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Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com 
ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 
www.ijera.com 62 | P a g e 
An Investigation of the Ability of Combined Zero – Sequence Cutoff Protection in Line High Voltage Slobodan Bjelić1, Zorica Bogićević2, 1Faculty of Technical Sciences, Kosovska Mitrovica, Serbia 2Advanced High Technical School, Zvecan, Serbia ABSTRACT Zero-sequence cutoff protection has found extensive use in 110-400 kV power networks. Level of value protection settings a starting over-current relay is selected from the requirement of its adjustment out against three zero-sequence current on the end of protected line. Sensitivity of zero-sequence cutoff protection on line is function of equivalent zero-sequence impedance reduction to point bus-bars with disposition protection. Owing to availability of transformers with earthed neutrals at each substation of a 110-400 kV network which are the source of a zero-sequence current, the possibility exists of wide use of zero-sequence cutoffs and stepped zero-sequence protections practically on all lines of medium and large length. From these reasons propose is the use ``cutoff``` protection. 
Keywords – cutoff, substation, simulation, protection, voltage 
I. INTRODUCTION The protection consists of over-current relay CR responding to an earth fault, power-directional relay CP determining the direction of the fault power flow, and time relay TR introducing a time delay into the protection operation needed according to the selectivity requirement, Fig 1. The starting current relay and the current winding of the power-directional relay are connected into the neutral wire of the current transformers for current 3I0 [9,13] where as the polarizing (voltage) winding of the power relay is fed with voltage 3V0 from the broken delta connection of the voltage transformer [3,4]. The starting element of the zero-sequence protection features high sensitivity as it is not necessary to adjust the element out against load currents. To speed up the clearance of faults to earth in circuits with solidly earthed neutral, use is made of cutoffs which respond to a zero-sequence current. Their operating principle is the same as that of the cutoffs responding to a phase current. Zero-sequence cutoffs are available in plain current and directional versions, with and without time delay. 
II. DESCRIPTION OF COMBINED OVER CURRENT ZERO-SEQUENCE CUTOFF PROTECTION The operating current of the starting relays of a zero-sequence over-current protection is selected from two condition: -the requirement of reliable action of the protection in the event of a fault at the end of the adjacent (second) circuit section and -from the requirement of its adjustment out against unbalance currents. It is in this aspect that the directional cutoff fundamentally differs from the non-directional cutoff. The operating current of the directional cutoff is smaller than that of the non-directional one. That is why the zone of action of the first cutoff is much greater than that of the second zone. As a power relay features a dead zone, the directional cutoff should be used only in those cases when the plain cutoff fails to satisfy the sensitivity condition [6,7,8]. The directional instantaneous cutoff scheme differs from directional over-current protections, Fig. 1. in that it lacks a time relay. Combined over-current zero- sequence cutoff protection a) with voltage transformer, b) voltage transformer is absent, Fig. 1. a. and 1.b.). The sensitivity of the zero-sequence protections can be small therefore. When a fault appears the zero-sequence impedance can be grows concerned with impedance under normal service, where zero-sequence of current grows, for examples a include line or transformer (or autotransformer) with neutral point.. This sensitivity can be grows bat widely used combined zero-sequence protection consist of two relays schemes [9,10]: zero-sequence over-current relay and zero-sequence voltage relay. Three schemes is represent in (Fig.1.a, b, c). The circuit is assumed to be a no-load circuit. 
RESEARCH ARTICLE OPEN ACCESS
Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com 
ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 
www.ijera.com 63 | P a g e 
Fig.1: Combined overcurrent zero-sequence cutoff 
protection a) with voltage transformer, b) voltage 
transformer is absent, c). shows some cases of 
equivalent zero-sequence circuit current flow in 
certain parts of the circuit. 
II.I. CALCULATION AND ANALYSIS 
Fig 1.c, shows some cases of equivalent 
zero-sequence circuit current flow in certain parts of 
the circuit. The operating current of the directional 
zero-sequence cutoffs are adjusted out against current 
3I0max in the event of an earth fault (phase to ground 
or two-phase to ground fault) Line L on the busbars 
of the opposite substation (point) K according to the 
expression similar. It is assumed to include two 
transformer (PT1, PT2) with neutral point and current 
is: 
. . 0.max I k 3I op pr A r  (1) 
 0.max I maximum value of flowing zero-sequence 
current inside a line in considere transient conditions 
service substation in the event of an earth fault (phase 
to ground or two-phase to ground fault) line L on the 
starting busbar in point K and where PT2 transformer 
is include (conditions of maximum current). 
When is used combined zero-sequence 
cutoff protection bay diagram 1.a a) with voltage 
transformer and two relays: current relay CR and 
voltage relay VR it is necessary selected value of 
operating voltage relay of zero-sequence voltage VR 
to relation ( because  1 2 Z , Z are parallel 
connection): 
1 2 
1 2 
. . 0.max 3 
Z Z 
Z Z 
U k I op pr A VR  
 (2) 
 1 2 Z ,Z zero-sequence impedance power 
transformers (PT1, PT2) in equivalent scheme zero-sequence, 
Fig.1.c). 
