Applications of Nonlinear Control by Meral Altınay - HTML preview

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Eq.(11) describes the voltage restriction relation after two diesel-generator sets enter into

parallel connection.

Eq.(9), Eq.(10) and Eq.(11) are the nonlinear mathematical model of two diesel-generator sets

on parallel connection, which reflects the relationship of interaction and mutual influence

between two diesel-generator sets, describing the variation law of power angle, speed and

voltage on two diesel-generator sets exactly.

3. Chaos oscillation analysis of diesel-generator set on parallel connection

This paper will make research on the stability of ship power system by the variation law of

power angle, speed and voltage on diesel-generator set. Due to the power transmission

between the diesel-generator sets on parallel connection, it is apt to produce power

oscillation. Power oscillation is the dynamic process of power of diesel-generator set

regulating repeatedly under the effect of some periodic interference.

Power oscillation is a chaos oscillation in nature from the point of view of chaos. The

fundamental feature of chaotic motion is highly sensitive to initial condition, the track which

is produced by two initial values which is very near each other, will separate according to

index pattern as time elapses, Lyapunov index is the quantity which describes the

phenomenon. Distinguishing methods of time series chaotic character include fix quantity

analysis and ocular analysis, first making numerical analysis for Lyapunov index and

judging the condition of chaos emerging, then determining if the chaos exists or not under

this condition by the method of ocular analysis. The methods of ocular analysis include time

course method, phase path chart method, strobe sampling method, Poincare cross section

method and power spectrum method. The methods of calculating Lyapunov index include

definition method, Wolf method and Jacobian method, Jacobian method is a method of

calculating Lyapunov index which develops in real application. This paper will use Jacobian

method to calculate Lyapunov index.

Considering following differential equation system

x  F( x)

(12)

Robust Control Research of Chaos

Phenomenon for Diesel-Generator Set on Parallel Connection

61

dx

In the equation: x 

,

m

x R . The evolution of tangent vector e of dot x( t) in the tangent

dt

space can be expressed by the equation as follow

F

e  T( x( t)) e , T

(13)

x

In the equation: T is Jacobian matrix of F . The solution of equation can be expressed as

(

e t)  U( t, (

e 0))

(14)

In the equation U : (0

e )  (

e t) is mapping of linear operator. The asymptotic behavior of

mapping U can be described by index as

1

(

e t)

( (

x 0), (

e 0))  lim ln

(15)

t t

(0

e )

So, the Lyapunov index of system (12) can be formulated as the mean of above repeat

process

1 k

((

e j  1) t

 )

  lim

ln

k k t

 

(

e j t

 )

j 1

(16)

1

((

e k  1) t

 )

(

e k t

 )

(

e 2 t

 )

 lim

ln

k kt

(

e k t

 )

(

e ( k  1) t

 )

(

e t

 )

For a phase space of n dimension, there will be n Lyapunov index, arranging them

according to the order from big to small, supposing       

1

2

n  ,

1 is called

maximum Lyapunov index. Generally speaking, having negative Lyapunov index

corresponds with contracting direction, the tracks which are near are stable in the part,

corresponding periodic motion. The positive Lyapunov index indicates that the tracks

which are near separate by index, the strange attractor is formed in phase space, the

Lyapunov index  is bigger, the chaotic nature of system is stronger, vice versa. For a phase

space of n dimension, the maximum Lyapunov index is whether bigger than 0 or not is the

basis of judging the system if has chaos oscillation or not.

Computing Lyapunov index of two diesel-generator sets on parallel running with light load

separately, two diesel-generator sets all use conventional controllers. Fig.1 and Fig.2 give the

phase diagram of power angle, speed and voltage of two diesel-generator sets on parallel

running with 12.5% load separately.

Two diesel-generator sets run for 100 seconds on parallel connection with 12.5% load, the

initial va1ue of No.1 diesel-generator set is: ( ,, U)  (0.1017,1.0662,0.9762) , Lyapunov

index is:  

 

  

1

0.076789 , 2 0.035235 , 3

0.197558 ; the initial va1ue of No.2 diesel-

generator set is: ( ,, U)  (0.1022,1.0662,0.9762) , Lyapunov index is:  

1

0.076806 ,

 

  

2

0.035230 , 3

0.197571 .

