DC/DC POWER TRANSFORMER

Abstract: The DC/DC power transformer is an arrangement for direct transformation of high electric powers from one DC voltage level to another DC voltage level without intermediate AC voltage network. The DC voltage is today basically used for transmission of high electric powers at long distances. The DC voltage levels for these transmissions are normally high. The DC/DC power transformer allows several DC voltage levels to be used in one and the same DC voltage network. The principle for this arrangement is that the valve windings (43, 45) from one or several converter transformers (47) are connected to two valve bridges, which generate opposing cyclically variating magnetic flows in the transformer cores (44). One of the valve bridges is operated as an inverter (49) and the other as a rectifier (46) and in this manner the power is transformed from one DC voltage level (Ud1) to another (Ud2). At the high voltage levels for which the invention is intended the leakage inductances in the transformers will be high as a consequence of the insulation levels and due to this special arrangements must be made in order to commutate the magnetic energy from one phase of the transformer to another without creating great losses. The arrangement is proposed in a line commutated alternative (figure 5) and in a selfcommutated alternative (figure 4). The first utilizes a third AC voltage reference winding (A3, B3, C3 in figure 5) for this commutation. In the second alternative an external over the bridge connected capacitor (48 in figure 4) is utilized for this commutation purpose. Both alternatives may be designed galvanically insulated or in autocoupling (figure 10).

Description: DC/DC POWER TRANSFORMER FIELD OF THE INVENTION This invention relates to an arrangement for direct transformation of electric power from one DC-(=direct current) voltage to another DC- voltage. BACKGROUND OF THE INVENTION In power transmission DC-voltage is used to transmit high electric powers from production centers to consumtion centers. Since the power is generated and distributed with AC networks (1,2) it is necessary to transform the AC-voltage to a DC-voltage (U in fig. 1) by means of a rectifier (3) and on the other end re-transform the DC-voltage to an AC-voltage by means of an alternator (4) . These convertors are composed of converter transformers (5,6) and valves (7) which are connected into valve bridges (8,9). The rectifier and the inverter as well as the val- vebridges are known and described in reference 1, chapter 2 and 3. The rectifier and the inventer can be provided with filters on the AC- voltage side (10, 11) as well as on the DC-voltage side (12, 13). These filters as well as the smoothing reactor (14, 15) on the DC-voltage side are provided in order to filter harmonics in current and voltage, which are generated as a consequence of the transformation from AC- to DC-voltage and vice versa. Each rectifier or inverter consequently needs a lot of equipment which also generates a lot of losses. This has strongly restricted the utilization of High Voltage Direct Current as means of transmitting electric power. THE STANDPOINT OF TECHNOLOGY With technology known today transformation of electric power from one high voltage DC-voltage level to another high voltage DC-voltage level, the power is by means of an alternator converted to an AC-voltage and then by means of a rectifier converted to the other DC-voltage level. Another known arrangement is serieconnection of a couple of converters for increasing or decreasing of the DC-voltage level in proportion to the power supplied to or withdrawn from the AC-voltage network (compare reference 2) . Known arrangements of DC/DC transformation for low voltage application (se e.g. chapter 7 in reference 3) are not suitable for power trans- mission and high voltage equipment, due to high requirement on low noise interference, low losses and high insulation levels and the high leakage inductances in the transformers related to the high voltage levels. The known rectifier (3) and inverter (4) are drawn in fig. 1. In the figure a 12-puls configuration is illustrated with star- and delta- connected converter transformers, which is the most common configuration today. This known configuration and corresponding firing sequence is described in chapter 2.9 of reference 1. In the 12-pulse configuration the firing varies cyclically from one valve to another in each 12-pulse group (8, 9). The two series connected 6-pulse groups in each of the rectifier and the inverter are phase shifted 30° since the transformer valve windings in the upper group are star connected (16, 18) and in the lower delta connected (17, 19). Due to restrictions in maximum power handling capacity of each transformer unit the trans¬ former windings may be divided