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ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010



      Centralized Optimal Control for a Multimachine
     Power System Stability Improvement Using Wave
                        Variables

                           Soheil Ganjefar*                                                                        A. Judi
                        Member of IEEE                                                                  Electrical Department
                      Bu-Ali Sina University                                                            Bu-Ali Sina University
                         Hamedan, Iran                                                                     Hamedan, Iran
                      S_ganjefar@basu.ac.ir                                                              Af.judi@gmail.com


Abstract— this paper introduces the application of wave variable          In this paper we proposed a 4 buses 2 generators system which
method in reducing the effect of delay during the transmission of         can be a common multimachine plant [10].
control signals via large distances in a multimachine power                  The single line diagram of the multimachine model is
system. Fast response and pure control signals applied to a power         described in Figure 1.
system have great importance in control process. At first we
design a centralized optimal control considering no transport
delay and then we compare them to the one considering this effect
in order to demonstrate the deteriorating effect of transmission
delay. Then we apply the wave variable method and it is shown
that performance of centralized optimal controller is improved.

   Keywords- Centralized optimal control, delay; multimachine;
wave variable

                           I.      INTRODUCTION
                                                                                                 Fig. 1: Two-machine four-bus system
    Over the past years, there have been many researches about
dynamic stability of power system and many solutions have                                       III.     LQR OPTIMAL FEEDBACK
been introduced. The Linear Quadratic Regulator (LQR)                        Here we explain briefly the LQR method used in this paper
optimal feedback is one of many tools to improve the stability            [4,6]. In general we should have the state space model of the
of an interconnected power system. Using LQR theory, it has               system. A power system model can be written in state space
been established that for a controllable LTI system, a set of
                                                                          equation as follows:
Power System Plant optimal feedback gains may be found
                                                                           &
                                                                           X(t) = Ax(t) + Bu(t)                                     (1)
which minimizes a quadratic index and makes the closed-loop
system stable [1,2,3].                                                    Y(t) = Cx(t)                                                         (2)
    Applying the control signals to a multimachine power                  Where A, B and C are system matrices and
system requires to sending these signals through large distances
of transmission channels which impose time delay to the control           x = [x1 , x 2 ,..., x n ]T , u = [u1 , u 2 ,..., u n ]T
signals. Control signals should be applied fast and accurate in
order to have their ameliorative effects. This issue is very
important particularly during the faults and disturbances.                The vectors x and u are considered as measurable state
                                                                          variables and input control signals. For example, assuming an
    Wave variable method applied in this paper significantly              n-machine model, that is written in variables x and u as
improve the performance of the optimal controller during the              follows:
changes occur because of the transmission delay. Therefore, this
idea gives a new practical way in stabilization large scale power
systems via a centralized optimal control.                                x = [ΔE′ , ΔE′ , Δδi , Δωi , ΔTmi , ΔCVi , ΔSR i , ΔE fi , ΔVRi , ΔVSi ]T
                                                                                 qi    di

                                                                          u = [U ei , U gi ]T , i = 1,2,..., n
                     II.        POWER SYSTEM PLANT
   A power system model can be regarded as an interconnected              A. Gain Determination
system that consists of generations, transmissions and loads [1].           Equation (1) and Equation (2) can be developed to solve an
                                                                          LQR optimal feedback solution. The Index value of LQR to be
* Corresponding author. Bu-Ali Sina University, Hamedan, Iran             minimized can be written as follows:




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© 2010 ACEEE
DOI: 01.ijepe.01.01.02
ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010

                                                                          u = [U e , U g ]T       and          ten          output   signals
          tf
        1
          ∫
                                                                                                                                     T
   J=     [x T (t)Qx(t) + u T (t)Ru(t)]dt                       (3)       x = [ΔE′ , ΔE′ , Δδ, Δω, ΔTm , ΔCV, ΔSR, ΔE f , ΔVR , ΔVS ] .Then
                                                                                 q     d
        2
          t0                                                              the interconnected system has 4 input signals and 20 output
                                                                          signals. The input nodes of the control signals are depicted in
  The solution of Equation (3) can be given as follows:                   Figure 3 and Figure 4 for the speed-governing system and the
                                                                          excitation system. Both figures also describe the models used
   S = A T S + SA − SBR −1BT S + Q
   &                                                            (4)       in this paper [1,10,11].
                                                                             The turbine model [1] also considered as a simple single
                                                                          degree model suitable for this study. The whole system
   If a time-varying positive symmetric matrix S(t) converges             structure is illustrated in Figure 5. All parameters are given in
at t f = ∞ the solution of Equation (4) can be obtained from an           TABLE I.
algebraic matrix Riccati equation as follows:

