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On the link between storage functions of allpass systems and - - PowerPoint PPT Presentation

On the link between storage functions of allpass systems and Gramians Chayan Bhawal, Debasattam Pal and Madhu N. Belur Control and Computing Group (CC Group) Department of Electrical Engineering Indian Institute of Technology Bombay IEEE


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SLIDE 1

On the link between storage functions of allpass systems and Gramians

Chayan Bhawal, Debasattam Pal and Madhu N. Belur

Control and Computing Group (CC Group) Department of Electrical Engineering Indian Institute of Technology Bombay

IEEE Conference on Decision and Control, Melbourne December 14, 2017

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 1 / 18

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SLIDE 2

Storage functions of allpass/lossless systems Dissipative systems and storage function

Dissipative systems and storage function

A dissipative system

1 has no source of

energy.

2 can only absorb

energy.

3 can store

energy.

Rate-change-stored-energy

  • d

dt QΨ(w)

+ Dissipated power

  • Q∆(w)

= Power supplied

  • QΣ(w)

Dissipative systems :

d dtQΨ(w) QΣ(w).

Power supplied with respect to system variable: QΣ(w)=wT Σw. e.g. Supply rate: w = (u, y) : QΣ(w) = wT I I

  • w = 2uT y.

Stored energy: Storage function1 QΨ(w) = xT Kx.

1Trentelman and Willems, SCL, Every storage function is a state function, 1997. C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 2 / 18

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SLIDE 3

Storage functions of allpass/lossless systems Dissipative systems and storage function

Dissipative systems and storage function

A dissipative system

1 has no source of

energy.

2 can only absorb

energy.

3 can store

energy.

Rate-change-stored-energy

  • d

dt QΨ(w)

+ Dissipated power

  • Q∆(w)

= Power supplied

  • QΣ(w)

Dissipative systems :

d dtQΨ(w) QΣ(w).

Power supplied with respect to system variable: QΣ(w)=wT Σw. e.g. Supply rate: w = (u, y) : QΣ(w) = wT I I

  • w = 2uT y.

Stored energy: Storage function1 QΨ(w) = xT Kx.

1Trentelman and Willems, SCL, Every storage function is a state function, 1997. C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 2 / 18

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SLIDE 4

Storage functions of allpass/lossless systems Dissipative systems and storage function

Dissipative systems and storage function

A dissipative system

1 has no source of

energy.

2 can only absorb

energy.

3 can store

energy.

Rate-change-stored-energy

  • d

dt QΨ(w)

+ Dissipated power

  • Q∆(w)

= Power supplied

  • QΣ(w)

Dissipative systems :

d dtQΨ(w) QΣ(w).

Power supplied with respect to system variable: QΣ(w)=wT Σw. e.g. Supply rate: w = (u, y) : QΣ(w) = wT I I

  • w = 2uT y.

Stored energy: Storage function1 QΨ(w) = xT Kx.

1Trentelman and Willems, SCL, Every storage function is a state function, 1997. C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 2 / 18

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SLIDE 5

Storage functions of allpass/lossless systems Dissipative systems and storage function

Dissipative systems and storage function

A dissipative system

1 has no source of

energy.

2 can only absorb

energy.

3 can store

energy.

Rate-change-stored-energy

  • d

dt QΨ(w)

+ Dissipated power

  • Q∆(w)

= Power supplied

  • QΣ(w)

Dissipative systems :

d dtQΨ(w) QΣ(w).

Power supplied with respect to system variable: QΣ(w)=wT Σw. e.g. Supply rate: w = (u, y) : QΣ(w) = wT I I

  • w = 2uT y.

Stored energy: Storage function1 QΨ(w) = xT Kx.

1Trentelman and Willems, SCL, Every storage function is a state function, 1997. C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 2 / 18

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SLIDE 6

Storage functions of allpass/lossless systems Dissipative systems and storage function

Dissipative systems and storage function

A dissipative system

1 has no source of

energy.

2 can only absorb

energy.

3 can store

energy.

Rate-change-stored-energy

  • d

dt QΨ(w)

+ Dissipated power

  • Q∆(w)

= Power supplied

  • QΣ(w)

Dissipative systems :

d dtQΨ(w) QΣ(w).

Power supplied with respect to system variable: QΣ(w)=wT Σw. e.g. Supply rate: w = (u, y) : QΣ(w) = wT I I

  • w = 2uT y.

Stored energy: Storage function1 QΨ(w) = xT Kx.

1Trentelman and Willems, SCL, Every storage function is a state function, 1997. C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 2 / 18

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SLIDE 7

Storage functions of allpass/lossless systems Dissipative systems and storage function

Passivity and bounded-real systems

Dissipative systems d dt

  • xT Kx
  • QΣ(w), where w = (u, y).

