IP Library Granted Patent US 8,195,412
Granted Patent B2
US 8,195,412 · App. 12/572,696 · Granted Jun 5, 2012

Iterative method for characterizing the frequency dependence of the linear properties of an electrical component

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Quick Facts
Patent No.
US 8,195,412
App. No.
12/572,696
Granted
Jun 5, 2012
Kind
B2
Abstract

A method and device characterize linear properties of an electrical component having n>1 ports. The linear properties of the component are described in a matrix relating a voltage applied to the ports to a current through the ports. A frequency dependence of the matrix is approximated to preserve eigenvalues of the matrix by a pole-residual model. The method includes: (a) obtaining a set of values of the matrix at discrete frequencies, and obtaining eigenvalues and eigenvectors for each value; (b) fitting a set of vector equations to the eigenvalues and eigenvectors with a first set of pole frequencies; and (c) calculating a second set of pole frequencies by a vector fitting process for all modes of an element of the matrix. Steps (b) and (c) are repeated using the second set of pole frequencies in step (c) in a subsequent step (b) until a stop condition is met.

Claims (491)

1. A method for characterizing linear properties of an electrical component having n>1 ports, which linear properties are described in a matrix Y relating a voltage applied to the ports to a current through the ports, wherein a frequency dependence of Y is approximated by

Y

(

s

)

Y

rat

(

s

)

=

m

R

m

s

-

a

m

+

D

+

sE

wherein the subscript “rat” denotes a rational function, m runs from 1 to a number N of poles, R m with m=1 to N are frequency independent matrices, D and E are frequency independent matrices or zero, s denotes a complex angular frequency iω, and a m with m=1 to N are complex angular frequencies of the poles,

said method comprising:

a) obtaining a set of values Y(s) of Y at discrete frequencies s, and, for each value Y(s), obtaining eigenvalues λ i and eigenvectors t i with i=1 to n;

b) fitting, in a processor of a computer processing device, a set of n vector equations

λ

i

λ

i

(

m

=

1

N

r

~

m

s

-

a

m

+

1

)

σ

(

s

)

t

i

1

λ

i

(

(

m

=

1

N

R

m

s

-

a

m

+

D

+

sE

)

·

t

i

)

to the eigenvalues λ i and eigenvectors t i , wherein {tilde over (r)} m is a frequency-independent scalar with m=1 to N, by using a first set of pole frequencies am and by varying {tilde over (r)} m , R m and, if assumed to be non-zero, D and E;

c) calculating, in the processor of the computer processing device, a second set of pole frequencies from:

{ a m }=eig( A−b·c T )

wherein A is a diagonal matrix holding the first set of pole frequencies am as diagonal elements, b is a vector of ones, c is a vector holding {tilde over (r)} m for m=1 to N as obtained by step b), and eig is an operator returning a vector holding eigenvalues of a matrix;

d) repeating steps b) and c) by using the second set of pole frequencies am of step c) as the first set of pole frequencies in a subsequent step b) until a stop condition is met; and

e) outputting a model approximating the linear properties of the electrical component in which the applied voltage is related to output currents in the electrical component.

2. The method of claim 1 , comprising:

f) setting σ(s)=1 in the equation of step b) and calculating R m .

3. The method of claim 2 , wherein the electrical component is connected to an external device, with linear properties of the external device being described by a matrix Y ext , wherein the equations of step b) include:

λ

i

λ

i

(

m

=

1

N

r

~

m

s

-

a

m

+

1

)

σ

(

s

)

t

i

1

λ

i

(

(

Y

ext

+

m

=

1

N

R

m

s

-

a

m

+

D

+

sE

)

·

t

i

)

.

4. The method of claim 3 , wherein the matrix Y describes the relation between a voltage v applied to the ports of the electrical component and currents i which are to run through the electrical component by

i×Yv.

5. The method of claim 4 , comprising:

utilizing a matrix-valued function F({b i }, s) that depends linearly on a set of parameters {b i } in the equations of step b).

6. The method of claim 1 , wherein the electrical component is connected to an external device and wherein linear properties of the external device are described by a matrix Y ext , wherein the equations of step b) include:

λ

i

λ

i

(

m

=

1

N

r

~

m

s

-

a

m

+

1

)

σ

(

s

)

t

i

1

λ

i

(

(

Y

ext

+

m

=

1

N

R

m

s

-

a

m

+

D

+

sE

)

·

t

i

)

.

7. The method of claim 1 , wherein the matrix Y describes a relation between a voltage v to be applied to the ports of the electrical component and currents i which are to run through the electrical component by:

i=Yv.

8. The method of claim 1 , comprising:

utilizing a matrix-valued function F({b i }, s) that depends linearly on a set of parameters {b i } in the equations of step b).

