ABB
Technology and Solutions
Protection and Substation Automation
© A B B S w it z e rl a n d L td . -1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R W
Topic:
Busbar
Protection
Measurement
System
ABB
© A B B S w it z e rl a n d L td . -2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WBusbar Protection – Measurement System
r Introduction
r BBP Requirement
r BBP Basics
r Special Condition for the BBP (≠ LP, TP, GP ….)
r The “problem” on CT Saturation
r High Impedance Measurement Principle
r Low Impedance Measurement Principle
q Example and Features of different Methods / Algorithms
q INX-2
q INX-5
q REB500
q REB670
r Calculation examples: Differential & Restraining Current / Differential Voltage
r Open CT / Differential current Supervision
r Additional Release / Tripping Criterias
r Intertripping
ABB
© A B B S w it z e rl a n d L td . -3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WIntroduction
q It is extremely important for Busbar Protection
applications to have good security since an unwanted
operation might have severe consequences
q The unwanted operation of the Busbar Protection will
have the similar effect as simultaneous faults on all
power system elements connected to the bus
q On the other hand, the BBP has to be dependable as
well. Failure to operate or even slow operation in case of
a busbar fault can have fatal consequences. Human
injuries, power system blackout, transient instability or
considerable damage to the surrounding substation
equipment and the close- by generators are some of the
possible outcomes
ABB
© A B B S w it z e rl a n d L td . -4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WIntroduction
q A fault on a busbar in the network is relatively
seldom: Statistically once in every 20 – 30 years per
switchgear
q A fault on an overhead line in the network is
statistically more than factor 100 higher
q The life time of busbar protection systems could be
more than 30 – 40 years
q According to studies all costs to integrate a BBP
system will be covered in case of ONE successful trip in
it’s life time
q Remember: maloperating / unwanted operating as
well as non operating BBP system can and have caused
blackouts
ABB
© A B B S w it z e rl a n d L td . -5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WBBP Requirements
Number the requirements depending on the importance
___ STABILITY in case of external faults (even with extreme CT saturation)
___ RELIABILITY (extensive self- supervision)
___ TRIPPING SPEED ___ easily EXTENDABLE ___ extensive SELFSUPERVISION
___ SIMPLE OPERATION (Maintenance & Commissioning)
___ low CT REQUIREMENTS ___ SELEKTIVITY (only the fault affected busbar is allowed to trip)
___ MALOPERATION extremely unacceptable
___ matching to all switchgear CONFIGURATIONS ___ integration of BREAKER FAILURE PROTECTION
(additional protection & monitoring functions)
ABB
© A B B S w it z e rl a n d L td . -6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WWho knows
Mr. Kirchhoff ?
BBP Basics
ABB
© A B B S w it z e rl a n d L td . -7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WKirchhoff’s 1st Law: Node Rule
I1 + I2 + I3 =
Σ
I =
0
The sum of all
currents must be zero
ABB
© A B B S w it z e rl a n d L td . -8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WKirchhoff’s 1st Law: Node Rule
I1 + I2 + I3 =
Σ
I
≠
0
⇒ Fault on the busbar
⇒ Trip circuit breaker
If
ABB
© A B B S w it z e rl a n d L td . -9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WDifferential current measurement
Σ I = I1 + I2 + I3
If
Σ I > differential current setting
⇒
Trip Busbar Protection
BBP Basics
the measurement (system) has to be phase segregated 3 (4) measurement systems: R; S; T (& special: N)
ABB
© A B B S w it z e rl a n d L td . -1 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WExternal Fault
BBP Basics
I1 I2 Σ I ⇒ No Differential Current ⇒ No TripABB
© A B B S w it z e rl a n d L td . -1 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WInternal Fault
BBP Basics
⇒ High Differential Current
⇒ Trip
I1 I2
ABB
© A B B S w it z e rl a n d L td . -1 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WExternal Fault – with DC component
BBP Basics
I1 I2
Σ I
⇒ No Differential Current
⇒ No Trip
A DC component will be super-imposed if the short circuit does not occur at the voltage peak
The DC component will decade with the network time constant τ = L / R
ABB
© A B B S w it z e rl a n d L td . -1 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WInternal Fault – with DC component
BBP Basics
⇒ High Differential Current
⇒ Trip
I1 I2
ABB
© A B B S w it z e rl a n d L td . -1 4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WProtection Zones
Special Condition for the BBP (≠ LP, TP, GP ….)
B u s b a r Busbar L in e T ra n s fo rm e r G e n e ra to r -T ra n s fo rm e r BB G
ABB
© A B B S w it z e rl a n d L td . -1 5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WAll protection system (excl. BBP):
The current in the current transformer (CT) due to a fault inside the protection zone is usually higher than the current in the CT due to a fault outside the protection zone. The reason for this is:
• In case on a feeder fault (near the busbar) the current in the feeders
CT is equal to the sum of all feeder currents connected to the busbar.
