Abstract:
A superconducting short circuit current limiter ( 40   a ) for an alternating current system includes AC reactors having superconducting direct current bias windings ( 4   a   , 4   b ) that at normal conditions maintain the reactor&#39;s cores in saturated state. There are at least two AC coils ( 3   a   , 3   b ) for each phase operating at opposite half periods or at both half periods. The reactor may also have an additional feedback coil ( 42   a   , 42   b ) that at least partly compensates for the bias field of the superconducting coil at fault conditions enhancing a limiting capacity of the reactor. The reactor&#39;s core can be configured for decreasing its dimensions and mass as compared with known devices and for decreasing core losses. High voltage/high current devices include several standard modules connected in series or/and in parallel. A positional relationship of the modules is defined for decreasing necessary numbers of Amp?re-turns of superconducting and non-superconducting coils.

Description:
FIELD OF THE INVENTION  
       [0001]     This invention relates to current limiting devices for AC electric grid.  
       REFERENCES  
       [0002]     In the following description, reference will be made to the following non-patent publications: 
    [1] B. P. Raju, K. C. Parton, T. C. Bartram, “A current limiting device using superconducting d.c. bias: applications and prospects,”  IEEE Transactions on Power Apparatus  &amp;  Systems , vol. 101, pp.3173-3177, 1982.     [2] J. X. Jin, S. X. Dou., C. Grantham, and D. Sutanto “Operating principle of a high T-c superconducting saturable magnetic core fault current limiter”.  Physica C,  282, Part 4: p. 2643-2644, 1997.     [3] J. X. Jin, S. X. Dou., C. Cook, C. Grantham, M. Apperley, and T. Beals, “Magnetic saturable reactor type HTS fault current limiter for electrical application”.  Physica C,  2000.341-348: p.2629-2630.     [4] V. Keilin, I. Kovalev, S. Kruglov, V. Stepanov, I. Shugaev, V. Shcherbakov, I.Akimov, D. Rakov, and A. Shikov, “Model of HTS three-phase saturated core fault current limiter”,  IEEE Transactions on Applied Superconductivity , vol.10, pp. 836-839, 2000.     [5] R. F. Giese, “Fault-current limiters—A second look,” Argonne Nat. Lab., Argonne, USA Mar. 16, 1995.    
 
       BACKGROUND OF THE INVENTION  
       [0008]     Fault current limiters (FCL) are expected to be among the first and most important power applications of high temperature superconductors (HTS). The advantages of HTS-FCL as compared to conventional circuit breakers, used world-wide in national electricity circuits, are their quick response and fast recovery, relatively low energy dissipation, tolerance to large fault currents and the possibility for virtually unlimited number of operations.  
         [0009]     More particularly, the present invention relates to current limiting devices based on a superconducting coil with saturated core. Such a device comprises at least two coils with ferromagnetic cores for each phase connected in series with a load. On both cores there are superconducting bias coils connected to a DC power supply. At normal state the bias coils saturate the cores and the impedance of the current limiter is very low. When the load decreases, the current sharply increases and the cores are driven out of saturation at alternate half-cycles. As a result the impedance of the current limiter builds up and limits the increase of the current.  
         [0010]     In U.S. Pat. No. 3,671,810 incorporated herein by reference this principle has been proposed for transient current limiting in electronic circuits. U.S. Pat. No. 4,045,823 incorporated herein by reference to K. C. Parton et al. describes a current limiting device for a power alternating current system. The current limiter has for each phase a pair of saturable reactors with the coils wound in opposite directions relative to superconducting bias coils. U.S. Pat. No. 4,117,524 incorporated herein by reference also to K. C. Parton et al. describes a modified form of current limiter having a screen of conductive material surrounding the bias winding to shield it against the alternating magnetic field. In this patent, one common bias coil is used for two reactors. Raju et al. [1] realize their current limiting device with a superconducting bias coil operating in a liquid helium bath and demonstrate its efficiency. U.S. Pat. No. 4,257,080 (Bartram et al.) incorporated herein by reference describes a further improvement of this current limiting device by placing the common bias coil on the central limbs of three or six cores of a three-phase reactor.  
