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The Influence of Three-Phase Auto-Reclosure of Transmission Line on the Dynamic Stability of Power Systems

Onuegbu JC*, Ezennaya SO, and Onyedikachi S

Department of Electrical Engineering, Nnamdi Azikiwe University, Awka, Anambra State, Nigeria.

Corresponding Author:
Onuegbu JC
Department of Electrical Engineering
Nnamdi Azikiwe University, Awka.

Received: 03/06/2013; Revised: 13/06/2013; Accepted: 02/07/2013

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Abstract

For a functional power system, the influence of automatic re-closure on the dynamic stability was ascertained by comparing calculated coefficients of system reserves during auto re-closure and without auto re-closure. It is only successful re-closure that was considered using double circuit power line and unsymmetrical short circuit. At the end of the work, a diagram was drawn to illustrate the pick-up area Ap and the retardation area Ar. For the calculation of the pick-up, retardation and then the coefficient of dynamic stability, there is also the need to find the re-closure angle δr and the re-closure time tr of the affected part. The dependence of re-closure angle on the re-closure time was tabulated. At the end of the investigation, coefficient of reserve of static stability kst at both normal regime and after short circuit regime was compared and found to have ensured higher stability when equipped with auto-re-closure. Lastly, the graph of switch-off angle limit δlim versus switch off time limit tlim was plotted and the result corresponded to the expected parameters.

Keywords

Fault clearance, automatic regulation, switch-off angle, re-closure angle, retardation angle, dynamic stability

Introduction

The paper examines the need to install automatic re-closure switchgears on the transmission lines. Two generator power station, double circuit transmission line with load was chosen to carry out this research. A complex parametric analysis of the system was carried out in per unit for normal system regime, faulty regime and post fault regime. In each stage of the calculation, the impedances, the admittances and the various self- and mutual angles for both generator and load were clearly stated. The system power was calculated for the conditions of absence of auto re-closure system, presence of semi auto re-closure and presence of automatic re-closure. The dependence of switch off angle on the switch off time was also investigated for 0 ≤ t ≤ 0.15 second. This clearly showed the transient behavior of the system, the speed up and the retardation angles and consequently the coefficient of dynamic stability for power system that is not equipped with automatic re-closure system as Kr = 1.4136. The result changed appreciably when the system was equipped with automatic re-closure system as the retardation angle increased 103.83° thereby raising the coefficient of dynamic stability to 1.5599. The fact that the coefficient of dynamic stability of the power system increased by 9.38 per cent when an automatic re-closure system was installed in the system shows that the installation of automatic re-closure system positively affects the dynamic stability of the power system.

Assumed input parameters used in the research work

engineering-technology-Generator-parameters

Table 1: Generator parameters

engineering-technology-Transformer-parameters

Table 2: Transformer parameters

Transmission line parameters: Voltage = 110KV,

Cosφ = 0.90, System voltage Vs = 35KV, line length = 50km,

Short circuit line length (from source) = 15km,

System power = 50.4 MW, Short circuit switch off time tsw = 0.15 sec., re-closure time tr = 0.1 sec.

Problem statement:

(1) To find static stability of the power system.

(2) To calculate dynamic stability of power system.

(3) To find the influence of auto re-closure on dynamic stability of transmission lines.

Calculation of system parameters

There are four sub-divisions of voltage level as can be seen from Fig.1.0. The calculation is done in per unit value taking the base values as Sb = 100 MVA and Vb = VbII = 115 KV. The base values of the remaining sections are: EquationEquation

Equation

Similarly, Equation

Equation

Equation

Similarly, Equation Fig. 2.0.

Line Parameters Equation where per unit reactance of aluminium conductor is 0.4 ohm/km [1].

Short circuit inductances X1k=(35/50)*0.151=0.1057; X2k=(15/50)*0.151=0.0453, where 50km = total line length and 15km=short circuit line length.

Conversion of system and load parameters to base values

Equation

Calculation of equivalent moment of inertia for the two generators

Equation

Similarly, Equation

Determination of reactive power of system and load

Load power is 54MW =(0.54+j0.235)

Equation

The next step is to simplify Fig. 2.0.

