Friday, 9 January 2015

                                                                
                                 OVER VOLTAGE PROTECTION                CHAPTER- 9

CAUSES OF OVER VOLTAGE
Introduction
Over voltages (or surge voltages) on the electric power systems are due to various reasons. If the system is working on the normal voltage satisfactorily then it will not stress the insulation severely due to normal working temperature cause of normal currents. But the voltage stresses due to over voltages can be so high that they may prove dangerous to the line, equipment and accessories. The system may be damaged. In order to avoid such happenings the equipments and lines are to be provided with protection device and schemes to work effectively under abnormal conditions and disconnect them for safety or divert the surge energy to the earth or absorb the surge energy in some absorbers.
The Voltage Surge Nature
                                   
Sudden rise in the voltage for a very small duration on the power system is called as voltage surge or transient voltage, as shown in the figure.
These surges are generally produced due to switching ON or OFF or lightning or fault occurrence due to some reasons.
A steep front wave in a short time t, when voltage reaches maximum value Em and time t1 is very short 1 to 5µ sec, Time t2 is the decay of wave to its half the maximum value Em/2. The wave is specified in the times t1 and t2, for example if t1 =1μ sec and t2 = 60μ sec. then surge is specified as 1/60 μ sec. surge.
Causes of Over Voltages
These are broadly divided into two categories:
1.    External causes of over voltages, 2. Internal causes of over voltages.

1.    External Causes: These are the severe cause and induce a very steep and high amplitude surge wave and dangerous to the power supply lines and equipments.
These causes may be due to the following:
i)              Direct lightning strokes.
ii)             Electro-magnetically induced due to lightning discharge taking place near the line.
iii)            Voltage induced due to change in atmospheric conditions along the line – length.
iv)           Electro statically induced voltages due to presence of charged clouds nearby.
v)            Electro statically induced voltages due to the frictional effects of small particles such as dirt, dust, snow.

2.    Internal Causes: The surge produced due to internal causes area not so steep and do not have much more amplitude as compared with surge due to lightning. The system voltage hardly increases to twice the normal voltage of the power lines. Internal causes may be:
i)      Switching surge, ii) Insulation failure, iii) Arcing grounds, iv) Resonance.

I)     Switching surge:
 a)    The circuit opened and closed causes the over voltage and produce a voltage surge of the nature oscillatory and take the form of damped sinusoidal. When unloaded line is connected to the voltage source a voltage wave is set up which travels along the line. On reaching the terminal point ‘A’ it is bounced back to the supply end without change in sign. On the system therefore double voltage id developed (2 x 2Erms). This is of temporary nature and line stabilizes with its normal voltage. The same effect is produced when unloaded line is switched off.

b)    In case of loaded line also a high voltage is developed on the line. This voltage will be 2 x instantaneous current  x impedance of the line i.e. = 2 I Zn. Where line impedance (called as natural impedance) Zn = L/C  where, L and C are line constants.

Taking a simple case,
            Zn = 1000, Lrms = 100 Amp.
   Voltage  = 2iZn
                  = 2 x 2 x 100 x 1000 volts
                      2 x 2 x 100 x 1000
                  = -------------------------- kV
                              1000
                  = 282.8 kV
Maximum voltage on the line is therefore,
                   = Vm + 282.8 kV where Vm is maximum of the line voltage.

c)    Current chopping: It is the phenomena of current interruption before natural current zero is reached.
                                   