         [0011]     Several laboratory scale models of saturable core current limiters have been realized with superconducting coils made of high-temperature superconductors (HTS) [2, 3, 4]. These one-phase [2, 3] and three-phase [4] devices were built according the design proposed in the above-mentioned US Patents all of which are incorporated herein by reference.  
         [0012]     The current limiter with saturated core has decisive advantages as compared with other superconducting current limiters: 
        its current limiting effect is not dependent on transition of the superconducting element to normal state, i.e. superconducting state is maintained all the time and no recovery time is necessary to return to ready state after fault. Moreover there is no dissipation of energy concerned with transition of the superconducting element to normal state;     the superconducting element is a coil made of standard superconducting wire manufactured on an industrial scale.     the superconducting coil operates in DC mode and is exposed to low AC magnetic fields.        
 
         [0016]     The known designs of FCL with saturated core have the essential shortcomings that prevent the development and realization of this type of FCL. Its weakest points are the large weight and dimensions that are about twice the weight and dimensions of a transformer of the same power [5]. Also, in known FCLs of this type the impedance of the AC coils does not reach its maximum possible value because the bias coils produce the magnetic flux in the cores that reduces the impedance of AC coils. This feature is necessary at normal conditions but it has a negative effect at fault conditions. Furthermore, at fault conditions the alternating magnetic field of the AC coils affects the superconducting bias coil, decreasing its critical current. In known designs, a cryostat with bias coils is placed in the window of the core thus increasing its size.  
         [0017]     A first objective of the present invention is to reduce the mass and dimensions of the ferromagnetic core of a current limiter having a saturated core, thereby reducing also the losses of the device.  
         [0018]     A further objective of the present invention is to propose a new design of the current limiter with saturated core where the bias field is compensated fully or partially at the time of a fault.  
         [0019]     Yet another objective of the present invention is to provide a modular design of current limiter with saturated core that can be manufactured at low cost.  
         [0020]     Additional objectives of the present invention are: 
        to reduce the alternating magnetic field on the superconducting bias coils thus preventing a degradation of their critical current;     to propose a design that leaves sufficient room for the cryostat of the bias coils without increasing the core size; and     to ensure the possibility of adjusting the limited value of the fault current according to system requirements.        
 
       SUMMARY OF THE INVENTION  
       [0024]     These objects are realized in accordance with a first aspect of the invention by a current limiting device for an AC supply, said current limiting device comprising for each phase of the AC supply:  
         [0025]     a magnetic core,  
         [0026]     at least one superconducting bias coil for said magnetic core for biasing the core into saturation at normal conditions, and  
         [0027]     two series-connected AC coils adapted to be connected in series with a load;  
         [0028]     said magnetic core comprising a pair of elongated rod-shaped magnetic limbs, and  
         [0029]     each of said AC coils being placed on a respective one of said limbs and being wound so as to produce magnetic fields of mutually opposing polarities so that in use during successive half cycles of the AC supply one of the AC coils produces a magnetic field that opposes a magnetic field of the bias coil.  
         [0030]     There may also be optionally provided feedback coils that are energized at the moment of increasing voltage on the FCL and fully or partially compensate for the magnetizing effect of the bias coils, thus increasing effective permeability of the cores such that the impedance of the AC coils increases. The feedback coils can be energized, for example, from an independent DC power supply controlled by voltage drop on FCL or by a power supply connected in parallel to the FCL and including a step-down transformer and rectifier. In the latter case, the input voltage of the power supply is proportional to the voltage drop across the FCL. At normal operation, current in the feedback coils is very small and has no influence on FCL operation. At fault conditions, the current in the feedback coils increases to compensate for the magnetizing effect of the bias coils. It is important that the current in the feedback coils reaches the necessary threshold during the first half cycle after a fault event to decrease the initial rise in current. The feedback coils can be made of copper wire with relatively small cross-section because they operate for only short time (4-5 half-cycles) and the resulting heating is therefore small.  