   0 = A T S + SA − SBR −1BT S + Q                              (5)

  The gain K can be written as follows:

   K = R −1B T S
   u = − Kx                                                     (6)
                                                                                              Fig. 3: Model of governing system
   Then Equation (1) can be written as a closed loop system so
that we can discuss the converging behavior using the
following equation:

   x = (A − BK)x
   &                                                            (7)

B. Weighting Matrices Q and R
   Weighting matrices Q and R are important components of an
LQR optimization process. The compositions of Q and R
elements have great influences on system performance. Q and
R are assumed to be a semi-positive definite matrix, and a                                    Fig. 4: Model of excitation system
positive definite matrix, respectively [4].
        IV.    CONTROL STRUCTURE AND SYSTEM MODEL                             V.     CENTRALIZED OPTIMAL CONTROL (COC) RESULTS

                                                                          A. COC Applied With No Delay
                                                                             The results are in response of a symmetrical three phase
                                                                          fault applied to the Bus 4 of the proposed system during 0.5 s
                                                                          considering breaker operation time and system restoration.
                                                                          System base is given in 1000 MVA.
                                                                             In this part we assume that the delay in transmitting the
                                                                          control signals is negligible so the delay is not considered in
                                                                          both sending and receiving signals.
                                                                             From the Figures 6-9, we can see the power angle and
                                                                          voltage variations. The Optimal control response is obviously
                                                                          the best achieved. Both voltage and frequency overshoots
                                                                          damp to the steady state sooner so the settling times improve.
                 Fig. 2: Interconnected system using LQR                  The control signals applied to the machines are shown in
                                                                          Figures 10-11.
   The power system assumed is constructed with                              The optimal controller has an obvious advantage in
interconnected two machines controlled by a LQR optimal                   stabilizing the power system.
controller as shown in Figure 2. The multimachine system is
represented in classical model based on Kundur [1]. The inputs
to the Generators are provided from the controller outputs, and
the inputs to the centralized controller are variables of the
generator plants. Each generator has two input signals




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© 2010 ACEEE
DOI: 01.ijepe.01.01.02
ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010




                                                  Fig. 5: The complete system structure

B. COC Applied Considering Transmission Delay                                              VI.     WAVE VARIABLES METHOD
   In this part the same conditions above are assumed. The                One of the useful methods for delay reduction is wave
LQR optimal controller is a centre which is positioned in some         variables method. In this method, by locating two transform
distance of the synchronous generators connected to centralized        functions on two sides of the signal path (between master and
controller in its area. Sending and receiving signals (as              slave), delay is reduced. Wave variables present a modification
mentioned before) through these large distances in a large scale       or extension to the theory of passivity which creates robustness
power system imposes the transport delay which can make a              to arbitrary time delays. The theory and its calculations are
change to the control signals and also the measured state              fully described in [5,9].
variables achieved from the generators. This change                       Here we introduce the wave variable transform. The
deteriorates the stabilizing effect of the optimal control and         parameter u is defined as the forward or right moving wave,
seriously damages the stability of the whole system. The               while v is defined as the backward or left moving wave. The
control signals are applied to the two major control systems           wave variables (u,v) can be computed from the standard power
which are the governing system and the AVR system as                   variables (x, F) by the following transformation.
                                                                                   &
described before.
   From the Figures 12-15, we can see the deteriorating effect                 bx + F
                                                                                &                bx − F
                                                                                                  &
of transmission delay both in power angle and voltage stability           u=              ,v =                                     (8)
cases. The optimal controller response is very bad and both                       2b               2b
generators are driven into unstable conditions.
   The voltage responses in both generators are oscillatory               Where b is the characteristic wave impedance and may be a
unstable and the power angles of each generators have                  positive constant or a symmetric positive definite matrix. It
increasing manner which means that the power angle stability           also has the role of a tuning parameter. We also have:
is lost. The control signals applied to the machines are shown
in Figure. 16.                                                            F = bx − 2b v, u = − v + 2b x
                                                                               &                      &                            (9)
   The delay time considered here is 2.22 up to 2.25 ms
approximately. The delay time is considered to be constant                All other combinations are also possible. Notice especially
during the simulation. We assumed that the distance between            the apparent damping element of magnitude b within the
the machines and the centralized optimal controller is the same        transformation. It retains the power necessary to compose the
which is only for convenience and has no effect on the whole           wave signal and then implicitly transmits the energy with the
concept.                                                               wave to the remote location [5].




