basic concept operation and control of hvdc transmission system
TRANSCRIPT
Basic Concept, Operation and Control of HVDC Transmission System
13.00-16.00 hrs. July 29, 2008Room 2003, T.102, EGAT Head Office
Nitus Voraphonpiput, Ph.D.Engineer Level 8
Technical Analysis – Foreign Power purchase Agreement BranchPower Purchase Agreement Division
Electricity Generating Authority of Thailand
2
Objective
Introducing operation, and control of the High Voltage Direct Current Transmission System.
Note: This presentation continues from the morning session. Basic mathematics and electrical engineering knowledge will be useful for attendee.
3
Contents
1. HVAC vs. HVDC2. HVDC PrincipleQ&A for 15 minutesCoffee break 10 minutes
3. Control of DC TransmissionQ&A for 15 minutes
4
1. HVAC vs. HVDCWhy use DC transmission?
This question is often asked. One response is that losses are lower, but is it true?
Reference [2] has been explained using Insulation ratio and Power capacity in order to proof this statement.
5
1. HVAC vs. HVDC
Insulation ratio of HVAC and HVDC (Ref. 1-2)A given insulation length for an overhead line, the
ratio of continuous working withstand voltage factor (k) is expressed as, (note )
0.1 voltage withstandAC
voltagewithstandDC
(rms)
==k
A line has to be insulated for over-voltages expected during faults, switching operations, etc. Normally AC transmission line is insulated against over-voltages of more than 4 times the normal effective (rms) voltage.
21 ≤≤ k
6
1. HVAC vs. HVDC
5.2 ground)-(phase Voltage AC Rated
levelInsulationAC
(rms)1 ==k
This insulation requirement can be met by insulation corresponding to an AC voltage of 2.5-3.0 times the normal rated voltage.
For suitable converter control the corresponding HVDC transmission ratio is expressed as
7.1 ground)-(pole Voltage DC Rated
levelInsulationDC2 ==k
7
1. HVAC vs. HVDC
d
P
VV
kkk
K
2
1(rms)
voltagewithstandDClevel insulation DC
voltagewithstandAClevel insulation AC
Pole DCeach for requiredlength insulationphase ACeach for requiredlength insulation)(ratioinsulation
==
=
Insulation ratio for a DC pole-ground voltage (Vd) and AC phase-ground (Vp) is expressed as
It can be seen that the actual ratio of insulation levels is a function of AC/DC voltage. Next, determine AC/DC voltage.
8
1. HVAC vs. HVDC
Determine AC/DC voltageAssumed resistances (R) of the lines are equal in both cases (HVDC and HVAC).
AC Loss = 3 x R x IL2 and DC Loss = 2 x R x Id2
Let losses in both cases are equal, so that,
The power of a HVAC system and a bipolar HVDC system are as:
Ld II23
=
φcos3 LP IVPowerAC = dd IVPowerDC 2=
9
1. HVAC vs. HVDC
dp VVφcos
132
=
At the same power transfer,
So that,
1cos23
2cos3
===d
P
dd
LP
VV
IVIV
PowerDCPowerAC φφ
It can be seen that HVDC requires insulation ratio at least 20% less that the HVAC which essentially reflects the cost.
Thus, insulation ratio (K) can be written as
φφ cos2.1
cos1
32
2
1 ≈=kkkK
10
1. HVAC vs. HVDC
Power CapacityCompared a double circuit HVAC line (6 lines) and double circuit DC line of Bipolar HVDC.
Power transmitted by HVAC (Pac) and HVDC (Pdc) are
acac
LPdc PPkkkIV
kkkP
φφ cos47.1
cos6
2
1
2
1 ==⎟⎟⎠
⎞⎜⎜⎝
⎛=
φcos6 LPac IVP = dddc IVP 6=
On the basic of equal current and insulation, Id = IL, K=1:
11
1. HVAC vs. HVDC
For the same values of k, k1 and k2 as above and pf is assumed to 1.0, the power transmitted by overhead lines can be increased to 147%. The percentage line losses, which is inversion of the power transmit, are reduced to 68%.
In addition, for underground or submarine cables, power transmitted by HVAC cable can be increase 294 % and line loss reduced to 34%.Note: for cable k equals at least two.
