theory of electric networks: the two-point resistance and impedance
DESCRIPTION
Theory of electric networks: The two-point resistance and impedance. F. Y. Wu. Northeastern University Boston, Massachusetts USA. Z. a. b. Impedance network. Ohm’s law. Z. I. V. Combination of impedances. Impedances. - PowerPoint PPT PresentationTRANSCRIPT
Theory of electric networks: The two-point resistance and impedance
F. Y. Wu
Northeastern UniversityBoston, Massachusetts USA
Z
Impedance network
?Z
Ohm’s law
Z
V
I
I
VZ
Combination of impedances
1z 2z
1z
2z
21 zzz
21
111
zzz
In the phasor notation, impedance for inductance L is
Ljz
Impedance for capacitance C is
Cjz /1
where 1j .
Impedances
=
-Y transformation: (1899)
z
zzZ Z
Z Zz
ZZ
ZZz
3
12
)2(2
Star-triangle relation: (1944)
1
32
Ising model
J
JJR
R
R
1
2 3
=
)()( 133221321
RJ Fee =
)(cosh2 321 J
1r
2r3r2R
3R
1R
-Y relation (Star-triangle, Yang-Baxter relation)
A.E. Kenelly, Elec. World & Eng. 34, 413 (1899)
321
321 RRR
RRr
321
132 RRR
RRr
321
213 RRR
RRr
133221
321321
11 111
111)(
1
rrrrrr
rrrrrr
rR
133221
321321
22 111
111)(
1
rrrrrr
rrrrrr
rR
133221
321321
33 111
111)(
1
rrrrrr
rrrrrr
rR
1
2 3
4
z1 z1
z1
z1
z2
?13 Z
1
2 3
4
z1 z1
z1
z1
z2
3
1
2 3
1
3
1
113 zZ ?13 Z
1
2 3
4
r1 r1
r1
r1
r2
3
1
2 3
1
3
1113 rR
?13 R
I
I/2I/2
I/2
I/2I
1
2 3
4
r1 r1
r1
r1
r2
112
112
1
13 rI
IrIrR
1
2
r
r
r
r
r
r
r
r
r
r
r
r
?12 R
1
2
r
r
r
r
r
r
r
r
r
r
r
r
rI
VR
IrrI
rI
rI
V
6
56
5
363
1212
12
I
I/3
I/3
I/3
I/3
I
1
2
r
r
r
r
r
r
r
r
r
r
r
r
?12 R
I/3
I/6I/6
Infinite square network
I/4I/4
I/4I/4
I
V01=(I/4+I/4)r
I/4I/4
I/4I/4
I
I
I/4
201
01
r
I
VR
Infinite square network
2
1
38
2
1
2
24
2
17
4
2
4
2 2
14
2
14
0
24
2
17 4
3
46
43
46
823
2
1
3
4
2
1
3
4
Problems:
• Finite networks• Tedious to use Y- relation
1
2
r
rR
)7078.1(
027,380,1
898,356,212
(a)
(b) Resistance between (0,0,0) & (3,3,3) on a 5×5×4 network is
r
rR
)929693.0(
225,489,567,468,352
872,482,658,687,327
I0
1
4
3
2 Kirchhoff’s law
z01z04
z02
z03
04
40
03
30
02
20
01
10
040302010
z
VV
z
VV
z
VV
z
VV
IIIII
Generally, in a network of N nodes,
N
ijjji
iji VV
zI
,1
1
Then set )( iii II I
VVZ
Solve for Vi
2D grid, all r=1, I(0,0)=I0, all I(m,n)=0 otherwise
I0
(0,0)
(0,1) (1,1)
(1,0)
00,0,),(4)1,()1,(),1(),1( InmVnmVnmVnmVnmV nm
Define
)1()(2)1()(
)1()()(2
nfnfnfnf
nfnfnf
n
n
Then 00,0,22 ),()( InmV nmnm
Laplacian
Harmonic functionsRandom walksLattice Green’s functionFirst passage time
• Related to:
• Solution to Laplace equation is unique
• For infinite square net one finds
2
0
2
02 2coscos
)(exp
)2(2
1),(
nmiddnmV
• For finite networks, the solution is not straightforward.
General I1 I2
I3
N nodes
,1
,1,1
N
ijjjijii
N
ijjji
iji VYVYVV
zI
ijij
N
ijj iji z
Yz
Y1
,1
,1
NNNNN
N
N
I
I
I
V
V
V
YYY
YYY
YYY
2
1
2
1
21
2221
1121
The sum of each row or column is zero !