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© 2010 ACEEE
DOI: 01.ijepe.01.01.02
ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010




                                                                                 Fig. 12: The effect of delay on the power angle of G1
                Fig. 6: Power angle variations of G1




                                                                               Fig. 13: The effect of delay on the terminal voltage of G1
                  Fig. 7: Voltage variations of G1




                                                                                 Fig. 14: The effect of delay on the power angle of G2
                Fig. 8: Power angle variations of G2




                                                                               Fig. 15: The effect of delay on the terminal voltage of G2

                  Fig. 9: Voltage variations of G2




                                                                  9
© 2010 ACEEE
DOI: 01.ijepe.01.01.02
ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010

                                                                        control signals that should be applied to generators. This
                                                                        process happens simultaneously as the control centre always
                                                                        monitors all the variations of the generators.
                                                                           Considering wave variables transform, the right moving and
                                                                        the left moving signals should have the same dimensions. For
                                                                        this reason we designed a kalman state estimator [12] in the
                                                                        optimal control centre that by using the generators outputs as
                                                                        measurement signals and some predetermined inputs of the
                                                                        generators as known inputs, estimates the state variables
                                                                        necessary for the LQR control. Notice that the estimator is
                                                                        designed fast enough to estimate the state variables correctly.
                                                                        Now we have two control inputs as right moving signals and
             Fig. 10: Optimal control signal applied to G1
                                                                        two outputs from each generator as left moving signals.
                                                                           The same fault condition assumed before is applied to the
                                                                        system and the delay time is considered 0.1 s and the parameter
                                                                        b is equal to 50.The Figures 18-21 show the results.




             Fig. 11: Optimal control signal applied to G2
                                                                                Fig. 18: Power angle variations using wave variables in G1




          Fig. 16: Optimal control signal applied to G1and G2                     Fig. 19: Voltage variations using wave variables in G1


     VII. CONTROL STRATEGY USING WAVE VARIABLES
   Figure 17 depicts the wave variable method used in this
paper. The master side which is the optimal control centre
receives the outputs of the generator which are the active
power P and the reactive power Q variations of the each
generator. Then the optimal control centre determines the




                                                                                Fig. 20: Power angle variations using wave variables in G2
                    Fig 17: Wave variable structure




                                                                   10
© 2010 ACEEE
DOI: 01.ijepe.01.01.02
ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010



                                                                                                  VIII.    CONCLUSION
                                                                           In this paper we discussed a new method in power system
                                                                        stabilization. We have considered the real situation of large
                                                                        scale power systems considering the deteriorating effect of
                                                                        time delay in the method proposed. Wave variables method
                                                                        proposed in this paper has the obvious ameliorating effect and
                                                                        reduces the effect of delay.