in one, two, three or six units. In each of these units there must be at least one AC-winding (20, 21) with the same phase shift as the valve windings in the respective transformer unit. The greatest quantity of transformer units and lowest power han¬ dling capacity per unit is achieved if only one valve winding and corresponding AC winding is placed in one and the same transformer unit. Since rectifying and inversion with today's power technology in per- formed with line commutated valves, the firing and extinction is achieved only with certain firing angle, , and extinction angle, 7, respectively. Commutation from the valve winding of one phase, to a valve winding of another phase will due to the transformer leakage in¬ ductance only be achieved with a certain overlap angle, u. Due to these a certain phase shift between the voltage and the current is created during the rectification and the inversion processes. This im¬ plies in a deficit of reactive power as described in reference 2. In order to compensate for this it has become useful to provide the con¬ verters not only with ac-filters (10, 11) but also with shunt capacitor banks (22, 23) for generation of reactive power. The DC-current control is an essential function of the known DC-transmission. The line direct current (I in fig. 1) in the known DC voltagetransmission is control¬ led by the DC voltages in the converter stations through the formula: I, = Line DC-current d U, = DC-voltage in rectifier U, - DC-voltage in inverter R = Line resistance The DC-voltages are controlled by the firing and extinction angles and the tap changers in the way described in chapter 7 of reference 4. AIM AND PRINCIPLE CHARACTERISTICS OF THE INVENTION This invention describes an arrangement and related couplings for direct transformation of electric power from one DC voltage to another. The arrangement is composed of an inverter bridge (24) , converter transformers (25) and a rectifier bridge (26) , in which the firing se¬ quence of the valves (27) is adjusted, so that both bridges generates variating electromagnetic fields of opposing polarity in the trans- former cores with related windings (25). If the converter transformers in the known converters are provided with two galvanically isolated valve windings (28 resp. 29, 30 resp. 31), on all phases, where the known arrangement only has one valve winding (16, 18, 17, 19) these valve windings can be connected to two independent bridges (24 resp 26) . These independent valve bridges can now follow two different cyclic firing sequencies. By arranging the phase shift between the valve windings from the two bridges, opposing magnetic field can be created in the core(s) of the converter transformer(s) (32, 33). By in this manner driving one of the valve bridges as an in- verter (25) and the other valve bridge as a rectifier (26) , power can be transformed from one DC-voltage level (U ,_. ) to another (U,_) . The relation in voltage and current is thus determined by the turns ratio in the two valve windings from the two valve bridges. If line com¬ mutated valves are used the firing and extinction must be achieved with certain delay angles in relation to an AC reference voltage wind¬ ing. An AC voltage winding (34, 35) can be connected to each phase and transformer unit for this purpose. This winding is connected to an AC voltage reference net (36), with one busbar per phase. The aim of this AC-voltage reference net is to form a voltage reference against which the delay angles of the rectifier and inverter bridges are referred. Sufficient power for the AC voltage reference may be ex¬ ternally generated or supplied by a three phase synchronous generator (37). The synchronous generator may also by itself or in parallel with shunt capacitor banks (38) provide reactive power corresponding to the reactive power consumtion of the line commutated DC/DC power trans¬ former due to the delay angles. AC-filters (39) may also be connected to the reference net in order to take care of current harmonics gener¬ ated during the rectification and inversion processes. THE PRINCIPLE OF THE INVENTION The principle of the known bridge coupling is that an AC voltage con¬ nected to a transformer core will provide a cyclically variating magnetic field. This variating magnetic field generates, through the turns ratio, voltages in the other windings connected to the same core. The cyclic firing sequence in the valve bridges (8, 9) will result in DC voltages with a certain ripple over the valve bridges. The smoothing reactors (14, 15) inhibit this voltage ripple to pass on to the DC lines. When the coupling is provided with a load, current is withdrawn. The current is transformed over the transformer core according to the principle of ampere turns ratio balance. This process is more detaily explained in chapter 