• In case on a busbar fault the currents in the CTs are limited by the
line or transformer reactance.
I
external fault< I
internal fault• Stability condition: on relatively low currents - CT saturation unlikely
• Tripping condition: on extremely high currents - CT saturation very likely
ABB
© A B B S w it z e rl a n d L td . -1 6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WBusbar protection system:
The current in the current transformer (CT) due to a fault outside the protection zone is usually higher than the current in the CT due to a fault inside the protection zone. The reason for this is:
• In case on a feeder fault (near the busbar) the current in the feeders
CT is equal to the sum of all feeder currents connected to the busbar.
• In case on a busbar fault the currents in the CTs are limited by the
line or transformer reactance.
I
external fault> I
internal fault• Stability condition: on extremely high currents - CT saturation very likely
• Tripping condition: on relatively low currents - CT saturation unlikely
ABB
© A B B S w it z e rl a n d L td . -1 7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WExternal Fault
CT Saturation
I1 I2 Σ I⇒ the CT saturation will produce a differential current which could result in a MALOPERATION
ABB
© A B B S w it z e rl a n d L td . -1 8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WExternal Fault – with DC component
CT Saturation
I1 I2
Σ I
The DC component will increase the saturation
⇒ the CT saturation will produce a differential current which could result in a MALOPERATION
ABB
© A B B S w it z e rl a n d L td . -1 9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
q The only BBP system which can handle CT
saturation without any other quantity than I
diff(
Σ I ) is the High Impedance Protection System.
q The High Impedance Measurement Principle
uses the physical behaviour of the CT
saturation to prevent (mal-) operation in case
of external fault with (high) CT saturation.
ABB
© A B B S w it z e rl a n d L td . -2 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
CT2 feeder 1 feeder 2 RR BB 1 CT1 U1 UR RL1 RL2 UR > 0 U2 Im Im
Principle / Components
CT secondary reactanceLine resistance from CT to relay
High impedance (input)
I2
I1
ABB
© A B B S w it z e rl a n d L td . -2 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
CT refresher course:
Im [A] 10’000 100 1’000 0.001 0.01 0.1 1 U [ V ] 2Excitation or magnetizing current
ABB
© A B B S w it z e rl a n d L td . -2 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
CT refresher course:
Im [A] 10’000 100 1’000 0.001 0.01 0.1 1 U [ V ] 2Excitation or magnetizing current
Magnetizing Curve
Knee point voltage
(when saturation starts)
Dynamical resistant: du/di = r <<<<<<
Dynamical resistant: du/di = r >>>>>>
ABB
© A B B S w it z e rl a n d L td . -2 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
CT2 feeder 1 feeder 2 RR BB 1 CT1 U1 UR RL1 RL2 UR > 0 U2 Im Im
Internal Fault
Principle:An internal fault will immediately result in a differential current and therefore a (high) voltage on the high impedance. The overvoltage relay which is measuring at the high impedance will pick up instantly. The pick up voltage level must be set depending on the lowest
possible fault current and the maximum load.
I2
I1
ABB
© A B B S w it z e rl a n d L td . -2 4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
CT2 feeder 1 feeder 2 RR BB 1 CT1 U1 UR RL1 RL2 UR > 0 U2 Im Im
Internal Fault
General setting rule: (since UR max = Uk)
RR = High Impedance (e.g. 2000Ω) UR = Voltage at the high impedance Uk = CT knee point voltage (e.g. 400V) N = CT ratio (e.g. 4000A/1A)
Uset = overvoltage pick up setting
I2
I1
Idiff = Σ I
• Uset≤ 400V
ABB
© A B B S w it z e rl a n d L td . -2 5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
feeder 1 feeder 2 RR BB 1 CT1 U1 UR RL1 RL2 UR > 0 U2 Im Im
External Fault
(without CT saturation)I2
I1
Idiff = Σ I
CT2
Principle:
An external fault (without CT saturation) will practically produce a very low differential current and therefore “no” voltage on the high
impedance. The overvoltage relay which is measuring at the high impedance will not pick up.
ABB
© A B B S w it z e rl a n d L td . -2 6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
feeder 1 feeder 2 RR BB 1 CT1 U1 UR RL1 RL2 UR > 0 U2 Im Im
External Fault
(with CT saturation)I2
I1
Idiff = Σ I
CT2
Principle:
In case of CT saturation the secondary reactance of the saturated CT will practically come to zero. Only the secondary resistant RCT (winding resistant) will result (du/di = r <<<<<<).
The High impedance will be bypassed by the relatively small sum of RW + 2RL2. Therefore the voltage UR will not reach the pick up level.