Positive-real Bounded-real Supply rate Σ I I

  • I

−I

  • Dissipation

inequality

d dt

  • xT Kx
  • 2uT y

d dt

  • xT Kx
  • uT u − yT y

Conservative counterpart

d dt

  • xT Kx
  • = 2uT y

d dt

  • xT Kx
  • = uT u − yT y

Name Lossless Allpass Example G(s) =

s s2+1

(LC circuits) G(s) = s−1

s+1

(allows all frequencies to pass)

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 3 / 18

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SLIDE 8

Storage functions of allpass/lossless systems Conservative systems

Passivity and bounded-real systems

Conservative systems d dt

  • xT Kx
  • = QΣ(w), where w = (u, y).

Positive-real Bounded-real Supply rate Σ I I

  • I

−I

  • Dissipation

inequality

d dt

  • xT Kx
  • 2uT y

d dt

  • xT Kx
  • uT u − yT y

Conservative counterpart

d dt

  • xT Kx
  • = 2uT y

d dt

  • xT Kx
  • = uT u − yT y

Name Lossless Allpass Example G(s) =

s s2+1

(LC circuits) G(s) = s−1

s+1

(allows all frequencies to pass)

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 3 / 18

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SLIDE 9

Storage functions of allpass/lossless systems Conservative systems

Passivity and bounded-real systems

Conservative systems d dt

  • xT Kx
  • = QΣ(w), where w = (u, y).

Positive-real Bounded-real Supply rate Σ I I

  • I

−I

  • Dissipation

inequality

d dt

  • xT Kx
  • 2uT y

d dt

  • xT Kx
  • uT u − yT y

Conservative counterpart

d dt

  • xT Kx
  • = 2uT y

d dt

  • xT Kx
  • = uT u − yT y

Name Lossless Allpass Example G(s) =

s s2+1

(LC circuits) G(s) = s−1

s+1

(allows all frequencies to pass)

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 3 / 18

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SLIDE 10

Storage functions of allpass/lossless systems Allpass systems

Allpass systems

System B : d

dtx = Ax + Bu, y = Cx + Du, (Minimal)

A ∈ Rn×n, C, BT ∈ Rn×p and D ∈ Rp×p. Necessary condition for allpass: I − DT D = 0. Dissipation equation:

d dt

  • xT Kx
  • = uT u − yT y.

Linear Matrix Equations (LME): Allpass if and only if there exists K = KT ∈ Rn×n AT K + KA + CT C KB + CT BT K + C

  • = 0

Rewriting the LME: Allpass if and only if there exists K = KT ∈ Rn×n AT K + KA + CT C = 0 KB + CT = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 4 / 18

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SLIDE 11

Storage functions of allpass/lossless systems Allpass systems

Allpass systems

System B : d

dtx = Ax + Bu, y = Cx + Du, (Minimal)

A ∈ Rn×n, C, BT ∈ Rn×p and D ∈ Rp×p. Necessary condition for allpass: I − DT D = 0. Dissipation equation:

d dt

  • xT Kx
  • = uT u − yT y.

Linear Matrix Equations (LME): Allpass if and only if there exists K = KT ∈ Rn×n AT K + KA + CT C KB + CT BT K + C

  • = 0

Rewriting the LME: Allpass if and only if there exists K = KT ∈ Rn×n AT K + KA + CT C = 0 KB + CT = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 4 / 18

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SLIDE 12

Storage functions of allpass/lossless systems Allpass systems

Allpass systems

System B : d

dtx = Ax + Bu, y = Cx + Du, (Minimal)

A ∈ Rn×n, C, BT ∈ Rn×p and D ∈ Rp×p. Necessary condition for allpass: I − DT D = 0. Dissipation equation:

d dt

  • xT Kx
  • = uT u − yT y.

Linear Matrix Equations (LME): Allpass if and only if there exists K = KT ∈ Rn×n AT K + KA + CT C KB + CT BT K + C

  • = 0

Rewriting the LME: Allpass if and only if there exists K = KT ∈ Rn×n AT K + KA + CT C = 0 KB + CT = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 4 / 18

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SLIDE 13

Storage functions of allpass/lossless systems Allpass systems

Allpass systems

System B : d

dtx = Ax + Bu, y = Cx + Du, (Minimal)

A ∈ Rn×n, C, BT ∈ Rn×p and D ∈ Rp×p. Necessary condition for allpass: I − DT D = 0. Dissipation equation:

d dt

  • xT Kx
  • = uT u − yT y.

Linear Matrix Equations (LME): Allpass if and only if there exists K = KT ∈ Rn×n AT K + KA + CT C KB + CT BT K + C

  • = 0

Rewriting the LME: Allpass if and only if there exists K = KT ∈ Rn×n AT K + KA + CT C = 0 KB + CT = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 4 / 18

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SLIDE 14

Storage functions of allpass/lossless systems Lossless systems

Lossless systems

System B : d

dtx = Ax + Bu, y = Cx + Du, (Minimal)

A ∈ Rn×n, C, BT ∈ Rn×p and D ∈ Rp×p. Necessary condition for allpass: D + DT = 0. Dissipation equation:

d dt

  • xT Kx
  • = 2uT y.