Properties of the Laplacian matrix
All cofactors are equal and equal to the spanning tree generating function G of the lattice (Kirchhoff).
Example1
2 3
y3
y1
y2 G=y1y2+y2y3+y3y1
2112
1313
2332
yyyy
yyyy
yyyy
L
Spanning Trees:
x
x
x
x
xx
y y
y
y
y
y
y
y
xS.T all
21),( nn yxyxG
G(1,1) = # of spanning trees
Solved by Kirchhoff (1847) Brooks/Smith/Stone/Tutte (1940)
1
4
2
3x
x
y y G(x,y)= +
x
x
x
xx
x
+ +yyyy y y
=2xy2+2x2y
yxxy
xyxy
yyxx
yxyx
yxL
0
0
0
0
),(
1 2 3 4
1
2
3
4
LN
yxG of seigenvalue nonzero ofproduct 1
),(
N=4
General I1 I2
I3
N nodes
,1
,1,1
N
ijjjijii
N
ijjji
iji VYVYVV
zI
ijij
N
ijj iji z
Yz
Y1
,1
,1
NNNNN
N
N
I
I
I
V
V
V
YYY
YYY
YYY
2
1
2
1
21
2221
1121
The sum of each row or column is zero !
I2I1
IN
network
Problem: L is singular so it cannot be inverted.
Day is saved:
Kirchhoff’s law says 01
N
jjI
Hence only N-1 equations are independent → no need to invert L
NNNNN
N
N
I
I
I
V
V
V
YYY
YYY
YYY
2
1
2
1
21
2221
1121
Solve Vi for a given I
Kirchhoff solutionSince only N-1 equations are independent, we can set VN=0 & consider the first N-1 equations!
1
2
1
1
2
1
12,11,1
1,2221
1,1121
NNNNN
N
N
I
I
I
V
V
V
YYY
YYY
YYY
The reduced (N-1)×(N-1) matrix, the tree matrix, now has an inverse and the equation can be solved.
0
0
131211
131211
131211
zcycxc
zbybxb
Izayaxa
0
0
333231
232221
131211 I
z
y
x
aaa
aaa
aaa
333231
232221
131211
aaa
aaa
aaa
3332
2322
1312
0
0
aa
aa
aaI
x
3331
2321
1311
0
0
aa
aa
aIa
y
0
0
3231
2221
1211
aa
aa
Iaa
z
Example1
2 3
y3
y1
y2
2112
1313
2332
yyyy
yyyy
yyyy
L
133221211
1311 yyyyyy
yyy
yyyL
2112 yyL
133221
21
1
1212 yyyyyy
yy
L
Lz
32112
111
zzzz
or
The evaluation of L & L in general is not straightforward!
)( iii II
I I Kirchhoff result:
Writing
L
LZ
Where L is the determinant of the Laplacian with the -th row & column removed.
L= the determinant of the Laplacian with the -th and -th rows & columns removed.
But the evaluation of Lfor general network is involved.
trees)spanning(
) and rootsh forest wit (spanning
G
G
NNNNN
N
N
I
I
I
V
V
V
YYY
YYY
YYY
2
1
2
1
21
2221
1121
)(
)(
)(
For resistors, z and y are real so L is Hermitian, we can then consider instead the eigenvalue equation
Solve Vi () for given Ii and set =0 at the end.
This can be done by applying the arsenal of linear algebra and deriving at a very simple result for 2-point resistance.