12
1. HVAC vs. HVDCFrom reference [3], losses are lower is not correct.“The level of losses is designed into a transmission system and is regulated by the size of conductor selected. DC and ACconductors, either as overhead transmission lines or submarine cables can have lower losses but at higher expense since the larger cross-sectional area will generally result in lower losses but cost more.”
The reasons that HVDC have been used are:1. An overhead d.c. transmission line with its towers can be designed to be less costly per unit of length.2. It is not practical to consider AC cable systems exceeding 50km (due to VAR charging of the cable).3. Some a.c. electric power systems are not synchronized to neighboring networks even though their physical distances between them is quite small.
13
2. HVDC Principle
The HVDC valve comprises the thyristors acting as controlled switch. In the ‘OFF’ state, the thyristor blocks the current to flow, as long as the reverse or forward breakdown voltages is not exceeded.
It changes to ‘ON’ state if it is forward biased (VAK > 0) and has small positive ‘Gate’ voltage applied between the Gate and the Cathode.
Anode (A)
Cathode (K)
Gate (G)
14
2. HVDC Principle
Thyristor switches between conducting state (ON) and non-conducting (OFF) state in response to control signal (firing) as its characteristic.The Gate voltage need not to be present when the thyristor is already in ON state.
15
2. HVDC Principle
Rd
VT
Rd = ∆VAK/ ∆IA
VT
Anode (A)
Cathode (K)Anode (A)
Cathode (K)
RrRr = ∆VAK/ ∆IA Ploss-ON state = VT.IA(avg.) + Rd.IA2
(rms)
Ploss-OFF state = Rr.Ir2(rms)
iA
ir
16
2. HVDC Principle
ON-OFF state- ON state continues until current drops to zero, even reverse bias
appears across the thyristor.- The critical time to clear charge carriers in the semi-conductor
is referred as the turn-off time toff . If forward bias appears to soon, t < toff, thyristor can not OFF.
ON
OFF
OFF
VAK > 0 and VG >0
IA < 0 VAK > 0 and t < toff
t > toff
17
2. HVDC Principle
ON State OFF State
18
2. HVDC Principle
Rd = 10Ω
Th1
Ld
Th3
Th4 Th2
o30V220US == α
Vd
Id
IsVs
Single Phase Bridge Rectifier
19
2. HVDC PrincipleVs
Id
Is
Vd
α = 30°
Th3
Th4
Th1
Th2
Th3
Th4
Voltage waveform of inductor (Ld), VLd = Vd – Rd Id
Voltage waveform of resistor (Rd), VRd = Rd Id
20
2. HVDC Principle
Is
Vd
Id
50 Hz
100 Hz
150 Hz
200 Hz
250 Hz 350 Hz
300 Hz
100 Hz
Harmonics in the voltage and current waveform.
DC
DC
21
2. HVDC Principle
Even DC side does not have reactive power (Q), the reactive power still presents on the AC side. The reactive power occurrence is caused by the delay angle (α) (or called firing angle) of the current waveform.
30°
VS
IS
Vs Is
α = 30°
P = |VS| |IS| cos α
Q = |VS| |IS| sin α
time360°20 ms
Phasor of fundamental component
22
2. HVDC Principle
Is
Vd
Id
50 Hz
100 Hz
150 Hz
200 Hz
250 Hz 350 Hz
300 Hz
100 Hz
Product of Vd and Idis (active) power (P).
Product of phasor VS and phasor IS is not the apparent power (S) . It represents the active power (P) and reactive power (Q).
There are harmonic distortion power, which is a new term caused by the higher harmonics (more than 50 Hz). It is represented by D (distortion power).
Finally, S2 = P2 + Q2 becamesS2 = P2 + Q2 + D2.
23
2. HVDC Principle
Lk
Rd
Ld
Ith2
Ith1
commutation
µ is overlap angle
Ith2
Ith1
µ
Vd
Id
IsVs
It can be seen that if current is high, overlap angel is increased. In addition, if inductance is high, overlap angle is also increased.
The inductance Lk represents reactance on AC side (called commutating reactance). Due to nature of an inductor, The inductor current can not change suddenly. Thus, during turn-off of the Th1 (and Th2) and turn-on of the Th3 (and Th4), both are in conducting state for a short time (overlap time). This phenomena occurs during commutation of the thyristors.
Increasing Lk
Increasing Id
24
2. HVDC PrincipleIs
Vd
Id
Vsα = 30°µ
Th3
Th4
Th1
Th2
Th3
Th4
Inductor current can not suddenly be changed, thus there is a slope.