ABB
© A B B S w it z e rl a n d L td . -2 7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R W CT2 feeder 1 feeder 2 RR BB 1 CT1 U1 UR RL1 RL2 UR > 0 U2 Im ImSetting rules for stability: UR = Voltage at the high impedance
Ikmax = maximum possible ext. fault current (e.g. 45kA) N = CT ratio (e.g. 4000A/1A)
Uset = overvoltage pick up setting RCT = CT winding resistant (e.g. 6Ω) RL2 = lead resistant (e.g. 2Ω)
2.5 = safety margin I2 I1 Idiff = Σ I ‚ Uset≥ 2.5 / 4000 * 45kA * (6Ω + 2 * 2Ω) ≥ 281V
External Fault
(with CT saturation)Uset ≥ 2.5 / N * Ikmax * (RCT + 2 * RL2)
RCT
ABB
© A B B S w it z e rl a n d L td . -2 8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WRR= High Impedance (e.g. 2000Ω)
Ikmin = minimum possible fault current (e.g. 1kA) N = CT ratio (e.g. 4000A/1A)
Uset= overvoltage pick up setting
IM = magnetising current at UK/2 (e.g. 0.3mA) x = number of CTs (e.g. 2)
Actual value of primary pick-up current
High Impedance Measurement Principle
Requirements: • Uset ≤ 400V ‚ Uset ≥ 281V
Minimum pick up value for the detection of the minimum primary fault current
Uset ≤ (Ikmin / N – x * IM) * RR
Uset ≤ (1000A / 4000 – 2 * 3mA) * 2KΩ Uset ≤ 488 V
Minimum primary fault current detection with actual setting of Uset = 300 V: Ikmin = N * (Uset / RR + x * IM)
Ikmin = 2000 * (300V / 2000Ω + 2 * 3mA) Ikmin = 624 A
ABB
© A B B S w it z e rl a n d L td . -2 9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
If necessary,
q an additional parallel resistor RP can be connected to change / adapt
the sensitivity
q an additional VDR can be connected to limit the voltage on the high
impedance (to prevent damage)
q an additional time delayed low stage overvoltage unit / function can be
connected to detect open / missing CT inputs during load condition
Alternatives (1)
Alarm Block UR U>> Trip RP VDR U> tABB
© A B B S w it z e rl a n d L td . -3 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
There is also the possibility to insert a current instead of voltage measurement.
Advantage: the Ikmin can be set directly in a current value: Ikmin = Iset * N
Alternatives (2)
Alarm Block UR RP VDR I>> Trip I> tABB
© A B B S w it z e rl a n d L td . -3 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
q simple, sensitive and extremely stable measurement system – CT could
theoretically be saturated / pre- magnetised 100%
q tripping time around one halfcycle
q easily extendable, if the correct CT is available!
q CT class TPS (old class X or BS) required – the TPS class defines q the knee point voltage
q the magnetising current at half of the knee point voltage q the winding resistance (at 75°C)
q inexpensive protection system – expensive CTs q all CTs have to be the same type incl. ratio
q no other protection devices are allowed in the same CT circuit q therefore no integration of CB Failure Protection etc. is possible
ABB
© A B B S w it z e rl a n d L td . -3 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
q in case multiple busbar configuration the current switching must be
realised mechanically (risk of maloperation during switching; burned /
damaged contacts / CTs !). A check zone and therefore a second CT core is strictly required (see following page)
q good testing facility of the measurement system but NOT of the current
switching logic (which is the sensitive / week part)
q the principal is a mix of physical behaviour of the CT and numerical (or
mechanical / analogue) current and voltage measurement – it is not possible to realize it 100% numerically (with a low impedance scheme)
q the possibility to record the CT currents is not given – therefore fault
evaluation is not possible
The state of the art:
Usually the High Impedance Protection Principle will only be installed in single busbar or 1 ½ CB configuration
ABB
© A B B S w it z e rl a n d L td . -3 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WHigh Impedance Measurement Principle
Multiple Busbar with CT Switching and Check Zone
I X X X II + I II Checkzone Discriminating Zone
ABB
© A B B S w it z e rl a n d L td . -3 4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle
Additional Quantity (s) to keep the Stability in case of
External Fault with CT Saturation
q as described in the previous slides the quantity Idiff (Σ I ) is
NOT sufficient in a Low Impedance Measurement System to guarantee Stability in case of External Fault with CT Saturation
q this additional quantity varies between the products and relay
generations
q some examples of “clever” solutions are shown SIMPLIFIED in
ABB
© A B B S w it z e rl a n d L td . -3 5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-2
– electronic relay generation
I
diff set< |
∑ I |
differential current measurement with instantaneous values
Phase Comparison
phase angle supervision = current direction supervision with
instantaneous values
&
t t = integration time TRIP CBs Setting:- Maximum load < Ikmin < minimum short circuit current
to prevent false operation in case of shorted CT and to detect lowest possible fault current
ABB
© A B B S w it z e rl a n d L td . -3 6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WTypical INX-2 Feature:
q centralised protection system, location in a centralised panel
q automatic test cycle which supervises around 50 – 60 % of all HW components
in the protection system and will block the system automatically in case of a HW fault
q sometimes it is tricky to find faulty components since the fault indication of
the automatic test is not very detailed and a lot of modules / electronic cards are available
q differential current and phase comparison (phase angle) measurement system
which evaluates instantaneous current values. The system includes no special CT saturation detection facility
q low CT requirements: 2-3 ms of current signal must be available. This
represents 5 times saturation on symmetrical fault currents (see following page)
q tripping time around 12ms