The current operating of the current relay 
zero-sequence CR, represent in Fig. 1.a.,b. bay part a) 
it is needed from condition are adjusted out against 
current 3I0 in the event of an fault (phase to ground or 
two-phase to ground fault) Line Lon the busbars of 
the opposite substation (point) K according to the 
expression similar and assumed it is off duty one 
transformer, exemple PT2 with neutral point. 
3 . 
op. pr.A r 0.min.out putPT 2 I  k I (3) 
 
0.min.out putPT 2 
I maximum value of flowing zero-sequence 
current inside a line in considere transient 
conditions service substation in the event of an earth 
fault (phase to ground or two-phase to ground fault) 
line L on the starting busbar in point K and where 
PT2 transformer is off duty (coditions of minimum 
current). 
Estimation of combined zero-sequence 
cutoff protection can by made with comparation 
under transient condition of a minimum value current 
and of a maximum value current in a fault scheme. 
If a value operating current combined zero-sequence 
is considere from relation (3) small 
concerned magnitude operating current zero-sequence 
is considere from relation (1) should be 
coordinated so that the opera ting currents with 
sensitivity voltage relay kvr combined zero-sequence 
protection. It is clear ,under transient condition of 
maximum value of current in bouth equivalent 
schemes on a combined zero-sequence cutof 
protection the operating current of current relay and 
operatin voltage of voltage relay thei have equal 
sensitivity. The operating curren t of a current relay 
and operating voltage of a voltage relay calculate 
from one equivalent scheme (under transient 
conditions where are include both transformers 
[2,3,4]. 
Under transient conditions of minimum 
value of current the sensitivity of voltage relay is 
bigger, bay relation (4), 
 
 
 
. . 0 
0 . . 
3 
3 
U I 
U I 
k 
k 
op pr A 
op pr A 
SC 
SV 
= 
2 
1 2 
1 2 
1 2 
0 . . 
0 1 . . 
3 
3 
Z 
Z Z 
Z Z 
Z Z 
I I 
I Z I 
op pr A 
op pr A  
 
 
 
(4) 
Under transient conditions of minimum 
value of current the voltage relay have (Z1+Z2)/Z2 
time selectivity then current relays, bay circuit 
equivalent Fig. 1. c. 
III. EVALUATION OF THE DIFFERENT 
COMBINED ZERO-SEQUENCE CUTOFF 
PROTECTION 
The operating principle of protection is sim-ple 
and reliable, which enables circuits with two-end 
supply to be protected selectively. A combination of 
combined cutoffs protection with a directional over-current 
protection provides a protection which in
Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com 
ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 
www.ijera.com 64 | P a g e 
many cases provides fairly fast clearance of faults 
and sensitivity. Analyze and the service practice 
shows that the combined protection functions reliably 
[11,12,14]. 
The disadvantages of the protection are: 
-long time delays, near the sources of supply in 
particular; 
-insufficient sensitivity in circuits with large loads 
and relatively small fault current multiples; 
- a dead zone in the event of three-phase faults; 
-the possibility of the incorrect choice of the direction 
with the voltage circuit, feeding the power-directional 
relay, being damaged. 
The directional over current protection is 
widely used as the main protection in networks up to 
35 kV with two-end supply. In 110- and 220-kV 
networks, the classic directional overcurrent 
protection finds its application as a back-up 
protection, but sometimes, when combined with a 
cutoff, as the main protection. 
The selection of operating current 
op pr I . according to the first requirement is made in 
the same way as for the over current protection, pro-ceeding 
from the considerations set forth , by formula 
[1,3,4]: 
rst 
sa st mah 
op pr K 
k k I 
I 1 
.  (5) 
The maximum value of current Imax should 
be determined from the most severe but possible in 
service conditions. In ring circuits and in radial 
circuits with two-end supply (see Fig. 2.a and b) 
maximum loads develop on the lines upon 
disconnection them. For instance, if line LII is 
disconnected in the circuit shown in Fig. 2..b, the 
load current on line LI reaches its maximum. 
In this case, the phases of the voltages 
applied to the protection are distorted and therefore 
the power-directional relay can close its contacts 
enabling the protection to operate even if the power 
flow is towards the busbars of the substation. 
According to the second requirement the operating 
current of the protection is derived from the formula: 
[2,3], : 
op pr saf h ph I k I . .  (6) 
where h ph ld sh c I I kI    . [3,4] , and safety factor 
ksaf is taken as 1.15 to 1.30 depending on how 
accurately the value of Ih.ph is evaluated.. Taken as 
the final value of Iop.pr is the greater magnitude 
derived from expressions (5) and (6). 