         [0031]     An additional effect of using the feedback coils consists (as a result of increasing the core permeability) in a strong reduction of the leakage AC field that has a negative influence on the superconducting bias coil.  
         [0032]     The feedback coils allow the mass of the device to be reduced regardless of the type of core employed. To this end, in accordance with a second aspect of the invention, there is provided a current limiting device for an AC supply, said current limiting device comprising for each phase of the AC supply:  
         [0033]     at least two series-connected AC coils adapted to be connected in series with a load, said coils being placed on respective limbs of at least one magnetic core, at least one superconducting bias coil for each magnetic core for biasing the core into saturation at normal conditions, and  
         [0034]     at least one feedback coil for each bias coil for creating a magnetic flux that is dependent on a voltage drop across the current limiting device and in an opposite direction to a direction of a magnetic flux of the bias coil.  
         [0035]     In accordance with another aspect of the invention, there is provided a method for reducing mass of a current limiting device for an AC supply, said current limiting device comprising for each phase of the AC supply:  
         [0036]     a magnetic core,  
         [0037]     at least one superconducting bias coil for said magnetic core for biasing the core into saturation at normal conditions, and  
         [0038]     two series-connected AC coils adapted to be connected in series with a load; said method comprising:  
         [0039]     (a) reducing a mass of the magnetic core by: 
        i) forming the magnetic core of a pair of elongated rod-shaped magnetic limbs;     ii) placing each of said AC coils on a respective one of said limbs; and     iii) configuring the AC coils so as to produce magnetic fields of mutually opposing polarities so that in use during successive half cycles of the        
 
         [0043]     AC supply one of the AC coils produces a magnetic field that opposes a magnetic field of the bias coil; and/or  
         [0044]     (b) reducing a mass of the AC coils by: 
        i) associating with the AC coils at least one feedback coil having a 5 magnetic flux that is in an opposite direction to respective magnetic fluxes of the bias coils for moving the core out of saturation thereby allowing the number of turns or the cross-sectional area of the AC coils to be reduced.        
 
         [0046]     In order to decrease the weight and dimensions of the device, the ferromagnetic cores may have the form of elongated rods in contrast to the closed magnetic circuit in the known FCL. Thus the volume of the cores is approximately halved. At the same time the effective permeability of the rod is much less than the effective permeability of the closed magnetic circuit as illustrated by their Weber-Ampere characteristics. As a result, with the same parameters of the coil and the core cross-section, the maximal current of the current limiter with the rod core is larger. Thus the current limiter with the rod core should preferably operate so that the flux linkage does not surpass the upper knee of its Weber-Ampere characteristic thus reducing the effective impedance of the FCL. In contrast to the closed magnetic circuits, the properties of the rods are dependent on the positional relationship of the rods that has to be taken into account when designing the current limiter. By selection of the proper positional relationship of the rods, the necessary number of Ampere-turns of the AC coils and/or the bias coils and feedback coils may be decreased.  
         [0047]     Another way of decreasing the weight and dimensions of the device is to use a combined structure in which the AC coils are located on two limbs of the elongated closed magnetic circuit. By such means, there is only one core instead of the two cores typically provided in known configurations. In the configuration according to the invention, the inductance of the two AC coils is about four times as large as the inductance of one coil because both AC coils are situated in a single magnetic circuit with additive polarity. This permits use of a core of smaller cross-section and/or fewer turns in the AC coils. Each bias coil and feedback coil encloses both long limbs of magnetic circuit. This arrangement ensures minimal AC magnetic field on the bias coil and minimal AC voltage on the bias coil and on the feedback coil because almost all the AC magnetic flux is enclosed within these coils. The AC field has a strong influence on the critical current of superconducting coils and for additionally decreasing this field a conductive and magnetic screen can be placed around the bias coil.  