This occurs mainly in air blast CB because they retain same extinguishing power irrespective of the magnitude of current to be interrupted.
When interrupting low inductive current e.g. magnetizing current of transformer, a rapid de-ionizing effect causes current, to fall to its zero value before natural current zero this is called currents chopping.
ii)       Insulation failure
If the insulation of the line fails due to conductor grounding i.e. conductor touches to ground a voltage of the system increases. This fault is shown in the above figure. Take the case of line is earthed at point x and the line has a potential of E volts. Then two equal voltages are caused i.e. –E volts travelling along point B in the section XB, and along XA and these sections contain currents equal to  -E/Zn and  +E/Zn respectively. Bothe these currents pass through fault point x to the earth = 2E/Zn.
iii)    Arcing grounds: The phenomenon of interminant arc taking place in line to ground fault of a 3-phase system with consequent production of transients is known as arcing grounds. These are cumulative and cause damage to the equipment in the power system by causing breakdown of insulation. This can be prevented by neutral earthing.

iv)   Resonance: We know that resonance is the condition of the circuit when inductive reactance XL and capacitive reactance XC of the line becomes equal and net reactance becomes zero. Impedance becomes minimum and power factor of the circuit becomes unity. In resonance voltage magnification takes place and voltage in the line increases. In transmission lines as XL is small the resonance condition is rare but it may be in case of cables buried under ground.
LIGHTNING PHENOMENON
The discharge of the charged cloud to the ground is called as Lightning Phenomenon.
Lightning is a huge spark and it takes place when the clouds are charged to such a high potential positive or negative w.r.t. the earth or a neighboring cloud and if this happens then there is possibility of insulation of air breaks down (destroyed).
An electric discharge between cloud and earth, between clouds or between the charge centers of the same cloud is known as lightning.
Lightning is huge spark and takes place when clouds are charged to such a high potential (positive or negative) with respect to earth or a neighboring cloud that the dielectric strength of neighboring medium (air) is destroyed. During the up rush of warm moist air from earth, the friction between the air and the tiny particles of water causes the building up of charges. When drops of water are formed, the larger drops become positively charged and the smaller drops become negatively charged. When the drops of water accumulate they form clouds. The charge of a cloud may become so great that it may discharge to another cloud or to earth and we call this discharge as lightning. The thunder which accompanies lightning is due to the fact that lightning suddenly heats up the air, thereby causing it to expand. The surrounding air pushes the expanded air back and forth causing the wave motion of air which we recognize as thunder.
How the Lightning Discharge is Produced
The charged clouds pass over the earth and hence as per the theory of induction of the earth acquires the equal and opposite charge. Taking the case that a positive charged cloud passes over the portion of the earth naturally earth portion will have negative charge on it. There exists a potential difference between the charged cloud and the earth. As the chare on the cloud increases the p.d. will also increase a stage  may come that when potential gradient is <5kV/cm>10kV/cm then insulation of air breaks down and lightning stroke starts from cloud to earth.
Let us study the mechanism of the lightning stroke in three stages.
Step 1                                
After the break in the air, leader streamer/pilot streamer carries charge from he cloud towards the earth. This process continues as long as the cloud feeds enough charge to the  streamer to maintain the voltage gradient on the tip of the leader streamer above the breaking strength of the air but if the gradient is not maintained the process stops and the leader streamer is unable to carry the charge to the earth. So, no lightning stroke on the earth as shown in the figure. In his situation the current in the streamer is less than 100 Amp. And its velocity of propagation is about 0.05% of the velocity of light and its luminosity is very weak and lightning is not seen by the eyes.
Stage 2  
If the leader streamer moves towards the earth it makes contact with some object on the earth, it is accompanied by points of luminescence travelling like jumping. This gives rises to stepped leaders as shown in the figure. In such situation the velocity of stepped leaders may exceed on sixth of that of the velocity of light and distance travelled in one step may be 50 metres. The step leaders are producing sufficient luminosity and give rise to first visual phenomenon of lightning discharge.
Stage 3:  
The path of leader streamer is a path of ionization and therefore of complete breakdown of insulation. As the leader streamer reaches near the earth, a return streamer shoots up from the earth to the cloud, following the same path as the main channel of the downward leader. The action can be compared with the closing of a switch between the positive and negative terminal; the downward leader having negative charge and return streamer the positive charge. This phenomenon causes a sudden spark which we call “ lightning”. The negative charge and positive charge come together and get neutralized at lightning stroke. The further lightning stroke may be initiated from the other portion of the cloud.
Following Points can be Noted About Lightning
1.    The lightning which is seen by our eyes appears to be a single flash but in fact it is made up of number of separate strokes.
2.    Strokes are one after the other from 0.0005 sec. to 0.5 seconds and hence will see a combined flash of these.
3.    Negatively charged clouds are about 87% in comparison with positively charged cloud which are only 13%.
4.    Information collected from all over the world speaks that there are about 100 lightning strokes produced per second.
5.    Currents in the lightning strokes are in the range of 10kA to 90kA.
Lightning Strokes.
We have seen how the lightning stroke is produced. This stroke may struck the electrical system (i) Directly or (ii) Indirectly.
i)      Directly Stroke: The lightning stroke discharges directly from the cloud to the subject equipment like over head lines (transmission or distribution lines). And the path of the current due to this stroke is from the cloud, to the line the insulators ten via poles (supports, towers) to the ground. The over voltages set up may so huge to flash over this path directly to the ground. This stroke again may be type (A) and (B) shown in the figure.
In stroke A, the lightning discharge is from the cloud to the subject equipment i.e. an overhead line in this case as shown in figure. The cloud will induce a charge of opposite sign on the tall object (overhead line). When the potential between the cloud and line exceeds the breakdown value of air, the lightning discharge occurs between the cloud and the line.
In stroke B, the lightning discharge occurs on the overhead line as a result of stroke A between the clouds as shown in the figure. There are three clouds P, Q and R having positive, negative and positive charges respectively. The charge on the cloud Q is bound by the cloud R. If the cloud P shifts too near to the cloud Q then lightning discharge will occur between them and charges on both these clouds disappear quickly. The result is that charge on cloud R suddenly becomes fee and it then discharges rapidly to earth, ignoring tall objects.
                                     
