Upload
others
View
5
Download
0
Embed Size (px)
Citation preview
1
Dielectric behavior
Topic 9
Reading assignment• Askeland and Phule, The Science
and Engineering of Materials, 4th
Ed., Sec. 18-8, 18-9 and 18-10.• Shackelford, Materials Science for
Engineering, Sec. 15.4.• Chung, Composite Materials, Ch. 7.
Insulators and dielectric properties
• Materials used to insulate an electric field from its surroundings are required in a large number of electrical and electronic applications.
• Electrical insulators obviously must have a very low conductivity, or high resistivity, to prevent the flow of current.
• Porcelain, alumina, cordierite, mica, and some glasses and plastics are used as insulators.
Dielectric strength• Maximum electric field that an insulator
can withstand before it loses its insulating behavior
• Lower for ceramics than polymers• Dielectric breakdown - avalanche
breakdown or carrier multiplication
2
Polarization in dielectrics• Capacitor – An electronic device, constructed
from alternating layers of a dielectric and a conductor, that is capable of storing a charge. These can be single layer or multi-layer devices.
• Permittivity - The ability of a material to polarize and store a charge within it.
• Linear dielectrics - Materials in which the dielectric polarization is linearly related to the electric field; the dielectric constant is not dependent on the electric field.
• Dielectric strength - The maximum electric field that can be maintained between two conductor plates without causing a breakdown.
Polarization mechanisms in materials:(a) electronic, (b) atomic or ionic, (c) high-frequency dipolar or orientation (present in ferroelectrics), (d) low-frequency dipolar (present in linear dielectrics and glasses), (e) interfacial-space charge at electrodes, and (f ) interfacial-space charge at heterogeneities such as grain boundaries.
©2003 Brooks/Cole, a division of Thomson Learning, Inc. Thomson Learning™ is a trademark used herein under license.A charge can be stored at the conductor plates in a vacuum (a). However, when a dielectric is placed between the plates (b), the dielectric polarizes and additional charge is stored.
3
, AQ = Do
, dV = ∑
Do = εo Σ
εo = 8.85 x 10-12 C/(V.m)
, dA
dA
VQC = Slope oo
oεε
=ΣΣ
==
4
, AQD =D om
κκ =
Dm = κ εo Σ = ε Σ
, Cd
Ad
AVQ = C o
oom κ
κεκεκ==
ΣΣ
=
P = Dm − Do= κ εoΣ − εoΣ= (κ − 1) εoΣ
E
5
, 1 = Q
QQ−
− κκ
, P 1= oΣ
=−ε
κχ
(bound charge)d = (κ − 1) Qd
, PA1)Q(
Ad1)Qd( =
VolumemomentDipole
=−
=− κκ
mCQ = V κ
κQ = Dm A = ε Σ A
xA
xA
= C om
εκε=
x
xAA = V Σ=
Σεε
6
Table 7.6 Values of the relative dielectric constant κ of various dielectric materials at 1 kHz (Data from Ceramic Source ’86, American Ceramic Society, Columbus, Ohio, 1985, and Design Handbook for DuPont Engineering Plastics).