As for protections in a circuit with small 
earth fault current (where h ph ld I  I . ) and 
protections in a circuit with solidly earthed neutral 
which are interlocked in the case of earth faults, the 
operating current of starting relays is selected 
according to the first requirement only, i.e., by 
formula (5). 
To provide selectivity, the sensitivity of the 
protections operating in one direction should be 
coordinated so that the operating currents grow as the 
power source is approached. Such coordination 
prevents the non-selective operation of the protection 
in the event of a fault current close in value to the 
operating currents of the protections. The aforesaid is 
illustrated by Fig.2.b. When a fault appears near the 
feeding busbars at point K1 the ratio of fault currents 
IKA and IKB is inversely proportional to 
impedance 1 ` K  z and 1 "K z , i.e., 
1 
1 
` 
" 
K 
K 
KB 
KA 
z 
z 
I 
I 
 (7) 
Fig. 2. Calculation of over current cutoff on 
parallel lines. Design schemes for selection of 
operating current of zero-sequence cutoffs on 
parallel lines (a, b, c) and nature of current I01 
variation in the case of fault on parallel line L2 
disconnected on one side (d) 
Consequently,, the operating current of a 
directional overcurrent cutoff is adjusted out against 
fault currents flowing from the busbars of the 
substation. 
Under these conditions the impedance of 
operative line L1 is reduced by mutual inductance 
due to current I02, which involves an increase in 
design current I01 and voltage. Three schemes is 
represent in (Fig.2.c). (see simulation Fig.4.a,b,c). 
Certain combinations of reactances xo of 
parts of the network under consideration may be 
responsible for a maximum current rise in line L1 not 
due to a fault on the busbars at point K1 but on the 
parallel line at point K when this line is disconnected 
on one side (Fig.2.c). (see simulation Fig.4.a,b,c.) 
Although the fault at point K2 is more 
distant than that at K1 current I01 in line L1 may now 
happen to be greater in value due to a change of' 
current flow in the parallel branches of the network 
because of a reduction in the impedance of line L1 
caused by the strong mutual inductance from line L2. 
Figure 2.d shows current I01 and full current Iok at the 
point of a fault plotted against the location of the
Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com 
ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 
www.ijera.com 65 | P a g e 
fault I0cal is represented by the greater of the 
obtained values of I01 . Zero-sequence currents 
should be calculated for that kind of an earth fault 
wherein their value is greatest. 
It is known from the fault current calculation 
theory that with equal total positive- and negative-sequence 
reactances of the equivalent circuit 
     1 2 x x current (1,1) 
0 
(1) 
0 I  I if    0 1 x x . 
After calculation and correlation of x0with 
x1we find the calculated form of the fault (single-phase- 
or two-phase-to-earth faults). 
IV. ANALYSIS OF THE SIMULATION RESULTS 
The Distributed Parameter Line block 
implements an N-phase distributed parameter line 
model with lumped losses. The model is based on the 
Bergeron's traveling wave method usedb y the 
Electromagnetic transient program (EMTP) [2,5]. 
The breaker block implements a circuit 
breaker where the opening and closing times can be 
controlled either from an external Simulink signal 
(external control mode), or from an internal control 
timer (internal control mode). The arc extinction 
process is simulated by opening the breaker device 
when the current passes through 0 (first current zero 
crossing following the transition of the Simulink 
control input from 1 to 0). Specifies the number of 
phases, N=3, of the model. 
Specifies the frequency used to compute the 
modal resistance R, inductance L, and capacitance C 
matrices of the line model. The resistance R per unit 
length, as an N-by-N matrix in ohm/km. For a 2- 
phase or three-phase continuously transposed line, 
you can enter the positive and zero-sequence 
resistances [R1 R0]. For a symmetrical six-phase line 
you can enter the sequence parameters plus the zero-sequence 
mutual resistance [R1 R0 R0m]. For 
unsymmet rical lines, you must specify the complete 
N-by-N resistance matrix. The inductance L per unit 
length, as an N-by-N matrix in henries/km (H/km). 
For a symmetrical line, you can either specify the N-by- 
N matrix or the sequence parameters. The 
capacitance C per unit length, in farads/km (F/km). 
For a symmetrical line, you can either specify the N-by- 
N matrix or the sequence parameters. For a 2 or 3 
phase continuously transposed line possible positive 
and zeo sequence (C1, C0). The line length, in km. 
(100km). 
Measurements: Select Phase-to-ground voltages to 
measure the sending end and receiving end voltages 
for each phase of the line model. Multi-meter block 
in model to display the selected measurement during 
the simulation. This model does not rep- resent 
accurately the frequency dependence of RLC 
parameter of real power lines, because of skin effects 
in the conductor and ground, the R and L matrice 
exhibit strong frequency dependence, causing an 
attenuation of the high frequencies. 
