Inte rnational Journal of Electrical and Ele ctronics Engineering Research (IJEEER) ISSN(P): 2250-155X; ISSN(E): 2278-943X Vol. 4, Issue 4, Aug 2014, 55-72 © TJPRC Pvt. Ltd. AN INVESTIGATION ON USE OF POWER SYSTEM STABILIZER ON TRANSIENT STABILITY OF POWER SYSTEM BHUWAN PRATAP SINGH1 , M. P. SHARMA2 & VISHU GUPTA3 1 M. Tech Student, Suresh Gyan Vihar University, Jaipur, Rajasthan, India 2 3 AEN, RVPNL, Jaipur, Rajasthan, India Assistant Professor, Suresh Gyan Vihar University, Jaipur, Rajasthan, India ABSTRACT This paper describes the effect of Power System Stabilizers (PSS) on transient stability of power system after occurrence of fault in power system. Studies have been carried out without and with PSS in AVR for a thermal power plant having 8 nos. identical generating units. A dynamic model of the RajWest Lignite Thermal Power Plant situated in the Western Rajasthan is adopted to simulate the effect of PSS for damping of po wer system oscillations. Simulation studies indicate that AVR having supplementary control signal from PSS, transient stability of power system increase. Power oscillations damp out faster. Frequency of generators reach in steady state condition in lesser time. With PSS, maximu m swing in power angle and power swing in transmission lines also reduce. KEYWORDS: Power System Stabilizers, Thermal Power Plant, Raj West Lignite Thermal Power INTRODUCTION Power System Stabilizers (PSS) are the most well-known and efficient devices to damp the power system oscillations caused by interruptions. The transient stability of a system can be improved by providing suitably tuned power system stabilizers on selected generators to provide damping to critical oscillatory modes. Suitably tuned Power System Stabilizers (PSS), will introduce a component of electrical torque in phase with generator rotor speed deviations resulting in damping of low frequency power oscillations in which the generators are participating. The input to stabilizer signal may be one of the locally available signals such as changes in rotor speed, rotor frequency, accelerating power, electrical power output of generator or any other suitable signal. This stabilizing signal is compensated for phase and gain to result in adequate component of electrical torque that results in damping of rotor oscillations and thereby enhance power transmission and generation capabilities. Constantly increasing intricacy of electric power systems, has enhanced interests in developing superior methodologies for Power System Stabilizers (PSS). Transient and dynamic stability considerations are among the main issues in the reliable and efficient operation of power systems. Low Frequency Oscillation (LFO) modes have been observed when power systems are interconnected by weak tie -lines. The LFO mode, with weak damping, is also called the electromechanical oscillation mode, and it usually happens in the frequency range of 0.1 to 2 Hz. PSSs are the most efficient devices for damp out these oscillations. POWER SYSTEM DATA 8×135 MW Lignite based pit head Rajwest power plant is situated in Barmer District of Rajasthan. All units are generating power at 13.8 kV voltage level. The two units are stepped up to 220 kV voltage level through 2x160 MVA, www.tjprc.org editor@tjprc.org 56 Bhuwan Pratap Singh, M. P. Sharma & Vishu Gupta 13.8/220 kV generating transformers and the remaining six units are stepped up to 400 kV voltage level through 6 x 160 MVA, 13.8/400 kV generating transformers. Further 400 kV and 220 kV busses inside the plant are interconnected through an ICT of 1×315 MVA, 400/220 kV. Then the power is evacuated to Jodhpur 400/220 kV, Barmer 400/220/132 kV, and Dhaurimanna 220/132 kV grid substations through 220 kV and 400 kV transmission lines. The following are the major interconnections with the Rajwest power plant to the Rajasthan grid 400kV Interconnections 400 kV S/C twin moose conductor line from Rajwest 400/220 kV substation to Barmer 400/220/132 kV substation with a line length of 15.311 km. 400 kV D/C twin moose conductor line from Rajwest 400/220 kV substation to Jodhpur 400/220 kV substation with a line length of 220 km. 1× 315 MVA, 400/220 kV Interconnecting transformer at Rajwest power plant. 