ii)     Indirect Stroke: Indirect strokes result from the electro-statically induced charges on the conductors due to the presence of charge clouds. This is illustrated in figure. A positively charged cloud is above the line and induces a negative charge on the line by electrostatic induction. This negative charge, however, will be only on that portion of the line right under the cloud and the portions of the line away from it will be positively charged as shown in figure. The induced positive charge leaks slowly to earth via the insulator. When the cloud discharges to earth or to another cloud, the negative charge on the wire is isolated it cannot flow quickly to earth over the insulators. The result is that negative charge rushes along the line in both directions in the form of travelling waves.
                                  
PROTECTION OF TRANSMISSION LINE SUB-STATION FROM DIRECT STROKE
The surges on the power system may originate from switching and from other causes but the important and dangerous surges are those caused by lightning. The lightning surges may cause serious damage to the expensive equipment in the power system (e.g. generators, transformers etc.) either by direct strokes on he equipment or by stroke on the transmission lines that reach the equipment as travelling wave. It is necessary to provide protection against both kinds of surges. Following devices are commonly used for protection against lightning surges.
1. Earthing screen.      2. Overhead ground wires.     3. Lightning arrestors or surge diverters.
Earthing screen provides protection to power stations and sub-station against direct stroke whereas overhead ground wires protect the transmission lines against direct lightning strokes. However, lightning arrestors or surge diverters protect the station apparatus against both direct strokes and the strokes that come into the apparatus as travelling waves.
1.    The earthing Screen: The power stations and sub-stations generally house expensive equipment. For their protection earthing screen is provided. It consists of a network of copper conductors (generally called shield or screen) mounted all over the electrical equipment in the sub-station or power station. The shield is properly connected to earth on at least two points through a low impedance. On the occurrence of direct stroke on he station, screen provides a low resistance path by which lightning surges are conducted to ground. In this way station equipment is protected against damage. The limitation of this method is that it does not provide protection against the travelling waves which may reach the equipment in the station.

