EP0216500A1 - Electromagnetic induction apparatus - Google Patents
Electromagnetic induction apparatus Download PDFInfo
- Publication number
- EP0216500A1 EP0216500A1 EP86306422A EP86306422A EP0216500A1 EP 0216500 A1 EP0216500 A1 EP 0216500A1 EP 86306422 A EP86306422 A EP 86306422A EP 86306422 A EP86306422 A EP 86306422A EP 0216500 A1 EP0216500 A1 EP 0216500A1
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- European Patent Office
- Prior art keywords
- winding
- transformer
- tap
- electromagnetic induction
- reactor
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- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F30/00—Fixed transformers not covered by group H01F19/00
- H01F30/06—Fixed transformers not covered by group H01F19/00 characterised by the structure
- H01F30/10—Single-phase transformers
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/34—Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
- H01F27/38—Auxiliary core members; Auxiliary coils or windings
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F29/00—Variable transformers or inductances not covered by group H01F21/00
- H01F29/02—Variable transformers or inductances not covered by group H01F21/00 with tappings on coil or winding; with provision for rearrangement or interconnection of windings
Definitions
- This invention relates to an electromagnetic induction apparatus which comprises a transformer and which is utilized for power transmission and distribution systems, etc., and more particularly to an electromagnetic induction apparatus which does not require the installation of a shunt reactor.
- Fig. 20 is a circuit diagram showing the single-line connection state of a substation which employs and electromagnetic induction apparatus comprising a transformer as has heretofore been utilized in a power transmission or distribution system
- Fig. 21 is a perspective view showing a practical construction in the case where the circuit in Fig. 20 is three phases.
- a primary side switching device 2 is connected to the primary winding la, a primary side transmission or distribution line 3 has one end connected to the primary side switching device 2 and the other end connected to an external circuit (not shown), and a capacitance 4 is formed between the primary side transmission or distribution line 3 and ground.
- a secondary side switching device 5 is connected to the secondary winding lb, a secondary side transmission or distribution line 6 has one end connected to the secondary side switching device 5 and the other end connected to an external circuit (not snown), and a capacitance 7 is formed between the secondary side transmission or distribution line 6 and ground.
- a tertiary side switching device 8 is connected to the tertiary winding lc, and a shunt reactor 9 has one end connected to the tertiary side switching device 8 and the other end grounded or which is star- or delta-connected in three phases. The flows 10 and 11 of "leading" reactive powers are supplied from the shunt reactor 9 to the respective capacitances 4 and 7 when the switching devices 2, 5 and 8 are closed.
- the switching devices 2, 5 and 8 are closed, so that the "leading" reactive powers are supplied from the shunt reactor 9 through the transformer 1 to the capacitance 4 of the primary side transmission or' distribution line 3 and the capacitance 7 of the secondary side transmission or distribution line 6 respectively as indicated by the arrows 10 and 11.
- the switching devices 2, 5 and 8 are opened, and the transformer 1 and the shunt reactor 9 are separated from the power system.
- Fig. 22 is a circuit diagram showing the single-line connection state of another prior-art example
- wnile Fig. 23 is a perspective view showing a practical construction in the case where the circuit in Fig. 22 is used in three phases.
- Symbols 2 - 7 denote the same constituents as those shown in Figs. 20 and 21.
- a transformer 20 has a primary winding 20a and a secondary winding 20b, a switching device 12 on the primary side is connected to the primary side transmission or distribution line 3, and a shunt reactor 13 on the primary side has one end connected to the switching device 12 and the other end grounded or which is star- or delta-connected in three phases.
- a switching device 14 on the secondary side is connected to the secondary side transmission or distribution line 6, and a shunt reactor 15 on the secondary side has one end connected to the switching device 14 and the other end grounded or which is star-or delta-connected in three phases.
- the flows 16 and 17 of "leading" reactive powers are respectively supplied from the shunt reactors 13, 15 through the switching devices 12, 14 to tne capacitances 4, 7 wnen the switching devices 12, 14 are closed.