3 of reference 1. The principle of the invention described herein is that the valve wind¬ ings of the inverter bridge (24) , through its cyclic firing sequence in the same manner as the known inverter may generate a cyclically variat¬ ing magnetic field in respective transformer core (32, 33). By means of a co-variating cyclic firing sequence in the rectifier bridge (26) the thus induced voltages will build up a DC voltage (ϋ. over the rectifier bridge, with generates an opposing magnetic field in the core. When the rectifier bridge is provided with a load, current will de transformed according to the principle of ampere turns ratio balance between primary and secondary windings of a transformer. It self commutated valves are utilized, no further windings are needed, since the cyclic sequence with forced commutation will lead to that currents are commutated from one phase to another according to a predetermined frequenc . A self commutated inverter for conversion of high voltage DC to three phase AC is known and described in chapter 6.1 of reference 3. In figure 6.1 of this reference the inverter is shown. Such a bridge cou¬ pling may be used as inverter bridge (42) in a self commutated DC/DC power transformer as illustrated in figure 4. In the known bridge cou¬ pling two opposing thyristors are always on. In the bridge coupling described here, on the contrary, only one thyristor in each three pulse group shall be on at the same time. Through the cyclic firing and ex- tinction sequence of the thyristors (G11-G16) : Gil => G12 ***■ > G13 ***■ > G14 **** > G15 **** > Gil ■*** .... a variating electromagnetic field is generating by the valve windings (43) in the transformer wind¬ ings and its core (44). The diode valves (D11-D16) commutates the current when an opposite valve has extinguished. When for example the thyristor valve Gil extinguishes the current will due to the trans¬ former leakage inductance continue through winding Al. The voltage in the blocked direction of the thyristor valve will therefore rapidly raise until the diode valve D14 starts to conduct. A commutating volt¬ age has been built up which commutates the current through the win- ding. The valve windings (43) from such an inverter (42) may be winded on the same transformer core (44) as the valve windings (45) connected to a rectifier (46) built up of diode valves (D21-D26). The inverter in the above described manner generates an electromagnetic field, which induces voltages in the valve windings (45) of the rectifier. By means of the diode valves (D21-D26) in the bridge coupling (46) these volt¬ ages are rectified. The firing and extinction sequence of the inverter is designed so that the thyristor valves (G11-G16) will be extinguished and fired in a cyclic sequence, as shown in figure 3, where: T - Time of a cycle F — Firing signal E - Extinction signal ty Overlap - — • T (p.u.) U -, U -., U_- - Phase voltages in inverter valve windings (p.u.) *A9' ^R2' ^ f ? ~ ^ ase voltages in rectifier valve windings (p.u.) U., U , U-, - Phase currents (p.u.) Two valves connected to different transformer windings are always on, T e.g. in time interval (0 - -?) the Gil connected to Al and the G16 con¬ nected to Bl are on. The voltage over the inverter bridge (II , ) will distribute uniformly over these windings. If we first regard the inter- T val outside the commutation, i.e. (LL, - 7*), the whole DC current will flow through both valve windings Al and Bl and be transformed by ampere turns ratio balance to valve windings A2 and B2 respectively. Since positive voltage is created in the connection point of A2 and currents flows in this direction, the diode valve D21 will conduct in the forward direction. The diode valve D26 will conduct current into valve winding B2 from negative polarity. A positive voltage (II „) is thus created over the rectifier bridge. The commutation process for the self commutated DC/DC power transformer is most easily described by an T T example. We regard the interval {--, -- + υ_ when the current is com¬ mutated from thyristor valve G16 to thyristor valve G12. G16 is ordered to extinguish and a firing signal is emitted to valve G12.The valve windings Bl and B2 will continue to conduct current in the same direc¬ tion as before due to the leakage inductance of the transformer. The voltage over valve G16 will therefore increase rapidly in the blocking direction, until the diode (D13) of the opposite valve starts to con¬ duct. Then a voltage is built up over the valve winding opposing the current flowing through it. This voltage will de-commutate the current through the winding. At the same time the positive voltage over valve winding CI will increase the current through this winding with a current derivative determined by the relation between applied commutating vol- tage and the