Linear Matrix Equations (LME): Lossless if and only if there exists K = KT ∈ Rn×n AT K + KA KB − CT BT K − C

  • = 0

Rewriting the LME: Lossless if and only if there exists K = KT ∈ Rn×n AT K + KA= 0 KB − CT = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 5 / 18

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SLIDE 15

Storage functions of allpass/lossless systems Allpass and Lossless systems

Allpass and Lossless systems

Lossless Allpass Supply rate Σ I I

  • I

−I

  • Conservative

counterpart

d dt

  • xT Kx
  • = 2uT y

d dt

  • xT Kx
  • = uT u − yT y

Example G(s) =

s s+1

(LC circuits) G(s) = s−1

s+1

(allows all frequency) Poles of the system On imaginary axis Symmetric about real and imaginary axis K satisfies LME AT K + KA = 0 KB − CT = 0 AT K + KA + CT C = 0 KB + CT = 0 Lossless: Lyapunov equation AT K + KA = 0 has non-unique solutions.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 6 / 18

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SLIDE 16

Storage functions of allpass/lossless systems Allpass and Lossless systems

Allpass and Lossless systems

Lossless Allpass Supply rate Σ I I

  • I

−I

  • Conservative

counterpart

d dt

  • xT Kx
  • = 2uT y

d dt

  • xT Kx
  • = uT u − yT y

Example G(s) =

s s+1

(LC circuits) G(s) = s−1

s+1

(allows all frequency) Zeros and poles of the system Interlace on jR Mirrored about jR K satisfies LME AT K + KA = 0 KB − CT = 0 AT K + KA + CT C = 0 KB + CT = 0 Lossless: Lyapunov equation AT K + KA = 0 has non-unique solutions.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 6 / 18

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SLIDE 17

Storage functions of allpass/lossless systems Allpass systems and lossless counterpart

Link between storage functions of lossless systems and allpass systems

Theorem Ball is an allpass system and Bℓ is its lossless counterpart. Then, the storage function of Ball and Bℓ is the same. Lossless Allpass Minimal i/s/o representation

d dtx = Ax + Bu

y = Cx + Du

d dtx = ˆ

Ax + ˆ B

  • u+y

√ 2

  • u−y

√ 2 = ˆ

Cx + ˆ D

  • u+y

√ 2

  • ˆ

A :=

  • A − B(I + D)−1C
  • , ˆ

B =

1 √ 2

  • B + B(I + D)−1(I − D)
  • ,

ˆ C = − √ 2(I + D)−1C and ˆ D := (I + D)−1(I − D). True for positive-real and bounded-real systems.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 7 / 18

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SLIDE 18

Storage functions of allpass/lossless systems Allpass systems and lossless counterpart

Link between storage functions of lossless systems and allpass systems

Theorem Ball is an allpass system and Bℓ is its lossless counterpart. Then, the storage function of Ball and Bℓ is the same. Lossless Allpass Minimal i/s/o representation

d dtx = Ax + Bu

y = Cx + Du

d dtx = ˆ

Ax + ˆ B

  • u+y

√ 2

  • u−y

√ 2 = ˆ

Cx + ˆ D

  • u+y

√ 2

  • ˆ

A :=

  • A − B(I + D)−1C
  • , ˆ

B =

1 √ 2

  • B + B(I + D)−1(I − D)
  • ,

ˆ C = − √ 2(I + D)−1C and ˆ D := (I + D)−1(I − D). True for positive-real and bounded-real systems.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 8 / 18

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SLIDE 19

Storage functions of allpass/lossless systems Allpass systems and lossless counterpart

Link between storage functions of lossless systems and allpass systems

Theorem Ball is an allpass system and Bℓ is its lossless counterpart. Then, the storage function of Ball and Bℓ is the same. Lossless Allpass Minimal i/s/o representation

d dtx = Ax + Bu

y = Cx + Du

d dtx = ˆ

Ax + ˆ B

  • u+y

√ 2

  • u−y

√ 2 = ˆ

Cx + ˆ D

  • u+y

√ 2

  • ˆ

A :=

  • A − B(I + D)−1C
  • , ˆ

B =

1 √ 2

  • B + B(I + D)−1(I − D)
  • ,

ˆ C = − √ 2(I + D)−1C and ˆ D := (I + D)−1(I − D). True for positive-real and bounded-real systems.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 8 / 18

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SLIDE 20

Storage functions of allpass/lossless systems Allpass systems and observability Gramian

Allpass systems and Observability Gramian

Theorem Stable, minimal, allpass system d dtx = Ax + Bu and y = Cx + Du, where A ∈ Rn×n, B, CT ∈ Rn×p and D ∈ Rp×p. Assume Q to be the observability Gramian of the system. Then, xT Qx is the unique storage function of the system. Corollary Allpass system Ball and its lossless counterpart Bℓ. Then, observability Gramian of Ball is the storage function of Bℓ.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 9 / 18