- the switching devices 2, 5, 12 and 14 are closed, so that the "leading" reactive powers are supplied from the shunt reactors 13 and 15 througn the corresponding transmission or distribution lines 3 and 6 to the respective capacitances 4 and 7 as indicated by tne arrows 16 and 17.
- the switching devices 2, 5, 12 and 14 are opened, and the transformer 20 and the shunt reactors 13, 15 are separated from the power system.
- the transmission or distribution lines 3 and 6 are overhead lines of long distances or where they are constructed of cables even when they are of short distances, they have great capacitances 4 and 7, wnich consume "leading" reactive powers.
- the supply of the reactive powers from a power station (not shown) in a remote place results in inflicting heavy power losses on the power transmission or distribution system and spoiling the stability of this system.
- the "leading" reactive powers which the transmission or distribution lines 3 and 6 require are supplied from the substation near these lines 3 and 6 by disposing the phase modifying means, namely, the shunt reactor 9 or shunt reactors 13, 15 as shown in Figs. 20 - 23.
- Fig. 24 is an equivalent circuit diagram of the transformer 20 having the two windings as shown in Fig. 22, and Fig. 26 is a horizontal partial sectional view of the transformer 20.
- 21 indicates the primary side terminal of the transformer 20, 22 the secondary side terminal of the transformer 20, 23 a magnetic space defined between the primary winding 20a and the secondary winding 20b, 24 a leakage flux generated in the space 23 by the primary winding 20a and the secondary winding 20b, X the leakage reactance of the transformer 20 induced by the leakage flux 24, r the winding resistance of the transformer 20, and Zm the excitation impedance of the transformer 20.
- the winding resistance r can be neglected as it is sufficiently small, and the excitation impedance Zm can be regarded as being infinitely large, so that the equivalent circuit in Fig. 24 is simplified as shown in Fig. 25. Accordingly, the shunt reactors (reactances connected in parallel with the power transmission or distribution system) do not exist equivalently.
- the equivalent circuit of the transformer 20 is expressed by only the leakage reactance X as shown in Fig. 25, so that the connection of the respective transmission or distribution lines 3 and 6 to the terminals 21 and 22 corresponds to connecting "a reactor whose reactance is X" in series with the power transmission or distribution system.
- 25 indicates the primary side terminal of the transformer 1, 26 the secondary side terminal thereof, and 27 the tertiary side terminal thereof.
- the prior-art electromagnetic induction apparatus in the substation is equipped with the shunt reactor 9 or shunt reactors 13, 15 as the phase modifying means for compensating the "leading" reactive powers which are consumed by the capacitances 4, 7 between the respective transmission or distribution lines 3, 6 and ground. Therefore, it has nad several problems to be explained below:
- This invention has been made in crder to solve all the problems as mentioned above, and has for its object the provision of an electromagnetic induction apparatus which is so constructed as to have the function of supplying "leading" reactive powers without the installation of a shunt reactor, thereby to reduce the space and to lower the power loss.
- Another ooject of this invention is to make the capacity of an equivalent shunt reactor which functions to supply "leading" reactive powers variable.
- An electromagnetic induction apparatus comprises a short-circuit winding which is electromagnetically coupled to at least two windings.
- An electromagnetic induction apparatus in another aspect of performance of this invention comprises a reactor winding which is electromagnetically coupled to at least two windings including a tap winding and which is inserted between one end of the tap winding and a tap.
- two windings operate as an ordinary transformer, while a leakage flux appears in the magnetic space between the two windings and a short-circuit winding, and it equivalently functions as a shunt reactor, to supply "leading" reactive powers to transmission or distribution lines and capacitances.
- a tap voltage whicn is lower than tne open-circuit voltage of a reactor winding is forcibly applied from a tap to the reactor winding, to generate a desired magnitude of leakage flux between the reactor winding and a tap winding.