transformer leakage inductance. When the entire current has commutated over from Bl to CI the diode valve D13 extinguishes. Since the current extinction of the bridge current (I 1 ) happens almost momentarily, while the current increase is gradual, a sawtand formed ripple is created in the bridge current of the inverter (I, _. of figure 3) . The same current changes which has occurred on the inverter valve winding will due to the ampere turns balance also occur in correspond¬ ing windings in the rectifier. Here the current only commutates between valves in the same direction. The bridge current in the rectifier (I ) will therefore not present a corresponding ripple. During the commutation process, the commutating voltages are not trans¬ ferred to the rectifier bridge. A sixpulse ripple in voltage will therefore occur in the rectifier (U,_ in figure 3) . In order to isolate this voltage ripple from the DC-line a smoothing reactor (49) may be placed inside the DC filter (51) . When the thyristor valve G16 extinguishes and G12 is fired a closed current loop is formed on the rectifier side over the diode valve D26, the valve windings B2 and C2 and diode valve D22. The current will only flow in this loop until the valve winding B2 has de-commutated the current to winding C2. Then the diode valve D26 extinguishes. Thus the commutation is completed. The turns ratio of the selfcommutated DC/DC power transformer N. : N„ determines the relation between the bridge voltages of the rectifier and the inverter II _. : U, ? and the bridge currents I- • I. _. , where b bl N- - number of turns in the valve winding of the inverter (43) and N„ - number of turns in the valve winding of the rectifier (45) . The inverter side DC line current, I ,- , is determined by the average value of the bridge current The rectifier side DC line voltage, U,„, is determined, by the average value of the bridge voltage U d2 - U B2 (1 - 3 V T ) " The effective turn ratio of the DC/DC power transformer is therefore a function of the load (-U : U, 2 - I _ : I,. - N- : N„ (1 - 3t /T) . The principle for the firing and extinction of the line commutated DC/DC power transformer is illustrated in figures 5 and 6. A schematic circuit diagram for a six pulse group is given in figure 5, with the thyristor valves of the rectifier (T21 - T26) , the valve winding of the rectifier (A2, B2, C2) , the inverter thyristor valves (Til - T16) , the inverter valve windings (Al, Bl, CI) and the windings to the AC voltage reference (A3, B3, C3) . The letters in these designations determines the phase of respective winding. The firing sequence of the sixpulse group of the line commutated DC/DC power transformer is shown in figure 6. The control pulses for the thyristor valves connected to the inverter are indicated by Til = * ... ***■ T16. The control pulses show the time interval when a valve shall be on and provided with firing pulses as soon as the blocking voltage be- comes positive. The currents through the to the inverter in a star con¬ nected valve windings are denominated I . - I 01 , I .. The control pulses Al, Bl ul for the thyristor valves connected to the inverter are indicated by T21 ~> ... => T26. The current through the to the rectifier in delta con¬ nected valve windings are denominated I -, I _, I_„. The differences between these currents corrected with respect to turns ratio are the ampere turns differences which each phase of the AC windings must com¬ pensate for. These AC currents denominated I , I R _ and I__ are shown in figure 6. The AC voltage reference currents may through Fourier analysis be regarded as a summary of a fundamental component, phase shifted 90° el after the voltage and a number of harmonics. The fundamental current component in the AC reference net represents the reactive power which must be provided to the DC/DC power transformer. The harmonics are compensated by the AC-filters connected to the AC reference net. The commutation process of the line commutated DC/DC power transformer is illustrated in figure 7. The AC voltage reference is exemplified by the phase voltage U _, which in the example in figure 5 is in phase firing of valve T14 at the instant when an angle (7 + u) remains before Y the phase-to-phase voltage U _. _. becomes zero. The commutation voltage U _. _. commutes the direct current from valve winding CI to valve wind¬ ing Al during the commutation interval "u". The DC-current through Y winding Al is demonstrated as I _. in figure 7. The valve winding of the rectifier is in the example in figure 5 phase shifted 30° el. before the inverter by means of a Yll coupling. The phase voltage U _ is thus phaseshifted 30° el before the AC reference winding voltage. The phase- to-phase voltage U 9r „ comes 30° el after the phase voltage and is consequentially in phase with the AC reference winding voltage. The commutation from thyristor valve T25 to thyristor valve T21 in the in¬ verter starts a degrees after zero passage of the phase-to-phase voltage U.