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SLIDE 21

Storage functions of allpass/lossless systems Allpass systems and observability Gramian

Allpass systems and Observability Gramian

Theorem Stable, minimal, allpass system d dtx = Ax + Bu and y = Cx + Du, where A ∈ Rn×n, B, CT ∈ Rn×p and D ∈ Rp×p. Assume Q to be the observability Gramian of the system. Then, xT Qx is the unique storage function of the system. Corollary Allpass system Ball and its lossless counterpart Bℓ. Then, observability Gramian of Ball is the storage function of Bℓ.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 9 / 18

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SLIDE 22

Storage functions of allpass/lossless systems Allpass systems and observability Gramian

Allpass systems and Observability Gramian

Theorem Stable, minimal, allpass system d dtx = Ax + Bu and y = Cx + Du, where A ∈ Rn×n, B, CT ∈ Rn×p and D ∈ Rp×p. Assume Q to be the observability Gramian of the system. Then, xT Qx is the unique storage function of the system. Corollary Allpass system Ball and its lossless counterpart Bℓ. Then, observability Gramian of Ball is the storage function of Bℓ.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 9 / 18

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SLIDE 23

Storage functions of allpass/lossless systems Allpass systems and observability Gramian

Allpass systems and Observability Gramian

Theorem Stable, minimal, allpass system d dtx = Ax + Bu and y = Cx + Du, where A ∈ Rn×n, B, CT ∈ Rn×p and D ∈ Rp×p. Assume Q to be the observability Gramian of the system. Then, xT Qx is the unique storage function of the system. Corollary Allpass system Ball and its lossless counterpart Bℓ. Then, observability Gramian of Ball is the storage function of Bℓ.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 9 / 18

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SLIDE 24

Storage functions of allpass/lossless systems Example

Link between storage functions of lossless systems and allpass systems

Lossless system G(s) = 0.2s s2 + 0.1. i/s/o representation: d dt iL vC

  • =

1 2

− 1

5

iL vC

  • +

1 5

  • i,

v =

  • 1

iL vC

  • .
  • iL
  • i

vC

5F 2H

+ +

v

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 10 / 18

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SLIDE 25

Storage functions of allpass/lossless systems Example

Storage functions of lossless systems

Lossless system: G(s) = 0.2s s2 + 0.1. d dt iL vC

  • =

1 2

− 1

5

iL vC

  • +

1 5

  • u,

y =

  • 1

iL vC

  • .

Allpass counterpart: G(s) = s2 − 0.2s + 0.1 s2 + 0.2s + 0.1. i/s/o representation: d dt iL vC

  • =

1 2

− 1

5

− 1

5

iL vC

  • +

2 5

u + y √ 2

  • ,

u − y √ 2

  • =

√ 2 iL vC

  • +1

u + y √ 2

  • .

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 11 / 18

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SLIDE 26

Storage functions of allpass/lossless systems Example

Storage functions of lossless systems

Lossless system: G(s) = 0.2s s2 + 0.1. d dt iL vC

  • =

1 2

− 1

5

iL vC

  • +

1 5

  • u,

y =

  • 1

iL vC

  • .

Allpass counterpart: G(s) = s2 − 0.2s + 0.1 s2 + 0.2s + 0.1. i/s/o representation: d dt iL vC

  • =

1 2

− 1

5

− 1

5

iL vC

  • +

2 5

u + y √ 2

  • ,

u − y √ 2

  • =

√ 2 iL vC

  • +1

u + y √ 2

  • .

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 11 / 18

slide-27
SLIDE 27

Storage functions of allpass/lossless systems Example

Storage functions of allpass and lossless systems

Lossless: G(s) = 0.2s s2 + 0.1.

d dt

  • iL

vC

  • =
  • 1

2

− 1

5

  • A
  • iL

vC

  • +

1 5

  • B

i, v = 1

  • C
  • iL

vC

  • .

Allpass: G(s) = s2 − 0.2s + 0.1 s2 + 0.2s + 0.1.

d dt

  • iL

vC

  • =
  • 1

2

− 1

5

− 1

5

  • ˆ

A

  • iL

vC

  • +

2 5

  • ˆ

B

u + y √ 2

  • ,

u − y √ 2

  • =

√ 2

  • ˆ

C

  • iL

vC

  • + 1

u + y √ 2

  • .

Observability Gramian matrix: Q = 2 5

  • Stored energy = 2i2

L + 5v2 c.

(Recall: power = 2vi) AT Q + QA = 0 QB − CT = 0. ˆ AT Q + Q ˆ A + ˆ CT ˆ C= 0 Q ˆ B + ˆ CT = 0. xT Qx is the storage function of both the systems.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 12 / 18

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SLIDE 28

Storage functions of allpass/lossless systems Example

Storage functions of allpass and lossless systems

Lossless: G(s) = 0.2s s2 + 0.1.

d dt

  • iL

vC

  • =
  • 1

2

− 1

5

  • A
  • iL

vC

  • +

1 5

  • B

i, v = 1

  • C
  • iL

vC

  • .