                                                                                                      REFERENCES
         Fig. 21: Voltage variations using wave variables in G2         [1] P.Kundur, Power System Stability and Control. NewYork: McGrawHill,
                                                                        1994.
                       TABLE I: Machines Data                           [2] P.M.Anderson, A.A. Fouad, Power System Control and Stability. The Iowa
                                                                        State University Press, 1977.
  Parameter                 Generator 1              Generator 2        [3] I.Robandi, K.Nishimori, R.Nishimura, N.Ishahara, “Optimal Feedback
  Type                        Steam                    Steam            Control Design Using Genetic Algorithm in Multimachine Power System,”
  Rated MVA                   920.35                     911            Electrical Power & Energy Systems, 2001.
                                                                        [4] D.E.Kirk, Optimal Control Theory. NewYork: Dover Publications,Inc,
  Rated KV                       18                       26            2004.
  Power Factor                  0.9                      0.9            [5] G. Niemeyer, J.E. Slotine, “Using Wave variables for System Analysis and
                                                                        Robot Control,” IEEE Trans., pp. 1619-1625, 1997.
  Speed (rpm)                  3600                     3600            [6] M. Johnson, MJ. Grimble, “Recent Trends in Linear Optimal Quadratic
  D (pu)                         2                        2             Multivariable Control System Design,” IEE Proc. Part D, 1987.
                                                                        [7] W. E. Dixon, D. M. Dawson, B. T. Cpstic, M. S. Queiroz, “Toward the
  H (s)                         3.77                     2.5            Standardization of a MATLAB-based Control Systems Laboratory Experience
   rs (pu)                    0.0048                    0.001           for Undergraduate Students”, in Proc. American Control Conf. Arlington, VA,
   x ls (pu)                   0.215                    0.154           pp. 1161-1166, 2001.
                                                                        [8] F.P. DeMello, C. Corcordia, “Concepts of Synchronous Machine Stability
   x d (pu)                    1.79                     2.04            as Affected by Excitation Control,” IEEE Trans., Vol. PAS-88, pp. 316-329,
  x ′ (pu)
    d                          0.355                    0.266           April 1969.
                                                                        [9] M. Alise, R.G. Roberts, D.W Repperger, “The Wave Variable Method for
   x q (pu)                     1.66                    1.96            Multiple Degree of Freedom Teleoperation System with Time Delay” , IEEE
   x ′ (pu)
     q                         0.570                    0.262           International Conference, pp. 2908-2913, May 2006.
                                                                        [10] C. Ong, Dynamic Simulation of Electric Machinery. Prentice Hall, 1998.
   K A (pu)                      50                       50            [11] IEEE Recommended Practice for Excitation System Models for Power
   TA (s)                       0.07                    0.06            System Stability Studies, IEEE Standards 421.5, 1992.
     max                                                                [12] G. Welch, G. Bishop, An Introduction to the Kalman Filter. University of
  VR (pu)                         1                        1            North Carolina at Chapel Hill, 1995.
     min
  VR (pu)                        -1                       -1
  K E (pu)                   -0.0465                  -0.0393
  TE (s)                       0.052                    0.44
  A Ex (pu)                   0.0012                   0.0013
  B Ex (pu)                    1.264                    1.156
  K f (pu)                    0.0832                    0.07
  Tf (s)                         1                        1
    ′
  Tdo (s)                       7.9                       6
    ′
  Tqo (s)                      0.41                      0.9
  KG                             20                       20
  TSR (s)                       0.1                      0.1
  TSM (s)                       0.3                      0.3
  Ttu (s)                       0.3                     0.27

        TABLE II: Impedances of tie lines and admittance of load
   Z14 (pu)                                    0.004 + j0.1
   Z 24 (pu)                                   0.004 + j0.1
   Z 34 (pu)                                   0.008 + j0.3
   y 40 (pu) (load bus)                         1.2 – j0.6




                                                                   11
© 2010 ACEEE
DOI: 01.ijepe.01.01.02

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Centralized Optimal Control for a Multimachine Power System Stability Improvement Using Wave Variables