Example of simulation influence parallel line I and 
II. 
The psbmonophaseline.mdl illustrate as a 
100 km line connected on a pu(1), 50 Hz infinite 
source The line deenergized and reenenrgized after 2 
cycles.The simulation is performed simultaneously 
with the distributed parameters line block in Fig. 3. 
Fig. 3: The receiving end voltage obtained with 
distributed Parameter Line block. Phase (deg) 0, 
The influence phase (A) line I on phase (A) line II, 
closed Breaker 1 and 2 
Fig. 4. a) Phase (deg) 0, simulation of influence 
phase (A) line I upon phase (A) line II, open 
Breaker 2 , AI-yellow, AII-pink., b) Phase (deg) 
+120, simulation of influence phase (A) line I upon 
phase (B) line II, open Breaker 2. A- pink, B 
yellow, c) Phase (deg) +120, simulation of 
influence phase (A) line I upon phase (C) line II, 
open Breaker 2. , A- pink, C yellow.
Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com 
ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 
www.ijera.com 66 | P a g e 
V. CONCLUSION 
From increase sensitivity of protection in in protection from phase-to ground fault and two-phase to ground fault the combined zero-sequence cutoff protection is widely used as the main protection in network 110-400 kV. Consequently,, the operating parameters of a current and voltage relays in combined zero- sequence directional overcurrent cutoff is adjusted out against fault currents flowing from the busbars of the opposite substation. It is clear , from analysis, where is realized combined zero-sequence directional over-current and voltage cutoff is adjusted out against fault currents flowing from the busbars of the other lines with conditions selectivity of current and voltage relay. The zero-sequence cutoff protection is widely used as the main protection in network 110- 400 kV From increase of sensitivity in protection from phase-to ground fault and two-phase to ground fault. The operating principle of directional combined zero-sequence cutoff protection is simple and reliable, which enables circuits with two-end supply to be protected selectively. 
REFERENCES 
[1] S Bjelic, Z Bogićevic, Computer Simulation of Theoretical Model of Electromagnetic Transient Processes in Power Transformers, International Journal of Information Technology and Computer Science, (IJITCS)6, no. 1(2013): 1. 
[2] Dommel, H, Digital Computer Solution of Electromagnetic Transients in Single and Multiple Networks, IEEE Transactions on Power Apparatus and Systems, Vol. PAS- 88, No. 4, April, 1969. 
[3] J. Lewis Blackburn Thomas J. Domin: ``Protective Relaying Principles and Applications``,Third Edition, 2006 by Taylor&Francis Group, LLC., : 416-428. 
[4] Bjelic S. Overcurrent protections of distribution electrical networks / Prekostrujne zaštite distributivnih električnih mreža, 2009, UDK 621.313(075.8) SITOPRINT Niš, (2010), COBISS.SR-ID 512270494, 
[5] MATLAB SIMULINK Sim Power System, Copyright 1984-2002 the Math Works, Version 6.5.0, 180913a, June 2, 2000. 
[6] Bjelic S., Jelic N., Automatic Secondary VAR Control: A Multivariable Approach , ★★★★★ , 1995 01/01, German National Library of Science and Technology (GetInfo) BL CP. 
[7] Antonin Veverka: TECHNIKA VYSOKÝCH NAPĚTÍ SNTL/ALFA, DT621.3027.3: 621.315.31:II, Elektrickě 
razově jevy ve vinutih transforma torů a točivýh strojů, Praha, 1982. 
[8] Bjelic, S.,Mladenovic, V, Algorithm and possible method of emergency control electrical network View in Scopus | Show abstract, 9th Symposium on Neural NetworkApplications in ElectricalEngineering,NEUREL2008Proceeding,pp. 69 
[9] Markovic, N., Bjelic, S., Bogicevic, Z, Graphical zero-sequence cut-offs method of determining of fault to earth in electrical lines, View in Scopus | Show abstract, 9th Symposium on Neural Network Applications in Electrical Engineering, NEUREL 2008 Proceedings , pp. 73 
[10] S Bjelić, U Jakšić, N Marković., Informatical Model of the System of Automatic Breakdown Control in Energetic Systems ELEKTRONIKA IR ELEKTROTECHNIKA, Vol. 1, 2011, p. 87–92. 
[11] N Marković, S Bjelić, M Vujičić Development of new measuring systems based on symmetric components in electric networks- Electronics and Electrical Engineering.–Kaunas:,2010 Journal Arhive Kaunas University Lituania, ISSN 1392- 1215,Electronics&electrical engineering, T120,No 8(104), 2010, p.57–62. 
[12] S Bjelic, Z Bogicevic, N Kreckovic… - cired.net, estimation of curents flow, loss of power and voltage fall down in distributive networks by using pdm kmp, q program , Cite, 19 International Conference of Electrical Distribution, Paper 0907, Block 4.2, Method and tools, Cired, Wien, 2007. 