- Fig. 1 is a circuit diagram in a single-line connection state showing the embodiment of this invention as a transformer which has, for example, three windings
- Fig. 2 is a perspective view showing a practical construction corresponding to Fig. 1
- Fig. 3 is a horizontal partial sectional view corresponding to Fig. 2
- Fig. 4 is a circuit diagram showing in a single-line connection state a case where the transformer in Fig. 1 is applied to a substation
- Fig. 5 is a perspective view showing a case where tne circuit in Fig. 4 is used in three phases
- Fig. 6 is an equivalent circuit diagram corresponding to Fig. 1, Fig.
- FIG. 7 is a perspective view showing an embodiment in which the transformer is constructed of a core type transformer
- Fig. 8 is a horizontal partial sectional view showing an embodiment in which a magnetic space is formed of a gapped core
- Fig. 9 is a circuit diagram showing a single-line connection state in the case wnere an embodiment having a switching device added to a short-circuit winding is applied to a substation
- Fig. 10 is a perspective view showing a case where the circuit in Fig. 9 is used in three phases
- Figs. 11 and 12 are horizontal partial sectional views respectively showing the states in which the switching device in Fig. 9 is opened and closed.
- la-lc, 2-7, 10 and 11 indicate the same portions as in the prior art examples stated before, and 1A indicates a transformer corresponding to the transformer 1.
- the core of the transformer 1A is denoted by ld and S is a short-circuit line which short-circuits both the ends of the tertiary winding lc and due to which the tertiary winding lc becomes a short-circuit winding.
- a leakage flux 18 is induced between the tertiary winding lc and the primary winding la or secondary winding lb by the short-circuit current of the tertiary winding lc, and tnougn not shown, such a leakage flux is also generated between the primary winding la and the secondary winding lb.
- the leakage flux 18 passes through a magnetic space 19 which is illustrated only between the secondary winding lb and the tertiary winding lc nere.
- a switching device 29 added to the short-circuit line S may well be connected between one end of the tertiary winding lc and ground by leading the terminal of the tertiary winding lc out of the transformer 1A as shown in Fig. 9, or between the lines of the tertiary winding connected in three phases.
- a power source V 0 such as a power station (not shown) or the like is connected to the primary winding la, and a magnetic flux 18A is generated in the core ld by the power source V 0 when the switching device 29 has been opened.
- the tertiary winding lc falls into an unshorted state, and a snunt reactor function vanishes.
- the switcning device 29 is closed as depicted in Fig. 12
- the tertiary winding lc serves as the short-circuit winding and gives rise to the shunt reactor function, quite similarly to the state in which the short-circuit line S is provided as illustrated in Figs. 1 and 2. That is, the supply of the "leading" reactive powers 10, 11 can be on-off-controlled as is necessary by means of the switching device 29.
- the power source V 0 of the power station (not shown) is connected to the primary winding la to excite the transformer lA.
- the magnetic flux 18A is generated in the core ld and interlinks with the primary winding la, secondary winding 1b and tertiary winding lc in common.
- voltages proportional, to the numbers of turns of the respective windings are generated across the primary winding la, secondary winding lb and tertiary winding lc. That is, in the state of Fig.
- the output terminals of the secondary winding lb are connected to the external circuit (not shown), thereby to operate as the output terminals of the ordinary transformer.
- the tertiary winding lc since the tertiary winding lc is in the open state, it is merely generating the voltage. Accordingly, no current flows through the tertiary winding lc, and the tertiary winding lc is not supplying electric power externally.
- magnetic energy Q is generated in the magnetic space 19, and the value thereof is expressed by" where f denotes the frequency of the power source V 0 , B the flux density of the magnetic space 19 and V the volume of the magnetic space 19.
- a short-circuit current 1 3 of a magnitude establishing a magnetic field of the flux density B in the magnetic space 19 flows through the tertiary winding lc.