220kV Interconnections 220 kV D/C zebra conductor line from Rajwest 400/220 kV substation to Barmer 400/220/132 kV substation with a line length of 15.311 km. 220 kV S/C zebra conductor line from Rajwest 400/220 kV substation to Dhaurimanna 220/132 kV substation with a line length of 90 km. Figure 1 gives the interconnection diagram in the vicinity of the Raj West power plant Figure 1: Interconnection Diagram in the Vicinity of the Raj West Power Plant Network Reduction In order to study the local modes of oscillations where the Rajwest power plant generators oscillates with the rest of the Rajasthan system, it is sufficient to reduce the n etwork at the boundary busses i.e. Barmer 220 kV and 400kV, Impact Factor (JCC): 5.9638 Index Copernicus Value (ICV): 3.0 57 An Inve stigation on Use of Power System Stabilizer on Transient Stability of Power System Dhaurimanna 220 kV and Jodhpur 400 kV with the dynamic equivalents. In the process of network reduction, some fictitious transformers are also added at the boundary busses based on the fault levels at the boundary buses. Three Phase Fault Levels at Boundary Buses To arrive at the equivalent impedance at the boundary buses, three phases to ground fault is created at the boundary busses with the full system and the contribution from the other braches which are of no interest (not represented in reduced network) and to be represented in the equivalents are calculated and represented in the equivalent system. Table 1 shows the three phases to ground fault contribution from all branches connected to the specified buses. Table 1: 3-Φ Fault Current at the Boundary Buses S. No. Fault at Bus 1 Barmer 220 kV Dhaurimanna 220 kV Jodhpur 400 kV Barmer 400 kV 2 3 4 3-Phase Fault with Reduced System in kA 18.893 3-Phase Fault with Full System in kA 17.854 8.722 8.462 14.216 12.163 13.433 11.096 Single line diagram of power system network with load flow study results is placed in figure 2. Figure 2: Single Line Diagram of Power System for Simulation Transmission Line Parameters Based on data available on transmission design followed by RRVPNL, per kilometer line parameters are given in Table 2 www.tjprc.org editor@tjprc.org 58 Bhuwan Pratap Singh, M. P. Sharma & Vishu Gupta Table 2: Transmission Line Parameters S. No 1 2 3 4 5 6 7 Description Conductor Type Voltage Rating Positive sequence resistance in ohm/km/ckt Positive sequence reactance in ohm/km/ckt Positive sequence half line charging susceptance in mho/km/ckt (B/2) Zero sequence resistance in ohm/km/ckt Zero sequence reactance in ohm/km/ckt Zero sequence half line charging susceptance in mho/km/ckt (B/2) Twin Moose 400 0.029792 0.332 1.734375 e-006 Conductor Type Zebra 220 0.0748746 0.3992516 1.466942 e-006 Panther 132 0.1622174 0.3861158 1.46349 e-006 0.16192 1.24 1.12e-006 0.219976 1.339228 9.20041e-007 0.4056307 1.6221744 1.317141e-007 Generator Parameters There are total 8 units of 135 MW rating at the Rajwest power plant. Generator parameters are same for all generators. Generator parameter are given in Table 3. Table 3: Generator Parameters S. No 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 Parameter Description MW rating MVA rating No. of units Rated voltage in kV Rated power factor Armature Resistance (Ra) in pu (Stator Resistance per phase at 75 C) Negative Sequence Reactance (Unsaturated) Potier Reactance Zero Sequence Reactance (Unsaturated) Direct Axis Reactance (Xd) (unsaturated) Direct Axis Transient Reactance (Xd') (Unsaturated) Direct Axis Sub- Transient Reactance (Xd") (Unsaturated) Quadrature Axis Reactance (Xq) (unsaturated) Quadrature Axis Transient Reactance (Xq') (Unsaturated) Direct Axis Sub- Transient Reactance (Xq") (Unsaturated) Direct Axis Transient Open Circuit Time Constant (T‟do) (Unsaturated) Direct Axis Sub – Transient Open Circuit Time Constant (T”do) (Unsaturated) Quadrature Axis Transient Open Circuit Time Constant (T‟qo) (Unsaturated) Quadrature Axis Sub – Transient Open Circuit Time Constant (T”qo) (Unsaturated) Generator Inertia Constant H (Generator +turbine + governor +excitation system) in MJ/MVA 21 NGT Voltage rating 22 NGR Value 135 158.8 8 13.8 0.85 (Lag) 1.02565e-3 0.19 pu 0.24 pu 0.19 pu 2.21 pu 0.24 pu 0.18 pu 2.072 pu 0.391 pu 0.195 pu 9.34 s 0.017 s 0.904 s 0.034 s 2.51 13.8/.240 kV 0.46 ohms Generator Transformer Details Raj west Power Plant two units are stepped up to 220 kV level through 13.8/220 kV generating tra nsformers and the remaining units are stepped up to 400 