Nonlinear Control Design of Series FACTS Devices for Damping Power System Oscillation

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American Journal of Applied Sciences 8 (): 4-8, 0 ISSN 546-939 00 Science Publications Nonlinear Control Design of Series FACTS Devices for Damping Power System Oscillation Prechanon Kumkratug Department of Electrical Engineering, Faculty of Engineering at Si Racha, Kasetsart University, 99 M.6, Tungsukhla, Si Racha, Chonburi, 030, Thailand Abstract: Problem statement: The disturbance in the complicated network of power system may cause in nonlinear response. Static Synchronous Series Compensator (SSSC) is a power electronic based device that has the capability of controlling the line current. This study applies the SSSC to decrease the over line current in power system during dynamic state. Approach: This study proposes the control strategy of a SSSC to enlarge the stability region of a simple power system. The control is determined very carefully to satisfy the Lyapunov s stability criterion and is found to be a non-linear function of system states. The proposed nonlinear control of SSSC for damping power system oscillation is investigated through the sample system. Results: The maximum generator rotor angle of the faulted system without a SSSC is continuously oscillation and the maximum value is much more than the system with a SSSC. Conclusion: SSSC based the proposed nonlinear control can damp power system oscillation. Key words: Power system stability, power system oscillation, FACTS devices, static synchronous series compensator, Static Synchronous Series Compensator (SSSC), Single Machine Infinite Bus (SMIB), voltage injection, voltage source, short circuit INTRODUCTION Modern power system network is getting much more complicated and heavily loaded than ever before. The consequences of such are the difficulty of power flow and risk of stability problem. Flexible AC Transmission System (FACTS) devices have been proposed to improve stability of power system (Barbuy et al., 009; Heraldo et al., 009; Osuwa and Igwiro, 00; Omar et al., 00; Zarate-Minano et al., 009). They have proposed many methods to improve stability of power system such as load shedding, High Voltage Direct Current (HVDC), Flexible AC Transmission System (FACTS), (Hannan et al., 009; Kumkratug, 00a; 00b; 00c; Hassan et al., 00a; 00b; Magaji and Mustafa, 009; Meshkatoddini et al., 009). A Static Synchronous Series Compensator (SSSC) is a member of the FACTS family that is connected in series with power system. The SSSC consists of a solid state voltage source converter with GTO thyristor switches or other high performance of semi-conductor and transformer. The SSSC can electrically mimic reactor and capacitor by injecting a shunt current in quadrature with the line voltage. The reactive power (or current) of the SSSC can be adjusted by controlling the magnitude and phase angle of the output voltage of the shunt converter (Al-Husban, 009; Mustafa and Magaji, 009). The disturbance in the complicated network of power system may cause in nonlinear response. This study presents the nonlinear control of SSSC for damping power oscillation. The proposed control is based on Lyapunov s theory. The simulation results are tested on a sample system. The effect of SSSC on damping power system oscillation is investigated in various cases. MATERIALS AND METHODS Mathematical model: Consider a single machine infinite bus system with a SSSC as shown in Fig. a. The equivalent circuit of the system is shown in Fig. b where the SSSC is represented by a variable synchronous voltage source of V s (Al-Husban, 009) and the generator is modeled by a constant voltage source behind transient reactance. Reactance X represents the sum of generator transient reactance and transformer leakage reactance and X represents the equivalent reactance of the parallel lines. The leakage reactance of the series transformer of SSSC can be included either in X or X. The phasor diagram of the system is shown in Fig. for various operating conditions of the SSSC. It can be seen in Fig. that, for given E and V, the SSSC voltage V s changes only the magnitude of the current but not its angle. 4