2)cos(coscos µααφ ++
≈
25
2. HVDC PrincipleThe impact of the overlap angle (µ) is the reduction of the average dc voltage (Vd).It decreases the harmonic content of the ac current (Is) and power factor of the AC side.
Vd
Id
Ideal case Vdo
dKdod IXVVπ2
−=
KK LfX π2=
Vd
IdVoltage drop due to
commutating reactance is represented as DX
XK
RdId
DX
DR
VT
VT and DR are very less compared to DX. Thus, there are usually neglected.
Overall voltage drop
Vd
26
2. HVDC Principle
Rd
IL
Th1
Ld
VA
Th2
Th3
Vdα
VB
VC
IL
t
o60=α o90=α o120=αo0=α
Vdα
αα coscos17.1 0dPd VVV ==
Natural commutation
VA = √ 2 VP sin ωt
VB = √ 2 VP sin ωt-120°
VC = √ 2 VP sin ωt+120°
∞→d
d
RL
3-pulse converter
27
2. HVDC Principle
1.0
-1.0
0.5
-0.5
Rectifier
Inverter
α
o60=α
o45 o180o135o90
0d
d
VV
αcos0
=d
d
VV
Positive average voltage
Negative average voltage
Inverter mode can be performed when firing angle is more than 90 degrees.
Rectifier mode can be performed when firing angle is less than 90 degrees.
Average voltage is zero when the firing angle is 90 degrees.
28
2. HVDC Principle
α=60° α=30°
Vd
Id
29
2. HVDC Principle
VA, IA
Id
VB, IB
VC, IC
Th1 Th2 Th3 Th1 Th2 Th3
120°
30
2. HVDC Principle
VA, IA
Id
Vd
α=30°α=120°
Inverter mode can be performed as long as the DC current continues flow.
Positive voltage
Negative voltage
Reversing phase sequence
31
2. HVDC Principle
t
IB ICIA
t
µ
α
αdVVA
VB
Lk
Id
Lk
Vk
IC
dkX
Xdd
ILD
DVV
ωπ
α
23
cos0
=
−=
IBIA
µ
α
Vk
VA
VB
DX
32
2. HVDC Principle
γ
γ
t
µα
dV
Vk
µ
DX
α
The commutating reactance (Xk) results in decreasing of DC voltage, but it increases DC voltage in inverter mode.
It can also be seen that the overlap time will increase when DC current is high and this can cause commutation failure in inverter mode.
Note: α + µ < 180°The extinction angle (γ) = 180 - α - µ
IBIAIBIA
180°180°
dkX
Xdd
ILD
DVV
ωπ
α
23
cos0
=
+=
33
2. HVDC Principle6-pulse converter
Vd+
Vd-
Vd+
Vd-
Vd
Vd= Vd+ - Vd-
α=0°
α=0°
-Vd-Vd+
The 6-pulse bridge consists of two 3-pulse bridges (positive and negative) connected in parallel.
34
2. HVDC Principle6-pulse bridge HVDC
Vdr Vdi
Id
Id
The HVDC comprises two converters connected in anti-parallel through smoothing reactors and DC lines. One converter is operated in rectifier mode to transmit power from the AC network to the other side whereas the other side converter is operated in inverter mode to receive power into the (other side) AC network.
Smoothing reactor
Smoothing reactor
DC line
DC line
power
power power
Reactive power
Reactive power
35
2. HVDC Principle
30°
VI.cosφ
II.sinφ
o
ooo
30
866.02
)2515cos(15cos2
)cos(coscos
≈
=++
≈
++≈
φ
µααφ
Rectifier Operation of the 6-pulse bridge converter
Assume α = 15° and µ = 25°
The converter operates in rectifier mode. It transmits active power while consumes reactive power.
36
2. HVDC Principle
145°
VI.cosφ
II.sinφ
o
ooo
145
823.02
)25135cos(135cos2
)cos(coscos
≈
=++
≈
++≈
φ
µααφ
Inverter operation of the 6-pulse bridge converter
Assume α = 135° and µ = 25°
The converter operates in inverter mode. It receives active power while consumes reactive power.
37
2. HVDC Principle
For convenience, the converter operated in inverter mode is often referred to extinction angle (γ). Thus direct voltage in inverter mode (Vdi) are expressed as
dkX
Xdd
ILD
DVV
ωπ
αα
23
90,cos0
=
>+= o
Actually, inverter is commonly controlled at constant extinction angle to prevent commutation failure. Therefore, it is not only for convenience, but also for converter control purpose. It is important to note that voltage drop caused by commutating reactance (Dx) is now negative.