kV level through 13.8/400 kV generating transformers. The 13.8/220 kV and 13.8/400 kV generator transformer details is given in Table 4. Impact Factor (JCC): 5.9638 Index Copernicus Value (ICV): 3.0 59 An Inve stigation on Use of Power System Stabilizer on Transient Stability of Power System Table 4: Details of 13.8/220 kV and 13.8/400 kV Generating Transformer Parameters Transformer Name MVA Rating Primary Voltage in kV Secondary Voltage in kV % Positive sequence Impedance % Zero sequence Impedance Winding Configuration Type of tap changer (On load or Off load) Total no of taps Nominal tap Set tap Minimum & Maximum Tap range in pu (or) % Tap Minimum voltage in kV Voltage Maximum voltage in kV Tap Position Specification Generator Transformer (13.8 kV/230 kV) 160 13.8 230 12.5 11.25 Delta / Star grounded Off Load tap changer 5 3 3 Specification Generator Transformer (13.8 kV/ 420 kV) 160 13.8 230 12.5 11.25 Delta / Star grounded Off Load tap changer 5 3 2 •±5% •±5% 218.5 241.5 399 441 Exciter System Details The main function of AVR is to automatically adjust the field current of the sy nchronous generator to maintain the terminal voltage within continuous capability of the generator. All the generating units have the identical excitation systems i.e. AC excitation system (Field controlled alternator rectifier excitation system). The rect ifier in this excitation system is stationary and is fed from the generator terminal. The voltage regulator controls the firing angles of the thyristo rs and converts AC in to appropriate DC. This DC supply is fed to field winding of the alternator through slip rings. The block diagram of the excitation system in the figure 3. Figure 3: Block Diagram of Excitation System The Excitation system parameters are same for all units i.e. the generators which are stepped up to 220 kV voltage level as well as the generators stepped up to 400 kV voltage level. Excitation parameters are given in table 5. Table 5: Excitation System Parameters Constant KA TR TA TS Uk max Uk min www.tjprc.org Name Exciter Gain Amplifier time constant in s Integral Time Constant Gate Control Unit and Converter Time Constant Maximum voltage in pu Minimum voltage in pu Parameter Value 25 0.02 8.335 0.005 7.42 -5.7 editor@tjprc.org 60 Bhuwan Pratap Singh, M. P. Sharma & Vishu Gupta Power System Stabilizer (PSS) High performance excitation systems are essential for maintaining steady state and transient stability of modern synchronous generators, apart from providing fast control of the terminal voltage. But the fast acting exciters with high AVR gain can contribute to oscillatory instability in the power systems. This type of instability is characterized by low frequency (0.1 to 3 Hz) power oscillations which can persist (or even grow in magnitude) for no apparent reasons. This type of instability can endanger system security and limit power transfer. The major factors that contrib ute to the instability are Loading of the generator or Tie line Power transfer capability of transmission lines Power factor of the generators (Leading power factor operation is more problematic than the lagging power factor) AVR gain A cost effective and satisfactory solution to the problem of oscillatory instability is to provide damping for generator rotor oscillations. This is conveniently done by providing Power System Stabilizers (PSS) which are supplementary controllers in the excitation systems. This supplementary signal is derived from rotor velocity, frequency, electrical power or combination of these variables. PSS Block Diagram The block diagram of PSS used in the Rajwest power plant is shown in Fig ure 4. All the units in power plant have the same type of PSS. Figure 4: PSS Block Diagram The input to the PSS is electrical power (active) which is derived from the terminal of the generator. Each synchronous generator has the same input arrangement and the output of the PSS will act as a supplementary signal to AVR as shown in Figure 5. The PSS block diagram consists of Wash out circuit, dynamic lead lag compensators, and a limiter to limit the absolute value of PSS output. Impact Factor (JCC): 5.9638 Index Copernicus Value (ICV): 3.0 61 An Inve stigation on Use of Power System Stabilizer on Transient Stability of Power System Figure 5: AVR with PSS Block Diagram Washout Circuit The washout circuit is