         [0048]     Introducing a small air gap in this closed elongated core configuration allows the FCL parameters to be adjustable. To decrease the number of Ampere-turns of the bias coil, two magnetic circuits having respective bias fields in opposite directions can be placed very close one to another thus decreasing the reluctance of the magnetic circuit of the bias coils.  
         [0049]     The proposed designs according to the invention, both that having rod cores and that having combined closed cores, give the additional advantage of leaving sufficient space for disposition of cryostats with superconducting bias coils. These advantages are tangible regardless of whether the feedback coil is used as provided for by the invention. Thus operational performance of the FCL may be enhanced by using an additional feedback coil while physical size of the FCL may be reduced by the novel magnetic structure of the invention and these benefits can be used either singly or in combination.  
         [0050]     A further realization of the invention is evident with the addition of a third central limb to the closed magnetic cores described above. The bias coil and the optional feedback coil are mounted on the said central limb. The two AC coils are placed on the outermost limbs. An additional advantage of this design as compared with those described above is the closed magnetic circuit of the bias coil and feedback coil that allows their Ampère-turns to be reduced in number.  
         [0051]     According to a further embodiment of the present invention, in order to decrease manufacturing cost of the current limiter, it is assembled with standard modules that have the optimal size for the convenience of manufacturing and installation. 
     
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0052]     In order to understand the invention and to see how it may be carried out in practice, some preferred embodiments will now be described, by way of non-limiting example only, with reference to the accompanying drawings, in which:  
         [0053]      FIG. 1  shows pictorially a prior art closed core configuration of a saturated core single phase FCL;  
         [0054]      FIG. 2  is a schematic circuit diagram showing the prior art single phase FCL of  FIG. 1  in use;  
         [0055]      FIG. 3  shows linkage-current Ψ(I AC ) curves of the saturated core FCL shown in  FIG. 1  with and without feedback coils;  
         [0056]      FIGS. 4   a ,  4   b  and  4   c  show rod shaped cores for a single phase FCL according to different embodiments of the invention;  
         [0057]      FIG. 5   a ,  5   b ,  5   c  and  5   d  show a saturated core FCL for a single phase with having a closed saturated core according to different embodiments.  
         [0058]      FIG. 6  shows a saturated core FCL according to another embodiment of the invention having two AC coils on outermost limbs and bias and feedback coils on a central limb of a closed shell-type core; and  
         [0059]      FIG. 7   a  is a schematic circuit diagram showing a single phase FCL according to the invention with independent power supply of the feedback coils;  
         [0060]      FIG. 7   b  is a schematic circuit diagram showing a single phase FCL according to the invention with power supply of the feedback coils connected in parallel with the FCL. 
     
    
     DETAILED DESCRIPTION OF THE INVENTION  
       [0061]     In the following description various embodiments are described. To the extent that many features are common to different embodiments, identical reference numerals will be employed to refer to components that are common to more than one figure.  
         [0062]     In order more fully to appreciate the benefit of the invention, it will be instructive first to consider a typical prior art single phase FCL. To this end,  FIG. 1  shows pictorially a prior art saturated core single phase FCL designated generally as  1  having a pair of closed magnetic cores  2   a  and  2   b  each supporting a respective AC coil  3   a  and  3   b . The cores further support a pair of DC superconducting bias coils  4   a  and  4   b.    