2.    Overhead Ground Wires: The most effective method of providing protection to transmission lines against direct lightning strokes is by the use of overhead ground wires as shown in fig. The ground wires are placed above the line conductors at such positions that practically all lightning strokes are intercepted by them. The ground wires are grounded at each tower or pole through as low resistance as possible. Due to their proper location, the ground wires will take up all  the lightning strokes instead of allowing them to line conductors.

Footing resistance of the tower must be kept as low as possible so that surge current immediately passes to the ground without any chance of insulator flash-over.
                                              
Advantages of such ground wire system are:
i)              Good protection of line from lightning strokes.
ii)             It reduces voltage induced in the line conductors due to discharge of neighboring cloud.
iii)            Due to its action of short circuiting secondary ground wire provides damping effect on any disturbance travelling along the line.
Disadvantages:
i)              Additional cost of ground conductor.
ii)             Possibility of breaking of ground conductor and falling on line to create short circuit fault. 
3.    Lightning arrestors.
4.    Surge absorbers.
(3) and (4) are explained details which give protection against lightning surges and travelling waves.
LIGHTNING ARRESTOR
Earthing screens and ground wires are suggested for protection against direct lightning strokes but they are unable to protect he equipment against travelling waves. The lightning arrestors or surge diverters take care of the terminal equipments against such surges.
Function
The function of the lightning arrestor or surge diverter is to conduct the high voltage, surges on the power system to the ground, thus discharging the impulse surge to earth and to dissipate energy in the form of heat.
Schematic Representation and Functioning of Arrestor
                             
Basically, the arrestor has a spark-gap and to its series a non-linear resistor. (aprperty of non-linear resistance is that its resistance decreases as the voltage or current increases and vice-versa). One end of arrestor is connected to the equipment terminal and the other is perfectly earthed.
The spark gap can be set as per the system voltage. Its length is so selected that arc is not produced due to normal system voltage but due to an abnormal high voltage produces a spark (arc) in the spark-gap. The arc is formed due to breaking of insulation of air across the gap due high surge voltage.
Working of Arrestor/Surge Diverter
Step-1. No current jumps in the spark-gap when system voltage is having its normal value and equipment is working.
Step-2. When the line voltage increases due to surges, this high voltage breaks the gap and an arc is produced (current jumps through the gap and passes through resistance R to ground). The arc finds the low resistance path to ground and the surge is not sent back to the line.
Step-3. As the gap, sparks over due to over-voltage. Since, the property of non-linear resistance is to offer high resistance to high voltage it prevents the effect of short current.
Step-4. After the surge is over, the resistor offers high resistance to make the gap non-conducting.
Design of Lightning Arrestor
The design should be such that:
1.    When the surge is over, he arc should go out immediately otherwise the current through gap and resistant will be maintained to flow destroying gap and resistor.
2.    During the surge current the voltage drop i.e. Surge current (I) x Resistance should not exceed the breakdown strength of insulation of the equipment to be protected against such surges.
Types of Lightning Arrestors In all types of arrestors the mechanism is to provide a low resistance path for the surge currents to the ground so that the high voltage produced will not affect the equipment and its insulation remain in tack.
There are so many types depending upon:
(i)  Equipment to be protected            (ii) Type of gap produced
(iii) Chemicals used                            (iv) Discs used.
The main types to be studied under this topic are:
1. Rod-gap arrestor                 2. Horn-gap arrestor               3. Multi gap arrestor
4. Expulsion type arrestor       5. Thirties disc-valve type arrestor.

1. Rod Gap Arrestor: This is generally located across the bushings of transformer and generally used as back up protection in case of main arrestors.