Equation

engineering-technology-transmission-lines

Figure 1: Circuit diagram of transmission lines

engineering-technology-Impedance-diagram

Figure 2: Impedance diagram of the transmission lines shown in figure 1

Equation

engineering-technology-Simplified-impedance

Figure 3: Simplified impedance diagram

The total voltage at the system bus bar is Equation

Equation

Voltage at the load bus bar

Equation

Equation

Loss of reactive power in the inductances of X9 and X10

Equation

Equation

Over all power available in the system

Equation

The power generated by the turbine is P0=1.044

Equation

The angle between emf E' and system voltage Equation

The synchronous emf Eq ∠ δ'0 will be defined. For this purpose, the schematic impedance diagram of Fig. 2.0 will be adjusted by replacing the transient reactance X'd of the generator with the synchronous reactance Xd value. Therefore Fig. 3.0 will express X12 as:

Equation

Equation

Equation

The angle between emf Eq and system voltage Vs is δ'1=38.63°+9.28°=47.91° Voltage VG on the busbar of the equivalent diagram of generator excluding the generator resistance is represented by Fig. 2.0.

Equation

Equation

Equation

Calculation of self and mutual conductance at normal regime applying Fig. 3.0

Equation

a) Without auto regulation of excitation system the self inductance Z'11 will be:

Equation

The corresponding self impedance angle Equation

Self admittance of the circuit Equation

Mutual impedance of the current

Equation

Equation

The corresponding mutual admittance angle

Equation

Mutual admittance Equation

b) With the presence of semi-automatic excitation regulator, the impedance becomes:

Equation

The corresponding angle Equation

Self admittance Equation

Mutual impedance Equation

Equation

Equation

c) With the presence of automatic excitation regulator:

Equation

The corresponding self impedance angle Equation

Self admittance of the circuit Equation

Mutual impedance Equation

The corresponding mutual admittance angle

Equation

Mutual admittance Equation

Short circuit condition

In determining the shunt resistance created by one phase short circuit to ground, the diagram of Fig. 4.0 will be applied for reverse and zero sequences.

engineering-technology-System-reverse-sequence

Figure 4: System reverse sequence impedance diagram

For reverse sequence, load resistance is taken as 0.35Zload [2], therefore:

Equation

Rearranging the diagram of Fig. 4.0, it becomes:

Equation

Equation

Equation

Impedance transformation of figures 5 and 6

Equation

Equation

Equation

Equation

engineering-technology-impedance-conversion

Figure 5: Δ/Y impedance conversion

engineering-technology-Resultant-impedance

Figure 6: Resultant impedance from Figure 5

Equation

Equation

The equivalent impedance of the reverse sequence relative to the short circuit is Zeq.

Equation

engineering-technology-Zero-sequence-impedance

Figure 7: Zero sequence impedance diagram

For transmission lines, zero sequence reactance is defined as X0 = 3X1 [3]. Similarly, X20=3X5; X21=3X1k; X22=3X2k; X23=X2*X4/(X2+X4) = 0.0185*0.145/(0.0185+0.145) = j0.081

X24 = jX7/2 = j0.425/2 = j0.213 (Fig. 7.0).

engineering-technology-Conversion-impedance-diagram

Figure 8: Conversion of Δ/Y impedance diagram

Equation

Equation

Equation

Equation

Equation

The equivalent reactance of the zero sequence relative to the point of short circuit K(1) is defined as:

Equation

The impedance of the power line at the point of short circuit is:

Equation

Abnormal regime

Calculation of system reactance for single line-to-ground short circuit at15km distance from source.