- currents I 1 and I 2 satisfying the following flow through the primary winding la and the secondary winding 2b in accordance with a transformer operation: where N 1 : number of returns of the primary winding la,
- the leakage flux 18 functions equally to the shunt reactor(s) 9 or 13, 15 in tne prior-art examples shown in Figs. 20 to 23 and supplies the "leading" reactive powers 10, 11 to the capacitances 4, 7 of the primary side and secondary side transmission or distribution lines 3, 6 as shown in Figs. 4, 5, 9 and 10.
- the leakage flux 24 appears also in the two-winding transformer 20 or three-winding transformer 1 of the prior-art construction. As illustrated in the equivalent circuit of Fig. 25 or 27, however, the leakage reactance functions as the series reactance which is connected in series with the circuit.
- tne equivalent circuit of the transformer 1A with tne tertiary winding lc short-circuited is expressed as in Fig. 6.
- 25-27 and X 1 -X 3 are the same as in Fig. 27.
- the reactance X 3 on the tertiary side functions as a parallel reactance which is connected in parallel with the circuit. That is, connecting the primary side transmission or distribution line 3 and the secondary side transmission or distribution line 6 to the primary side terminal 25 and tne secondary side terminal 26 respectively corresponds to connecting "a shunt reactor whose reactance has the magnitude 1 3 " in parallel with the power transmission or distribution system. This signifies nothing but the fact that the magnetic space 19 shown in Figs. 3 and 12 functions physically as the magnetic space of the shunt reactor in the prior art.
- the two-winding transformer when it is further provided with the tertiary winding lc which is electromagnetically coupled to the primary winding la and the secondary winding lb, it becomes identical to the construction of the three-winding transformer 1A and can also be operated similarly to the shunt reactor.
- the three-winding transformer 1A with both the ends of the tertiary winding lc short-circuited functions also as the shunt reactor whose reactance has the magnitude X 3 , without spoiling the original voltage transformation function of the transformer and can supply the "leading" reactive powers to the capacitances 4, 7 of the transmission or distribution lines 3, 6.
- the voltage of the tertiary winding lc can be selected at will irrespective of the voltages of the primary transmission cr distribution line 3 and the secondary transmission or distribution line 6. Therefore, when the voltage across the tertiary winding lc is rendered sufficiently low, the transformer 1A need not be especially enlarged.
- the transformer 1A is constructed as a shell type
- the transformer may also be constructed with a core type one as shown in Fig. 7.
- a gapped-core structure may well be adopted by interposing a gapped core 28 as shown in Fig. 8.
- transformer 1A of the three windings has been explained as an example, it is needless to say that, even when the invention is applied to a transformer of four or more windings not shown, an electromagnetic induction apparatus having the same functional effect as stated above can be realized by short-circuiting the tertiary winding.
- FIG. 13 is a circuit diagram showing the embodiment of another aspect of performance of this invention
- Fig. 14 is a perspective view showing a practical construction corresponding to Fig. 13
- Figs. 15 and 16 are horizontal partial sectional views respectively showing the states in which a tertiary winding in Fig. 14 is opened and is connected to a tap.
- ia-ld, 18 and 19 denote portions similar to those described before
- 1B denotes a transformer corresponding to the transformer lA.
- the secondary winding lb is provided with a plurality of taps 30, and owing to wnich the secondary winding lt becomes a tap winding.
- the tertiary winding lc has one end connected tc one end of the secondary winding l b at a node P and has the other end connected to one of the plurality of taps 30, thereby to become a reactor winding.
- the primary side transmission or distribution line namely, the power source V 0 of a power station or the like be connected to the primary winding la in the state in which the tertiary winding lc as the reactor winding is open as depicted in F ig. 15.
- the magnetic flux 18A of a magnitude ⁇ 0 is generated in the core ld and interlinks with the primary winding la, secondary winding lb and tertiary winding lc in common.
- This state is the same as in the case of Fig. 11.
- a voltage equal to the supply voltage V 0 is generated across the primary winding la, and voltages according to the numbers of turns N l -N 3 of the respective windings la-lc are generated across the secondary winding lb and tertiary winding lc.