q integration of CB failure and End fault Protection is possible q installation from around year 1968 – 1985
q at present, the systems are still being extended (relatively seldom) q around 1200 systems are / were installed
Low Impedance Measurement Principle – BBP Type
INX-2
ABB
© A B B S w it z e rl a n d L td . -3 7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle
CT refresher course:
T -3 -2 -1 0 1 2 3 0 5 10 15 20 ms A1 A2 A3The areas
are equal
t
A1
=
A 2
=
A 3
=
∫
i(t) dt
•
10ms
Saturation at symmetrical current due to over-burdening or to high primary current
Ial = 1: current on
which the CT starts to saturates
5 – times saturation means
ABB
© A B B S w it z e rl a n d L td . -3 8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WI
kmin< |
∑ I |
differential current measurement with instantaneous values
k
set< |∑ I | / ∑ | I |
stabilising / restraining measure-ment with quantity Ires= ∑ | I | with
instantaneous values
&
t t = integration time TRIP CBs
CT saturation
detection
CT saturation detection with instantaneous values
Low Impedance Measurement Principle – BBP Type
INX-5
ABB
© A B B S w it z e rl a n d L td . -3 9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
D
if
fe
re
n
ti
a
l
c
u
rr
e
n
t
I
dif f=
|
Σ
I
|
Restraint current I
Rest=
Σ
| I |
inte rnal faul t no fault
I
kmink= 0,8
k= 1
0
Stabilised / Restraint Characteristic
Setting:
- Maximum load < Ikmin < minimum short circuit current
to prevent false operation in case of shorted CT and to detect lowest
possible fault current - K typically to 0.8
ABB
© A B B S w it z e rl a n d L td . -4 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
Internal Fault
ABB
© A B B S w it z e rl a n d L td . -4 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – without CT saturation
ABB
© A B B S w it z e rl a n d L td . -4 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation
ABB
© A B B S w it z e rl a n d L td . -4 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation
ABB
© A B B S w it z e rl a n d L td . -4 4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation
ABB
© A B B S w it z e rl a n d L td . -4 5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation
Depending on the saturation degree; the k – factor is reached for a longer or shorter time. Maloperation is still possible.
ABB
© A B B S w it z e rl a n d L td . -4 6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation
Depending on the saturation degree; the k – factor is reached for a longer or shorter time. Maloperation is still possible.
ABB
© A B B S w it z e rl a n d L td . -4 7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation
ABB
© A B B S w it z e rl a n d L td . -4 8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
Electronic circuit to generate Blocking Signals”: e.g. Negative Blocking Signal
ABB
© A B B S w it z e rl a n d L td . -4 9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation
The CT saturation detection will send blocking signals:
Positive CT saturation blocking signal will block the trip on negative differential current Negative CT saturation blocking signal will block the trip on positive differential current
POS BLOCKING SIGNAL (B+)
(B+)
– static relay generation
Neg BLOCKING
ABB
© A B B S w it z e rl a n d L td . -5 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation
(B+)
neg I diff
– static relay generation
neg I diff pos I diff pos I diff (B+) (B-) (B-)
ABB
© A B B S w it z e rl a n d L td . -5 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
The CT saturation detection will send blocking signals:
Positive CT saturation blocking signal will block the trip on negative differential current
Negative CT saturation blocking signal will block the trip on positive differential current
– static relay generation
&
t t = integration time TRIP CBsB-Idiff pos
&
tB+
Idiff neg
≥1
ABB
© A B B S w it z e rl a n d L td . -5 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation
The Stability is maintained
– static relay generation
(B+) neg I diff neg I diff pos I diff pos I diff (B+) (B-) (B-)
ABB
© A B B S w it z e rl a n d L td . -5 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
External Fault – with CT saturation & full DC offset
The Stability is maintained
(Idiff -)
(B+) (B+)
(B+) (B+)
(Idiff -) (Idiff -) (Idiff -)
BLOCKING METHOD: tripping in case of external fault with CT saturation will be blocked till the next zero crossing is reached
ABB
© A B B S w it z e rl a n d L td . -5 4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle – BBP Type
INX-5
Internal Fault – with CT saturation & full DC offset
TRIP (no blocking)
(Idiff +)
(B+) (B+)
(B+)
(Idiff +) (Idiff +)
The CT saturation detection will send blocking signals:
Positive CT saturation blocking signal will block the trip on negative differential current Negative CT saturation blocking signal will block the trip on positive differential current
ABB
© A B B S w it z e rl a n d L td . -5 5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WTypical INX-5 Feature:
q centralised protection system, location in a centralised panel
q automatic test cycle which supervises around 75 – 85 % of all HW
components in the protection system and will block the system automatically in case of a HW fault
q easy to find faulty components since the fault indication of the
automatic test is very detailed and a small number of modules / electronic cards are available
q restrained differential current measurement characteristic which
evaluates instantaneous current values. The system includes a CT saturation detection facility: BLOCKING METHOD. A blocking time which is too long delays the tripping command in case of evolving faults (fault evolves from external to internal)
Low Impedance Measurement Principle – BBP Type
INX-5
ABB
© A B B S w it z e rl a n d L td . -5 6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WTypical INX-5 Feature:
q low CT requirements: 2 ms of current signal must be available.