Equation

Equation

Equation

engineering-technology-Abnormal-regime

Figure 9: Abnormal regime impedance diagram

Equation

Equation

Equation

Equation

Equation

engineering-technology-Equivalent-generator

Figure 10: Equivalent generator circuit

Current quantity and its flow during abnormal regime Fig. 10

Equation

Equation

Equation

Equation

Equation

Equation

Input emf Equation

Self impedance: Equation

Self admittance angle: Equation

Self admittance Equation

Mutual admittance Equation

Mutual impedance angle: Equation

Mutual admittance: Equation

Self and mutual reactance after accidental regime

Equation

Equation

Equation

engineering-technology-Reactances-after-accidental-regime

Figure 11a: Reactances after accidental regime

engineering-technology-Equivalent-diagram-after-accidental-regime

Figure 11b: Equivalent diagram after accidental regime

Self impedance: Equation

Self admittance angle: Equation

Self admittance: Equation

Mutual impedance: Equation

Self admittance angle: Equation

Self admittance: Equation

Determination of maximum power at normal regime

(a) Without automatic excitation regulator on generator

Equation

(b) With semi-automatic excitation regulator

Equation

(c) With automatic excitation regulator

Equation

6. Calculation of power characteristics at different regimes:

1) Maximum power at normal regime

Equation

2) Maximum power at faulty regime

Equation

3) Maximum power after fault clearance

Equation

Taking values of δ′ from 0° to 180°, the values of Pm′ ,Pm″′,and Pm″ will be calculated as shown in Table 3.

engineering-technology-Values

Table 3: Values of Equation

Static stability at normal regime without auto-regulation of excitation

Equation

Static stability at normal regime with semi-automatic regulation of excitation

Equation

Static stability at normal regime with automatic regulation of excitation

Equation

Static stability regime after fault clearance

Equation

For three phase short circuit Pm″′=0 4 . The limit of switch off angle δlim of the short circuit is defined thus:

Equation

where Equation

The coefficient 57.3° converts degrees to radians.

Determination of switch off angle as a function of switch off time δ′=f(t) can be drawn by taking intervals of t=0.15 at Δt=0.05 second.

First interval Δt=0 to 0.05 second

Electrical power given out at the first moment after the short circuit is Pm″′=0, this is because there will be no system voltage Vs during three phase short circuit. Power at the initial interval is P0 =1.044. Increase in angle for this interval is:

Equation

Equation

Second interval Δt=0.05 to 0.1 second, ΔP1 =P0 =1.044

Equation

Equation

Third interval Δt=0.1 to 0.15 second, ΔP2 =1.044 (switch off time)

Equation

Equation

Forth interval Δt=0.15 to 0.20 second, ΔP3 =1.044 (first power imbalance)

For this interval, the switch off of the short circuit begins. The electrical power given out after the accident in the beginning of the forth interval will be:

Equation

Where Equation

Equation

Second power imbalance at the beginning of the forth interval

Equation

Increase in angle for this interval:

Equation

Angle at the end of the forth interval

Equation

Fifth interval at Δt = 0.2 to 0.25 second

Equation

Equation

Equation

Equation

engineering-technology-Result

Table 4: Results of δ′ = f(t)

Table 4.0 is illustrated in Fig. 12.0, showing (δ0′=24.78°) angle between the emf and the system voltage. δsw′= δ3′=63.18° - the switch off angle at t=0.15 second. δr′=δ5′= 103.83° – retardation angle at the elapsed time (re-closure angle).

engineering-technology-Generator-swing-curve

Figure 12: Generator swing curve

Speed up area Ap and possible retardation area Ar are defined in Fig. 13.0

Equation

Equation

Reserved coefficient of dynamic stability of the power system (Kr) is defined as Equation

engineering-technology-Dynamic-stability-curve

Figure 13: Dynamic stability curve

The influence of a successful auto-reclosure on the dynamic stability of the system has been presented. From table 4, it is seen that reclosure angle δr′ is equal to 103.83° and reclosure time is 0.1second. Therefore, the retardation areas before Ar1 and Ar2 can be defined as stated below. These parameters can be used to define the coefficient of dynamic stability of the system through the influence of auto-reclosure equipment installed on the power system.

Equation

Equation

Equation

Finally, the coefficient of dynamic stability of the system Equation

Conclusion

As a result of the presence of automatic re-closure system on the power line, the re-closure angle was improved to 147.65°. Consequently, the coefficient of dynamic stability was raised to 1.5597 as compared with the 1.4136 earlier obtained after fault clearance. This result proves that the reserve of dynamic stability with auto re-closure in the system is more than when there is no auto re-closure system on the transmission line. Therefore, a successful automatic re-closure of transmission lines positively influences the dynamic stability of power systems.

References