Construction:                                        
 As shown in figure the arrestor is in the form of bend-rods having spark-gap between the two. The upper rod is connected to the line electrically and the lower one is connected to earth to carry away surge current.
Dimensions: 1.5 cm rods bend at 900 as shown, distance ‘d’ between gap and bushing outside, face >1/3 gap length to avoid reaching of arc to the bushing body. The gap length is so adjusted that breakdown should occur at 0.8 of spark over voltage.
Working: Under normal voltage conditions the gap acts as a air insulation and non-conducting and the line voltage is ineffective to make the gap conducting.
Now when the voltage increases so suddenly due to surge on the line, this surge voltage breaks the gap between the rods and spark over (arc) is produced. Surge current passes from the line to spark-gap to second rod and finally to the earth within a very short time and the equipment is prot4ected. After the surge the gap as a insulator under normal voltage of the line.
Drawbacks and Limitations:
1.    It is expected that after the surge is over arc shall blow off but there is a chance of remaining it in the gap due to the normal voltage also. This is due to absence of non-linear resistance in its circuit. This may lead to short circuit.
2.    If not properly designed the rods may bend, melt, damage due to over heating caused by the arc.
3.    Rain water, humidity, temperatures may affect the gap and arrestor may not give good service.
4.    The polarity of the surge may also affect the performance of the arrestor.
So its uses are limited.

Applications:
i)              Transformer protection.
ii)             Backup protection with main arrestors.

2.   Horn Gap Arrestors:                                 
This type arrestor also used at the limited places due to it unreliability i.e. it is used  as back up protection with main arrestor.
Construction: (1) and (2) are the rods bent to give horn like construction with the air gap in between the shape of horns widening on the top portion and narrow at the bottom portion. The horns are supported on the insulating base of porcelain. As shown in figure, one horn connection goes to the apparatus to be protected through a resistance ‘R’ and a chocking coil ‘L’. The second horn connection goes to the ground for earth connection. The resistance ‘R’ plays an important part in the circuit. It helps in limiting the follow current to a small value. Inductance of chock coil ‘L’ also helps and protects the equipment by providing high reactance (XL = 2π ftL) where ft is the transient frequency which is very high. At normal frequency the reactance XL = 2π fL is small as f is only 50 Hz. Hence, chock coil does not allow the transients to enter the apparatus to be protected.
Working: The gap between the horns is so adjusted that normal voltage and frequency does not produce arc between the horns. The gap acts as an insulating media. But when over voltage occurs due to surges or transients, the voltage is sufficient to break the insulation of the air-gap and spark (arc) is produced. The air in the gaps heated up and hence goes up and speeded up due to magnetic effect as shown in the figure, the arc moves in stage 1, stage 2, stage3. At position 3, the distance is much more and the surge voltage cannot maintain the arc and it vanishes and normal condition is brought into the circuit. This way the equipment is protected from a voltage surge. The excess charge is conducted through portion 2 of the horn and goes to earth.
Advantages:
1.    This is superior than rod-type because arc is self clearing and no chance of short circuit.
2.    R and L limit the current to small values.
Drawbacks/Limitations:
1.    Time of operation is about 2 to 3 seconds, hence not reliable.
2.    Some materials or birds may fall in the horn gap creating troubles.
3.    Due to long use, corrosion and pitting takes place hence setting between the horns for proper air-gap is disturbed and hence performance is affected.
Uses: As said earlier its uses are limited due to unreliability and used for backup protection with main arrestors.