3.6Polyester
3.7Nylon-66 reinforced with glass fibers4.1-5.3Cordierite
6.7BeO (99.5%)9.8Al2O3 (99.5%)
___κ__Material
Σ = ( ),sinicosˆeˆ ti tt ωωω += ΣΣ
Dm = ( ) ( )[ ],)tsin(itcosD̂eD̂ mti
m δωδωδω −+−=−
( ) ,eˆeD̂ titim
ωδω εΣ=−
( ),sinicosˆD̂
eˆD̂ mi-m δδε δ −==
ΣΣ
, ofpart Real ofpart Imaginary tan
κκδ −=
7
, dtdvC
dt dQic ==
ν = V sin ωt
, T
2f2 ππω ==
, cosCVdtdvCic tωω==
cosC1/
V tωω
=
⎟⎠⎞
⎜⎝⎛ +
2sin πωt
2
sincos2
cossin πωπω tt +=
, cos tω=
, 2
sinC1/
Vic ⎟⎠⎞
⎜⎝⎛ +=
πωω
t
, sinRV
RiR tων
==
, 2
sinC1/
Vi c ⎟⎠⎞
⎜⎝⎛ +=
πωω
t
, sinRV
RiR tων
==
, CR1
CVV/Rtan
ωωδ ==
8
Energy stored = , di0
C∫τ
ν t
, dcossinCV0
2 ttt ωωωτ
∫=
, d2sin2
CV
0
2
tt∫=τ
ωω
[ ] , 2cos4
CV0
2τω
ωω t−=
( ) , 12cosCV41 2 −−= ωτ
Maximum energy stored = ½ CV2
This occurs when cos 2ωt = -1
Energy loss per cycle due to conduction through the resistor R
Energy loss = dsinsinR
V /2
0
2
ttt∫ωπ
ωω
( ) ( ) d2cos121
RV 2
0
2
tt ωωω
π
∫ −=
2sin21
21
RV
2
0
2 π
ωωω ⎥
⎦
⎤⎢⎣
⎡⎟⎠⎞
⎜⎝⎛ −= tt
( ) 000221
RV2
⎥⎦⎤
⎢⎣⎡ +−−= π
ω
. R
V2
ωπ
=
9
The smaller is R, the greater is the energy loss.
2/CV2
R/Vstoredenergymaximum2
cycleperlostEnergy2
2
πωπ
π=
×
δω
tan CR1
==
10
Frequency dependence of polarization mechanisms. On top is the change in the dielectric constant with increasing frequency, and the bottom curve represents the dielectric loss.
Quartz – polarization only under stress
11
©2003 Brooks/Cole, a division of Thomson Learning, Inc. Thomson Learning™ is a trademark used herein under license.
(a) The oxygen ions are at face centers, Ba+2 ions are at cube corners and Ti+4 is at cube center in cubic BaTi03.
(b) In tetragonal BaTi03 ,the Ti+4 is off-center andthe unit cell has a net polarization.
12
Different polymorphs of BaTiO3 and accompanying changes in lattice constants and dielectric constants.
Table 7.3 Contribution to dipole moment of a BaTiO3 unit cell by each type of ion.
Total = 17 x 10-30
4.2 x 10-30-0.13(10-10)(-2)(1.6 x 10-19)O2- (top and bottom of cell)
6.4 x 10-30-0.10(10-10)2(-2)(1.6 x 10-19)2O2- (side of cell)6.4 x 10-30+0.10(10-10)(+4)(1.6 x 10-19)Ti4+
00(+2)(1.6 x 10-19)Ba2+
Dipole moment (C.m)
Displacement (m)
Charge (C)Ion
3302
30
m103.984.03C.m1017
−
−
×××
=P
= 0.27 C.m-2
13
-Ec E
14
(b) single crystal.
c) Polycrystalline BaTiO3 showing the influence of the electric field on polarization.
The effect of temperature and grain size on the dielectric constant of barium titanate. Above the Curie temperature, the spontaneous polarization is lost due to a change in crystal structure and barium titanate is in the paraelectric state. The grain size dependence shows that similar to yield-strength dielectric constant is a microstructure sensitive property.
Effect of grain size Ferroelectric domains in polycrystalline BaTiO3.
15
E
,tt
logru
uu
1
2
1
12 =−
Piezoelectric aging rate rDepoling
u : parameter such as capacitancet: number of days after polarization
Ferroelectric - A material that shows spontaneous and reversible dielectric polarization.
Piezoelectric – A material that develops voltage upon the application of a stress and develops strain when an electric field is applied.
16
©2003 Brooks/Cole, a division of Thomson Learning, Inc. Thomson Learning™ is a trademark used herein under license.The (a) direct and (b) converse piezoelectric effect. In the direct piezoelectric effect, applied stress causes a voltage to appear. In the converse effect (b), an applied voltage leads to development of strain.