  • 1. ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010 Centralized Optimal Control for a Multimachine Power System Stability Improvement Using Wave Variables Soheil Ganjefar* A. Judi Member of IEEE Electrical Department Bu-Ali Sina University Bu-Ali Sina University Hamedan, Iran Hamedan, Iran S_ganjefar@basu.ac.ir Af.judi@gmail.com Abstract— this paper introduces the application of wave variable In this paper we proposed a 4 buses 2 generators system which method in reducing the effect of delay during the transmission of can be a common multimachine plant [10]. control signals via large distances in a multimachine power The single line diagram of the multimachine model is system. Fast response and pure control signals applied to a power described in Figure 1. system have great importance in control process. At first we design a centralized optimal control considering no transport delay and then we compare them to the one considering this effect in order to demonstrate the deteriorating effect of transmission delay. Then we apply the wave variable method and it is shown that performance of centralized optimal controller is improved. Keywords- Centralized optimal control, delay; multimachine; wave variable I. INTRODUCTION Fig. 1: Two-machine four-bus system Over the past years, there have been many researches about dynamic stability of power system and many solutions have III. LQR OPTIMAL FEEDBACK been introduced. The Linear Quadratic Regulator (LQR) Here we explain briefly the LQR method used in this paper optimal feedback is one of many tools to improve the stability [4,6]. In general we should have the state space model of the of an interconnected power system. Using LQR theory, it has system. A power system model can be written in state space been established that for a controllable LTI system, a set of equation as follows: Power System Plant optimal feedback gains may be found & X(t) = Ax(t) + Bu(t) (1) which minimizes a quadratic index and makes the closed-loop system stable [1,2,3]. Y(t) = Cx(t) (2) Applying the control signals to a multimachine power Where A, B and C are system matrices and system requires to sending these signals through large distances of transmission channels which impose time delay to the control x = [x1 , x 2 ,..., x n ]T , u = [u1 , u 2 ,..., u n ]T signals. Control signals should be applied fast and accurate in order to have their ameliorative effects. This issue is very important particularly during the faults and disturbances. The vectors x and u are considered as measurable state variables and input control signals. For example, assuming an Wave variable method applied in this paper significantly n-machine model, that is written in variables x and u as improve the performance of the optimal controller during the follows: changes occur because of the transmission delay. Therefore, this idea gives a new practical way in stabilization large scale power systems via a centralized optimal control. x = [ΔE′ , ΔE′ , Δδi , Δωi , ΔTmi , ΔCVi , ΔSR i , ΔE fi , ΔVRi , ΔVSi ]T qi di u = [U ei , U gi ]T , i = 1,2,..., n II. POWER SYSTEM PLANT A power system model can be regarded as an interconnected A. Gain Determination system that consists of generations, transmissions and loads [1]. Equation (1) and Equation (2) can be developed to solve an LQR optimal feedback solution. The Index value of LQR to be * Corresponding author. Bu-Ali Sina University, Hamedan, Iran minimized can be written as follows: 6 © 2010 ACEEE DOI: 01.ijepe.01.01.02
  • 2. ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010 u = [U e , U g ]T and ten output signals tf 1 ∫ T J= [x T (t)Qx(t) + u T (t)Ru(t)]dt (3) x = [ΔE′ , ΔE′ , Δδ, Δω, ΔTm , ΔCV, ΔSR, ΔE f , ΔVR , ΔVS ] .Then q d 2 t0 the interconnected system has 4 input signals and 20 output signals. The input nodes of the control signals are depicted in The solution of Equation (3) can be given as follows: Figure 3 and Figure 4 for the speed-governing system and the excitation system. Both figures also describe the models used S = A T S + SA − SBR −1BT S + Q & (4) in this paper [1,10,11]. The turbine model [1] also considered as a simple single degree model suitable for this study. The whole system If a time-varying positive symmetric matrix S(t) converges structure is illustrated in Figure 5. All parameters are given in at t f = ∞ the solution of Equation (4) can be obtained from an TABLE I. algebraic matrix Riccati equation as follows: 0 = A T S + SA − SBR −1BT S + Q (5) The gain K can be written as follows: K = R −1B T S u = − Kx (6) Fig. 3: Model of governing system Then Equation (1) can be written as a closed loop system so that we can discuss the converging behavior using the following equation: x = (A − BK)x & (7) B. Weighting Matrices Q and R Weighting matrices Q and R are