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University Electromagnetism: Electric field and potential of a capacitor that is partly filled (vertically or horizontally) with dielectric material (connected or not to a battery)
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Partly filling a capacitor with dielectric 1
Filling a capacitor with a dielectricII: Partial filling
© Frits F.M. de Mul
Partly filling a capacitor with dielectric 2
Partial filling a capacitor (1)
Available: Flat capacitor : = surface area A , = distance of plates d , = no fill (εr = 1) .
A
d Assume: initially, plates are charged with +Q , -Q.
+Q
-Q
Question: What will happen with Q , σ, E, D, ∆V and C upon PARTIAL filling the capacitor with dielectric material (with εr > 1) ???
Partly filling a capacitor with dielectric 3
Partial filling a capacitor (2)
A. Series B. Parallel
I. Free
II. Connected to battery
Options:
Partly filling a capacitor with dielectric 4
Partial filling a capacitor (3)
A B
I
II
Suppose:• when empty: Q0 , V0 .....etc.• fillingfilling for 1/3 of volumevolume• with εr = 5
Assumption :
no “edge effects” : d << plate dimensions
Consequences :
no E-field leakage
• planar symmetry everywhere
• Gauss’ Law is applicable
• straight field lines (E and D)
Partly filling a capacitor with dielectric 5
RelationsA
d
+Q
-Q
Qf
Gauss:
D dA• = = ∫∫∫∫∫ Q dVf fVA
ρ
D
E Material constants:
D = ε0 εr E
Potential:
∆Vpath
= •∫ E dl
∆V
Capacitance:
C Q Vf= / ∆
AADQ ff .. σ==
dEV .=∆
Partly filling a capacitor with dielectric 6
Options: main featuresOptions: main features
A.I and B.I: total charge unchanged
A B
I
IIA.II and B.II: total potential unchanged
A.I and A.II: potentials in series
B.I and B.II: potentials parallel
Suppose:• when empty: Q0 , V0 ......• when filled: Q’, V’ , ......• fillingfilling for 1/3 of volumevolume
(depth or surface area)• with εr = 5
Partly filling a capacitor with dielectric 7
A.I. Horizontal fill, not A.I. Horizontal fill, not connectedconnected
Qf
DE
∆V
db , dt : bottom and top layerFill: db = d0 /3 with εr = 5
dt = 2d0 /3 with εr = 1db
dt
Qf,t’
-Qf,b’
Qf’ D’ E’ d’
51
31
∆V’
151
32
32
1511
∆V’ C’
1115
o = oldt = topb = bottom} total
11
Start
Partly filling a capacitor with dielectric 8
A.II. Horizontal fill, connectedA.II. Horizontal fill, connectedQf
D
E
∆VFill: db = d0 /3 with εr = 5
dt = 2d0 /3 with εr = 1
Qf’ D’ E’ d’51
31
∆V’
151
1510
32 =3
2
∆V’
C’
1115
db
dt
Qf,t
-Qf,b
∆V0
∆V’
111
1110
11
E’113
1115
32
1110 : =
1115
1115
D’ Qf’
o = oldt = topb = bottom} total
Consider ratios:
11
1115
<01115
Partly filling a capacitor with dielectric 9
B.I. Vertical fill, not connectedB.I. Vertical fill, not connectedQf
D
E
∆VFill: Ar = A0 /3 with εr = 5
Al = 2A0 /3 with εr = 1
Qf’D’E’
73
51
715 : =
73
E’ C’
37
o = oldl = leftr = right } total
Qf,l’
-Qf,r’
Qf,r’
-Qf,l’
Al Ar
Consider ratios:
∆V’
11
32
31
A’
32
Qf’
757
235
Qf’
715
31
75 : =
73
32
72 : =
D’
×5
73
73
∆V’
Partly filling a capacitor with dielectric 10
B.II. Vertical fill, connectedB.II. Vertical fill, connectedQf
D
E
∆VFill: Ar = A0 /3 with εr = 5
Al = 2A0 /3 with εr = 1
Qf’D’E’
×5
C’
37
o = oldl = leftr = right } total
Consider ratios:
∆V’
11 3
2
31
A’
32
Qf’
37
35
Qf,l’
-Qf,r’
Qf,r’
-Qf,l’
Al Ar
∆V0
Partly filling a capacitor with dielectric 11
Options: overviewOptions: overview
BB.I and B.II: potentials parallel
C : 15/11 xQf : unchanged∆V : 11/15 x
∆V : unchangedQf : 15/11 x
C : 7/3 xQf : unchanged∆V : 3/7 x
∆V : unchangedQf : 7/3 x
AA.I and A.II: potentials in series
I II
Partly filling a capacitor with dielectric 12
With combination rulesWith combination rules
B B.I and B.II: parallel
A A.I and A.II: series
I II d
AC rεε0= Filling with εr=5
in 1/3 of volume
A
d
A
d
A
d
CCC bt .15
11
.
3/2
5.
3/11
'
1
000 εεε=+=+=
01115' CC =
d
A
d
A
d
ACCC rl
.
3
73/.5.3/2.' 000 εεε =+=+= 03
7' CC =
Partly filling a capacitor with dielectric 13
Finally...Finally...
B B.I and B.II: parallel
A
A.I and A.II: seriesI II
bt CCC
11
'
1 +=
rl CCC +=' the end
fQ∫∫ =• dAD
D = ε0 εr E∫ •=∆ dlEV
Qf
DE
∆V
VQC f ∆= / AADQ ff .. σ==
dEV .=∆