         [0063]      FIG. 2  shows schematically a circuit diagram showing the single phase FCL  1  in use. An AC supply  5 , typically from the electric power grid, is connected to a load  6  via a circuit breaker  7 . In series with the load  6  are connected the two AC coils  3   a  and  3   b  of the FCL. The respective superconducting bias coils  4   a  and  4   b  are connected to a DC power supply  10 . At any moment the direction of the bias magnetic flux  11  in one core coincides with the direction of the magnetic flux  12  of AC coil whereas the direction of the bias magnetic flux  11 ′ in the other core is opposite to the direction of the magnetic flux  12 ′ of the AC coil. Under normal conditions, the bias coils  4   a  and  4   b  saturate the respective cores  2   a  and  2   b . Under fault conditions, the AC coils  3   a  and  3   b  draw the respective cores  2   a  and  2   b  out of saturation during opposite half cycles of the AC cycle, thereby causing their average inductance to increase and thus limiting an increase of the current.  
         [0064]      FIG. 3  shows graphically in curve  21  the linkage-current Ψ(I AC ) characteristic of the prior art saturated core FCL, shown in  FIG. 1 . The curves  22  and  23  shown alongside the curve  21  are corresponding flux linkage-current Ψ(I AC ) characteristics of a saturated core FCL according to the invention and are explained in greater detail below. The amplitude of magnetic flux linkage of the coil is proportional to the amplitude of the voltage drop on the FCL. When the flux linkage is below the lower knee  29  of the curve  21  the cores are saturated and the voltage drop across the FCL is small. At fault conditions, however, the voltage drop on the FCL can be close to the voltage of the grid and the current increases. But after the lower knee  29  on the curve  21  corresponding to an unsaturated core, the magnetic flux linkage rises more steeply for a given change in current since the FCL exhibits a larger average inductance that slows the current increase for a given change in voltage.  
         [0065]     As noted above, one aspect of the invention is the use of feedback coils.  FIG. 3  also shows the characteristic Ψ(I AC )  22  of the core with the feedback coils, that fully compensate for the magnetic fluxes of the bias coils, intersects the point of origin and corresponds to the steep part only of the characteristic  21  of the core without the feedback coils. Thus the maximal current corresponding to a given flux linkage (and voltage) at fault conditions can be decreased. A given flux linkage  28  corresponds to a current magnitude  27  for the FCL without feedback coils and to a lesser current magnitude  26  for the FCL with feedback coils. When the flux created by the feedback coils is less than the flux of the bias coil, the characteristic Ψ(I AC )  24  mediates and the average inductance of the AC coils has an intermediate value.  
         [0066]     It will be understood from the foregoing that the use of feedback coils provides improved performance even when used with the prior art core shown in  FIG. 1 . Specifically, according to present invention the feedback coils can be used in any design of saturated core FCL.  
         [0067]     The use of the feedback coils allows the magnetic core design to be changed such that the mass of the core decreases. The cancellation of the bias field during a fault increases the effective permeability of the magnetic core. As a result, the core cross section may be reduced as compared to an FCL with the same primary coil impedance and without feedback coil. Three different exemplary designs will now be described.  
         [0068]      FIGS. 4   a  and  4   b  show a first design having two elongated rod-shaped cores  41   a ,  41   b  for a single phase instead of the two closed cores used in known designs (shown in  FIG. 1 ). The volume of the rod-shaped cores is about half that of the closed cores shown in  FIG. 1 . The AC coil  3   a , bias coil  4   a  and optionally a feedback coil  42   a  are mounted coaxially on the rod-shaped core  41   a . In like manner, the AC coil  3   b , bias coil  4   b  and optional feedback coil  42   b  are mounted coaxially on the rod-shaped core  41   b . Separate bias coils may be used with a feedback coil on every core (as shown in  FIG. 5   a ) or a common bias coil  4   a  and optional feedback coil  42  may be wound on both cores (as shown in  FIG. 4   b ). Use of common bias coils has the advantage of smaller induced AC voltage across the bias coils as well as reduction of the mass of the core.  