This represents 5 times saturation on symmetrical fault currents
q tripping time around 12ms
q integration of CB failure and End fault Protection is possible q installation from around year 1980 – 2003
q at present, the systems are still being extended frequently q around 800 systems are / were installed
Low Impedance Measurement Principle – BBP Type
INX-5
ABB
© A B B S w it z e rl a n d L td . -5 7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
I
kmin< |
∑ I |
differential current measurement with fundamental current values
k
set< |∑ I | / ∑ | I |
stabilising / restraining measure-ment with quantity Ires = ∑ | I | with
fundamental current values
&
TRIP CBs
Phase Comparison
phase angle supervision = current direction supervision with fundamental current values
F ir s t h a rm o n ic ( fu n d a m e n ta l) fi lt e ri n g b y F o u ri e r fi lt e r
The REB500 BBP system will evaluate only the fundamental frequency current signal. This increases accuracy in the case of
ABB
© A B B S w it z e rl a n d L td . -5 8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
I1 I1 I1 I1 I2 I2 I2 I 2 0 t 0 I2 t
Primary current
Restrained differential current and phase comparison algorithms which evaluates “only” the fundamental wave of the current signal:
ABB
© A B B S w it z e rl a n d L td . -5 9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R W I1 I1 I1 I1 I2 I2 I2 I 2 0 t 0 I1 I2 tSecondary
current
Low Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Restrained differential current and phase comparison algorithms which evaluates “only” the fundamental wave of the current signal:
ABB
© A B B S w it z e rl a n d L td . -6 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R W I1 I1 I1 I1 I2 I2 I2 I 2 0 t 0 I1 I2 tFundamental
frequency
component
Low Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Restrained differential current and phase comparison algorithms which evaluates “only” the fundamental wave of the current signal:
ABB
© A B B S w it z e rl a n d L td . -6 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
The result is a huge amplitude change (Δ a) and a
big phase shift (Δ α) between the two current signals
which could result in a maloperation in condition of
extreme CT saturation
0 t I Δ a Δ αFundamental
frequency
component
Restrained differential current and phase comparison algorithms which evaluates “only” the fundamental wave of the current signal:
ABB
© A B B S w it z e rl a n d L td . -6 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Result with extreme CT saturation
t ms 50 IN I / In Ires / In
Restrained differential current algorithm Restrained differential current and phase comparison algorithms which
ABB
© A B B S w it z e rl a n d L td . -6 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Result with extreme CT saturation
t ms 50 IN I / In t
Restrained differential current algorithm
k
Restrained differential current and phase comparison algorithms which evaluates “only” the fundamental wave of the current signal:
ABB
© A B B S w it z e rl a n d L td . -6 4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Result with extreme CT saturation
t ms 50 IN I / In t
Phase comparison algorithm
k P h a s e s h if t Δ α
Restrained differential current and phase comparison algorithms which evaluates “only” the fundamental wave of the current signal:
ABB
© A B B S w it z e rl a n d L td . -6 5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WRestrained differential current and phase comparison
algorithms which evaluate the fundamental wave of the
reconstructed current signal:
q The REB500 system will evaluate reconstructed
fundamental current values (Fourier filtered values).