3.   Multi gap Arrestor: This type is used for power lines voltage not exceeding 33 kV.   
Construction: This arrestor is superior than the rod-gap and horn type arrestor. There  are arc (air) gaps between A, B and C. And shunt resistance is connected between B and C etc. are made from the last C connection goes to earth via series resistance. The cylinders A, B C etc. are made of zinc alloys and are separated by gaps and insulated from one another. Cylinder ‘A’ is connected electrically to the H.V. line as shown 33 kV. The last ‘C’ cylinder connection goes to earth via series resistance. By introducing series resistance the degree of protection against travelling waves is reduced but this is compensated by connecting shunt resistance between B and C.
Working: Under normal working voltage (say 33kV) ’B’ is at the ground potential, hence series gaps are open and no arcing between the gaps is possible. If now over voltage such as transients or surges are developed this very high voltage is sufficient to produce arc between gap A and B. This surge heavy current will follow the straight through path to earth via shunted gap B and C instead of alternative path through shunt resistance. When sure is over the arc B to C go out and at all if any current persists it is limited by these two resistances which form a series circuit. This current is too small to maintain the arc between A and B. In this way the normal conditions are re-stored and system functions on normal working voltage. The equipment is thus protected from over voltage.
Use: These are suitable for the power line equipment up to 33 kV.
4.    Expulsion Type Arrestor: The other name of the arrestor is “Protector Tube”. This arrestor is used on the power lines up to 33 kV. As the name suggests the gases formed during its operation are expelled from he tube through a vent.                                   
There are two gaps provided one is ‘rod gap’ and the other gap is in the fibre tube. The first gap is external gap and second is the internal gap. Bothe these gaps are in series. The external gap is similar to the rod gap arrestor connected to the conductor. The lower connection goes to ground (earth). The fibre tube encloses these two metal electrodes in which second gap is present. For 3-phase lines such three units are required connection of one unit is shown is the figure.

Working: Under the normal working conditions both gaps appear and act as insulators and no arc if production in normal conditions. But on the voltage surge a tremendous voltage is produced an arc is strict in the upper gap between the rods. The arc is also produced between the electrodes inside the fibre tube (i.e. in second gap). A lot of heat is produced due to high surge current. This heat vaporizes some of the fibre material on the tube and a neutral gas is produced. This gas is an un-ionized mixture of water vapor and decomposition product of fibre. A very high pressure is built up in the tube gap due to this gas formation in a very short time. This is expelled through the lower hollow electrode. As the gas leaves the tube violently, it carries away the ionized air around the arc. The effect is so strong; the arc is extinguished at current zero state and does not restrict.
This arrestor is superior to the previous types.

Advantages:
1.    Cost is cheap.
2.    Installation is very easy.
3.    The re-striking possibility of the arc is nil.
Drawback/Limitations:
1.    Volt/Ampere characteristic of this arrestor is poor and hence not used for costly equipments.
2.    Life is short due to consumption of fibre of the tube if the strokes are repeated.
3.    This arrestor cannot be mounted in an enclosed equipment due to gas discharges during operations.
Use: This is suitable for power lines and equipment rated up to 33kiV.
These are used to prevent flash-over of line insulators, isolators and bus-insulators..

5. Thyrite Disc-Valve Type Arrestor: These are suitable on High Voltage Power Lines. This is non-linear diverter.
                                   
Construction: The unit consists of spark gaps in series and also the assembly consists of a series of electrodes, some of which are flat and the others are specially shaped designs with pressed out projections.
The resistance elements are generally made up in the form of blocks compose of small crystals, silicon carbide bound together by means of an inorganic binder, the assembly being heat treated in an oven. Both assemblies i.e. of spark-gap and resistors are accommodated in series within a completely tight porcelain housing. The housing is perfectly sealed so that moisture, humidity not to enter inside. These arrestors are classified as Ii) Station type, (ii) Line type, (iii) Distribution type.
The voltage distribution across the gaps is linearised by means of additional resistances dlements called as grading resistors.
The assembly of grading resistances, spark gaps and non-linear resistances which are housed in the air tight porcelain are shown in the figure, whereas, connection of line, arrestor and earth is shown in the figure.
The specialty of non-linear resistance is such that they offer a high resistance to the current when normal system voltage is applied but very low resistance to the high value surge currents so that surge current is quickly passes through these resistances to the ground.
Working: Under the normal conditions the normal line voltage is insufficient to break the air gaps and no arc is produce and equipments work safety. On the occurrence of very high voltage due to transients or surges breakdown of series gaps takes place. The non-linear resistance offers a low resistance path to the surge current and it passes to the earth within a very short time. The arc vanishes does not re-strike back over the line. When the surge is over, the resistances offer a very high insulation (resistance) to the normal supply voltage of the system and stop the flow of current.
Advantages:
1.    Provide very reliable and effective protection to the equipment like cables, transformers and other equipments.