         [0069]      FIG. 4   c  shows schematically in plan view an assembly of two pairs of cores as shown in  FIG. 4   b  that are juxtaposed so that the magnetic fields of adjacent bias coils are additive. For each pair of cores only the AC coils  3   a ,  3   b  and the bias coil  4   a  are shown. In the lower part of the figure (corresponding to the core shown in elevation in  FIG. 4   b ), a single bias coil  4   a  encompasses both cores  2   a  and  2   b . The upper part of the figure corresponds to another core matching the one shown in elevation in  FIG. 4   b  and having similar reference numerals distinguished by the prime symbol (′). In this case also, a single bias coil  4   a ′ encompasses both cores  2   a ′ and  2   b ′. However, the magnetic flux of the two bias coils  4   a  and  4   a ′ are in opposite directions: one going into the paper and the other coming out of the paper so that the resulting magnetic forces are mutually attractive. The cores are shown by way of example with an open magnetic circuit, but a closed magnetic circuit may also be used.  
         [0070]      FIGS. 5   a  and  5   b  show a second design of device shown as  50   a  and  50   b  respectively that includes for each phase at least one elongated closed core  50   a  having limbs  41   a  and  41   b  each supporting a respective AC coil. The limbs  41   a  and  41   b  are coupled at opposite ends by respective magnetic arms  51  thereby closing the magnetic circuit. In the device  50   a  the magnetic circuit is closed completely, while in the device  50   b  an air gap  52  is provided. By adjusting the thickness of the air gap  52 , magnetic properties of the substantially closed core may be varied.  
         [0071]      FIGS. 5   c  and  5   d  show devices  50   c  and  50   d , respectively that are similar in arrangement to those shown in  FIGS. 5   a  and  5   b , respectively. However, whereas in the devices  50   a  and  50   b  shown in  FIGS. 5   a  and  5   b , separate AC and bias coils are wound around each limb  41   a ,  41   b  of the core, in the devices  50   c  and  50   d  separate AC coils  3   a ,  3   b  are wound around each limb  41   a ,  41   b  of the core but a single bias coil  4   a  is commonly wound around both limbs as is the optional feedback coil  42 , thus further reducing the mass of the core.  
         [0072]     Referring back to  FIG. 3 , the closed core has a much steeper Ψ(I AC ) characteristic  23  than an open core. This ensures a smaller current magnitude  25  or allows decreasing the cross-section of the core and/or number of Ampere-turns of the AC coils. The aiding connection of AC coils ensures about two times bigger inductance of both AC coils as compared with other designs because the AC coils have a common magnetic flux. The bias coil  3   a  and feedback coil  42  enclose both limbs of the core and surround both AC coils. Almost all the magnetic flux of the AC coils passes inside the core, thus the total alternating magnetic flux inside the bias and feedback coils almost vanishes and the AC voltage on these coils is very small.  
         [0073]      FIG. 6  shows a third design that includes for each phase at least one shell-type core  71  with two AC coils  3   a ,  3   b  on the outermost limbs and a common bias coil  4   a  and an optional feedback coil  42  (shown dotted) placed on a central limb  72  of the core. Magnetically, the shell-type core  71  may be considered as a closed core as shown in  FIG. 5   a  or  5   c  whose limbs  2   a ,  2   b  constitute the outermost limbs of the shell-type core  71  but having an extra limb in between the limbs  2   a ,  2   b . This design has the same advantages as the previous design. The magnetic flux of the AC coils does not pass inside the central limb of the core and thus inside bias coil and feedback coil. Actually at normal conditions there is no induced AC voltage on the bias coils because the full AC magnetic flux inside the bias coil is zero. However, at fault conditions, the bias coil is exposed to alternating magnetic fields that decrease the critical current of the superconducting bias coil and degrade its performances. The coil design has to take into account the AC fields during fault time. A conductive electromagnetic screen may to be used to minimize these fields. The 3-phase FCL includes at least three identical elements, at least one element for each phase.  