Allpass: G(s) = s2 − 0.2s + 0.1 s2 + 0.2s + 0.1.

d dt

  • iL

vC

  • =
  • 1

2

− 1

5

− 1

5

  • ˆ

A

  • iL

vC

  • +

2 5

  • ˆ

B

u + y √ 2

  • ,

u − y √ 2

  • =

√ 2

  • ˆ

C

  • iL

vC

  • + 1

u + y √ 2

  • .

Observability Gramian matrix: Q = 2 5

  • Stored energy = 2i2

L + 5v2 c.

(Recall: power = 2vi) AT Q + QA = 0 QB − CT = 0. ˆ AT Q + Q ˆ A + ˆ CT ˆ C= 0 Q ˆ B + ˆ CT = 0. xT Qx is the storage function of both the systems.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 12 / 18

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SLIDE 29

Storage functions of allpass/lossless systems Example

Storage functions of allpass and lossless systems

Lossless: G(s) = 0.2s s2 + 0.1.

d dt

  • iL

vC

  • =
  • 1

2

− 1

5

  • A
  • iL

vC

  • +

1 5

  • B

i, v = 1

  • C
  • iL

vC

  • .

Allpass: G(s) = s2 − 0.2s + 0.1 s2 + 0.2s + 0.1.

d dt

  • iL

vC

  • =
  • 1

2

− 1

5

− 1

5

  • ˆ

A

  • iL

vC

  • +

2 5

  • ˆ

B

u + y √ 2

  • ,

u − y √ 2

  • =

√ 2

  • ˆ

C

  • iL

vC

  • + 1

u + y √ 2

  • .

Observability Gramian matrix: Q = 2 5

  • Stored energy = 2i2

L + 5v2 c.

(Recall: power = 2vi) AT Q + QA = 0 QB − CT = 0. ˆ AT Q + Q ˆ A + ˆ CT ˆ C= 0 Q ˆ B + ˆ CT = 0. xT Qx is the storage function of both the systems.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 12 / 18

slide-30
SLIDE 30

Storage functions of allpass/lossless systems Example

Storage functions of allpass and lossless systems

Lossless: G(s) = 0.2s s2 + 0.1.

d dt

  • iL

vC

  • =
  • 1

2

− 1

5

  • A
  • iL

vC

  • +

1 5

  • B

i, v = 1

  • C
  • iL

vC

  • .

Allpass: G(s) = s2 − 0.2s + 0.1 s2 + 0.2s + 0.1.

d dt

  • iL

vC

  • =
  • 1

2

− 1

5

− 1

5

  • ˆ

A

  • iL

vC

  • +

2 5

  • ˆ

B

u + y √ 2

  • ,

u − y √ 2

  • =

√ 2

  • ˆ

C

  • iL

vC

  • + 1

u + y √ 2

  • .

Observability Gramian matrix: Q = 2 5

  • Stored energy = 2i2

L + 5v2 c.

(Recall: power = 2vi) AT Q + QA = 0 QB − CT = 0. ˆ AT Q + Q ˆ A + ˆ CT ˆ C= 0 Q ˆ B + ˆ CT = 0. xT Qx is the storage function of both the systems.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 12 / 18

slide-31
SLIDE 31

Storage functions of allpass/lossless systems Storage function in balanced realization

Allpass systems and Balanced realization

Definition System representation is said to be in balanced state space basis if controllability Gramian P = observability Gramian Q. Theorem Stable, allpass system:

d dtx = Ax + Bu, y = Cx + Du in a balanced

state space basis. Then, Storage function K = I. Allpass systems2 have PQ = I. Balanced transformation: P = Q. Then Q2 = I. System is stable: Q > 0 = ⇒ Q = I.

  • 2K. Glover, IJC, 1984

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 13 / 18

slide-32
SLIDE 32

Storage functions of allpass/lossless systems Storage function in balanced realization

Allpass systems and Balanced realization

Definition System representation is said to be in balanced state space basis if controllability Gramian P = observability Gramian Q. Theorem Stable, allpass system:

d dtx = Ax + Bu, y = Cx + Du in a balanced

state space basis. Then, Storage function K = I. Allpass systems2 have PQ = I. Balanced transformation: P = Q. Then Q2 = I. System is stable: Q > 0 = ⇒ Q = I.

  • 2K. Glover, IJC, 1984

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 13 / 18

slide-33
SLIDE 33

Storage functions of allpass/lossless systems Storage function in balanced realization

Allpass systems and Balanced realization

Definition System representation is said to be in balanced state space basis if controllability Gramian P = observability Gramian Q. Theorem Stable, allpass system:

d dtx = Ax + Bu, y = Cx + Du in a balanced

state space basis. Then, Storage function K = I. Allpass systems2 have PQ = I. Balanced transformation: P = Q. Then Q2 = I. System is stable: Q > 0 = ⇒ Q = I.

