships by using a frequency-d...
 
UNIT I_3.pdf
UNIT I_3.pdfUNIT I_3.pdf
UNIT I_3.pdf
 
Phase diagram at finite T & Mu in strong coupling limit of lattice QCD
Phase diagram at finite T & Mu in strong coupling limit of lattice QCDPhase diagram at finite T & Mu in strong coupling limit of lattice QCD
Phase diagram at finite T & Mu in strong coupling limit of lattice QCD
 
Direct method for soliton solution
Direct method for soliton solutionDirect method for soliton solution
Direct method for soliton solution
 
Measurement-induced long-distance entanglement with optomechanical transducers
Measurement-induced long-distance entanglement with optomechanical transducersMeasurement-induced long-distance entanglement with optomechanical transducers
Measurement-induced long-distance entanglement with optomechanical transducers
 
Finite frequency H∞control design for nonlinear systems
Finite frequency H∞control design for nonlinear systemsFinite frequency H∞control design for nonlinear systems
Finite frequency H∞control design for nonlinear systems
 

Último

Booking open Available Pune Call Girls Pargaon 6297143586 Call Hot Indian Gi...
Booking open Available Pune Call Girls Pargaon  6297143586 Call Hot Indian Gi...Booking open Available Pune Call Girls Pargaon  6297143586 Call Hot Indian Gi...
Booking open Available Pune Call Girls Pargaon 6297143586 Call Hot Indian Gi...Call Girls in Nagpur High Profile
 
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night StandCall Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Standamitlee9823
 
Design For Accessibility: Getting it right from the start
Design For Accessibility: Getting it right from the startDesign For Accessibility: Getting it right from the start
Design For Accessibility: Getting it right from the startQuintin Balsdon
 
Call Girls Pimpri Chinchwad Call Me 7737669865 Budget Friendly No Advance Boo...
Call Girls Pimpri Chinchwad Call Me 7737669865 Budget Friendly No Advance Boo...Call Girls Pimpri Chinchwad Call Me 7737669865 Budget Friendly No Advance Boo...
Call Girls Pimpri Chinchwad Call Me 7737669865 Budget Friendly No Advance Boo...roncy bisnoi
 
Intro To Electric Vehicles PDF Notes.pdf
Intro To Electric Vehicles PDF Notes.pdfIntro To Electric Vehicles PDF Notes.pdf
Intro To Electric Vehicles PDF Notes.pdfrs7054576148
 
Call Girls Wakad Call Me 7737669865 Budget Friendly No Advance Booking
Call Girls Wakad Call Me 7737669865 Budget Friendly No Advance BookingCall Girls Wakad Call Me 7737669865 Budget Friendly No Advance Booking
Call Girls Wakad Call Me 7737669865 Budget Friendly No Advance Bookingroncy bisnoi
 
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 BookingVIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Bookingdharasingh5698
 
VIP Call Girls Palanpur 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Palanpur 7001035870 Whatsapp Number, 24/07 BookingVIP Call Girls Palanpur 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Palanpur 7001035870 Whatsapp Number, 24/07 Bookingdharasingh5698
 
Work-Permit-Receiver-in-Saudi-Aramco.pptx
Work-Permit-Receiver-in-Saudi-Aramco.pptxWork-Permit-Receiver-in-Saudi-Aramco.pptx
Work-Permit-Receiver-in-Saudi-Aramco.pptxJuliansyahHarahap1
 
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXssuser89054b
 
Thermal Engineering -unit - III & IV.ppt
Thermal Engineering -unit - III & IV.pptThermal Engineering -unit - III & IV.ppt
Thermal Engineering -unit - III & IV.pptDineshKumar4165
 
Bhosari ( Call Girls ) Pune 6297143586 Hot Model With Sexy Bhabi Ready For ...
Bhosari ( Call Girls ) Pune  6297143586  Hot Model With Sexy Bhabi Ready For ...Bhosari ( Call Girls ) Pune  6297143586  Hot Model With Sexy Bhabi Ready For ...
Bhosari ( Call Girls ) Pune 6297143586 Hot Model With Sexy Bhabi Ready For ...tanu pandey
 