Direct piezoelectric effect
Reverse (converse) piezoelectric effect
17
E
E
18
P = dσ∂P = d ∂σ
σκε
∂∂
Σ= od
d: Piezoelectric coupling coefficient (piezoelectric charge coefficient)
Direct piezoelectric effect
Table 7.1 The piezoelectric constant d (longitudinal) for selected materials
80 x 10-12PbNb2O6
250 x 10-12PbZrTiO6
100 x 10-12BaTiO3
2.3 x 10-12Quartz
Piezoelectric constant d (C/N = m/V)Material
( )1o −∂
=Σ∂κε
P
( )1o −∂
=Σ∂κεσd
∂V = l∂Σ,
( )1o −∂
=∂κεσdV l
P = Dm − Do
= κ εoΣ − εoΣ
= (κ − 1) εoΣ
( )1o −∂
=∂κεσdV l
( ) 1 oεκ −
=dg
∂V = lg∂σg: piezoelectric voltage coefficient
19
Reverse piezoelectric effect
S = dΣ∂S = d∂Σ
PS
=Σσ
PS∂∂
=∂Σ∂σ
Reverse piezoelectric effect
( ) 1 o Σ∂−∂
=∂Σ∂
εκσS
( ) 1 oΣ
=Σ
εκσ -S
( ) 1 oεκσ −
=Σ d
( ) 1 oεκσ −
=∂Σ∂ d
S = dΣ
( ) 1 oΣ
=Σ
εκσ -S
20
Σ = gσ∂Σ = g∂σ
( ) 1 oεκσ −
=Σ d
( ) 1 oεκ −
=dg
σ = ES
Σ = gES
Hooke’s law
Σ = gσ
gE
S Σ=
1gE
d =
1gd
E =
S = dΣ
energy electricalinput
energymechanicaloutput=2k
energy mechanicalinput energyelectricaloutput
=2k
Electromechanical coupling factor(electromechanical coupling coefficient) k
21
Substitution of A and B sites in BaTiO3PZT: PbZrO3-PbTiO3 solid solution or lead zirconotitanate
Table 7.4 Properties of commercial PZT ceramics
0.710.675k15
-0.334-0.388k31
0.700.752k33
Piezoelectric coupling factors496741d15
-123-274d31
289593d33
Piezoelectric coefficients (10-12 m/V)328193Curie temperature (Tc, °C)
0.0040.02Dielectric loss (tan δ at 1 kHz)13003400Permittivity (κ at 1 kHz)
PZT4(hard)
PZT-5H(soft)Property
22
Table 7.2 Measured longitudinal piezoelectric coupling coefficient d, measured relative dielectric constant κ, calculated piezoelectric voltage coefficient g and calculated voltage change resulting from a stress change of 1 kPa for a specimen thickness of 1 cm in the direction of polarization.
15151024136PZT
8.58.5493.62 ± 0.40Cement paste with carbon fibers
8.78.72700208 ± 16Cement paste with steel fibers and PVA
2.22.2350.659 ± 0.031Cement paste (plain)
Voltage change (mV)†g (10-4 m2/C)†κ†d (10-13 m/V)*Material
Piezopolymer
Bimorph (bi-strip)
Cantilever beam configuration for actuation
Composites with piezoelectric/ferroelectric material sandwiched by metal faceplates fo enhancing the piezoelectric coupling coefficient
Moonie
Cymbal
23
Pyroelectric - The ability of a material to spontaneously polarize and produce a voltage due to changes in temperature.
,dTd
dTdPp o
κε Σ==
p = pyroelectirc coefficientP = polarization
Table 7.5 Pyroelectric coefficient (10-6 C/m2.K)
0.002Cement paste
27PVDF
380PZT
20BaTiO3
o 1)-(Px = V
εκ
σεκσεκσ dd
dd
dd P
)1(xx
1)-(P = V
oo −+
Voltage sensitivity
Compliance Piezoelectric coupling coefficient d
24
Piezoelectric composite • When any material undergoes polarization (due to an applied electric field), its ions and electronic clouds are displaced, causing the development of a mechanical strain in the material. polarization.
• This phenomenon is known as the electrostriction.
Examples of ceramic capacitors. (a)Single-layer ceramic capacitor
(disk capacitors). (b) Multilayer ceramic capacitor
(stacked ceramic layers).