  • 2K. Glover, IJC, 1984

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 13 / 18

slide-34
SLIDE 34

Storage functions of allpass/lossless systems Storage function in balanced realization

Allpass systems and Balanced realization

Definition System representation is said to be in balanced state space basis if controllability Gramian P = observability Gramian Q. Theorem Stable, allpass system:

d dtx = Ax + Bu, y = Cx + Du in a balanced

state space basis. Then, Storage function K = I. Allpass systems2 have PQ = I. Balanced transformation: P = Q. Then Q2 = I. System is stable: Q > 0 = ⇒ Q = I.

  • 2K. Glover, IJC, 1984

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 13 / 18

slide-35
SLIDE 35

Storage functions of allpass/lossless systems Storage function in balanced realization

Allpass systems and Balanced realization

Definition System representation is said to be in balanced state space basis if controllability Gramian P = observability Gramian Q. Theorem Stable, allpass system:

d dtx = Ax + Bu, y = Cx + Du in a balanced

state space basis. Then, Storage function K = I. Allpass systems2 have PQ = I. Balanced transformation: P = Q. Then Q2 = I. System is stable: Q > 0 = ⇒ Q = I.

  • 2K. Glover, IJC, 1984

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 13 / 18

slide-36
SLIDE 36

Storage functions of allpass/lossless systems Storage function in balanced realization

Allpass systems and Balanced realization

Definition System representation is said to be in balanced state space basis if controllability Gramian P = observability Gramian Q. Theorem Stable, allpass system:

d dtx = Ax + Bu, y = Cx + Du in a balanced

state space basis. Then, Storage function K = I. Allpass systems2 have PQ = I. Balanced transformation: P = Q. Then Q2 = I. System is stable: Q > 0 = ⇒ Q = I.

  • 2K. Glover, IJC, 1984

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 13 / 18

slide-37
SLIDE 37

Storage functions of allpass/lossless systems Storage function in balanced realization

Allpass systems and Balanced realization

Definition System representation is said to be in balanced state space basis if controllability Gramian P = observability Gramian Q. Theorem Stable, allpass system:

d dtx = Ax + Bu, y = Cx + Du in a balanced

state space basis. Then, Storage function K = I. Allpass systems2 have PQ = I. Balanced transformation: P = Q. Then Q2 = I. System is stable: Q > 0 = ⇒ Q = I.

  • 2K. Glover, IJC, 1984

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 13 / 18

slide-38
SLIDE 38

Storage functions of allpass/lossless systems Adjoint system

Positive-real system and its adjoint

System B :: states x Minimal i/s/o representation ˙ x = Ax + Bu y = Cx + Du Adjoint system B⊥Σ :: co-states λ Minimal i/s/o representation ˙ λ = −AT λ + CT f e = BT λ − DT f Interconnect: u to f and y to e = ⇒ B ∩ B⊥Σ formed. First order representation of B ∩ B⊥Σ:        d dt   In In 0  

  • E

−   A B 0 −AT CT C −BT D + DT  

  • H

      

  • Hamiltonian pencil R(ξ)

  x λ u   = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 14 / 18

slide-39
SLIDE 39

Storage functions of allpass/lossless systems Adjoint system

Positive-real system and its adjoint

System B :: states x Minimal i/s/o representation ˙ x = Ax + Bu y = Cx + Du Adjoint system B⊥Σ :: co-states λ Minimal i/s/o representation ˙ λ = −AT λ + CT f e = BT λ − DT f Interconnect: u to f and y to e = ⇒ B ∩ B⊥Σ formed. First order representation of B ∩ B⊥Σ:        d dt   In In 0  

  • E

−   A B 0 −AT CT C −BT D + DT  

  • H

      

  • Hamiltonian pencil R(ξ)

  x λ u   = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 14 / 18

slide-40
SLIDE 40

Storage functions of allpass/lossless systems Adjoint system

Positive-real system and its adjoint

System B :: states x Minimal i/s/o representation ˙ x = Ax + Bu y = Cx + Du Adjoint system B⊥Σ :: co-states λ Minimal i/s/o representation ˙ λ = −AT λ + CT f e = BT λ − DT f Interconnect: u to f and y to e = ⇒ B ∩ B⊥Σ formed. First order representation of B ∩ B⊥Σ:        d dt   In In 0  

  • E

−   A B 0 −AT CT C −BT D + DT  

  • H

      

  • Hamiltonian pencil R(ξ)

  x λ u   = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 14 / 18

slide-41
SLIDE 41

Storage functions of allpass/lossless systems Adjoint system

Positive-real system and its adjoint

System B :: states x Minimal i/s/o representation ˙ x = Ax + Bu y = Cx + Du Adjoint system B⊥Σ :: co-states λ Minimal i/s/o representation ˙ λ = −AT λ + CT f e = BT λ − DT f Interconnect: u to f and y to e = ⇒ B ∩ B⊥Σ formed. First order representation of B ∩ B⊥Σ:        d dt   In In 0  

