Capacitance and Resistance
description
Transcript of Capacitance and Resistance
![Page 1: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/1.jpg)
Resistance and Resistance and Capacitance Capacitance Electrostatic Electrostatic Boundary value problems;Boundary value problems;
Sandra Cruz-Pol, Ph. D.Sandra Cruz-Pol, Ph. D.INEL 4151 INEL 4151 ch6ch6
Electromagnetics IElectromagnetics IECE UPRMECE UPRM
Mayagüez, PRMayagüez, PR
https://www.youtube.com/watch?v=JEIkB_8v7qk
![Page 2: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/2.jpg)
Last Chapters: Last Chapters: we knew either V or we knew either V or charge distribution, to find E,Dcharge distribution, to find E,D..
NOW: we NOW: we only know values of V or only know values of V or Q at some places (boundaries). Q at some places (boundaries).
![Page 3: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/3.jpg)
Some applicationsSome applications
ResistanceResistance CapacitorsCapacitors Microstrip lines capacitanceMicrostrip lines capacitance
![Page 4: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/4.jpg)
To find E, we will use:To find E, we will use:
PoissonPoisson’’ss equation: equation:
LaplaceLaplace’’ss equation: equation: (if charge-free)(if charge-free)
They can be derived from They can be derived from GaussGauss’’s Laws Law
02 V
vV 2
VE
ED v
![Page 5: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/5.jpg)
Depending Depending on the geometryon the geometry::
We use appropriate coordinates:We use appropriate coordinates:
Cartesian:Cartesian:
cylindrical:cylindrical:
spherical:spherical:
vV 2
v
z
V
y
V
x
V
2
2
2
2
2
2
v
z
VVV
2
2
2
2
2
11
vV
r
V
rr
Vr
rr
2
2
2222
2 sin
1sin
sin
11
(It’s a scalar)
1. Solve for Laplace or Poisson depending on value of v
2. Use Separation of Variables to solve for V3. Apply Boundary values to find unique answer for V
02 V
![Page 6: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/6.jpg)
ResistanceResistance Defined as:Defined as:
The problem of finding the resistance of a conductor of nonuniform cross section can be solved by :1.Choose a suitable coordinate system2.Assume Vo a the potential difference between conductor’s terminals3.Solve Laplace’s eq. for V, then obtain E and I from and4. Finally obtain R as Vo/I
![Page 7: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/7.jpg)
Resistance PE 6.8Resistance PE 6.8A disc of thicknessA disc of thickness tt has radius has radius bb and a central hole of radius a. Take and a central hole of radius a. Take = conductivity, find R = conductivity, find R
a.a.between hole and rim of the diskbetween hole and rim of the disk
b.b.Between the 2 fat sides of diskBetween the 2 fat sides of disk
![Page 8: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/8.jpg)
P.E. 6.8 Part a) find Resistance of disk P.E. 6.8 Part a) find Resistance of disk of radius of radius bb and central hole of radius and central hole of radius aa..
oVbV
aVBC
)(
0)(:
aab
VV o
ln/ln
ˆd
dVVE
)/ln(
2
ab
tVSdEI o
S
ˆddzSd
a
t
BAV ln
b
01
V0
112
2
2
2
2
z
VVV
![Page 9: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/9.jpg)
P.E. 6.8 Part b) find Resistance of disk P.E. 6.8 Part b) find Resistance of disk Between the 2 fat sides of diskBetween the 2 fat sides of disk
S
oo
SdE
V
I
VR
a
t
b
![Page 10: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/10.jpg)
ResistenceResistence
Resist the flow of
electrons
0 Negro
1 Marrón
2 Rojo
3 Naranja
4 Amarillo
5 Verde
6 Azul
7 Violeta
8 Gris
99 BlancoBlanco
![Page 11: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/11.jpg)
CapacitanceCapacitance Is defined as the ratio of Is defined as the ratio of
the charge on one of the the charge on one of the plates to the potential plates to the potential difference between the difference between the plates:plates:
Assume Q and find V Assume Q and find V ((Gauss or CoulombGauss or Coulomb))
Assume V and find Q Assume V and find Q ((LaplaceLaplace))
And substitute E in the And substitute E in the equation.equation.
FaradsV
QC
FldE
SdE
V
QC
l
S
The (-) sign in V can be ignored because we want the absolute value of V
![Page 12: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/12.jpg)
Two cases: CapacitanceTwo cases: Capacitance
1.1. Parallel plateParallel plate
2.2. Coaxial Coaxial
![Page 13: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/13.jpg)
Parallel plate CapacitorParallel plate Capacitor Charge Charge QQ and – and –QQ
oror
Dielectric,
Plate area, S
S
Qs
d
S
V
QC
S
Qddx
S
QldEV
dd
00
SESdEQ x
![Page 14: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/14.jpg)
Effect of Effect of rr on Capacitance on Capacitance
d
S
V
QC
![Page 15: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/15.jpg)
Coaxial CapacitorCoaxial Capacitor
Charge +Charge +QQ & & -Q-Q
LESdEQ 2
abL
V
QC
ln
2
Dielectric,
Plate area, S
S
Qd
S
QdSEV
dd
00
++
+
+
+
-
-
-
-
--
-
-
-
c
a
b
L
Qd
L
QldEV
a
b
ln2
ˆˆ2
![Page 16: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/16.jpg)
Capacitors connectionCapacitors connection
SeriesSeries
ParallelParallel
21 CCC
21
111
CCC
![Page 17: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/17.jpg)
How to tell if C is in:How to tell if C is in: Parallel:Parallel: when they have same voltage when they have same voltage
across their plates. across their plates. EE is || is || to interface. to interface.
SeriesSeries: when : when E & D are normal E & D are normal to the to the dielectric interface.dielectric interface.
21
1221
111
CCC
21 CCC
![Page 18: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/18.jpg)
So In summary we obtainedSo In summary we obtained::Capacitor C R (not derived)
Parallel Plate
Coaxial
Spherical(not derived)
ba11
4
S
d
ab
L
ln
2d
S
Lab
2
ln
4
11
ba
![Page 19: Capacitance and Resistance](https://reader035.fdocuments.in/reader035/viewer/2022062422/56813e93550346895da8dc39/html5/thumbnails/19.jpg)
ba
a CCC
CCC
2
2
FpC 3.14
They are connected in parallel and series
800,91
000,472
21mm
mm5
aC
2CbC
pFmmd
SC o
a 3.17)5.2(
)1000/5.0(800,9 2
Fmmd
SC o
b 7.8)5(
1000/)5.0(9800 2
pFmmd
SC o 3.8
)5.2(
1000/5.047000 2
2
Find the capacitance ofFind the capacitance of
Barium titanatepolymer