         [0074]      FIG. 7   a  is a schematic circuit diagram showing a FCL according to the first embodiment of the invention. It will be seen that the FCL includes all elements of the known FCL as described above with reference to  FIG. 5   a  and in addition includes two feedback coils  42   a  and  42   b  energized by a DC power supply  33   a . During a fault condition, the voltage drop across the AC coils  3   a  and  3   b  increases. The power supply is energized according to this voltage drop and thereby causes the current through the feedback coils also to increase. The magnetic flux  34  and  34 ′ created by the feedback coils is in the opposite direction to the respective magnetic fluxes  11  and  11 ′ of the bias coils  4   a  and  4   b , and therefore moves the whole core out of saturation. In this condition both AC coils have high impedance during both halves of cycle. As a result, the voltage drop across each AC coil is only half of the voltage drop across the FCL. This allows the number of turns of the AC coils to be decreased. In this connection, it will be noted that the inductance is given by L˜μA N 2 . The feedback increases μ thus allowing either A (core cross-section) or N (number of turns in the AC coil) to be reduced while maintaining the overall FCL impedance. Thus the feedback coil provides another way to achieve the objective of the invention of reducing core size.  FIG. 7   b  shows schematically an FCL having the same components as shown in  FIG. 7   a  but with power supply  33   b  of the feedback coils connected in parallel to the FCL or to the pair of its AC coils that are concerned with these feedback coils. In this case the feedback is realized directly. During a fault, a voltage drop on the FCL and thus on the power supply increases and results in increasing current in the feedback coils.  
         [0075]     The invention also proposes an FCL assembly having a saturated core with standard elements (modules) of a size that allows building an FCL assembly with necessary parameters by connecting a required number of modules in series and/or in parallel. Each module is an FCL as described above with reference to FIGS.  4  to  6  of the drawings. When placing the modules together it is necessary to calculate the parameters of the FCL assembly taking into account a superposition of the magnetic fluxes of the adjacent modules. This superposition can ensure a smaller amount of Ampere-turns of bias coils and AC coils. Each module can have separate bias and feedback coils or the bias and feedback coils can be common for several modules. For example, as shown schematically in  FIG. 4   c  two modules having closed cores can be placed one near the other in such a way that the magnetic fluxes of their bias coils have opposite directions. It will be understood that the bias coil has an open magnetic circuit in the elongated core configuration, so that placing two proximate modules in opposite directions has the effect of closing their magnetic circuit. In this case the reluctance of the magnetic circuit of these coils is smaller, and a smaller number of Ampere-turns is required.  
         [0076]     According to another aspect of the invention any of the core designs described with reference to FIGS.  4  to  6  can be used in a saturated core FCL or in an FCL assembly comprising such FCL modules with or without feedback coils.  
         [0000]     Example of FCL with 1 closed core for each phase  
         [0077]     This FCL assembly example consists of modules that include for a single phase one closed saturated core having two AC-coils: one coil on each leg; bias coil and feedback coil are wound around the core with AC coils. It is used as a module in the 3-phase FCL assembly.  
         [0078]     Parameters:  
                                                       Rated power   W = 1.67 MVA           Rated voltage   V = 3 kV           Rated current   I = 0.556 kA           Rated impedance   Z = 5.4 Ohm           Reactance at normal operation   X = 0.23 Ohm           Reactance at fault conditions   X = 2.2 Ohm           Steady state current at fault conditions   I SS  = 1.93 kA           Maximal fault current   I MAX  = 7 kA                      
 
         [0079]     Dimensions and masses:  
                                                           Height of the core   3.15   m           Diameter of the core   0.18   m           Mass of the core   1.4   tonne           Mass of the copper coils   0.4   tonne           Mass of the feedback coils   0.06   tonne           SC bias coil   77   kAmpère-turns                      
 
         [0080]     3-phase FCL with 1 closed core for each phase  
                                                   Rated power, MVA   5   10   15   20       Numbers of modules   3   6   9   12       Rated phase voltage, kV   3   6   9   12       Rated phase current, kA   0.556   0.556   0.556   0.556       Rated impedance, Ohm   5.4   10.8   16.2   21.6       Total mass of the cores, tonne   4.2   8.4   12.6   16.8