  • E

−   A B 0 −AT CT C −BT D + DT  

  • H

      

  • Hamiltonian pencil R(ξ)

  x λ u   = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 14 / 18

slide-42
SLIDE 42

Storage functions of allpass/lossless systems Adjoint system

Positive-real system and its adjoint

System B :: states x Minimal i/s/o representation ˙ x = Ax + Bu y = Cx + Du Adjoint system B⊥Σ :: co-states λ Minimal i/s/o representation ˙ λ = −AT λ + CT f e = BT λ − DT f Interconnect: u to f and y to e = ⇒ B ∩ B⊥Σ formed. First order representation of B ∩ B⊥Σ:        d dt   In In 0  

  • E

−   A B 0 −AT CT C −BT D + DT  

  • H

      

  • Hamiltonian pencil R(ξ)

  x λ u   = 0

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 14 / 18

slide-43
SLIDE 43

Storage functions of allpass/lossless systems Adjoint system

Lossless system and its adjoint

System B :: states x Minimal i/s/o representation ˙ x = Ax + Bu y = Cx + Du Adjoint system B⊥Σ :: co-states z Minimal i/s/o representation ˙ λ = −AT λ + CT f e = BT λ − DT f Interconnect: u to f and y to e = ⇒ B ∩ B⊥Σ formed. First order representation of B ∩ B⊥Σ:        d dt   In In 0  

  • E

−   A B 0 −AT CT C −BT  

  • H

      

  • Hamiltonian pencil R(ξ)

  x λ u   = 0 and det(sE−H) = 0.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 14 / 18

slide-44
SLIDE 44

Storage functions of allpass/lossless systems Static relations states and costates

Static relations: states and costates

Lossless system B: (A, B, C, D) minimal realization. B ∩ B⊥Σ:

  • E d

dt − H

 x λ u   = 0 and y = Cx + Du. Q: observability Gramian of allpass counterpart of B. Then, there exists a unique K = KT ∈ Rn×n such that d dtxT Kx = 2uT y for all u y

  • ∈ B.

if and only if rank

  • R(ξ)

−K I

  • = rank R(ξ).

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 15 / 18

slide-45
SLIDE 45

Storage functions of allpass/lossless systems Static relations states and costates

Static relations: states and costates

Lossless system B: (A, B, C, D) minimal realization. B ∩ B⊥Σ:

  • E d

dt − H

 x λ u   = 0 and y = Cx + Du. Q: observability Gramian of allpass counterpart of B. Then, there exists a unique K = KT ∈ Rn×n such that d dtxT Kx = 2uT y for all u y

  • ∈ B.

if and only if rank

  • R(ξ)

−K I

  • = rank R(ξ).

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 15 / 18

slide-46
SLIDE 46

Storage functions of allpass/lossless systems Static relations states and costates

Static relations: states and costates

Lossless system B: (A, B, C, D) minimal realization. B ∩ B⊥Σ:

  • E d

dt − H

 x λ u   = 0 and y = Cx + Du. Q: observability Gramian of allpass counterpart of B. Then, there exists a unique K = KT ∈ Rn×n such that d dtxT Kx = 2uT y for all u y

  • ∈ B.

if and only if rank

  • R(ξ)

−K I

  • = rank R(ξ).

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 15 / 18

slide-47
SLIDE 47

Storage functions of allpass/lossless systems Static relations states and costates

Static relations: states and costates

Lossless system B: (A, B, C, D) minimal realization. B ∩ B⊥Σ:

  • E d

dt − H

 x λ u   = 0 and y = Cx + Du. Q: observability Gramian of allpass counterpart of B. Then, there exists a unique K = KT ∈ Rn×n such that d dtxT Kx = 2uT y for all u y

  • ∈ B.

if and only if rank

  • R(ξ)

−K I

  • = rank R(ξ).

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 15 / 18

slide-48
SLIDE 48

Storage functions of allpass/lossless systems Static relations states and costates

Static relations: states and costates

Lossless system B: (A, B, C, D) minimal realization. B ∩ B⊥Σ:

  • E d

dt − H

 x λ u   = 0 and y = Cx + Du. Q: observability Gramian of allpass counterpart of B. Then, there exists a unique K = KT ∈ Rn×n such that d dtxT Kx = 2uT y for all u y

  • ∈ B.

if and only if rank

  • R(ξ)

−K I

  • = rank R(ξ).

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 15 / 18

slide-49
SLIDE 49

Storage functions of allpass/lossless systems Static relations states and costates

Static relations: states and costates

Lossless system B: (A, B, C, D) minimal realization. B ∩ B⊥Σ:

  • E d

dt − H

 x λ u   = 0 and y = Cx + Du. Q: observability Gramian of allpass counterpart of B. Then, there exists a unique K = KT ∈ Rn×n such that d dtxT Kx = 2uT y for all u y

  • ∈ B.

if and only if rank

  • R(ξ)

−K I

  • = rank R(ξ).