The system will approximate the saturated current
values to it’s origin
q This is realized with the from ABB patented so
called “Maximum Prolongation Algorithm”. With this it
can be obtained that the system is never blocked due
to CT saturation: UNBLOCKING METHOD
Low Impedance Measurement Principle - BBP Type
REB500
ABB
© A B B S w it z e rl a n d L td . -6 6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WMaximum Prolongation Algorithm
Low Impedance Measurement Principle - BBP Type
REB500
ABB
© A B B S w it z e rl a n d L td . -6 7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Restrained differential current and phase comparison algorithms which uses the “Maximum Prolongation Algorithm” followed by the fundamental wave filter (Fourier filter)
I1 I1 I1 I1 I2 I2 I2 I 2 0 t 0 I1 I2 t
Reconstructed
current signal
ABB
© A B B S w it z e rl a n d L td . -6 8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
The result is a relatively small amplitude
change (Δ a) and more important a very
small phase shift (Δ α) between the two
current signals
0 t I Δ a Δ α Fundamental frequency Component of the Maximum Prolongation signalRestrained differential current and phase comparison algorithms which uses the “Maximum Prolongation Algorithm” followed by the fundamental wave filter (Fourier filter)
ABB
© A B B S w it z e rl a n d L td . -6 9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Result using the “Maximum Prolongation Algorithm”
with extreme CT saturation
t ms 50 IN I / In Ires / In
ABB
© A B B S w it z e rl a n d L td . -7 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
t ms 50 IN I / In t
Restrained differential current algorithm
k
Result using the “Maximum Prolongation Algorithm”
with extreme CT saturation
ABB
© A B B S w it z e rl a n d L td . -7 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
t ms 50 IN I / In t
Phase comparison algorithm
k P h a s e s h if t Δ α
Result using the “Maximum Prolongation Algorithm”
with extreme CT saturation
ABB
© A B B S w it z e rl a n d L td . -7 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Conclusion:
By prolonging the maximum value, the signal
is compensated such that the best possible
approximation of the PHASE ANGLE and
AMPLITUDE of the origin primary signal is
achieved
ABB
© A B B S w it z e rl a n d L td . -7 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
I
kmin< |
∑ I |
differential current measurement with reconstructed fundamental
current values
k
set< |∑ I | / ∑ | I |
stabilising / restraining measure-ment with quantity Ires = ∑ | I | with reconstructed fundamental current
values
&
TRIP CBs
Phase Comparison
phase angle supervision = current direction supervision with reconstructed fundamental current
values F ir s t h a rm o n ic ( fu n d a m e n ta l) fi lt e ri n g b y F o u ri e r fi lt e r m a x im u m p ro lo n g a ti o n o n a ll C T C u rr e n t s ig n a l
ABB
© A B B S w it z e rl a n d L td . -7 4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Measurement Algorithm: Stabilized differential current
Restraint Current I
RestDifferential current
I
Diff Inte rnal Fau lt No FaultI
kmink= 0,85
k= 1
0
ABB
© A B B S w it z e rl a n d L td . -7 5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB500
– numerical relay generation
Measurement Algorithm: Phase comparison
Im
Re Case 1: external fault ∆ϕ ≥ 74°
ϕ12 =139° I2 I1 Im Re ϕ12=40° Case 2: internal fault ∆ϕ < 74°
I1 I2 I2 I1 Tripping area P h a s e d if fe re n c e ∆ϕ No Fault Internal Fault Fall 1 2 ∆ϕ min = 74° 74° 180° 0°
ABB
© A B B S w it z e rl a n d L td . -7 6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WTypical REB500 Feature:
q decentralised protection system, location might be in a a
centralised panel or distributed (e.g. in the feeder protection panels)
q continuous self- supervision which supervises around 90 – 95 %
of all HW components and SW tasks in the protection system and will block the system automatically in case of a HW / SW fault
q very easy to find faulty components since the fault indication of
the continuous self- supervision is very detailed and a very small number of modules / electronic cards are available
q restrained differential current measurement (INX-5) and phase
comparison (phase angle) (INX-2) algorithm which evaluates
reconstructed fundamental current values (Fourier filtered values). The system will approximate the saturated current values to it’s
origin with a from ABB patented (so called “maximum prolongation”) algorithm: UNBLOCKING METHOD (the system is never blocked due to CT saturation). No problem in case of evolving faults (fault
evolves from external to internal)
Low Impedance Measurement Principle - BBP Type
REB500
ABB
© A B B S w it z e rl a n d L td . -7 7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WTypical REB500 Feature:
q the restrained differential current measurement; phase
comparison (phase angle) measurement and the maximum
prolongation algorithm could be activated individually for special application
q typical tripping time around 25ms
q integration of CB failure and End fault Protection as well as Line & Transformer Protection Functions is possible. Additional
measurement functions as event- & disturbance recorder as well as additional release functions like I> or U< are available
q low CT requirements: 2 ms of current signal must be available.