Unleashing the Power of the SORA AI lastest leap
Unleashing the Power of the SORA AI lastest leapUnleashing the Power of the SORA AI lastest leap
Unleashing the Power of the SORA AI lastest leapRishantSharmaFr
 
Generative AI or GenAI technology based PPT
Generative AI or GenAI technology based PPTGenerative AI or GenAI technology based PPT
Generative AI or GenAI technology based PPTbhaskargani46
 
Thermal Engineering-R & A / C - unit - V
Thermal Engineering-R & A / C - unit - VThermal Engineering-R & A / C - unit - V
Thermal Engineering-R & A / C - unit - VDineshKumar4165
 
KubeKraft presentation @CloudNativeHooghly
KubeKraft presentation @CloudNativeHooghlyKubeKraft presentation @CloudNativeHooghly
KubeKraft presentation @CloudNativeHooghlysanyuktamishra911
 

Último (20)

Booking open Available Pune Call Girls Pargaon 6297143586 Call Hot Indian Gi...
Booking open Available Pune Call Girls Pargaon  6297143586 Call Hot Indian Gi...Booking open Available Pune Call Girls Pargaon  6297143586 Call Hot Indian Gi...
Booking open Available Pune Call Girls Pargaon 6297143586 Call Hot Indian Gi...
 
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night StandCall Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
 
Design For Accessibility: Getting it right from the start
Design For Accessibility: Getting it right from the startDesign For Accessibility: Getting it right from the start
Design For Accessibility: Getting it right from the start
 
Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar ≼🔝 Delhi door step de...
Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar  ≼🔝 Delhi door step de...Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar  ≼🔝 Delhi door step de...
Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar ≼🔝 Delhi door step de...
 
(INDIRA) Call Girl Bhosari Call Now 8617697112 Bhosari Escorts 24x7
(INDIRA) Call Girl Bhosari Call Now 8617697112 Bhosari Escorts 24x7(INDIRA) Call Girl Bhosari Call Now 8617697112 Bhosari Escorts 24x7
(INDIRA) Call Girl Bhosari Call Now 8617697112 Bhosari Escorts 24x7
 
Call Girls Pimpri Chinchwad Call Me 7737669865 Budget Friendly No Advance Boo...
Call Girls Pimpri Chinchwad Call Me 7737669865 Budget Friendly No Advance Boo...Call Girls Pimpri Chinchwad Call Me 7737669865 Budget Friendly No Advance Boo...
Call Girls Pimpri Chinchwad Call Me 7737669865 Budget Friendly No Advance Boo...
 
Intro To Electric Vehicles PDF Notes.pdf
Intro To Electric Vehicles PDF Notes.pdfIntro To Electric Vehicles PDF Notes.pdf
Intro To Electric Vehicles PDF Notes.pdf
 
Call Girls Wakad Call Me 7737669865 Budget Friendly No Advance Booking
Call Girls Wakad Call Me 7737669865 Budget Friendly No Advance BookingCall Girls Wakad Call Me 7737669865 Budget Friendly No Advance Booking
Call Girls Wakad Call Me 7737669865 Budget Friendly No Advance Booking
 
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 BookingVIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
 
VIP Call Girls Palanpur 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Palanpur 7001035870 Whatsapp Number, 24/07 BookingVIP Call Girls Palanpur 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Palanpur 7001035870 Whatsapp Number, 24/07 Booking
 
Work-Permit-Receiver-in-Saudi-Aramco.pptx
Work-Permit-Receiver-in-Saudi-Aramco.pptxWork-Permit-Receiver-in-Saudi-Aramco.pptx
Work-Permit-Receiver-in-Saudi-Aramco.pptx
 
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
 
Thermal Engineering -unit - III & IV.ppt
Thermal Engineering -unit - III & IV.pptThermal Engineering -unit - III & IV.ppt
Thermal Engineering -unit - III & IV.ppt
 
Bhosari ( Call Girls ) Pune 6297143586 Hot Model With Sexy Bhabi Ready For ...
Bhosari ( Call Girls ) Pune  6297143586  Hot Model With Sexy Bhabi Ready For ...Bhosari ( Call Girls ) Pune  6297143586  Hot Model With Sexy Bhabi Ready For ...
Bhosari ( Call Girls ) Pune 6297143586 Hot Model With Sexy Bhabi Ready For ...
 