V E cos θ= tan δ Esin δ () From Fig. b, the general equation of the current can be E Vs V E V Vs I = = + = I0 +ΔI (3) jx jx jx Fig. : Single machine infinite bus system schematic diagram equivalent circuit Here I is an additional term appears because of the SSSC voltage V s. The electrical output power P e of the generator can be { * } P = R EI = P +ΔP (4) e e Here, P is the generator output power without SSSC (V s = 0) and is given by: P = P sinδ (5) max where, Pmax = E V/X. The additional power term P e appears in (4) is due to the SSSC voltage V s and can be * Vs EV s Pe sin( ) Δ =R E = δ α (6) jx X When V s lags the current by 90 (α = θ-90 ), P e becomes: EV s Δ Pe = cos( δ θ ) (7) X Fig. : Single machine infinite bus system with a SSSC schematic diagram equivalent circuit of system with a SSSC represented by a series voltage injection When V s = 0, the current I 0 of the system can be written as: E V I 0 = () jx Here, X = X +X. The angle θ of the current can be 5 After some mathematical manipulations of (), the term cos(δ-θ) can be expressed as: V cos( δ θ ) = cosθ E From Fig. 3, cosθ can be Esin δ Esin δ cosθ= = + δ xy E V E Vcos Using (7)-(9), P e can be expressed as: e s (8) (9) Δ P = CVP (0)

Thus the electrical output power of the generator in the presence of a SSSC becomes: Pe = P + CVP s () The dynamic of the generator, in classical model, can be expressed by the following differential equations: δ =ω () ω = [P m P e D ω ] (3) M Here δ, ω, P m, D and M are the rotor angle, speed deviation, input mechanical power, damping constant and moment inertia, respectively, of the generator. Equation and 3 can be rewritten in the following general form x = f(x,u) = f (x) + uf (x) (4) 0 Where: (c) Fig. 3: Phasor diagram without a SSSC with a SSSC operating in capacitive mode (c) with a SSSC operating in reactive mode Where: C = + δ (E ) V E Vcos x x δ ω = = x f 0(x) ω u = Vs f 0(x) = Pm P = f 0(x) M 0 f (x) f(x) = CP = f (x) M Control strategy: This study applies the Lyapunov s stability criterion to derive strategy of SSSC. The Lyapunov s function E of the system may be considered as: δ ω = ω δ δ+ (5) E(, ) M Pm Pmaxcos C0 Here, C 0 is a constant that makes E(x) = 0 at the post fault stable equilibrium point. The Lyapunov s stability criterion is defined by E(x) 0for all x. Using (4), the time derivative of E can be Note that C 0 for all possible values of E, V and δ. When V s leads the current by 90 (α = θ + 90 ), P e can also be determined from (0) by replacing V s by-v s. 6 E(x) x E(x) = x t = E(x)f (x) + E(x)uf (x) 0 (6)

The first term on the right side of (6) represents E(x) of the system without SSSC and can be expressed as: E(x)f (x) = [( P + P sin δ) M ω ] 0 m max ω P 0 m P D = ω M (7) Note that (7) is at least negative semi-definite for all values of ω. The contribution of SSSC appears in the second term on right hand side of (6) and which can Fig. 4: Sample system 0 E(x)f (x) = [( Pm + Pmaxsin δ) M ω]u CP M = CP uωsin δ max (8) To satisfy the negative semi definiteness criteria of Lyapunov s concept, the second term of (6) must also be satisfied in same criteria. This can be satisfied by properly selecting the value of the control u of (8). One of the possible candidates of u is: Fig. 5: The generator rotor angle of the system with and without a SSSC u = K ωsinδ (9) where, K is a gain. It can be seen in (9) that the control is a nonlinear type and it depends on the system states δ and ω. RESULTS The proposed nonlinear control of SSSC for damping power system oscillation will be investigated through the sample system. Figure 4 shows the sample system. The system parameters are: M=5.6, X t = 0., X d = 3, X L =0.4, X L =0.4, X L3 =0.9, X L4 =0.4, P m =0.9 Fig. 6: The generator rotor angle of the system with various gains of SSSC DISCUSSION It is considered that a 3-phase fault appears on line It can be observed from the simulation results that L and it is cleared by opening the faulted line. Figure 5 the system without a SSSC (K = 0) the generator rotor shows the generator rotor angle curve of the system angle increases monotonously and it is considered as with and without a SSSC. Figure 6 shows the generator unstable whereas the system with a SSSC (K = 30) can rotor angle curve of the system with various gains of a be considered as stable. This study also investigates the SSSC. effect of increasing the gain on damping improvement. 7