This represents 5 times saturation on symmetrical fault currents
q state of the art: installation from year 1994 – future q over 1500 systems are in service (so far)
Low Impedance Measurement Principle - BBP Type
REB500
ABB
© A B B S w it z e rl a n d L td . -7 8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
• I
kmin< |
∑ I |
differential current measurement with RMS current values
‚s
set< |∑ I | / ∑ | I
in|
stabilising / restraining measurement with quantity Ires= ∑ | Iin |
with RMS current values
&
TRIP CBs
ƒ external fault detection
(decision 1.2 ms after zero crossing)
detection internal / external fault with instantaneous / sampled current values
ABB
© A B B S w it z e rl a n d L td . -7 9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
ABB
© A B B S w it z e rl a n d L td . -8 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
Calculation of the instantaneous value of the differential current:
Calculation of the instantaneous sum of positive currents:
ABB
© A B B S w it z e rl a n d L td . -8 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
Calculation of the incoming and outgoing currents:
ABB
© A B B S w it z e rl a n d L td . -8 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
ABB
© A B B S w it z e rl a n d L td . -8 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
Condition at Internal Fault:
sudden split between of RMS Iin and RMS Iout will indicate an internal fault
if • & ‚ (Ikmin & s) is fulfilled the protection will trip since ƒ will not see an external fault
ABB
© A B B S w it z e rl a n d L td . -8 4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
ABB
© A B B S w it z e rl a n d L td . -8 5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
Condition at External Fault with CT Saturation:
ƒ will detect an external fault within 1.2ms after the Iin zero crossing (before the CT gets into saturation) and will blocktill the next zero crossing is reached
ABB
© A B B S w it z e rl a n d L td . -8 6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
Test assembly:
ABB
© A B B S w it z e rl a n d L td . -8 7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
Test values & result:
The CT TX war pre- magnetised with a DC current in order to get maximum remanence. Therefore the CT saturates within 1.2 ms! The primary test current level was 26kA RMS with the full DC offset
ABB
© A B B S w it z e rl a n d L td . -8 8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
ABB
© A B B S w it z e rl a n d L td . -8 9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WLow Impedance Measurement Principle - BBP Type
REB670
– numerical relay generation
Stabilised / Restraint Characteristic Setting:
- Maximum load < Ikmin (Diff Oper Level) < minimum short circuit current to prevent false operation in case of shorted CT and to detect lowest possible fault current
The sensitive (non restraint) operational level is designed to be able to detect internal busbar faults in low impedance earthed power systems: Limited earth fault current to certain level (300 – 2000A)
ABB
© A B B S w it z e rl a n d L td . -9 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WTypical REB670 Feature:
q centralised protection system, location in a centralised panel
q continuous self- supervision which supervises the most of the HW
components and SW tasks in the protection system and will block the system automatically in case of a HW / SW fault
q very easy to find faulty components since a very small number of
modules / electronic cards are available
q restrained differential current measurement algorithm which
evaluates RMS current values. The system can decides within 1.2ms after the zero crossing of the current if the fault is external or
internal. In case of external fault the measurement will be blocked till the next zero crossing: BLOCKING METHOD. A blocking time which is too long delays the tripping command in case of evolving faults (fault evolves from external to internal)
Low Impedance Measurement Principle - BBP Type
REB670
ABB
© A B B S w it z e rl a n d L td . -9 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WTypical REB670 Feature:
q very low (“almost no”) CT requirements: the system was
successfully tested with just 1.2 ms of current signal. This
represents >> 5 times saturation on symmetrical fault currents
q tripping time around one halfcycle
q integration of CB Failure, OC protection as well as event- &
disturbance recorder, monitoring function is possible
q state of the art: installation from year 2005 – future
q the system is a consequently further development / improvement
of the well proven BBP systems RADSS, REB103, RED521
Low Impedance Measurement Principle - BBP Type
REB670
ABB
© A B B S w it z e rl a n d L td . -9 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WBusbar fault condition
I1 = 1000A
single injection
ABB
© A B B S w it z e rl a n d L td . -9 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WCalculation examples
∆ U = ∆ Isec * RR = 0.5A * 2000Ω = 1 kV (spike) à TRIP Σ Iin = + + I1 = + 1 kA = 1 kA Σ I = + + I1 = + 1 kA = 1 kA ∆ Isec = I1/N = 1 kA / 2000 = 0.5 A ∆ I = + I1 = + 1 kA = 1 kA ∆ I = + I1 = + 1 kA = 1 kA High Impedance System(with CT ratio: N = 2000A / 1A; Impedance: RR= 2000 Ω; Knee Point V: UK = 400V) Low Impedance Measurement System REB670 Low Impedance Measurement System REB500
ABB
© A B B S w it z e rl a n d L td . -9 4 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WD
if
fe
re
n
ti
a
l
c
u
rr
e
n
t
I
dif f=
|
Σ
I
|
►trip measurement system !!!