µαπγγ
−−=−= Xdd DVV cos0
38
α is the control variable for rectifier and γ is the control variable for inverter.
2. HVDC PrincipleVoltage vs. current (VI) characteristics at steady state
dN
d
II
0d
d
VV
dN
d
II
0d
d
VV
α = 0°
αmax < 180 °
1.0
-1.0
1.0
1.0
-1.0
1.0
α = 0°
γ = 0°
Slope is DX
Rectifier
Inverter
Rectifier
Inverter
Incr
easi
ng α
Incr
easi
ng α
Incr
easi
ng γ
39
2. HVDC Principle12-pulse bridge HVDC
Vdr∆Vdi∆
Id
VdrY VdiY
∆ ∆
Y Y
Y
Y
Y
YId
The 12-pulse converter is required to improve harmonic current on AC sides. It comprises two 6-pulse converters connected in series. Harmonic current on AC sides are odd orders starting from 11th, 13th …. whereas even orders present on the DC side (12th, 14th…). To achieve 12-pulse, phase displacement of 30° generated by Star (Y) and Delta (∆) connection of the transformers are employed.
40
2. HVDC Principle
Y Y
Y ∆
IA
IA∆
IAY
IA
IA∆IAY
Vd∆
VdY
Vd∆VdYVd
Vd
Rectifier operation of the 12-pulse bridge converter
Assume α = 15°
and µ = 25°
41
2. HVDC Principle
Y Y
Y ∆
current
VdiVdrY Y
∆ YId
Vdi
Vdr
Id
voltageαmin < α
αmin = 5° - 7°
γmin < γ
γ min = 15° - 17°
½ Rd
½ Rd
To ensure all thyristor valves are enough forward bias to turn on.
To keep reactive power requirement on inverter side as low as possible.
Voltage drop caused by line resistance (Rd) is taken into account and the VI characteristic presents operating point of the HVDC system.
decreasing α
power
power power
Reactive power Reactive power
42
2. HVDC Principle
Detail Configuration of the HVDC
43
2. HVDC Principle
Alternatives for the implementation of a HVDC powertransmission system
i) Mono-polar Configuration
ii) Bipolar Configurationa) Earth Return
b) Metallic Return
iii) Homo-polar Configuration
44
2. HVDC Principle
Alternatives for the implementation of a HVDC powertransmission system (continued)
45
Can we use manual control for the rectifier (vary α) and the inverter (vary γ)?If we can not do that, which side should be controlled (rectifier or inverter) or control them both?What is/are the control purpose(s)?
3. Control of the DC Transmission
46
3. Control of the DC Transmission
Typical control strategies used in a HVDC system consists of:
Firing ControlRectifier Current Control (CC)Inverter Constant Extinction Angle (CEA) Control Inverter Current Margin Control (CM)Inverter Voltage Control (VC)Voltage Dependent Current Limit (VDCL)Tap change Controls (TCC)Power Reversal
47
3. Control of the DC Transmission
Firing ControlFunction of the firing control is to convert the firing angle
order (α*) demanded fed into the valve group control system. There might be voltage distortions due to non-characteristic harmonics, faults and other transient disturbances such as frequency variation. Thus, phase-locked loop (PLL) based firing system is generally applied.
Phase Detector
vA
vB
vC
PI Controller Voltage Controlled Oscillator
sin(.)
sin(.)
sin(.)
comparator
α*
comparator
comparator
……
⅔ π
θvo
-
verror
…
uA
uB
uC Gate firing
TsTsK )1( +
48
3. Control of the DC Transmission
verror
uA vA
time
time
Firing Control (Continued)
2π
θ
timeFiring pulse of phase A
α*
α0
0
0
49
3. Control of the DC Transmission
Current Control (CC)The firing angle is controlled with a feedback control
system as shown in figure. The dc voltage of the converter increases (by decrease α*) or decreases (by increase α*) to adjust the dc current to its set-point (Id*).
α*αmax
αmin
PIid*
id
-
+
Y Y
Y ∆
Vdr
Current measurement
Firing Control
vA, vB , vC
6
6
IdTsTsK )1( +
50
3. Control of the DC Transmission
Constant Extinction Angle Control (CEA)The firing angle of the inverter is controlled at minimum
angle (γmin) to reduce reactive power requirement. This can be achieved by using Gamma control (γ-control).