Breakdown voltage under surge condition
2.    The impulse ratio = --------------------------------------------------------------- is practically unity.
                                             Breakdown voltage under low frequency condition
3.    Speed of operation is very high (operation overs in less than one second).
4.    It sparks over at a predetermined voltage.
5.    They dissipate surge energy.
6.    They discharge high frequency surges without any change in spark-over characteristic.
Drawbacks/Limitations;
1.    They may fail to check the surges of very steep wave front from reaching the terminal apparatus.
2.    If moisture enters in the loose their performance.
Uses: To protect important equipment in power stations operation on voltage up to 22kV and higher. Used in the station, handling voltages up to 66 kV.
SURGE ABSORBERS
Sudden rise in the voltage for a very short period on the power system is known as a voltage surge on transient voltage. When lightning struck a line; the surge rushes along the line just as flood of water along a narrow valley.
The lightning introduces a steep fronted wave. Steeper the wave front, more rapid is the build-up of voltage at any point in the network. The voltage surge is generally specified in terms of rise time t1 to react and the time t2 to decay to half of the peak value (Em/2) if the t1 = 1μsec, and t2 = 50µsec. The surge is specified 1/50 μ-sec. The travelling wave damages the terminal apparatus. The damage depends upon the amplitude of the surge (i.e. Em) and also upon the steepness of the wave front (i.e. if t1 is very very small).
                                 
If, purpose of installing a “surge absorber” is to reduce the steepness of the wave front of the surge wave.
Surge absorber is therefore a protective device which reduces the steepness of wave front of a surge by absorbing surge energy.
Surge Absorber
Surge Diverter/Lightning Arrestor.
1.    Absorbs the surge energy to eliminate the surge and to protect he equipment.
1. Diverts the surge to the earth and eliminate the surge to protect the equipment.
2.    Construction very simple and less costly.
2. Construction not so simple but some what  costly.
Let us study some of the surge absorbers:
1.    Condenser surge absorber,
2.    Chock and resistance surge absorber.
3.    Ferranti surge absorber.

1. Condenser Surge Absorber:                                   
 Capacitive reactance XC = 1/2πfC is large and hence no current flows from line to earth at normal voltage and normal frequency of the line.
Bus when over voltage appears due to transients or surges due to the high frequency of the surge voltage XC becomes very very small and shorted and thus immediately the current (energy) passes to the ground. Hence, capacitor absorbs surge energy and allows it to dissipate in the ground and the equipment like transformer windings are protected from surges.

2. Chock and Resistance Surge Absorber:                                       
In this type of absorber, a resistance and inductor coil connected in parallel forming a series circuit of line, R and L and the equipment (transformer).
At the normal conditions and power frequency XL(=2πfL) is small. But in case of surge voltage developed in the line XL becomes very large and the current passes through the resistance where he energy is absorbed (I2Rt). Thus, the surge energy is dissipated in ‘R’ to produce heat.
3. Ferranti Surge Absorber: This is the most modern type of absorber. It consists of an air-cored inductor connected in series with each line and surrounded by a grounded (earth). This sheet is called as dissipater. The sheet is thus magnetically coupled to inductor but electrically isolated from it by air.
This arrangement acts as a air-cored transformer whose primary is an inductor coil and metallic dissipater is a short circuited secondary of a single turn. Whenever, the travelling wave is incident on the surge absorber, the energy contained in the wave is dissipated in the form of heat generated in the dissipater sheet (i) due to current set up in it by ordinary transformer action and (ii) by eddy currents. The steepness of the wave front is also reduced because of the series inductance of the inductor coil.
                                            