Unleashing the Power of the SORA AI lastest leap
Unleashing the Power of the SORA AI lastest leapUnleashing the Power of the SORA AI lastest leap
Unleashing the Power of the SORA AI lastest leap
 
Generative AI or GenAI technology based PPT
Generative AI or GenAI technology based PPTGenerative AI or GenAI technology based PPT
Generative AI or GenAI technology based PPT
 
Thermal Engineering-R & A / C - unit - V
Thermal Engineering-R & A / C - unit - VThermal Engineering-R & A / C - unit - V
Thermal Engineering-R & A / C - unit - V
 
NFPA 5000 2024 standard .
NFPA 5000 2024 standard                                  .NFPA 5000 2024 standard                                  .
NFPA 5000 2024 standard .
 
KubeKraft presentation @CloudNativeHooghly
KubeKraft presentation @CloudNativeHooghlyKubeKraft presentation @CloudNativeHooghly
KubeKraft presentation @CloudNativeHooghly
 
Call Girls in Netaji Nagar, Delhi 💯 Call Us 🔝9953056974 🔝 Escort Service
Call Girls in Netaji Nagar, Delhi 💯 Call Us 🔝9953056974 🔝 Escort ServiceCall Girls in Netaji Nagar, Delhi 💯 Call Us 🔝9953056974 🔝 Escort Service
Call Girls in Netaji Nagar, Delhi 💯 Call Us 🔝9953056974 🔝 Escort Service
 