[13] T Jagan Mohan Rao, P Anil Kumar, Ch. Krishna Rao, Voltage Source Inverter/Converter for the Improvement of Power Quality Using Fuzzy Logic Controller, Int. Journal of Engineering Research and Applications, ISSN : 2248- 9622, Vol. 4, Issue 5( Version 1), May 2014, pp.46-50 
[14] Marković, N., Bjelić, S., Živanić, J., Jakšić, U. Numerical simulation and analytical model of electrical arc impedance in the transient processes | Symulacje i analiza modelu impedancji łuku elektrycznego w stanach nieustalonych, 2013, View in Scopus | Show abstract, Przeglad Elektrotechniczny 89 (2 A) , pp. 113, .

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K046016266

  • 1. Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 www.ijera.com 62 | P a g e An Investigation of the Ability of Combined Zero – Sequence Cutoff Protection in Line High Voltage Slobodan Bjelić1, Zorica Bogićević2, 1Faculty of Technical Sciences, Kosovska Mitrovica, Serbia 2Advanced High Technical School, Zvecan, Serbia ABSTRACT Zero-sequence cutoff protection has found extensive use in 110-400 kV power networks. Level of value protection settings a starting over-current relay is selected from the requirement of its adjustment out against three zero-sequence current on the end of protected line. Sensitivity of zero-sequence cutoff protection on line is function of equivalent zero-sequence impedance reduction to point bus-bars with disposition protection. Owing to availability of transformers with earthed neutrals at each substation of a 110-400 kV network which are the source of a zero-sequence current, the possibility exists of wide use of zero-sequence cutoffs and stepped zero-sequence protections practically on all lines of medium and large length. From these reasons propose is the use ``cutoff``` protection. Keywords – cutoff, substation, simulation, protection, voltage I. INTRODUCTION The protection consists of over-current relay CR responding to an earth fault, power-directional relay CP determining the direction of the fault power flow, and time relay TR introducing a time delay into the protection operation needed according to the selectivity requirement, Fig 1. The starting current relay and the current winding of the power-directional relay are connected into the neutral wire of the current transformers for current 3I0 [9,13] where as the polarizing (voltage) winding of the power relay is fed with voltage 3V0 from the broken delta connection of the voltage transformer [3,4]. The starting element of the zero-sequence protection features high sensitivity as it is not necessary to adjust the element out against load currents. To speed up the clearance of faults to earth in circuits with solidly earthed neutral, use is made of cutoffs which respond to a zero-sequence current. Their operating principle is the same as that of the cutoffs responding to a phase current. Zero-sequence cutoffs are available in plain current and directional versions, with and without time delay. II. DESCRIPTION OF COMBINED OVER CURRENT ZERO-SEQUENCE CUTOFF PROTECTION The operating current of the starting relays of a zero-sequence over-current protection is selected from two condition: -the requirement of reliable action of the protection in the event of a fault at the end of the adjacent (second) circuit section and -from the requirement of its adjustment out against unbalance currents. It is in this aspect that the directional cutoff fundamentally differs from the non-directional cutoff. The operating current of the directional cutoff is smaller than that of the non-directional one. That is why the zone of action of the first cutoff is much greater than that of the second zone. As a power relay features a dead zone, the directional cutoff should be used only in those cases when the plain cutoff fails to satisfy the sensitivity condition [6,7,8]. The directional instantaneous cutoff scheme differs from directional over-current protections, Fig. 1. in that it lacks a time relay. Combined over-current zero- sequence cutoff protection a) with voltage transformer, b) voltage transformer is absent, Fig. 1. a. and 1.b.). The sensitivity of the zero-sequence protections can be small therefore. When a fault appears the zero-sequence impedance can be grows concerned with impedance under normal service, where zero-sequence of current grows, for examples a include line or transformer (or autotransformer) with neutral point.. This sensitivity can be grows bat widely used combined zero-sequence protection consist of two relays schemes [9,10]: zero-sequence over-current relay and zero-sequence voltage relay. Three schemes is represent in (Fig.1.a, b, c). The circuit is assumed to be a no-load circuit. RESEARCH ARTICLE OPEN ACCESS
  • 2. Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 www.ijera.com 63 | P a g e Fig.1: Combined overcurrent zero-sequence cutoff protection a) with voltage transformer, b) voltage transformer is absent, c). shows some cases of equivalent zero-sequence circuit current flow in certain parts of the circuit. II.I. CALCULATION AND ANALYSIS Fig 1.c, shows some cases of equivalent zero-sequence circuit current flow in certain parts of the circuit. The operating current of the directional zero-sequence cutoffs are adjusted out against current 3I0max in the event of an earth fault (phase to ground or two-phase to ground fault) Line L on the busbars of the opposite substation (point) K according to the expression similar. It is assumed to include two transformer (PT1, PT2) with neutral point and current is: . . 