provided to eliminate steady state bias in the output of PSS which will modify the generator terminal voltage. The PSS is expected to respond only to transient variations in the input signal and not to the DC offsets in the signal. The washout circuit acts essentially as a high pass filter and it must pass all frequencies that are of interest. Dynamic Compensator The dynamic compensator consists of lead lag (phase) compensator blocks. The phase compensation block provides the appropriate phase lead characteristic to compensate for the phase lag between exciter input and the generator electrical (air-gap) torque. The dynamic compensator as shown in Fig ure 4 has two lead lag stages and has the following transfer function. There are two design criteria for the lead lag circuit namely, The time constants, T1 to T4 in the above equation are to be chosen from the requirements of the phase compensation to achieve desired damping torque. The gain of the PSS is to be chosen to provide adequate damping of all critical modes under various operating conditions. It is to be noted that PSS is tuned at a particular operating condition (full load condition with strong or weak AC system) which is most critical. Although PSS may be tuned to give optimum damping under such condition, the performance will not be optimal under other conditions. Limiter The output of the PSS must be limited to prevent the PSS acting to counter the action of the AVR. For example, when load rejection takes place, the AVR acts to reduce the terminal voltage when PSS action calls for higher value of the terminal voltage. It may be desirable to trip the PSS in case of load rejection. The negative limit of PSS output is of importance during back swing of the rotor (after initial acceleration is over). The AVR action is required to maintain the voltage (and thus prevent loss of synchronism) after the angular separation has increased. The PSS action in the negative direction must be curtailed more than in the positive direction. For this purpose, the PSS available at the Rajwest Power www.tjprc.org editor@tjprc.org 62 Bhuwan Pratap Singh, M. P. Sharma & Vishu Gupta plant has the following setting limits and is same for all the generating units. The parameters for the PSS and its settable range with actual settings are tabulated in Table 6. Table 6: PSS Parameter Settings Range Parameter T1 TW1 Ks1 TL1 TL2 TL3 TL4 Usmax Usmin Description Filter Time constant Washout Time Constant PSS Gain Factor Time constant of conditioning network Time constant of conditioning network Time constant of conditioning network Time constant of conditioning network Upper limit of stabilizing Value Lower limit of stabilizing Value Unit s s pu s s s s pu pu Range 0.003~0.02 0.01~15 0.1~100 0.01~10 0.01~10 0.01~10 0.01~10 100% 100% Actual Settings 0.01 5 -30 0.02 0.01 0.02 0.01 +1.0 1.0 Governor Parameters The block diagrams of governor-turbine model for 8x135 MW machines are as shown in Fig ure 6 and Figure 7 respectively. The time constants associated with governor and turbine system are shown in Table 7. Figure 6: Block Diagram of Governor Model for 135 MW Generator Figure 7: Block Diagram of Turbine Model for 135 MW Generator Table 7: Steam Turbine Data for 135 MW Generator S. No 1 2 3 4 5 6 7 8 9 10 11 Impact Factor (JCC): 5.9638 Constant Droop T1 T2 K1 K2 K3 Thp Tip Tlp Pmax Pmin Description Droop T1 in seconds Servo motor time constant in s Power extraction at HP turbine Power extraction at IP turbine Power extraction at LP turbine HP section time constant in second IP section time constant in second LP section time constant in second Maximum power limit in pu Minimum power limit in pu Value 0.05 0.3 2 0.3 0.397 0.303 0.1 10.12 0.14 1.1 0.01 Index Copernicus Value (ICV): 3.0 63 An Inve stigation on Use of Power System Stabilizer on Transient Stability of Power System SIMULATION RESULTS Faults of varying severity are simulated and stability of RWPL generators is investigated without and with PSS. Plots of following parameters are analyzed: Electrical power output of generators Swing curve of generators Frequency variation of generators The terminal voltage of generators The field voltage in pu The power flow on 220 kV D/C Rajwest-Jodhpur line The power flow on 400 kV D/C Rajwest-Jodhpur line Case 1: Single line to ground fault at Rajwest 220 kV bus created at 