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 15 / 18

slide-50
SLIDE 50

Storage functions of allpass/lossless systems Static relations states and costates

Static relations: states and costates

For lossless systems:     ξI − A −B ξI + AT −CT −C BT −K I       x λ y   = 0 Static realtions between states x and co-states λ: λ = Kx States and co-states are related by observability Gramian.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 16 / 18

slide-51
SLIDE 51

Storage functions of allpass/lossless systems Static relations states and costates

Static relations: states and costates

For lossless systems:     ξI − A −B ξI + AT −CT −C BT −Q I       x λ y   = 0 Static realtions between states x and co-states λ: λ = Qx States and co-states are related by observability Gramian.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 16 / 18

slide-52
SLIDE 52

Storage functions of allpass/lossless systems Example revisited

Static relations: example

Lossless behavior B with transfer function G(s) =

0.2s s2+0.1.

d dt iL vC

  • =

1 2

− 1

5

iL vC

  • +

1 5

  • i

and v =

  • 1

iL vC

  • +0 i

Hamiltonian pencil:

R(ξ) =       ξ − 1

2 1 5

ξ − 1

5

ξ − 1

5 1 2

ξ −1 −1

1 5

      .

  • iL
  • i

vC

5F 2H

+ +

v

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 17 / 18

slide-53
SLIDE 53

Storage functions of allpass/lossless systems Example revisited

Static relations: example

Lossless behavior B with transfer function G(s) =

0.2s s2+0.1.

d dt iL vC

  • =

1 2

− 1

5

iL vC

  • +

1 5

  • i

and v =

  • 1

iL vC

  • +0 i

Hamiltonian pencil:

R(ξ) =           ξ − 1

2 1 5

ξ − 1

5

ξ − 1

5 1 2

ξ −1 −1

1 5

−2 1 −5 1           .

  • iL
  • i

vC

5F 2H

+ +

v

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 17 / 18

slide-54
SLIDE 54

Storage functions of allpass/lossless systems Example revisited

Static relations: example

Lossless behavior B with transfer function G(s) =

0.2s s2+0.1.

d dt iL vC

  • =

1 2

− 1

5

iL vC

  • +

1 5

  • i

and v =

  • 1

iL vC

  • +0 i

−1 5(ξ − 2) 0.5 (2 − ξ) 5ξ2 − 10ξ + 0.5 5

     ξ − 1

2 1 5

ξ − 1

5

ξ − 1

5 1 2

ξ −1 −1

1 5

      = −2 1 −5 1

  • =
  • −Q

I

  • C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian

Allpass systems and Gramian EE Dept. IIT Bombay 17 / 18

slide-55
SLIDE 55

Conclusion

Conclusion

1 One-to-one correspondence between lossless and allpass system:

The storage function remains same.

2 Observability Gramian is the storage function for allpass/lossless

systems.

3 Easy computation of storage functions of lossless systems. 4 In balanced basis, storage function is induced by identity matrix. 5 Static relations between states and its corresponding costates

induced by storage function.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 18 / 18

slide-56
SLIDE 56

Conclusion

Conclusion

1 One-to-one correspondence between lossless and allpass system:

The storage function remains same.

2 Observability Gramian is the storage function for allpass/lossless

systems.

3 Easy computation of storage functions of lossless systems. 4 In balanced basis, storage function is induced by identity matrix. 5 Static relations between states and its corresponding costates

induced by storage function.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 18 / 18

slide-57
SLIDE 57

Conclusion

Conclusion

1 One-to-one correspondence between lossless and allpass system:

The storage function remains same.

2 Observability Gramian is the storage function for allpass/lossless

systems.

3 Easy computation of storage functions of lossless systems. 4 In balanced basis, storage function is induced by identity matrix. 5 Static relations between states and its corresponding costates

induced by storage function.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 18 / 18

slide-58
SLIDE 58

Conclusion

Conclusion

1 One-to-one correspondence between lossless and allpass system:

The storage function remains same.

2 Observability Gramian is the storage function for allpass/lossless

systems.

3 Easy computation of storage functions of lossless systems. 4 In balanced basis, storage function is induced by identity matrix. 5 Static relations between states and its corresponding costates

induced by storage function.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 18 / 18

slide-59
SLIDE 59

Conclusion

Conclusion

1 One-to-one correspondence between lossless and allpass system:

The storage function remains same.

2 Observability Gramian is the storage function for allpass/lossless

systems.

3 Easy computation of storage functions of lossless systems. 4 In balanced basis, storage function is induced by identity matrix. 5 Static relations between states and its corresponding costates

induced by storage function.

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 18 / 18

slide-60
SLIDE 60

Thank you

Thank You Questions?

C.Bhawal, D.Pal, M.Belur (CC Grp.) (Control and Computing Group (CC Group)Department of Electrical EngineeringIndian Allpass systems and Gramian EE Dept. IIT Bombay 18 / 18