α*αmax
αmin
PIγ*
γ
-
+
Current measurement
Firing Control
vA, vB , vC
6
6
VdiY Y
∆ Y
γ measurement
Valve voltage
51
3. Control of the DC TransmissionVI Characteristic of the CC and the CEA
current
Vdi
Vdr
Id
voltage
γ* = γmin
α*
VI Characteristic
current
VdiVdr
Id
voltage
γ* = γminα*=α min
If AC voltage on rectifier side decreases, CC decreases α* down to αmin to increase DC current (Id), but there is no operating point (X). This problem can be solved using CMC.
X
AC voltage decreasing
The intersection (X) is the operating point of the DC transmission line.
52
3. Control of the DC Transmission
Current Margin Control (CMC)A better way is to use the inverter to control current less
than of the rectifier by an amount of current margin (∆Id) when the rectifier can not perform CC.
α*αmax
αmin
PI
γ*
-+Current
measurement
Firing Control
vA, vB , vC
6
VdiY Y
∆ Y
id*
id
∆id = 0.1 to 0.15
+
γ - Control
Min
imum
se
lect
ion
53
3. Control of the DC TransmissionVI Characteristic of CC, CEA and CMC
current
Vdi
Vdr
Id
voltage
γ* = γmin
α*
Combined characteristics of CC, CEA and CMC
α*=α min
If AC voltage on rectifier side decreases, CC decreases α* down to αmin to increase DC current (Id), but there is no operating point (X). This problem can be solved by CMC.
X
AC voltage decreasing
current
VdiVdr
Id
voltage
γ* = γminX
∆Id ∆IdCMC
CEA
CC
This method can maintain stable operation when AC voltage of both sides are fluctuated.
54
3. Control of the DC TransmissionWhat will happen if AC network of the inverter side is too weak!
current
Vdi
Vdr
Id
voltage
γ* = γmin
α*
In this range the intersection is poorly to define and both current controllers will hunt between the operating points.
This problem can be solved by adjust VI characteristic of the inverter to voltage control (VC) in order to avoid hunting between two controllers.
X
∆IdCMCCEA
Weak AC
current
Vdi
Vdr
Id
voltage
γ* = γminα*
∆IdCMC
CEA
VCγ* > γmin
X
More Weak
55
3. Control of the DC Transmission
Voltage Control (VC)it is very effective when the inverter is connected to a weak
AC network. The normal operating point X corresponds to a value of γ higher than the minimum. Thus, the inverter (rectifier as well) consumes more reactive power compared to inverter with CEA.
α*
αmax
αmin
PI
γ*
-+
Firing Control
vA, vB , vC
6
6
VdiY Y
∆ Y
vdi*
vdi
γ - Control
Min
imum
se
lect
ion
Voltage measurement
CMC
Max
imum
se
lect
ion
56
3. Control of the DC TransmissionVoltage Dependent Current Limit (VDCL)
Commutation failures can occur during an AC fault on the inverter side. It results in continue conduction of a valve beyond its 120° conduction interval. The CC will regulate the DC current to its rated value, but in the worst case, two inverter valves may form DC short circuit and continue conducting for a long time, which can cause valve damage. To prevent this problem, DC current must be reduced. One possible to detect the AC side fault is thelowering of the DC voltage. This voltage is typically chosen at 40% of the rated voltage.
Id
57
3. Control of the DC TransmissionVoltage Dependent Current Limit (VDCL)
The VDCL is a limitation imposed by the ability of the AC system to sustain the DC power flow when the AC voltage at the rectifier bus is reduced due to some disturbance as well. The VDCL characteristics is presented below.
current
Vdi
Vdr
Idmax
voltage
α*
∆IdCMC
VC
X
Id-min
≈ 0.4
VDCL∆Idcurrent
Vdi
Vdr
Id
voltage
α*
∆IdCMC
VC
X
Id-min
≈ 0.4
VDCL∆IdIdmax
VDCL VDCLVDCL
58
3. Control of the DC Transmission
Voltage Dependent Current Limit (VDCL)
id*
vd
v
Vd
Ts+11
Voltage measurement
i
Minim
um
selectionvd
CC
VDCL
iv
59
3. Control of the DC Transmission
Tap Change Control (TCC)When voltage of the AC system of the rectifier and/or of the
inverter is fluctuated, transformer taps (both side) can adjust to keep the DC voltage within desired limits or suitable operating point. Generally, the tap will be changed when the firing angle of the rectifier/inverter still reach its more than 10-15 minutes to avoid interaction of other controls.