1.0 sec and cleared at 1.16 sec Plots for foresaid disturbance are placed from figure 8 to figure 14. Figure 8: Electric Power Variation of Generators (G1 + G2) without and with PSS Figure 9: Swing Curve of Generators (G1 + G2) without and with PSS www.tjprc.org editor@tjprc.org 64 Bhuwan Pratap Singh, M. P. Sharma & Vishu Gupta Figure 10: Frequency Variation of Generators (G1 + G2) without and with PSS Figure 11: Terminal Voltage Variation of Generators (G1 + G2) without and with PSS Figure 12: Electric Field Voltage Variation of Generators (G1 + G2) without and with PSS Impact Factor (JCC): 5.9638 Index Copernicus Value (ICV): 3.0 65 An Inve stigation on Use of Power System Stabilizer on Transient Stability of Power System Figure 13: Power Flow on 220 kV D/C Raj West-Barmer Line without and with PSS Figure 14: Power Flow on 400 kV D/C Raj West-Jodhpur Line without and with PSS Case 2: Single line to ground fault at Rajwest 220 kV bus created at 1.0 sec and cleared at 1.16 sec with opening of one circuit of 220 kV D/C RajWest LTPS -Barmer line Plots for foresaid disturbance are placed from figure 15 to figure 21. Figure 15: Electric Power Variation of Generators (G1 + G2) without and with PSS www.tjprc.org editor@tjprc.org 66 Bhuwan Pratap Singh, M. P. Sharma & Vishu Gupta Figure 16: Swing Curve of Generators (G1 + G2) without and with PSS Figure 17: Frequency Variation of Generators (G1 + G2) without and with PSS Figure 18: Terminal Voltage Variation of Generators (G1 + G2) without and with PSS Impact Factor (JCC): 5.9638 Index Copernicus Value (ICV): 3.0 67 An Inve stigation on Use of Power System Stabilizer on Transient Stability of Power System Figure 19: Electric Field Voltage Variation of Generators (G1 + G2) without and with PSS Figure 20: Power Flow on 220 kV D/C Raj West-Barmer Line without and with PSS Figure 21: Power Flow on 400 kV D/C Raj West-Jodhpur Line without and with PSS Case 3: Single line to ground fault at Rajwest 400 kV bus created at 1.0 sec and cleared at 1.16 sec Plots for foresaid disturbance are placed from figure 22 to figure 28. www.tjprc.org editor@tjprc.org 68 Bhuwan Pratap Singh, M. P. Sharma & Vishu Gupta Figure 22: Electric Power Output Variation of Generators (G3 to G6) without and with PSS Figure 23: Swing Curve of Generators (G3 to G6) without and with PSS Figure 24: Frequency Variation of Generators (G3 to G6) without and with PSS Impact Factor (JCC): 5.9638 Index Copernicus Value (ICV): 3.0 69 An Inve stigation on Use of Power System Stabilizer on Transient Stability of Power System Figure 25: Terminal Voltage Variation of Generators (G3 to G6) without and with PSS Figure 26: Electric Field Voltage Variation of Generators (G3 to G6) without and with PSS Figure 27: Power Flow on 220 kV D/C Raj West-Barmer Line without and with PSS www.tjprc.org editor@tjprc.org 70 Bhuwan Pratap Singh, M. P. Sharma & Vishu Gupta Figure 28: Power Flow on 400 kV D/C Raj West-Jodhpur Line without and with PSS OBSERVATIONS With PSS, initial peak in the electrical power output is slightly more than without PSS due to the fact that under faulty condition, the voltage is reduced and at the same time active power output also reduces. Since the AVR and PSS action under this condition is to increase the power output of the generator. This is due to the peculiar design of the AVR-PSS module where in the output signal of the PSS is added at the field voltage rather than at th e generator reference voltage. But it is also noted that, the oscillations in the electrical power output subsequent to the first peak are better damped. The oscillations in the electrical power are damped in lesser time with PSS as compared to without PSS. Swing curves indicate that with PSS, maximum oscillation in power angle of generators are reduce in first as well as subsequent swings. The oscillations in the generators power angle are damped in lesser time with PSS as compared to without PSS. Frequency curves indicate that oscillations in the generators frequency is reduce in first as well as subsequent swings. The oscillations in the generators frequency are damped in faster with PSS. With PSS, generator field voltage is increase due to addition of PSS output in the AVR output so that oscillations in the generator speed are damped out. With PSS, there is a lesser reduction in generators terminal voltage