0.max I k 3I op pr A r  (1)  0.max I maximum value of flowing zero-sequence current inside a line in considere transient conditions service substation in the event of an earth fault (phase to ground or two-phase to ground fault) line L on the starting busbar in point K and where PT2 transformer is include (conditions of maximum current). When is used combined zero-sequence cutoff protection bay diagram 1.a a) with voltage transformer and two relays: current relay CR and voltage relay VR it is necessary selected value of operating voltage relay of zero-sequence voltage VR to relation ( because  1 2 Z , Z are parallel connection): 1 2 1 2 . . 0.max 3 Z Z Z Z U k I op pr A VR   (2)  1 2 Z ,Z zero-sequence impedance power transformers (PT1, PT2) in equivalent scheme zero-sequence, Fig.1.c). The current operating of the current relay zero-sequence CR, represent in Fig. 1.a.,b. bay part a) it is needed from condition are adjusted out against current 3I0 in the event of an fault (phase to ground or two-phase to ground fault) Line Lon the busbars of the opposite substation (point) K according to the expression similar and assumed it is off duty one transformer, exemple PT2 with neutral point. 3 . op. pr.A r 0.min.out putPT 2 I  k I (3)  0.min.out putPT 2 I maximum value of flowing zero-sequence current inside a line in considere transient conditions service substation in the event of an earth fault (phase to ground or two-phase to ground fault) line L on the starting busbar in point K and where PT2 transformer is off duty (coditions of minimum current). Estimation of combined zero-sequence cutoff protection can by made with comparation under transient condition of a minimum value current and of a maximum value current in a fault scheme. If a value operating current combined zero-sequence is considere from relation (3) small concerned magnitude operating current zero-sequence is considere from relation (1) should be coordinated so that the opera ting currents with sensitivity voltage relay kvr combined zero-sequence protection. It is clear ,under transient condition of maximum value of current in bouth equivalent schemes on a combined zero-sequence cutof protection the operating current of current relay and operatin voltage of voltage relay thei have equal sensitivity. The operating curren t of a current relay and operating voltage of a voltage relay calculate from one equivalent scheme (under transient conditions where are include both transformers [2,3,4]. Under transient conditions of minimum value of current the sensitivity of voltage relay is bigger, bay relation (4),    . . 0 0 . . 3 3 U I U I k k op pr A op pr A SC SV = 2 1 2 1 2 1 2 0 . . 0 1 . . 3 3 Z Z Z Z Z Z Z I I I Z I op pr A op pr A     (4) Under transient conditions of minimum value of current the voltage relay have (Z1+Z2)/Z2 time selectivity then current relays, bay circuit equivalent Fig. 1. c. III. EVALUATION OF THE DIFFERENT COMBINED ZERO-SEQUENCE CUTOFF PROTECTION The operating principle of protection is sim-ple and reliable, which enables circuits with two-end supply to be protected selectively. A combination of combined cutoffs protection with a directional over-current protection provides a protection which in
  • 3. Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 www.ijera.com 64 | P a g e many cases provides fairly fast clearance of faults and sensitivity. Analyze and the service practice shows that the combined protection functions reliably [11,12,14]. The disadvantages of the protection are: -long time delays, near the sources of supply in particular; -insufficient sensitivity in circuits with large loads and relatively small fault current multiples; - a dead zone in the event of three-phase faults; -the possibility of the incorrect choice of the direction with the voltage circuit, feeding the power-directional relay, being damaged. The directional over current protection is widely used as the main protection in networks up to 35 kV with two-end supply. In 110- and 220-kV networks, the classic directional overcurrent protection finds its application as a back-up protection, but sometimes, when combined with a cutoff, as the main protection. The selection of operating current op pr I . according to the first requirement is made in the same way as for the over current protection, pro-ceeding from the considerations set forth , by formula [1,3,4]: rst sa st mah op pr K k k I I 1 .  (5) The maximum value of current Imax should be determined from the most severe but possible in service conditions. In ring circuits and in radial circuits with two-end supply (see Fig. 2.a and b) maximum loads develop on the lines upon disconnection them. For instance, if line LII is disconnected in the circuit shown in Fig. 2..b, the load current on line LI reaches its maximum. In this case, the phases of the voltages applied to the protection are distorted and therefore the power-directional relay can close its contacts enabling the protection to operate even if the power flow is towards the busbars of the substation. According to the second requirement the operating current of the protection is derived from the formula: [2,3], : op pr saf h ph I k I . .  (6) where h ph ld sh c I I kI    . [3,4] , and safety factor ksaf is taken as 1.15 to 1.30 depending on how accurately the value of Ih.ph is evaluated.. Taken as the final value of Iop.pr is the greater magnitude derived from expressions (5) and (6). As for protections in a circuit with small earth fault current (where h ph ld I  I . ) and protections in a circuit with solidly earthed neutral which are interlocked in the case of earth faults, the operating current of starting relays is selected according to the first requirement only, i.e., by formula (5). To provide selectivity, the sensitivity of the protections operating in one direction should be coordinated so that the operating currents grow as the power source is approached. Such coordination prevents the non-selective operation of the protection in the event of a fault current close in value to the operating currents of the protections. The aforesaid is illustrated by Fig.2.b. When a fault appears near the feeding busbars at point K1 the ratio of fault currents IKA and IKB is inversely proportional to impedance 1 ` K  z and 1 "K z , i.e., 1 1 ` " K K KB KA z z I I  (7) Fig. 2. Calculation of over current cutoff on parallel lines. Design schemes for selection of operating current of zero-sequence cutoffs on parallel lines (a, b, c) and nature of current I01 variation in the case of fault on parallel line L2 disconnected on one side (d) Consequently,, the operating current of a directional overcurrent cutoff is adjusted out against fault currents flowing from the busbars of the substation. Under these conditions the impedance of operative line L1 is reduced by mutual inductance due to current I02, which involves an increase in design current I01 and voltage. Three schemes is represent in (Fig.2.c). (see simulation Fig.4.a,b,c). Certain combinations of reactances xo of parts of the network under consideration may be responsible for a maximum current rise in line L1 not due to a fault on the busbars at point K1 but on the parallel line at point K when this line is disconnected on one side (Fig.2.c). (see simulation Fig.4.a,b,c.) Although the fault at point K2 is more distant than that at K1 current I01 in line L1 may now happen to be greater in value due to a change of' current flow in the parallel branches of the network because of a reduction in the impedance of line L1 caused by the strong mutual inductance from line L2. Figure 2.d shows current I01 and full current Iok at the point of a fault plotted against the location of the
  • 4. Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 www.ijera.com 65 | P a g e fault I0cal is represented by the greater of the obtained values of I01 . Zero-sequence currents should be calculated for that kind of an earth fault wherein their value is greatest. It is known from the fault current calculation theory that with equal total positive- and negative-sequence reactances of the equivalent circuit      1 2 x x current (1,1) 0 (1) 0 I  I if    0 1 x x . After calculation and correlation of x0with x1we find the calculated form of the fault (single-phase- or two-phase-to-earth faults). IV. ANALYSIS OF THE SIMULATION RESULTS The Distributed Parameter Line block implements an N-phase distributed parameter line model with lumped losses. The model is based on the Bergeron's traveling wave method usedb y the Electromagnetic transient program (EMTP) [2,5]. The breaker block implements a circuit breaker where the opening and closing times can be controlled either from an external Simulink signal (external control mode), or from an internal control timer (internal control mode). The arc extinction process is simulated by opening the breaker device when the current passes through 0 (first current zero crossing following the transition of the Simulink control input from 1 to 0). Specifies the number of phases, N=3, of the model. Specifies the frequency used to compute the modal resistance R, inductance L, and capacitance C matrices of the line model. The resistance R per unit length, as an N-by-N matrix in ohm/km. For a 2- phase or three-phase continuously transposed line, you can enter the positive and zero-sequence resistances [R1 R0]. For a symmetrical six-phase line you can enter the sequence parameters plus the zero-sequence mutual resistance [R1 R0 R0m]. For unsymmet rical lines, you must specify the complete N-by-N resistance matrix. The inductance L per unit length, as an N-by-N matrix in henries/km (H/km). For a symmetrical line, you can either specify the N-by- N matrix or the sequence parameters. The capacitance C per unit length, in farads/km (F/km). For a symmetrical line, you can either specify the N-by- N matrix or the sequence parameters. For a 2 or 3 phase continuously transposed line possible positive and zeo sequence (C1, C0). The line length, in km. (100km). Measurements: Select Phase-to-ground voltages to measure the sending end and receiving end voltages for each phase of the line model. Multi-meter block in model to display the selected measurement during the simulation. This model does not rep- resent accurately the frequency dependence of RLC parameter of real power lines, because of skin effects in the conductor and ground, the R and L matrice exhibit strong frequency dependence, causing an attenuation of the high frequencies. Example of simulation influence parallel line I and II. The psbmonophaseline.mdl illustrate as a 100 km line connected on a pu(1), 50 Hz infinite source The line deenergized and reenenrgized after 2 cycles.The simulation is performed simultaneously with the distributed parameters line block in Fig. 3. Fig. 3: The receiving end voltage obtained with distributed Parameter Line block. Phase (deg) 0, The influence phase (A) line I on phase (A) line II, closed Breaker 1 and 2 Fig. 4. a) Phase (deg) 0, simulation of influence phase (A) line I upon phase (A) line II, open Breaker 2 , AI-yellow, AII-pink., b) Phase (deg) +120, simulation of influence phase (A) line I upon phase (B) line II, open Breaker 2. A- pink, B yellow, c) Phase (deg) +120, simulation of influence phase (A) line I upon phase (C) line II, open Breaker 2. , A- pink, C yellow.