Fig.3 and Fig.4 give the phase diagram of power angle, speed and voltage of two diesel-

generator sets on parallel running with 25% load separately.

62

Applications of Nonlinear Control

1.6

1.4

1.2

U1

1

0.8

-40

1.5

-30

1

-20

0.5

-10

0

0

10

-0.5

ω1

δ1

Fig. 1. Phase diagram of No.1 diesel-generator set when two sets load 12.5% on parallel

connection

1.6

1.4

1.2

U2

1

0.8

-40

1.5

-30

1

-20

0.5

-10

0

0

10

-0.5

ω2

δ2

Fig. 2. Phase diagram of No.2 diesel-generator set when two sets load 12.5% on parallel

connection

Robust Control Research of Chaos

Phenomenon for Diesel-Generator Set on Parallel Connection

63

1.3

1.2

1.1

U1

1

0.9

-15

1.1

-10

1

0.9

-5

0.8

0

0.7

5

ω1

δ1

Fig. 3. Phase diagram of No.1 diesel-generator set when two sets load 25% on parallel

connection

1.3

1.2

1.1

U2

1

0.9

-15

1.1

-10

1

0.9

-5

0.8

0

0.7

5

ω2

δ2

Fig. 4. Phase diagram of No.2 diesel-generator set when two sets load 25% on parallel

connection

Two diesel-generator sets run for 100 seconds on parallel connection with 25% load, the

initial va1ue of No.1 diesel-generator set is: ( ,, U)  (0.1812,1.0607,0.9686) , Lyapunov

index is:  

 

  

1

0.079251 , 2 0.034251 , 3

0.199955 ;the initial va1ue of No.2 diesel-

64

Applications of Nonlinear Control

generator set is: ( ,, U)  (0.1820,1.0607,0.9686) , Lyapunov index is:  

1

0.078311 ,

 

  

2

0.034953 , 3

0.199742 .

From Fig.1 to Fig.4 we can see, all maximum Lyapunov indexes of the system are greater than

0, showing that the system exists chaotic phenomenon. Two diesel-generator sets with light

load on parallel connection, enter into chaotic state after running a length of time, their specific

expression are the oscillation of power angle and speed. Two diesel-generator sets on parallel

connection load the lighter, the oscillation of power angle and speed is severer. The oscillation

of power angle means the oscillation of power, the reason is the nonlinearity of ship power

system and the power transmission between the two diesel-generator sets. The controller in

this paper is proportional controller, which is a linear controller. It can’t control the nonlinear

character of ship power system, it can’t average the load in parallel operation control, there is a

power angular difference between the diesel-generator sets, thus engendering the power

transmission between the sets, which results in the happening of chaotic phenomenon.

Fig.5 and Fig.6 give the phase diagram of power angle, speed and voltage of two diesel-

generator sets on parallel running with 25% load plus periodicity load separately. The

periodicity load usually appears in ship power system, it is widespread.

Two diesel-generator sets run for 100 seconds on parallel connection with 25% load increasing

periodicity load 0.01sint, the initial va1ue of No.1 diesel-generator set is:

( ,, U)  (0.1812,1.0607,0.9686) , Lyapunov index is:  

 

1

0.073257 ,

2

0.031824 ,

  

3

0.191497 ; the initial va1ue of No.2 diesel-generator set is:

( ,, U)  (0.1820,1.0607,0.9686) , Lyapunov index is:  

 

1

0.073393 ,

2

0.030161 ,

  

3

0.189995 .

1.6

1.4

1.2

U1

1

0.8

-30

1

-20

0.8

-10

0.6

0

0.4

10

0.2

ω1

δ1

Fig. 5. Phase diagram of No.1 diesel-generator set when two sets increase periodicity load

meanwhile load 25% on parallel connection

Robust Control Research of Chaos

Phenomenon for Diesel-Generator Set on Parallel Connection

65

1.6

1.4

1.2

U2

1

0.8

-30

1

-20

0.8

-10

0.6

0

0.4

10

0.2

ω2

δ2

Fig. 6. Phase diagram of No.2 diesel-generator set when two sets increase periodicity load

meanwhile load 25% on parallel connection

From Fig.5 and Fig.6 we can see, all maximum Lyapunov indexes of the system are greater

than 0, showing that the system exists chaotic phenomenon. The oscillation of power angle

and speed in two diesel-generator sets is severer than the state of not increasing periodicity

load. Because the periodicity load is nonlinear, increasing periodicity load intensifies the

nonlinearity of system, thus aggravating the power oscillation of system[4-6].