-, r9 and ends u degrees later. After commutation of the DC current to the valve T21 the DC current in the rectifier will pass through valve T26 and windings C2 in series with A2 parallel to the winding B2. During the time T21 and T26 conduct only a third of I „ flows through winding A2. When the valve T26 commutes the current to the valve T22 the DC-current will pass through winding A2 parallel to windings C2 in series with B2. Then the DC-current through winding A2 will increase to 2/3 I, and so on in the way illustrated by current I . in figure 7. The current amplitude I „ is expressed in per unit valve referred to the AC reference winding side and is therefore multified with factor γ3 as turns ratio factor for delta connected windings. The differential current, I _, between rectifier and inverter windings of phase A, is delivered to the AC reference winding. If the summary angle (α + 7 + u) is the same as the phase shift between these two, this current will have the smooth shape as in figure 6. Otherwise current peaks will occur in the way demonstrated by current I , Y.ll in figure 7. In order to minimize current harmonics it is therefore desirable to control the summary angle (α + 7 + u) against the same value as the phase shift between rectifier and inverter valve windings. DESCRIPTION OF THE INVENTION In figure 1 is shown the known high voltage DC transmission. In figure 2 is shown the proposed arrangement of a 12 pulse line com- mutate DC/DC Power Transformer. In figure 3 is illustrated the valve voltages and currents of a self commutated sixpulse DC/DC power Transformer. In figure 4 is shown the circuit diagram of a sixpulse self commutated DC/DC Power Transformer. In figure 5 is shown the circuit diagram of a sixpulse line commutated DC/DC Power Transformer. In figure 6 is shown the firing and extinction sequence with valve currents of a 12 pulse line commutated DC/DC Power Transformer. In figure 7 is shown the valve and winding currents and voltages of a 12 pulse line commutated DC/DC Power Transformer. In figure 8 is shown the power control strategy of a line commutated DC/DC Power Transformer. In figure 9 is shown a physical configuration of the valve windings in a three phase DC/DC Power Transformer. In figure 10 is shown the circuit diagram of a 12 pulse line commutated auto DC/DC Transformer. THE SELF COMMUTATED DC/DC POWER TRANSFORMER The circuit diagram of a sixpulse selfcommutated DC/DC power trans¬ former is shown in figure 4. As already mentioned a voltage ripple is created on the rectifier side due to the commutation process. In order to isolate this voltage ripple from the dc line a smoothing reactor (49) may be connected to the valve bridge and a dc filter (51) outside the smoothing reactor. The dc-commutation with the diodes (D11-D16) on the inverter side gen¬ erates a sixpulse ripple in the current (L, in figure 3), which with a finite dc capacitor (48) will result in a certain voltage ripple also over this valve bridge. In order to reduce current and voltage ripple the dc capacitor may be designed as a filter. If two sixpul- sebridges (42) shifted 30° el between each other with respect to fi- ring and extinction sequence are series connected the voltage ripple will be reduced and its frequency doubled. The remaining voltage har¬ monics are absorbed the smoothing reactors (49, 50) . The in fig. 4 demonstrated self commutated DC/DC power transformer can only transmit power from the inverter side to the rectifier side. If power transmission is desired in both directions the rectifier bridge (46) may be exchanged to another inverter bridge (42) , provided with selfcommutated thyristors and antiparallel connected diodes, where the former are disactivated during rectifier operation. The power transmis¬ sion direction is thereby determined by which of the two bridges is activated in inverter mood through forced firing and extinction se¬ quence. The DC-filter (48) then ought to be connected to either side of the smoothing reactor depending upon power flow direction. In principle the valves in the inverter are built up of selfcommutated thyristors (G11-G16) antiparallel connected diodes (D11-D16) , which both for high voltages must be series connected, and provided with common voltage divider elements and heat sinks. A self commutated DC/DC Power Transformer built up according to the principle described here may have normal current control for dc lines as described in chapter 7 and reference 4. The current through the transformer is determined by the difference in voltage between power source net and power load net, and pulse frequency since these affect the transformer turns ratio N. : N.