  • 5. Zorica Bogićević Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 6( Version 1), June 2014, pp.62-66 www.ijera.com 66 | P a g e V. CONCLUSION From increase sensitivity of protection in in protection from phase-to ground fault and two-phase to ground fault the combined zero-sequence cutoff protection is widely used as the main protection in network 110-400 kV. Consequently,, the operating parameters of a current and voltage relays in combined zero- sequence directional overcurrent cutoff is adjusted out against fault currents flowing from the busbars of the opposite substation. It is clear , from analysis, where is realized combined zero-sequence directional over-current and voltage cutoff is adjusted out against fault currents flowing from the busbars of the other lines with conditions selectivity of current and voltage relay. The zero-sequence cutoff protection is widely used as the main protection in network 110- 400 kV From increase of sensitivity in protection from phase-to ground fault and two-phase to ground fault. The operating principle of directional combined zero-sequence cutoff protection is simple and reliable, which enables circuits with two-end supply to be protected selectively. REFERENCES [1] S Bjelic, Z Bogićevic, Computer Simulation of Theoretical Model of Electromagnetic Transient Processes in Power Transformers, International Journal of Information Technology and Computer Science, (IJITCS)6, no. 1(2013): 1. [2] Dommel, H, Digital Computer Solution of Electromagnetic Transients in Single and Multiple Networks, IEEE Transactions on Power Apparatus and Systems, Vol. PAS- 88, No. 4, April, 1969. [3] J. Lewis Blackburn Thomas J. Domin: ``Protective Relaying Principles and Applications``,Third Edition, 2006 by Taylor&Francis Group, LLC., : 416-428. [4] Bjelic S. Overcurrent protections of distribution electrical networks / Prekostrujne zaštite distributivnih električnih mreža, 2009, UDK 621.313(075.8) SITOPRINT Niš, (2010), COBISS.SR-ID 512270494, [5] MATLAB SIMULINK Sim Power System, Copyright 1984-2002 the Math Works, Version 6.5.0, 180913a, June 2, 2000. [6] Bjelic S., Jelic N., Automatic Secondary VAR Control: A Multivariable Approach , ★★★★★ , 1995 01/01, German National Library of Science and Technology (GetInfo) BL CP. [7] Antonin Veverka: TECHNIKA VYSOKÝCH NAPĚTÍ SNTL/ALFA, DT621.3027.3: 621.315.31:II, Elektrickě razově jevy ve vinutih transforma torů a točivýh strojů, Praha, 1982. [8] Bjelic, S.,Mladenovic, V, Algorithm and possible method of emergency control electrical network View in Scopus | Show abstract, 9th Symposium on Neural NetworkApplications in ElectricalEngineering,NEUREL2008Proceeding,pp. 69 [9] Markovic, N., Bjelic, S., Bogicevic, Z, Graphical zero-sequence cut-offs method of determining of fault to earth in electrical lines, View in Scopus | Show abstract, 9th Symposium on Neural Network Applications in Electrical Engineering, NEUREL 2008 Proceedings , pp. 73 [10] S Bjelić, U Jakšić, N Marković., Informatical Model of the System of Automatic Breakdown Control in Energetic Systems ELEKTRONIKA IR ELEKTROTECHNIKA, Vol. 1, 2011, p. 87–92. [11] N Marković, S Bjelić, M Vujičić Development of new measuring systems based on symmetric components in electric networks- Electronics and Electrical Engineering.–Kaunas:,2010 Journal Arhive Kaunas University Lituania, ISSN 1392- 1215,Electronics&electrical engineering, T120,No 8(104), 2010, p.57–62. [12] S Bjelic, Z Bogicevic, N Kreckovic… - cired.net, estimation of curents flow, loss of power and voltage fall down in distributive networks by using pdm kmp, q program , Cite, 19 International Conference of Electrical Distribution, Paper 0907, Block 4.2, Method and tools, Cired, Wien, 2007. [13] T Jagan Mohan Rao, P Anil Kumar, Ch. Krishna Rao, Voltage Source Inverter/Converter for the Improvement of Power Quality Using Fuzzy Logic Controller, Int. Journal of Engineering Research and Applications, ISSN : 2248- 9622, Vol. 4, Issue 5( Version 1), May 2014, pp.46-50 [14] Marković, N., Bjelić, S., Živanić, J., Jakšić, U. Numerical simulation and analytical model of electrical arc impedance in the transient processes | Symulacje i analiza modelu impedancji łuku elektrycznego w stanach nieustalonych, 2013, View in Scopus | Show abstract, Przeglad Elektrotechniczny 89 (2 A) , pp. 113, .