The resistance of the arc can be
increased by three different methods A, B, and C as below:
a) Lengthening
the arc by means of arc runners: The arc runners have horn like shape and
arc made up of conducting material. The arc originates at the bottom and it is
pulled upwards due to electromagnetic force which increases arc length. Thus, arc
can be extinguished.
Material: Tungsten base alloy.
b) Splitting the arc with arc splitters:
The arc splitters (plates of resin bonded fibre) are placed perpendicular to
arc and arc is pulled in them by electromagnetic force. The arc travels upwards
and it splits so its length increases and it is cooled. So the arc is
elongated, constrained and cooled. By virtue of this it is extinguished.
c) Cooling of arc: Cooling of arc results
in deionization. Cooling removes heat from the arc. Effective cooling may be
obtained by cooled air or gas blasted along the arc. This removes heat from
arc. It brings about recombination of ionized particles. Dielectric strength is
developed between the two contacts of C.B. and prevents re-striking of arc.
2. Low Resistance or Zero Current Method;
All modern high power A.C. circuit breakers employ this method. In a AQC. system
current drops to zero after every half cycle. So the arc is interrupted at
current zero. At current zero space between contacts is demonized by
introducing fresh dielectric such as SF6, oil, air. So dielectric strength of
gap between contact should increase to an extent such that arc should not
re-strike after current zero. A high voltage (called re-str5iking voltage)
appears across contacts which may reestablish the arc if the breakdown strength
of gap is less than re-striking voltage in this case, the arc continues for
another half cycle and may get extinguished at next current zero.
Some Important Terms:
1. Arc Voltage: It is the voltage that
appears across the contacts of the circuit breakdown during the arcing period
as the contacts are opened.
2. Re-striking Voltage: It is the
transient voltage that appears across the contact at or near current zero
during arcing period.
At
current zero a high frequency transient voltage appears across the contacts
which is caused by rapid distribution of energy between magnetic and electric
fields associated with the plant and transmission line. So the transient
voltage appears i.e. re-striking voltage. If dielectric strength rise is
greater than rise of re-striking voltage then arc will not re-strike.
3. Recovery Voltage: It is the normal
frequency (50 Hz) r.m.s. voltage that appears across the contacts of C.B. after
final arc extinction. It is approximately equal to system voltage. Problem
in current interruption: Power system has appreciable amount of inductance
and capacitance. When fault occurs, energy stored in these elements is
appreciable so when C.B. performs the function of interrupting the circuit, it
must dissipate as much energy (oscillatory nature) as possible.
4. Rate of Rise of Re-striking Voltage (RRRV):
It is the rate of increase of re-striking voltage. It is measured in kV/μ sec.
Consider a system as shown in Fig.
When
fault occurs capacitance ‘C’ is shorted so S.C. current through C.B. is limited
by ‘L’ only. So ‘I’ lags ‘v’ by 900 when C.B. contacts are separated
voltage of generator. Suddenly gets applied to L-C combination which forms
oscillatory circuit, frequency of which is
fn
= 1/2μ√LC
Which
appear across ‘C’ and C.B. contacts. So the transient re-striking voltage may
reach a value of 2Em as shown in figure.
Thus
RRRV depends upon:
i)
Recovery
voltage
ii)
Natural
frequency of oscillation.
5. Current Chopping: It is the phenomena
of current interruption before natural current zero is reached.
This
occurs mainly in air blast C.B. because they retain same extinguishing power
irrespective of the magnitude of current to be interrupted. When interrupting
low inductive current e.g. magnetic current of transformer, a rapid deionising
effect causes current, to fall to its zero value before natural current zero
this is called currents chopping.
Consider
the following figure (a) and (b0 shown I arc is current at point ‘a’ when
chopping is done i.e. it is made zero. So energy stored in the inductance i.e.
it is made zero. So energy stored in the inductance i.e. ½ Li2 is
transferred to the capacitor which charges it latter to a voltage.
V =
i√L/C
½
Li2 = ½ CV2J
fn
= 1/2π√L/C
v =
i√L/C
This
voltage is very high, such a transient voltage. This high voltage causes
re-striking of arc before the voltage reaches its maximum value. Re-striking of
arc draws energy from capacitor and so voltage across capacitor decreases. The
point to which this re-striking voltage will rise will depend on RRRV. If it is
less then time taken to reach maximum value is more and de-ionizing effect will
be more predominant. Demonizing effect which is still in action will produce
second current Chop. This value of current is smaller than previous one. Again
re-striking voltage builds up having high RRRV appears across the contacts,
unless the arc continues. If arc re-strikes further several chops may occur
before the final interruption of current and C.B. may fail to clear the fault.
If re-striking does not occur a very high voltage appears across.
6. Resistance Switching is Adopted to Overcome
the Effect of Over Voltages due to Current Chopping:
Capacitive current braking: Consider a unloaded
transmission line which has predominant amount of capacitance. So I leads V by
900 when is opened ‘er’ is maximum and is lagging I by
900. The capacitor is charged to a voltage ec . And ‘A’ of CB still
carries nominal sinusoidal voltage (er).
At
t1 the voltage at point ‘A’ is at its negative maximum and capacitor is at
positive voltage. So voltage across CB becomes twice (i.e. 2Vgm).
This voltage can re-strike the arc. This is shown in below figure. If re=strike
occurs the line capacitance now discharges and the LC circuit will oscillate at
a frequency fn = 1/2π√L/C.
This current tries to maintain the arc. The voltage across terminals may rise
up to 4 p.u. due to one re-strike and up to 6 p.u. with 2nd
re-strike. The peak value of initial transient voltage is twice he voltage at
an instant i.e. -Vgm. This
causes transmission line voltage to swing to – 4Vgm to SGP + Vgm
i.e. -3Vgm. Once again the two sides of circuits are separated at this (-3Vgm)
voltage. After half cycle again the line may be left with a potential of 5Vgm
above earth potential. The energy of half CV2 is dissipated during
arc, which is very large, which may damage, so CBs should be re-strike free.
7. Resistance Switching: The switching
resistor (R) is connected in parallel with C.B. contacts. The current chopping,
capacitive current breaking produces high voltage oscillations which can be
prevented by above method. During arc interruption CB contact separate first
and after arc gets extinguished ‘S’ opens depending upon time delay provided to
it.
Referring
above figure (a) and (b) when fault occurs, the CB contact open and arc is
struck between them. Since, R is in parallel with CB contacts a part of arc
current flows through this resistance so arc current decreases and deionization
rate increases. Consequently, the arc resistance also increases so current
through R increases. This continues till arc current is insufficient to
maintain the arc.
The
resistance ‘R’ also helps in limiting the growth of re-striking voltage and
cause to grow exponentially up to recovery voltage.
So
the resistance across C.B. contact performs the following functions:
i)
To
reduce the RRRV and the peak value of re-striking voltage.
ii)
To
reduce the voltage surges due to current chopping and capacitive current
breaking.
iii)
To
ensure even sharing of re-striking voltage transient across the various
breakers in multi break.
Before
studying the different types of circuit breakers let us know the related terms:
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