Modul
e
e
4and5
Linear
a
a
ndNonl
i
i
near
Die
l
l
ectricC
e
e
ramics
1. Plot t
h
reaso
n
2. A 2 c
m
7.2 μ
F
a. P
b.
E
c.
E
3. Si ha
s
diele
c
Obse
r
such
b
4. A 0.5
mate
r
5. Follo
w
a.
D
b.
D
c. P
d.
U
w
6. Plot t
h
Titan
a
7. Piezo
show
n
actin
g
equal
h
e dielectric
c
n
s for each r
e
m
diameter a
n
F
and a dissi
p
ermittivity o
f
E
lectric loss f
a
E
lectrical susc
s
an atomic r
a
c
tric constant
r
ved value is
b
ehavior.
cm thick die
r
ials if used a
t
w
ing are two
D
erive the ex
p
D
erive the ex
p
lot these qua
n
U
nder what c
o
w
ould be the
p
h
e free energ
y
a
te and sche
m
electric ZnS
u
n
in the figur
e
g
such tha
t
te
n
magnitude a
r
C
c
onstant and
l
e
gion in each
n
d 0.25 mm
t
p
ation factor
o
f
dielectric
a
ctor
eptibility
a
dii of 110 p
m
contribution
?
about 11-12.
lectric mater
i
t
100 Hz and
electrical cir
c
p
ressions of t
h
p
ressions of t
h
n
tities as a fu
n
o
nditions, wo
u
p
hysical mea
n
y
-displacem
e
m
atically sho
w
u
pon applica
t
e
below. Thi
s
n
sile stresses
r
e along [1
1
0
R
l
oss vs frequ
e
material.
t
hick disk of
s
o
f 72. Deter
m
m
. What type
?
Calculate t
h
Compare an
d
i
al has a diel
e
1000V, calc
u
c
uits (series
R
h
e impedanc
e
h
e real and i
m
n
ction of fre
q
u
ld the Deby
e
n
ing?
e
nt and susce
p
w
the behavi
o
t
ion of stress
s
crystal is su
b
are along [1
1
0
] and [
1
10
]
e
ncy for two
m
s
teatite was
m
m
ine the follo
w
of mechanis
m
h
e dielectric
c
d
comment o
n
e
ctric constan
t
u
late the pow
e
R
-C and para
l
e
and admitta
n
m
aginary diel
e
q
uency.
e
equations l
o
p
tibility vs te
m
o
r across its
C
becomes no
n
b
ject to the e
q
1
0] and [
1 1
0
]
directions.
A
m
aterials: G
e
e
and ZrO
2
. B
r
r
iefly explai
n
m
easured and
w
ing propert
i
m
s you expe
c
c
onstant of Si
n
the differen
t
of 75 and l
o
e
r loss densit
y
l
lel R-C). Att
n
ce of both c
i
e
ctric consta
n
o
ok similar to
m
perature pl
o
C
urie tempera
t
n
-centrosym
m
q
uilibrium ar
r
0
] directions
A
nswer the f
o
C
R
found to hav
i
es:
c
t in Si to con
t
using appro
p
ce, if any, an
d
o
ss tangent o
f
y
in the diele
c
empt the foll
o
i
rcuits.
n
t and loss ta
n
obtained fro
m
o
ts for ferroel
t
ure.
m
etric. Its (00
1
r
angement o
f
and compres
s
o
llowing:
C
R
e a capacitan
c
t
ribute to its
p
riate express
i
d
any reason
s
f
20. If the
c
tric.
o
wing:
n
the
c
e of
i
on.
s
for
n
gent.
m
(b). What
ectric Bariu
m
m
1
) plan view
i
f
shear stress
e
s
ive stresses
o
i
s
e
s τ
o
f
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