as compared to without PSS. With PSS, Power oscillations in transmission lines are less as compared to without PSS. CONCLUSIONS In this paper simulation studies have been carried out for a thermal power plant having 8 nos. identical units for different types of faults to find out the effect of power system stabilizers on transient stability of power system. Studies have been performed without and with PSS for different types of faults in the power system. Simulation studies indicate that AVR having supplementary control signal from PSS, transient stability of power system increase. Power oscillations damp out faster. Frequency of generators reach in steady state condition in lesser time. With PSS, maximum swing in power angle and power swing in transmission lines are also reduce. Impact Factor (JCC): 5.9638 Index Copernicus Value (ICV): 3.0 71 An Inve stigation on Use of Power System Stabilizer on Transient Stability of Power System REFERENCES 1. K. R. Padiyar, „Power system dynamics, stability & control‟, (Book), BS Publications, 2006. 2. Prabha Kundur, „Power system stability & control‟, (Book), Tata McGraw Hill, 2007. 3. E. V. Larsen, P. Swann, „Applying Power system stabilizers, Part I, II and III‟, IEEE Transactions on Power Apparatus & systems, Vol. PAS 100, No.6, pp 3017-3046, June 1981. 4. Y. Hsu, S. Shyue, C. Su, “Low frequency oscillations in longitudinal systems: experience with dynamic stability of Taiwan power system”, IEEE Trans., Vol. PWRS-2, No. 1, February 1987, pp. 92-100. 5. B. E. Elliason, D. J. Hill, “Damping structure and sensitivity in the NORDEL power system”, IEEE Trans. on Power Systems, Vol. 7, NO. 1, 1992, pp. 97-105. 6. Chung-Liang Chang, Chuan-Sheng Liu, Chun-Kuang KO, Experience with power system stabilizers in a longitudinal power system”, IEEE Trans. on Power Systems, Vol. 10, No. 1, February 1995. pp. 539-545. 7. F. Aboytes, G. Arroyo, “Application of static VAR compensators in longitudinal power systems”, IEEE Trans. On Power Apparatus and Systems, Vol. PAS-102, No. 10, October, 1983, pp. 3460-3466 8. F. P. deMello and C. Concordia, "Concepts of Spmnous Machine Stability as Affected by Excitation Control". IEEE Transadions on Power Apparatus and Systems, Vol. PAS88-4, April 19. pp 316-330. 9. P. L. Dandeno. A. N. Karas. K. R. McClymont and W. Watson. "Effect of High-speed Rectifier Excitation Systems on Generator Stability Limits". IEEE Transactions on Power Apparatus and Systems, Vol. PAS87-1. January 1 9 6 8, pp 190-201 10. W. Watson and G. Manchur. "Experience with Supplementary Damping Signals fo r Generator Static Excitation Systems". IEEE Transactions on Power Apparatus & Systems, Vol. PAW-1, Jan/Feb. 1973, pp 199-204. AUTHOR’S DETAILS Mr. Bhuwan Pratap Singh has received his B. Tech degree in Electrical Engineering from Rajasthan Technical University, Kota in 2011. He is currently pursuing M. Tech.(Power System) from Suresh Gyan Vihar University, Jaipur (email: halobhuwan@gmail.com) Dr. M. P. Sharma received the B. E. degree in Electrical Engineering in 1996 Govt. Engineering College, Kota, Rajasthan and M. E. degree in Power Systems in 2001 and Ph. D. degree in 2009 from Malaviya Regional www.tjprc.org editor@tjprc.org 72 Bhuwan Pratap Singh, M. P. Sharma & Vishu Gupta Engineering College, Jaipur (Now name as MNIT). He is presently working as Assistant Engineer, Rajasthan Rajya Vidhyut Prasaran Nigam Ltd., Jaipur. He is involved in the system studies of Rajasthan power system for development of power transmission system in Rajasthan and planning of the power evacuation system for new power plants. His research interest includes Reactive Power Optimization, Power System Stability, Islanding of power system, reduction of T&D losses and protection of power system.(email:mahavir_sh@rediffmail.co m) Ms Vishu Gupta has finished her bachelor of science in Electrical Engineering(B. S. S.E) in 2009 and Master of Science in Electrical Engineering(M. S. E. E.) in 2012 from the University of Idaho, Mascow, Idaho, USA. She is currently working in Suresh Gyan Vihar University, Jaipur, India as an Assistant Professor in the department of Electrical Engineering. Research interest includes low power consumption in power electronics devices, embedded system application in power system and power electronics. Impact Factor (JCC): 5.9638 Index Copernicus Value (ICV): 3.0