Eigenvectors and eigenvalues of L
1
1
1
0
1
1
1
21
2221
1121
NNN
N
N
YYY
YYY
YYY
L
0 is an eigenvalue with eigenvector
1
1
1
1
N
L is HermitianL has real eigenvaluesEigenvectors are orthonormal
IGV
IVL
)()(
)()(
Consider
where1)]([)( LG
i
i
2i
1 :)( of sEigenvalue
:)( of sEigenvalue
, ,0 :)0( of sEigenvalue
G
L
L
LLet
This gives
N
i i
ii
NG
2
*1
)(
Z and
0 sinceout drops 1
Term i
iIN
Example
1
2 3
4
r1 r1
r1
r1
r2
21121
111
21211
111
2
20
2
02
ccccc
ccc
ccccc
ccc
L
)1,0,1,0(2
1 ),(2
)0101(2
1 ,2
)1111(2
1 ,4
3214
313
212
cc
,,,c
,,,c
)(4
)32()(
1)(
1)(
1
)(1
)(1
)(1
21
21124441
4
23431
3
22421
214
12
43414
23331
3
22321
213
rr
rrrr
rr
0 and
,,2,1
1
Ni
L iii
For resistors let
iN
i
i
i
2
1
= orthonormal
Theorem for resistor networks:
2
2
1
ii
N
i i
R
This is the main result of FYW, J. Phys. A37 (2004) 6653-6679 whichmakes use of the fact that L is hermitian and is orthonormal
Corollary:
)1
)((1 2
22
ii
N
i i
N
iiN
) and rootsh forest wit spanning( G
Example: complete graphs
111
111
111
1
N
N
N
rL
N=3
N=2
N=4
110
121 ),/2exp(1
121 ,
,00
,N-,,α
,,N-,,nNniN
,N-,,nr
N
n
n
rN
R2
1 2 3 N-1r rr r N
100
021
011
1
rL
r
Nn
Nn
Nn
N
rR
N
i
1
1
2
cos1
)21
cos()21
cos(
N
n
N
N
N
n
n
n
)2
1cos(
2
1
cos12
0
If nodes 1 & N are connected with r (periodic boundary condition)
][ /1
2cos1
/2exp/2exp
2
1
1
2Per
Nr
Nn
NniNni
N
rR
N
iαβ
NniN
N
n
n
n
/2exp1
2cos12
201
021
112
1
rL
New summation identities
1
0 coscos
cos1
)(N
n
Nn
Nn
l
NlI
NlNN
lNlI
l
20 ,2/cosh4
)1(1
sinh
11
sinhsinh
)cosh()(
221
NlN
lNlI
0 ,
2/sinhsinh
)2/cosh()(2
New product identity
2sinh
2coscosh
1
0
2 N
N
nN
n
M×N network
N=6
M=5
r
s
sNMNMNM TIs
ITr
L 11
1000
0210
0121
0011
NT IN unit matrix
1,,2,1 ,2
1cos
2
0 ,1
2cos1
22cos1
2
)(
)()(),(
),(
NN
n
N
N
N
n
rM
m
s
Nn
Nn
Mmnm
nm
s
r
rr
M, N →∞
Resistance between two corners of an N x N
square net with unit resistance on each edge
2ln
2
141ln
4NRNxN
......082069878.0ln4
N
where ...5772156649.0 Euler constant
N=30 (Essam, 1997)
Finite lattices
Free boundary condition
Cylindrical boundary condition
Moebius strip boundary condition
Klein bottle boundary condition
Klein bottleMoebius strip
Free
Cylinder
Klein bottle
Moebius strip
Klein bottle
Moebius strip
Free
Cylinder
Torus
)3,3)(0,0(R on a 5×4 network embedded as shown
Resistance between (0,0,0) and (3,3,3) in a 5×5×4 network with free boundary
In the phasor notation, impedance for inductance L is
Ljz
Impedance for capacitance C is
Cjz /1
where 1j .
Impedances
For impedances, Y are generally complex and the matrixL is not hermitian and its eigenvectors are not orthonormal; the resistor result does not apply.
But L^*L is hermitian and has real eigenvelues.We have
N1,2,..., , 0 , ^* α LL
with
.
1
:
:
1
1
N
1 0, 11
N1,2,..., , 0 , ^* α LL
Theorem
Let L be an N x N symmetric matrix with complexMatrix elements and
Then, there exist N orthnormal vectors u
satisfying the relation
NuuL ,...,2,1 *,
where * denotes complex conjugate and
real. ,
ie
Remarks:
For nondegenerate one has simply
u
For degenerate
,
, one can construct
as linear combinations of u
ieLv *)(
0 and
,,2,1
*
1
Ni
uLu iii
For impedances let
iN
i
i
i
u
u
u
u
2
1
= orthonormal
Theorem for impedance networks:
2,0 if ,
2 ,0 if ,)(1 2
2
i
iuuZ
i
iii
N
i i
This is the result of WJT and FYW, J. Phys. A39 (2006) 8579-8591
The physical interpretation of Z
is the occurrence of a resonance such asin a parallel combination of inductance Land capacitance C the impedance is
Z =
Lj
Cj
Cj
Lj
))((
LC/1at , =
Generally in an LC circuit there can exist multiple resonances at frequencies where . 0i
In the circuit shown, 15 resonance frequencies at
M=6N=4
.3,..,1;5,..,1 ,1
)2/sin(
)2/sin( nm
LCMm
Nnmn
Summary
• An elegant formulation of computing two-point impedances in a network, a problem lingering since the Kirchhoff time.
• Prediction of the occurrence of multi-resonances in a network consisting of reactances L and C, a prediction which may have practical relevance.
FYW, J. Phys. A 37 (2004) 6653-6673
W-J Tzeng and FYW, J. Phys. A 39 (2006), 8579-8591