The computer simulation results show that it exists chaotic oscillation phenomenon when

two diesel-generator sets run on parallel connection with light load. Primary cause of

emerging this phenomenon is the nonlinearity of ship power system, minor cause is the

power transmission between the two diesel-generator sets. Besides this, using conventional

linear controller is also a key factor of generating the chaotic oscillation of system. Only

using nonlinear controller, making the nonlinear characteristic of ship power system offset

and compensate, can we solve the problem of system chaotic oscillation fundamentally. The

chaotic oscillation phenomenon is transition state between stable state and unstable state, it

must be prevented in order to ensure the stability of system.

4. Design of nonlinear robust synthetic controller

Mixed H-two/H-infinity control theory is a robust control theory that has speed

development from the eighties of 20 century, which can solve the problem of robust stability

and robust performance[7-10]. Because diesel-generator set control system is a nonlinear

control system, using the method of direct feedback linearization to linearize the nonlinear

system, the state feedback controller is designed for linearization system using mixed H-

two/H-infinity control theory, thus acquiring nonlinear robust control law in order to reach

the purpose of restraining the chaotic phenomenon of ship power system, improving the

stability of ship power system.

66

Applications of Nonlinear Control

Because of coupling action between speed and voltage, the nonlinear robust synthetic

controller is designed for diesel-generator set in order to control speed and voltage

synthetically, making the both interaction in minimum range, thus improving the stability of

frequency and voltage in ship power system.

The principle diagram of diesel-generator set synthetic control system based on nonlinear

robust synthetic controller is shown in Fig.7. The diesel-generator set synthetic control

system is made up of diesel engine, generator, nonlinear robust synthetic controller,

actuator, oil feeding mechanism and exciter. Nonlinear robust synthetic controller is made

up of two parts, one is nonlinear H-two/H-infinity speed controller, another is nonlinear H-

two/H-infinity voltage controller.

The differential equation of actuator is

d L

L

K

1

 

u

(17)

dt

1

1

T

1

T

The differential equation of exciter is

d E

E

K

fd

fd

2

 

u

(18)

dt

2

2

T

2

T

Fig. 7. Principle diagram of diesel-generator set synthetic control system

First step, we design nonlinear H-two/H-infinity speed controller.

Combining Eq.(1) with Eq.(17), we can get the nonliear mathemaical model of diesel engine

speed regulation system.

d

  1,

d t

2

d

T

1

c

1

 

q

E U

1 U X

X

2

d

q

b

 

 

1

c

L

sin

sin 2 , (19)

d t

T

T

T

T X

T  2

a 0

a 0

a 0

a 0

d

a 0

XdXq

d L

L

K 1

 

u

 dt

1

1

T

1

T

Since Eq.(19) has nonlinear feature, the method of direct feedback linearization is used to

linearize Eq.(19). Order x  

 

1

, x

2

1 ,

Robust Control Research of Chaos

Phenomenon for Diesel-Generator Set on Parallel Connection

67

2

T

1

c

EU

U X  X

2

1

q

1

d

q

b

x

 

 

 , so Eq.(19) can be

3

1

c

L

sin

sin 2

T

T

T

T X

T  2

a 0

a 0

a 0

a 0

d

a 0

XdXq

written as

 x 1 x 2

 x  

(20)

2

x 3

1

d w

2

T

c K

c

EU

U ( X  X )

2 1

2

q

x 

x

u

L

cos (  1)

d

q

b

c os2  

 3

3

1

(

1)



a

T 0

a

T 1

T 0

a

T 1

T 0

a

T Xd 0

a

T XdXq 0

In the equation: 1

d w is the undesired signal which is assumed for using H-two/H-infinity

control method, including equivalence disturbance which is generated by disturbance

torque and modeling error.

Assigning virtual controlled variable

2

c K

c

EU

U ( X  X )

2 1

2

q

v

u

L

cos (  1)

d

q

c os2  

(21)

1

(

1)