With the K= 30, the maximum generator rotor angle is around 0. With K = 0, the maximum is decreased to 98. CONCLUSION Static Synchronous Series Compensator (SSSC) is shunt FACTS devices. It has capability of improving power system oscillation. This study presents the nonlinear control of Static Synchronous Series Compensator (SSSC) for damping power system oscillation. The proposed control strategy is derived from Lyapunov s theory. The proposed nonlinear control of a SSSC is tested on sample system. It was found that the SSSC can damp power system oscillation. The maximum of the generator rotor angle can be decreased by increasing the gain. REFERENCES Al-Husban, A.N., 009. An eigenstructure assignment for a static synchronous compensator. Am. J. Eng. Applied Sci., : 8-86. DOI: 0.3844/ajeassp.009.8.86 Barbuy, H.S., A. Rocco, L.A.P. Fernandes and G.C. Guimaraes, 009. Voltage collapse risk associated to under-voltage capacitive compensation in electric power system operation. Am. J. Applied Sci., 6: 646-65. DOI: 0.3844/ajassp.009.646.65 Hannan, M.A., A. Mohamed, A. Hussian and M.A. Dabbay, 009. Development of the unified seriesshunt compensator for power quality mitigation. Am. J. Applied Sci., 6: 978-986. DOI: 0.3844/ajassp.009.978.986 Kumkratug, P., 00a. Fast decoupled power flow for power system with high voltage direct current transmission line system. Am. J. Applied Sci., 7: 5-7. DOI: 0.3844/ajassp.00.5.7 Kumkratug, P., 00b. Application of interline power flow controller to increase transient stability of power system. J. Comput. Sci., 6: 490-493. DOI: 0.3844/jcssp.00.484.487 Kumkratug, P., 00c. Improvement of transient stability of power system by Thyristor controlled phase shifter transformer. Am. J. Applied Sci., 7: 495-499. DOI: 0.3844/ajassp.00.495.499 Hassan, L.H., M. Moghavvemi and H.A.F. Mohamed, 00a. Takagi-sugeno fuzzy gains scheduled pi controller for enhancement of power system stability. Am. J. Applied Sci., 7: 45-5. DOI: 0.3844/ajassp.00.45.5 Hassan, L.H., M. Moghavvemi and H.A.F. Mohamed, 00b. Power system oscillations damping using unified power flow controller-based stabilizer. Am. J. Applied Sci., 7: 393-395. DOI: 0.3844/ajassp.00.393.395 Magaji, N. and M.W. Mustafa, 009. Optimal thyristor control series capacitor neuro-controller for damping oscillations. J. Comput. Sci., 5: 980-987. DOI: 0.3844/jcssp.009.980.987 Mustafa, M.W. and N. Magaji, 009. Optimal location of static var compensator device for damping oscillations. Am. J. Eng. Applied Sci., : 353-359. DOI: 0.3844/ajeassp.009.353.359 Meshkatoddini, M. R., M. Majidi, M. Sadeghierad and H. Lesani, 009. Comparison of UPFC-Based stabilizer and PSS performances on damping of power system oscillations. Am. J. Applied Sci., 6: 40-406. DOI: 0.3844/ajassp.009.40.406 Osuwa, J.C. and E. C. Igwiro, 00. Uninterruptible power supply using solar rechargeable battery. Phy. Int., : 77-8. DOI: 0.3844/pisp.00.77.8 Omar, R., N.A. Rahim and M. Sulaiman, 00. New control technique applied in dynamic voltage restorer for voltage sag mitigation. Am. J. Applied Sci., 3: 4-48. DOI: 0.3844/ajeassp.00.4.48 Zarate-Minano, R., T. Van Custsem, F., Milano, A.J. Conejo, 00. Securing transient stability using time-domain simulations within an optimal power flow. IEEE Trans. Power Syst., 5: 43-53. DOI: 0.09/TPWRS.009.030369 8