⇒ ( if I∆ > Ikmin)
Calculation examples
Restraint current IRest = Σ | I |
Restraint current IRest = Σ | Iin |
no fault
I
kmink
REB500= 0,85
k= 1
0
Inte rnal faul t RE B50 0 Inte rnal faul t REB 670k
REB670= 0,53
ABB
© A B B S w it z e rl a n d L td . -9 5 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WBusbar fault condition
I1 = I2 = I3 = I4 = 1000A 2500A 1500A 2000A
multiple injection
ABB
© A B B S w it z e rl a n d L td . -9 6 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R W ∆ U = ∆ Isec * RR = 3.5A * 2000Ω = 7 kV (spike) à TRIP Σ Iin = ++ I1++ I2+ + I3++ I4 = + 1 kA + 2.5 kA + 1.5 kA + 2 kA = 7 kA Σ I = ++ I1++ I2+ + I3+ + I4 = + 1 kA + 2.5 kA + 1.5 kA + 2 kA = 7 kA ∆ Isec = I1/N = 7 kA / 2000 = 3.5 A ∆ I = + I1 + I2 + I3 + I4 = + 1 kA + 2.5 kA + 1.5 kA + 2 kA = 7 kA ∆ I = + I1 + I2 + I3 + I4 = + 1 kA + 2.5 kA + 1.5 kA + 2 kA = 7 kA High Impedance System(with CT ratio: N = 2000A / 1A; Impedance: RR= 2000 Ω; Knee Point V: UK = 400V) Low Impedance Measurement System REB670 Low Impedance Measurement System REB500
ABB
© A B B S w it z e rl a n d L td . -9 7 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WD
if
fe
re
n
ti
a
l
c
u
rr
e
n
t
I
dif f=
|
Σ
I
|
►trip measurement system !!!
⇒ ( if I∆ > Ikmin)
Calculation examples
Restraint current IRest = Σ | I |
Restraint current IRest = Σ | Iin |
no fault
I
kmink
REB500= 0,85
k= 1
0
Inte rnal faul t RE B50 0 Inte rnal faul t REB 670k
REB670= 0,53
load depending tripping value!!!
Internal fault condition
ABB
© A B B S w it z e rl a n d L td . -9 8 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R We.g. line fault
External fault condition
I2 = I3 = I4 = 2500A 1500A 2000A I1 =
6000A
ABB
© A B B S w it z e rl a n d L td . -9 9 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R W ∆ U = ∆ Isec * RR = 0A * 2000Ω = 0 kV à NO TRIP Σ Iin = + I2+ +I3++ I4 = 2.5 kA + 1.5 kA + 2 kA = 6 kA Σ I = ++ I1++ I2+ +I3++ I4 = + 6 kA + 2.5 kA + 1.5 kA + 2 kA = 12 kA ∆ Isec = I1/N = 0 kA / 2000 = 0 A ∆ I = + I1 + I2 + I3 + I4 = - 6 kA + 2.5 kA + 1.5 kA + 2 kA = 0 kA ∆ I = + I1 + I2 + I3 + I4 = - 6 kA + 2.5 kA + 1.5 kA + 2 kA = 0 kA High Impedance System(with CT ratio: N = 2000A / 1A; Impedance: RR= 2000 Ω; Knee Point V: UK = 400V) Low Impedance Measurement System REB670 Low Impedance Measurement System REB500
ABB
© A B B S w it z e rl a n d L td . -1 0 0 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WD
if
fe
re
n
ti
a
l
c
u
rr
e
n
t
I
dif f=
|
Σ
I
|
►no trip
►stable !!!
Calculation examples
Restraint current IRest = Σ | I |
Restraint current IRest = Σ | Iin |
no fault
I
kmink
REB500= 0,85
k= 1
0
Inte rnal faul t RE B50 0 Inte rnal faul t REB 670k
REB670= 0,53
ABB
© A B B S w it z e rl a n d L td . -1 0 1 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R Wduring fault condition (
Ι)
Current transformer failure (
Ι
)
I2 = I3 = I4 = 2500A 1500A 2000A I1 =
6000A
CT shorted !!!
ABB
© A B B S w it z e rl a n d L td . -1 0 2 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R W ∆ U = ∆ Isec * RR = 1A * 2000Ω = 2 kV (spike) à TRIP !!! Σ Iin = + + I1 = + 6 kA = 6 kA Σ I = + + I1+ + I2 + + I3 + + I4 = + 6 kA + 2.5 kA + 1.5 kA + 0 kA = 10 kA ∆ Isec= I1/N = 2 kA / 2000 = 1 A ∆ I = + I1 + I2 + I3 + I4 = - 6 kA + 2.5 kA + 1.5 kA + 0 kA = 2 kA ∆ I = + I1 + I2 + I3 + I4 = - 6 kA + 2.5 kA + 1.5 kA + 0 kA = 2 kA High Impedance System(with CT ratio: N = 2000A / 1A; Impedance: RR= 2000 Ω; Knee Point V: UK = 400V) Low Impedance Measurement System REB670 Low Impedance Measurement System REB500
ABB
© A B B S w it z e rl a n d L td . -1 0 3 C H P 1 3 3 _ B B P _ M S / 2 0 0 7 0 9 / R WD
if
fe
re
n
ti
a
l
c
u
rr
e
n
t
I
dif f=
|
Σ
I
|
Calculation examples
Restraint current IRest = Σ | I |
Restraint current IRest = Σ | Iin |
no fault