(1-3LL,/T) • The control system of the transformer substation ought to be provided with protections against blocking by dc line fault and other short circuits creating harmful overcurrents and overvoltages. LINE COMMUTATED DC/DC POWER TRANSFORMERS The necessary commutation voltage for the line commutated valves is most easily provided by an AC voltage reference winding connected to each transformer unit and phase. The AC voltage reference (36) gene- rates a sinusoidal flow in the core. The rectifier and inverter bridges sets their delay angles in relation to this reference voltage. In order to maintain the ampere turns balance in each transformer core (32, 33) the windings in the rectifier and inverter bridges are phase shifted, so that the valve windings from respective rectifier and in¬ verter bridges conduct as much as possible simultaneously. Then the best ampere turns balance is achieved. As a consequence of the firing, extinction and overlap angles the phase shift between rectifier and in- verter can never be completily balanced out on a transformer core. A reactive power deficit occurs that must be compensated by the AC volt¬ age reference winding (34, 35). The necessary reactive power can be supplied from a synchronous generator (36) or via thyristor- and/or breaker switched shunt capacitor banks, if necessary in combination with SVC control of known technology, described in chapter 10 of reference 4. In the presently known thyristor valves the firing angle (α) in the rectifier is normally controlled between 5° and 20". In the invert the extinction angle is normally kept over 17". Normal values of the over- lap angle are 10° - 15°. With these delay angles the summary angle (α + 7 + u) of the DC/DC Power Transformer would become between 30" and 60°. With improved firing and extinction characteristics the nominal value of the summary angle (α + u + 7) should be possible to reduce. In the example in figure 2 a phase shift between rectifier and inverter of 30° has been chosen. This is achieved by couplings Ydll and Dyll ac¬ cording to SEN 270101. In order to achieve greater phase shifts the valve windings of either one or both sides can be connected in a Z- coupling or with extended delta. By series connection of sixpulse bridges in the rectifier and inverter phase shifted in relation to each other and to the AC windings the cur¬ rent harmonics are reduced in the same manner as for the known 12 pulse converter (see reference 1 chapter 8.2), which reduces necessity for harmonic AC-filters (39). The phase and phase-to-phase voltages and different phase A transformer winding currents of the line commutated DC/DC power transformer in figure 2 are shown in figure 7. In this ex¬ ample following delay angles have been chosen α - 10°, 7 - 15° and u - 10". The valve winding currents of the sixpulse group with Ydll coupling are denominated I _ n in the rectifier and I.. in the inverter. Al γdll Corresponding AC reference winding current, I _ , equals the dif¬ ference between these currents. The valve winding currents of the other Y Dyll-coupled sixpulse group are in the rectifier denominated I . and D in the inverter I., and is deduced in the same manner as for the first Al sixpulse group. The difference between these currents, I ^ , is the Ydll corresponding AC reference winding current. The summary of I - and I.„ is the total phase current, I A , which the AC reference wind- A3 r A3 ing shall supply to the DC/DC power transformer. The fundamental com- ponent of this current is the reactive power current of the DC/DC power transformer phaseshifted 90° el after the voltage. The spikes in this current is due to that the summary angle ( + 7 + u) in this case (=35°) deviates from the phaseshift between rectifier and inverter (-30°). In order to achieve a greater phaseshift between the valve win- dings of the rectifier and inverter, the rectifier windings can be con¬ nected into a "Z" or to an extended delta phase shifter x° el before the AC reference winding. The phaseshift x can be designed freely be¬ tween 0° and 30°, through choice of number of turns between the delta and star part of the extended delta. The inverter valve winding can at the same time be connected to a delta, phaseshifted 30° el after the AC reference winding. In this manner any desired phaseshift between 30° el 60° el can be obtained. The phaseshift between the two in all other respect equal series connected sixpulse groups can be obtained by star- connection of one of the AC reference windings and delta connection of the other. This procedure is demonstrated for the autocoupled DC/DC power transformer in figure 10. The phaseshift between rectifier and inverter should, in order to minimize the current harmonics, be chosen so that it coincides with normal stationary operational value of the summary