9. A device for characterizing linear properties of an electrical component having n>1 ports, which linear properties are described in a matrix Y relating a voltage applied to the ports to a current through the ports, wherein a frequency dependence of Y is approximated by:

Y

(

s

)

Y

rat

(

s

)

=

m

R

m

s

-

a

m

+

D

+

sE

wherein the subscript “rat” denotes a rational function, m runs from 1 to a number N of poles, R m with m=1 to N are frequency independent matrices, D and E are frequency independent matrices or zero, s denotes a complex angular frequency iω and a m with m=1 to N are complex angular frequencies of the poles,

said device comprising:

a computer having a processor configured to execute a computer program recorded on a non-transitory computer-readable recording medium, the program causing the processor to execute operations comprising:

a) obtaining a set of values Y(s) of Y at discrete frequencies s, and, for each value Y(s), obtaining eigenvalues λ i and eigenvectors t i with i=1 to n;

b) fitting a set of n vector equations:

λ

i

λ

i

(

m

=

1

N

r

~

m

s

-

a

m

+

1

)

σ

(

s

)

t

i

1

λ

i

(

(

m

=

1

N

R

m

s

-

a

m

+

D

+

sE

)

·

t

i

)

to the eigenvalues λ i and eigenvectors t i , wherein {tilde over (r)} m is a frequency-independent scalar with m=1 to N, by using a first set of pole frequencies am and by varying {tilde over (r)} m , R m and, if assumed to be non-zero, D and E;

c) calculating a second set of pole frequencies from:

{ a m }=eig( A−b·c T )

wherein A is a diagonal matrix holding the first set of pole frequencies am as diagonal elements, b is a vector of ones, c is a vector holding {tilde over (r)} m for m=1 to N as obtained by step b), and eig is an operator returning a vector holding eigenvalues of a matrix;

d) repeating operations b) and c) by using the second set of pole frequencies am of step c) as the first set of pole frequencies in a subsequent step b) until a stop condition is met; and

e) outputting a model approximating the linear properties of the electrical component in which the applied voltage is related to output currents in the electrical component.

10. The device of claim 9 , wherein a design of the electrical component and/or a desired operational frequency of the electrical component is based on the stop condition.

11. The device of claim 10 , wherein the electrical component is designed for connection to an external device, with linear properties of the external device being described by a matrix Y ext , wherein the equations of operation b) include:

λ

i

λ

i

(

m

=

1

N

r

~

m

s

-

a

m

+

1

)

σ

(

s

)

t

i

1

λ

i

(

(

Y

ext

+

m

=

1

N

R

m

s

-

a

m

+

D

+

sE

)

·

t

i

)

.

12. The device of claim 11 , wherein the matrix Y describes the relation between a voltage v to be applied to the ports of the electrical component and currents i which are to run through the electrical component by:

i=Yv.

13. The device of claim 12 , wherein the equations of operation b) include a matrix-valued function F({b i }, s) that depends linearly on a set of parameters {b i }.

14. The device of claim 9 , wherein the electrical component is designed for connection to an external device, with linear properties of the external device being described by a matrix Y ext , wherein the equations of operation b) include:

λ

i

λ

i

(

m

=

1

N

r

~

m

s

-

a

m

+

1

)

σ

(

s

)

t

i

1

λ

i

(

(

Y

ext

+

m

=

1

N

R

m

s

-

a

m

+

D

+

sE

)

·

t

i

)

.

15. The device of claim 9 , wherein the matrix Y describes a relation between a voltage v to be applied to the ports of the electrical component and currents i which are to run through the electrical component by:

i=Yv.

16. The device of claim 9 , wherein the equations of operation b) includes a matrix-valued function F({b i }, s) that depends linearly on a set of parameters {b i }.

Assignments (5)
CORRECTIVE ASSIGNMENT TO CORRECT THE CONVEYING PARTY "ABB TECHNOLOGY LTD."SHOULD READ "ABB TECHNOLOGY AG" PREVIOUSLY RECORDED AT REEL: 040621 FRAME: 0822. ASSIGNOR(S) HEREBY CONFIRMS THE MERGER. Recorded May 11, 2022
From: ABB TECHNOLOGY AG
To: ABB SCHWEIZ AG
Reel/Frame 059927/0691 →
CHANGE OF NAME Recorded Dec 31, 2021
From: ABB POWER GRIDS SWITZERLAND AG
To: HITACHI ENERGY SWITZERLAND AG
Reel/Frame 058666/0540 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Mar 6, 2020
From: ABB SCHWEIZ AG
To: ABB POWER GRIDS SWITZERLAND AG
Reel/Frame 052916/0001 →
MERGER Recorded Nov 15, 2016
From: ABB TECHNOLOGY LTD.
To: ABB SCHWEIZ AG
Reel/Frame 040621/0822 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 2, 2009
From: GUSTAVSEN, BJORN; HEITZ, CHRISTOPH; TIBERG, MARTIN
To: ABB TECHNOLOGY AG
Reel/Frame 023321/0112 →