Example: if the firing angle (α) of the rectifier reaches minimum limit (αmin) for long time. It means that the AC voltage of the converter is not appropriate. Thus, AC voltage of the converter must be reduced by tap changing of the converter transformer to free the firing angle of the rectifier.
60
3. Control of the DC TransmissionPower Reversal
The VI characteristic of power reversion is presented below (VDCL and VC are not included). The station 1 (rectifier) increases firing angle (α) into the inverter region and the station 2 (inverter) decreases its firing angle (α) into rectifier region. This can be performed without altering the direction of current flow.
current
V2di
V1dr
Id
voltage
γ* = γminα* X
current
V2dr
V1di
Id
voltage
γ* = γminα* X
61
3. Control of the DC Transmission
VdiY Y
∆ Y
Y Y
Y ∆ Id
Firing C
ontrol Min
.Min.
Max. M
ax.
p*/vdCAE
CC
VC
VDCL
Power order
γmin
Vd*
Firin
g C
ontr
ol
CAE
CC
VC
VDCL
γmin
Vd*
∆id
Modulation Signal
id*
p*
Vdr
TCC TCC
Master Control
∆p
α*α*
po
Vd, Id,α, γ
62
3. Control of the DC TransmissionCIGRE’s HVDC benchmark was simulated on ATP-EMTP with the typical HVDC control schemes, which the CC mode was employed at rectifier and VC mode was applied at inverter. All simulation results are presented in normalized values.
Start Up HVDC
Rectifier Current Control Inverter Voltage Control
63
3. Control of the DC Transmission
Start Up HVDC
Firing Angle (α) of Rectifier Firing Angle (α) of Inverter Extinction angle (γ) is also shown
The HVDC started at 0.1 sec. The firing angle of rectifier started at 90° while the extinction angle of inverter started at 90°.
64
3. Control of the DC Transmission
Power Reversal
Firing Angle (α) of Rectifier and Inverter
DC Current
The HVDC started to reverse power flow direction at 0.5 sec. Firing angle of the rectifier increased (with a ramp rate) into inverter zone while firing angle of the inverter decreased (with a ramp rate) into rectifier zone.
65
3. Control of the DC Transmission
Power Reversal
The power flow direction of the HVDC reversed at 0.9 sec.
66
3. Control of the DC TransmissionVDCL performance during 1-phase fault at AC network of the rectifier station.
1 –phase Fault at AC network of the rectifier station
cba V VV
67
3. Control of the DC Transmission
Fault at AC network of rectifier station
REFIdI
diV
didREF VI I.u.p Degree )( Alpha_i )( r_Alpha ir αα
rα
iα
68
3. Control of the DC TransmissionVDCL performance during 1-phase fault at AC network of the inverter station.
1-phase Fault at AC network of the inverter station
cba V VV
69
3. Control of the DC Transmission
Fault at AC network of inverter station
REFIdIdiV
didREF VI I.u.p )( Alpha_i )( r_Alpha ir αα
iα
rα
Degree
70
3. Control of the DC TransmissionModulation signal is employed when a power system has a special requirement such as frequency control, power oscillation damping, etc. For example, the addition frequency control loop is included into HVDC control system to stabilize frequency of the AC system.
71
3. Control of the DC Transmission
Modulation Function of EGAT-TNB HVDC
72
3. Control of the DC Transmission
Power Swing Damping (PSD) Function of EGAT-TNB HVDC
Thank you very much for your attention
74
References1. Ani Gole, “HVDC Transmission Lecture Note”, University of Manitoba, 2000.2. Jos Arrilaga, “High Voltage Direct Current Transmission”, 2nd , IEE-Press, 1998. 3. Dennis A. Woodford, “HVDC Transmission”, Manitoba HVDC Research Center,
Canada, 1998.4. Erich Uhlmann, “Power Transmission by Direct Current”, Springer Verlag, 1975.5. Vijay K. Sood, “HVDC and FACTS Controllers”, Kluwer. 2004.6. Edward Wilson Kimbark, “Direct Current Transmission” vol.1, Wiley-
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