angle (α + 7 + u) . The control of the line commutated DC/DC power transformer may also be adjusted for control against nominal value of the summary angle. The control system of high voltage DC transmission is known and described in chapter 7 of reference 4. For a DC/DC power transformer with line commutated valves certain additional control parameters are to be considered due to the influence of the AC voltage reference net. Figure 8 illustrates schematically the power control of the line commutated DC/DC power transformer (54) . The cur¬ rent control of each converter is performed in the known manner. The coordination between the different current orders and the voltage of the AC voltage reference net assures that balance is maintained between incoming (P. ) and outgoing (P ) active power. The balance between the consumtion of reactive power (Q) and the generation of reactive power (Qg) provided by AC voltage reference net is controlled by the reactive power control (53) . The power order (52) is set in one of the stations, for example in the rectifier of the supplying dc-network. From here current orders to the entire dc-net are emitted. The power change may not be faster that what the reactive power control of the DC/DC power transformer permits. The current order between supplying net (I , _) and the supplied net (I , τs and the inverter of the DC/DC power transformer (I , η ) and orderl) ' order its rectifier (I , Λ ) are coordinated. Normally current orders are order set so that inverters control the voltage, while the rectifiers control the current. Increased stability on the AC voltage reference net is achieved if also the current control (55) in the inverter of the sup¬ plied ac-network is allowed to control the current (I. in the supplied dc-net. The different windings in the DC/DC power transformer (28-31, 34-35) may all be placed in one and the same transformer unit. In its most compact form, which probably only is applicable on lower powers, all windings are placed in one transformer unit. In figure 9 such a threephase threewinding transformer is shown, for example for windings 30, 31, 35 and core 33 in figure 2. Each transformer core leg (56, 57, 58) has in this transformer been provided with three windings from the same phase. The innermost windings (59A, 59B, 59C) are in this case the three phases (A, B, C) of the AC reference winding (34). The inter¬ mediate windings (60A, 60B, 60C) are in this case the three phases of the inverter valve windings (30) connected into a star. The outmost windings (61A, 61B, 61C) are the three phases of the rectifier valve windings (31) , closed in a delta. The smallest power per unit, which also means the highest number of separate units, is achieved if only one valve winding belonging to each bridges (25 resp 26) and one AC-winding (34, 35) are placed into one unit. The AC voltage reference net (36) then interconnects the diffe- rent AC windings of each transformer unit for each phase. AUTO COUPLED DC/DC POWER TRANSFORMER In reference 2 a form of series and parallel connection of inverters and rectifiers are shown which is called "D.C. voltage transformation in high tension systems". A rectifier (62) and an inverter (63) are connected in opposite direc¬ tions in a DC voltage transformation point so that the power is transformed from one DC voltage level (U...) to another DC voltage level (U, ? ) without sectionizing power. If the valve windings of the rectifier (64, 65) and of the inverter (66, 67) in this combined bridges are connected to the same transformer core (68, 69) an auto coupled DC/DC power transformer is achieved as shown in figure 10. The rectifier bridge (62) is here cascade connected to the inverter bridge (63). With this autocoupling the high voltage valve bridge only needs to be voltage wise designed for the difference in voltage (U „ - U ) and the low voltage valve bridge only needs to be current wise designed for the difference in current (Id--l - I a.„l). The result is that less costly equipment is needed, lower losses are generated as well as less reactive power is consumed as compared with basic concept. In example in figure 10 is shown how the rectifier valve windings (64, 65) are phaseshifted 45° before the inverter valve windings (66, 67) and how at the same time 30° phaseshift is achieved between the two AC reference windings (71, 71). The auto coupling is of course also suitable for DC/DC power trans¬ former with self commutated valves. References Ref. 1 E.W. Kimbark "Direct Current Transmission", Volume I, 1971 by John Wiley & Sons. Ref. 2 Kanngiesser US Patens 3 942 089 may 1976 "DC Voltage Transformation in High Tension Systems". Ref. 3 K. Thorborg "Power Electronics", 1988, Prentice-Hall International (UK) Ltd. Ref. 4 A. Ekstrόm "Kompendium i Hόgeffektelektronik" , KTH/EKC an 1988.