important components of an LQR optimization process. The compositions of Q and R elements have great influences on system performance. Q and R are assumed to be a semi-positive definite matrix, and a Fig. 4: Model of excitation system positive definite matrix, respectively [4]. IV. CONTROL STRUCTURE AND SYSTEM MODEL V. CENTRALIZED OPTIMAL CONTROL (COC) RESULTS A. COC Applied With No Delay The results are in response of a symmetrical three phase fault applied to the Bus 4 of the proposed system during 0.5 s considering breaker operation time and system restoration. System base is given in 1000 MVA. In this part we assume that the delay in transmitting the control signals is negligible so the delay is not considered in both sending and receiving signals. From the Figures 6-9, we can see the power angle and voltage variations. The Optimal control response is obviously the best achieved. Both voltage and frequency overshoots damp to the steady state sooner so the settling times improve. Fig. 2: Interconnected system using LQR The control signals applied to the machines are shown in Figures 10-11. The power system assumed is constructed with The optimal controller has an obvious advantage in interconnected two machines controlled by a LQR optimal stabilizing the power system. controller as shown in Figure 2. The multimachine system is represented in classical model based on Kundur [1]. The inputs to the Generators are provided from the controller outputs, and the inputs to the centralized controller are variables of the generator plants. Each generator has two input signals 7 © 2010 ACEEE DOI: 01.ijepe.01.01.02
  • 3. ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010 Fig. 5: The complete system structure B. COC Applied Considering Transmission Delay VI. WAVE VARIABLES METHOD In this part the same conditions above are assumed. The One of the useful methods for delay reduction is wave LQR optimal controller is a centre which is positioned in some variables method. In this method, by locating two transform distance of the synchronous generators connected to centralized functions on two sides of the signal path (between master and controller in its area. Sending and receiving signals (as slave), delay is reduced. Wave variables present a modification mentioned before) through these large distances in a large scale or extension to the theory of passivity which creates robustness power system imposes the transport delay which can make a to arbitrary time delays. The theory and its calculations are change to the control signals and also the measured state fully described in [5,9]. variables achieved from the generators. This change Here we introduce the wave variable transform. The deteriorates the stabilizing effect of the optimal control and parameter u is defined as the forward or right moving wave, seriously damages the stability of the whole system. The while v is defined as the backward or left moving wave. The control signals are applied to the two major control systems wave variables (u,v) can be computed from the standard power which are the governing system and the AVR system as variables (x, F) by the following transformation. & described before. From the Figures 12-15, we can see the deteriorating effect bx + F & bx − F & of transmission delay both in power angle and voltage stability u= ,v = (8) cases. The optimal controller response is very bad and both 2b 2b generators are driven into unstable conditions. The voltage responses in both generators are oscillatory Where b is the characteristic wave impedance and may be a unstable and the power angles of each generators have positive constant or a symmetric positive definite matrix. It increasing manner which means that the power angle stability also has the role of a tuning parameter. We also have: is lost. The control signals applied to the machines are shown in Figure. 16. F = bx − 2b v, u = − v + 2b x & & (9) The delay time considered here is 2.22 up to 2.25 ms approximately. The delay time is considered to be constant All other combinations are also possible. Notice especially during the simulation. We assumed that the distance between the apparent damping element of magnitude b within the the machines and the centralized optimal controller is the same transformation. It retains the power necessary to compose the which is only for convenience and has no effect on the whole wave signal and then implicitly transmits the energy with the concept. wave to the remote location [5]. 8 © 2010 ACEEE DOI: 01.ijepe.01.01.02
  • 4. ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010 Fig. 12: The effect of delay on the power angle of G1 Fig. 6: Power angle variations of G1 Fig. 13: The effect of delay on the terminal voltage of G1 Fig. 7: Voltage variations of G1 Fig. 14: The effect of delay on the power angle of G2 Fig. 8: Power angle variations of G2 Fig. 15: The effect of delay on the terminal voltage of G2 Fig. 9: Voltage variations of G2 9 © 2010 ACEEE DOI: 01.ijepe.01.01.02