Hybrid Piezoelectric FGM plate shape control

  • 1. DEFLECTION CONTROL OF HYBRID PIEZOELECTRIC FUNCTIONALLY GRADED PLATE S. A. Patare & K. M. Bajoria Department of Civil Engineering, IIT Bombay
  • 2. Introduction ● Shape control of FGM plate coupled with Piezoelectric material ● Four variable plate theory for simple formulation ● Constant displacement feedback control algorithm ● Approximate analytical solution for simply supported and clamped plate ● Static deflection control
  • 4. Displacement Field [03] u=uo−z ∂wb ∂ x − (4 z3 3ht 2 ) ∂ws ∂x v=vo−z ∂wb ∂ y − (4z3 3ht 2 ) ∂ws ∂ y w=wb+ws { σx σ y σxy σxz σ yz }= [ C11 C12 0 0 0 C12 C22 0 0 0 0 0 C66 0 0 0 0 0 C44 0 0 0 0 0 C55 ]{ ϵx ϵy γxy γxz γ yz }− [ 0 0 ¯e31 0 0 ¯e31 0 0 0 e15 0 0 0 e15 0 ]{ Ex Ey Ez } { Dx Dy Dz }= [ 0 0 0 e15 0 0 0 0 0 e15 ¯e31 ¯e31 0 0 0 ]{ ϵx ϵy γxy γxz γ yz }+ [ Ω11 0 0 0 Ω11 0 0 0 Ω33 ]{ Ex Ey Ez } Constitutive Law[05]► Electric Displacement[05]►
  • 5. Electric Potential Function Φ= { Π T [1− (z−h/2−hp/2 hp/2 ) 2 ]+AT z+BT ;for⟨h 2 z⩽⩽ h 2 +hp ⟩ Π B [1− (− z−h/2−hp/2 hp/2 ) 2 ]+AB z+BB ;for⟨− h 2 −hp z⩽⩽− h 2 ⟩} Φ(z=± h 2 )=0, Dz (z=±(h 2 +hp))=0Boundary Conditions for Open Circuit ► BT =−(h 2)AT ;BB=(h 2)AB Φ= {ΠT [1− (z −h/2−hp /2 hp/2 ) 2 ]+ AT (z− h 2) for⟨h 2 ⩽z⩽ h 2 +hp ⟩ ΠB [1− (− z−h/2−hp/2 hp/2 ) 2 ]+ AB(z+ h 2) for ⟨− h 2 −hp ⩽z ⩽− h 2 ⟩
  • 6. Hamilton’s Principle 0=∫ 0 T (δU+δV−δK)δt δU=∫ A ∫ − h 2 − hp h 2 +hp (σx δϵx +σy δϵy +σxy δγxy +σyz δγyz +σxz δγxz)dzdA δV =−∫ A q δ (wb+ws)dA ◄Strain Energy Variation Work Done Variation►
  • 7. Governing Formulation δu0 : ∂Nx ∂x + ∂ Nxy ∂ y =0 δv0: ∂ N y ∂ y + ∂ Nxy ∂ x =0 δ wb : ∂ 2 Mx b ∂ x 2 + ∂ 2 M y b ∂ y 2 +2 ∂ 2 M xy b ∂ x ∂ y +qw=0 δ ws: ∂ 2 M x s ∂ x 2 + ∂ 2 M y s ∂ y 2 +2 ∂ 2 M xy s ∂ x ∂ y + ∂Qxz ∂ x + ∂Q yz ∂ y +qw=0
  • 8. ∫ h 2 h 2 +hp (∂ Dx ∂x + ∂Dy ∂ y + ∂Dz ∂z )dz+ ∫ − h 2 −hp − h 2 (∂Dx ∂ x + ∂ Dy ∂ y + ∂Dz ∂z )dz=0 λ1(∂2 ws ∂ x 2 + ∂2 ws ∂ y 2 )− λ2(∂2 wb ∂ x 2 + ∂2 wb ∂ y 2 )−λ3(∂2 ΠT ∂ x 2 + ∂2 ΠT ∂ y 2 ) − λ4(∂ 2 ΠB ∂ x2 + ∂ 2 ΠB ∂ y2 )− λ5 ΠT − λ6 ΠB }=0 Fifth Governing Equation► Fifth Equation & Maxwell’s Law ◄Displacement Feedback Control Law [02] ΠT =Gd Π B+Gv ˙Π B
  • 9. Approximate Analytical Solution [04] u0=∑ m=1 ∞ ∑ n=1 ∞ U eiwt ∂ XM (x) ∂x YN ( y ) v0=∑ m=1 ∞ ∑ n=1 ∞ V eiwt XM (x) ∂YN ( y) ∂ y wb=∑ m=1 ∞ ∑ n=1 ∞ W b eiwt XM (x)YN ( y) ws=∑ m=1 ∞ ∑ n=1 ∞ W s eiwt XM (x)YN ( y ) Π=∑ m=1 ∞ ∑ n=1 ∞ Π eiwt XM (x)YN ( y)
  • 10. Numerical ● A square plate of 200mm size ● Thickness of FGM plate is 1 mm while Piezo layers is 0.1 mm ● Uniform load of 100 N/m2 ● FGM core of Ti-6Al-4V and Aluminium Oxide ● Power law is taken 2 (constant)
  • 11. Shape control for simpy supported plate
  • 12. Shape control for clamped Plate
  • 13. Conclusion ● It is possible to consider simple four variable plate theory for analysis of hybrid piezoelectric FGM plate ● Open circuit potential function for four variable plate theory is proposed and validated ● Good results are obtained for static bending of plate ● Approximate analytical solution further simplies the analysis for other boundary condition ● Smart hybrid piezoelectric FGM plate model is developed with minimum computational efforts ● Change in power law, aspect ratio and FGM materials can be considered for further study
  • 14. References 1) P. A. Jadhav and K. M. Bajoria: Stability analysis of thick piezoelectric metal based FGM plate using first order and higher order shear deformation theory, Int. J. Mech. Mater. Des., 11, 2015, pp. 387-403 2) T. Nguyen-Thoi, K. Nguyen-Quang, H. Dang-Trung, V. Ho-Huu and H. Luong-Van: Analysis and control of FGM plates integrated with piezoelectric sensors and actuators using cell-based smoothed discrete shear gap method, Compos. Struct., 165, 2016, pp. 115-129. 3) Seung-Eock Kim and Huu-Tai Thai: A simple higher-order shear deformation theory for bending and free vibration analysis of functionally graded plates, Compos. Struct., 96, 2013,pp. 165-173. 4) M. R. Barati, H. Shahverdi and A. M. Zenkour: Electro-mechanical vibration of smart piezoelectric FG plates with porosities according to a refined four- variable theory, Mech. Adv. Mater. Struct., 24 (12), 2017, pp. 987-998. 5) H. F. Tiersten: Linear piezoelectric plate vibrations, Plenum Press, New York, 1969.