HARMFUL EFFECTS OF TRAVELLING WAVES AND PROTECTION AGAINST TRAVELLING WAVES
As seen in the previous articles, shielding the lines and stations by overhead ground wires provided adequate protection against direct lightning strokes and also reduces electro-statically/electromagnetically induced over voltages. But this type of protection cannot prevent travelling waves which may reach terminal equipments.
The travelling waves can cause the following damages:
1.    Insulation of the windings may be damaged due to internal flash over by the high peak (Em) voltage of the voltage surge.
2.    Inter-turn insulation of transformer may be damaged due to steep front of the surge wave causing internal flash over.
3.    Insulators of the terminal equipment may be damaged due to external flash-over by the high peak (Em) surge wave.
4.    Resonance and high voltages resulting from the steep fronted wave may cause internal/external flash-over of an unpredicted nature causing building up of oscillations in the electrical equipments.
Hence, it is absolutely necessary to provide some protective device at the stations or substations for the protection of the equipment against the travelling waves caused by lightning. The protective devices used for this purpose are:
i)              Road gap lightning arrestors.
ii)             Arcing horns across string insulators.
iii)            Different types of lightning arrestors or surge diverters/absorbers.
iv)           Earthing screens.
v)            Overhead ground wires which have been studied in the previous articles.
INSULATION CO-ORDINATION
For each system voltage basic impulse insulation level has been fixed by most of the National and International Standers. The major substation equipment, viz., transformers, breakers, isolating switches, current transformers, potential transformers, are manufactured for the same insulation level, except where transformers may be manufactured for a lower step of the same insulation level in consideration of the economy possible. Sometimes, when the lightning arrestors are installed right on the terminals of the transformers. Sometimes, when the lightning equipment may fall outside the protective zone determined from the withstand level of the equipment, discharge voltage of the lightning arrestor and the distance between the equipment and the lightning arrestor and the equipment may be arranged with one step higher B.I.L. In general, four levels of insulation in a station are recognized; the bus insulation is highest, the post insulators, breakers, switches etc., next lower; the transmission former next lower; and the lightning arrestor is the lowest. The percentage of margins between these different levels are not uniform but can be attained on a reasonably constant basis by the use of commercially available components of equipment. With bus insulation, for example, it is a simple matter in high voltage station to add one or two insulator units in a strain bus without significant increase in cost. The insulation of the disconnecting switches is brought to a satisfactory level by usually using the next higher rated switch above the insulation class of the system. The transformers are insulated for the lowest level that can be protected with adequate margin of safety above the level of the arrestor which is required to withstand 50 cycle over-voltage of the system not only in normal service but also under fault conditions. The co-ordination of insulation as practiced by the AG and ESC in station equipment of various system voltages is shown in the following Table: 
Impulse kV
Rated System Voltage kV
Bus Installation
Switch and post Insulation
Transformers
Circuit Breakers
23
34.5
69
115
138
330
330
420
565
865
1000
1665
225
235
440
590
590
1475
150
200
350
550/450
550/450
1175
150
200
350
650
650
1175
The value for transformers and circuit breakers are with-stand values while those for bus and switch insulators are critical values.
Standard insulation levels as per practice of M.S.E.B. India.
System Voltage kV rms
Impulse Strength of Transformer Winding 1/50 μS Full Wave kV peak
Dry Flash Over Voltage kV rms
Wet Flash Over Voltage kV rms.
230
900
530
385
110
550
320
240
66
350
260
180
33
200
170
120
The following characteristics shows the basic concept of co-ordination of insulations.
                          
(b) Power system equipment
The lightning arrestor will spark-over at a voltage less than the insulation withstand voltage of the equipment i.e. to say the protective device must have a lowest protective level (B) characteristic than that of the equipment characteristic (A) i.e. characteristic (B) is below (A).
                            
EXERCISE
1.    Explain lightning phenomenon.
2.    Write a note on insulation co-ordination.
3.    What are harmful effects of travelling wave.
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