  • 5. ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010 control signals that should be applied to generators. This process happens simultaneously as the control centre always monitors all the variations of the generators. Considering wave variables transform, the right moving and the left moving signals should have the same dimensions. For this reason we designed a kalman state estimator [12] in the optimal control centre that by using the generators outputs as measurement signals and some predetermined inputs of the generators as known inputs, estimates the state variables necessary for the LQR control. Notice that the estimator is designed fast enough to estimate the state variables correctly. Now we have two control inputs as right moving signals and Fig. 10: Optimal control signal applied to G1 two outputs from each generator as left moving signals. The same fault condition assumed before is applied to the system and the delay time is considered 0.1 s and the parameter b is equal to 50.The Figures 18-21 show the results. Fig. 11: Optimal control signal applied to G2 Fig. 18: Power angle variations using wave variables in G1 Fig. 16: Optimal control signal applied to G1and G2 Fig. 19: Voltage variations using wave variables in G1 VII. CONTROL STRATEGY USING WAVE VARIABLES Figure 17 depicts the wave variable method used in this paper. The master side which is the optimal control centre receives the outputs of the generator which are the active power P and the reactive power Q variations of the each generator. Then the optimal control centre determines the Fig. 20: Power angle variations using wave variables in G2 Fig 17: Wave variable structure 10 © 2010 ACEEE DOI: 01.ijepe.01.01.02
  • 6. ACEEE International Journal on Electrical and Power Engineering, Vol. 1, No. 1, Jan 2010 VIII. CONCLUSION In this paper we discussed a new method in power system stabilization. We have considered the real situation of large scale power systems considering the deteriorating effect of time delay in the method proposed. Wave variables method proposed in this paper has the obvious ameliorating effect and reduces the effect of delay. REFERENCES Fig. 21: Voltage variations using wave variables in G2 [1] P.Kundur, Power System Stability and Control. NewYork: McGrawHill, 1994. TABLE I: Machines Data [2] P.M.Anderson, A.A. Fouad, Power System Control and Stability. The Iowa State University Press, 1977. Parameter Generator 1 Generator 2 [3] I.Robandi, K.Nishimori, R.Nishimura, N.Ishahara, “Optimal Feedback Type Steam Steam Control Design Using Genetic Algorithm in Multimachine Power System,” Rated MVA 920.35 911 Electrical Power & Energy Systems, 2001. [4] D.E.Kirk, Optimal Control Theory. NewYork: Dover Publications,Inc, Rated KV 18 26 2004. Power Factor 0.9 0.9 [5] G. Niemeyer, J.E. Slotine, “Using Wave variables for System Analysis and Robot Control,” IEEE Trans., pp. 1619-1625, 1997. Speed (rpm) 3600 3600 [6] M. Johnson, MJ. Grimble, “Recent Trends in Linear Optimal Quadratic D (pu) 2 2 Multivariable Control System Design,” IEE Proc. Part D, 1987. [7] W. E. Dixon, D. M. Dawson, B. T. Cpstic, M. S. Queiroz, “Toward the H (s) 3.77 2.5 Standardization of a MATLAB-based Control Systems Laboratory Experience rs (pu) 0.0048 0.001 for Undergraduate Students”, in Proc. American Control Conf. Arlington, VA, x ls (pu) 0.215 0.154 pp. 1161-1166, 2001. [8] F.P. DeMello, C. Corcordia, “Concepts of Synchronous Machine Stability x d (pu) 1.79 2.04 as Affected by Excitation Control,” IEEE Trans., Vol. PAS-88, pp. 316-329, x ′ (pu) d 0.355 0.266 April 1969. [9] M. Alise, R.G. Roberts, D.W Repperger, “The Wave Variable Method for x q (pu) 1.66 1.96 Multiple Degree of Freedom Teleoperation System with Time Delay” , IEEE x ′ (pu) q 0.570 0.262 International Conference, pp. 2908-2913, May 2006. [10] C. Ong, Dynamic Simulation of Electric Machinery. Prentice Hall, 1998. K A (pu) 50 50 [11] IEEE Recommended Practice for Excitation System Models for Power TA (s) 0.07 0.06 System Stability Studies, IEEE Standards 421.5, 1992. max [12] G. Welch, G. Bishop, An Introduction to the Kalman Filter. University of VR (pu) 1 1 North Carolina at Chapel Hill, 1995. min VR (pu) -1 -1 K E (pu) -0.0465 -0.0393 TE (s) 0.052 0.44 A Ex (pu) 0.0012 0.0013 B Ex (pu) 1.264 1.156 K f (pu) 0.0832 0.07 Tf (s) 1 1 ′ Tdo (s) 7.9 6 ′ Tqo (s) 0.41 0.9 KG 20 20 TSR (s) 0.1 0.1 TSM (s) 0.3 0.3 Ttu (s) 0.3 0.27 TABLE II: Impedances of tie lines and admittance of load Z14 (pu) 0.004 + j0.1 Z 24 (pu) 0.004 + j0.1 Z 34 (pu) 0.008 + j0.3 y 40 (pu) (load bus) 1.2 – j0.6 11 © 2010 ACEEE DOI: 01.ijepe.01.01.02