Claims: PATENT CLAIMS 1. An arrangement for transformation of high electric powers from one DC voltage level (U... ) to another DC voltage level (U, ? ) by means of transformers provided with valve windings (28 - 31) connected to valve bridges with several parallel bridgearms (A, B, C) . The valves are fired and extinguished in a cyclic sequence, so that the current cycli¬ cally commutates from one valve winding to another and a cyclically variating magnetic field is created in the transformer cores (32, 33) c h a r a c t e r i z e d b y, that one of the valve bridges works as a rectifier (26) and the other valve bridge works as an inverter (24) , and around one and the same transformer core is wound valve windings from the rectifier as well as the inverter with opposing magnetic fields in the transformer core and that the magnetic energy stored by the transformer core commutates from a transformer winding of one bridge arm to another according to a cyclic sequence. 2. An arrangement according to claim 1, c h a r a c t e r i z e d b y, that the rectifier bridge and the inverter bridge are connected in cas¬ cade; over the high voltage valve bridge the difference between the DC voltages is applied (/U,, - U,„/) and through this valve bridge with its valve windings passes the DC current of the higher potential; over the low voltage valve bridge the DC voltage with lower potential is applied and through this valve bridge and respective valve windings passes only the difference in current between rectifier and inverter 3. An arrangement according to claim 1, c h a r a c t e r i z e d b y, that around one and the same transformer core the rectifier and inver¬ ter valve windings are phase shifted so that the ampere turn ratio be¬ tween these to windings is to the greatest possible extent balanced under as much as possible of the conduction interval. 4. Arrangement according to claim 3, intended for valve bridges with line commutated valves, c h a r a c t e r i z e d b y, that apart from valve windings from both rectifier and inverter around each transformer core (32, 33), an AC-voltage reference winding (34, 35) is also provided in order to generate the necessary commutation voltage for commutation of the current from winding of one phase to another. This is achieved since the valves in both valve bridges are ired an extinguished with specified delay angles. The valve windings from the rectifier bridge (26) and inverter bridge (24) respectively are phase shifted in relation to the AC voltage reference winding through exter¬ nal connections in known star, delta, extended delta or other connections, so that best possible ampere turns balance is achieved be¬ tween rectifier and inverter valve windings. 5. Arrangement according to claim 1, c h a r a c t e r i z e d b y, that the cyclically variating magnetic field in the transformer core is created by that transformer windings (43) connected to a valve bridge with self commutated thyristor valves (42) is connected to a DC voltage source (U,- in figure 4) . The self commutated thyristor valves in the valve bridge are fired and extinguished in a predetermined cyclic se¬ quence, so that said variating magnetic field is created and the hereby stored magnetic energy is commutated from one winding to another via an external capacitor (48) . In other valve bridge (46) with the valve win- dings magnetically coupled to the same transformer core (44) as above, the voltages and currents induced into these windings (45) are now rec¬ tified so that the electric energy is transformed into another DC voltage (U,„ in figure 4) . 6 . Arrangement according to claim 5 , c h a r a c t e r i z e d b y, that the valve bridge connected to the DC-voltage source is made up of one (or several) 6-pulse inverter bridge (42) with cyclically extin¬ guished and fired (fig. 3) self commutated thyristors (Gil - G16) with diodes (Dll - D16) connected antiparallel to these thyristors. Both thyristors and diods can be seriesconnected into valves. The other valve bridge is a 6-pulse rectifier bridge (46) built up of diode valves (D21 - D26) . 7. Arrangement according to claim 6, c h a r a c t e r i z e d b y, that the inverter valves is built up with a common voltage divided and common cooling for both thyristors and diodes. 8. Arrangement according to claim 5, c h a r a c t e r i z e d b y, that both valve bridges are built as inverter bridges (42) , that is composed of selfcommutated thyristors in antiparallel to diodes (Dll - D16) series connected in the same valve or not. The power flow is determined by how and in which valve bridge the cyclic firing and ex¬ tinction sequence is applied.

Inventors: LALANDER MAGNUS, LALANDER, MAGNUS
Applicants: LALANDER MAGNUS, LALANDER, MAGNUS
Application year: 1990
Main classification: H02M3
IPC codes: H02M3, H02M5, H02M7