- the voltages generated across the windings la-lc, denoted by V 10 -V 30 respectively are expressed as follows: wnere K: constant. Accordingly, the secondary winding lb can be used for the ordinary transformer when connected to the secondary side transmission or distribution line, namely, the external circuit. Besides, since the tertiary winding lc is in the open state, it is merely generating the voltage V 30 and does not execute the reactor function at all.
- one end of the tertiary winding lc is connected to one end of the secondary winding lb through the node P, and the other end of the tertiary winding lc is connected to one of the taps 30, whereby a tap voltage V 3 lower than the open-circuit voltage V 30 as evaluated with Eqs. (3) and (5) is forcibly applied to the tertiary winding lc.
- the magnitude ⁇ of the magnetic flux 18B interlinking with the tertiary winding lc becomes a value satisfying the equation: in which V 3 and ⁇ are respectively substituted for V 30 and ⁇ 0 in Eq. (5). Accordingly, holds.
- the magnitude to of the magnetic flux 18A in the open-circuit condition becomes: in accordance with Eq. (5).
- the value ⁇ of the magnetic flux 18B upon being connected to the tap is expressed relative to the value ⁇ 0 of the magnetic flux 18A in the open-circuit condition as follows:
- the leakage flux 18C of the magnitude ⁇ flows through the magnetic space 19, whereby predetermined magnetic energy is generated to effect the shunt reactor function.
- the value : of the magnetic flux 18B interlinking with the tertiary winding lc varies in proportion to the tap voltage V 3 .
- the value ⁇ of the leakage flux 18C flowing through the magnetic space 19 changes simultaneously, so that the magnitude of the magnetic energy of the magnetic space 19 changes to change the capacity cf the shunt reactor.
- the state in which the tap voltage V 3 is rendered zero is the same as tne case illustrated in Fig. 12.
- the value ⁇ 0 of the magnetic flux 18A in the open-circuit condition flows entirely to the magnetic space 19 upon being connected to the tap and the capacity of the shunt reactor becomes the maximum.
- an electromagnetic induction apparatus comprising a shunt reactor of variable capacity can be realized even with a transformer of four or more windings by using one of the windings as a reactor winding and another as a tap winding.
- a changer 31 for changing the taps 30 in an on-load condition may well be disposed between the other end of the tertiary winding lc and the taps 30 as shown in a circuit diagram of Fig. 17.
- the change of the taps 30, in other words, tne alteration cf the capacity of the shunt reactor can be performed in the energized state.
- the magnetic space 19 through which the leakage flux 18C passes has been illustrated as the air-core structure as depicted in Fig. 16, it may well be a gapped-core structure with a gap core 28 interposed therein as depicted in Fig. 18.
- transformer 1B as the electromagnetic induction apparatus has been illustrated as the shell type transformer, it may well be a core type one as shown in Fig. 19.
- a short-circuit winding which is electromagnetically coupled to at least two windings is disposed.
- a reactor winding whicn is electromagnetically coupled to at least two windings, one being a tap winding, and whicn is connected between one end of the tap winding and a tap is disposed, and the difference flux of respective magnetic fluxes appearing when tne reactor winding is opened and is connected to the tap is generated in a magnetic space.
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Abstract
Description
- This invention relates to an electromagnetic induction apparatus which comprises a transformer and which is utilized for power transmission and distribution systems, etc., and more particularly to an electromagnetic induction apparatus which does not require the installation of a shunt reactor.
- Fig. 20 is a circuit diagram showing the single-line connection state of a substation which employs and electromagnetic induction apparatus comprising a transformer as has heretofore been utilized in a power transmission or distribution system, while Fig. 21 is a perspective view showing a practical construction in the case where the circuit in Fig. 20 is three phases.
- Referring to the figures, designates a transformer having a primary winding la and a secondary winding lb, and a tertiary winding lc which is electromagnetically coupled to the primary winding la as well as the secondary winding lb. A primary
side switching device 2 is connected to the primary winding la, a primary side transmission ordistribution line 3 has one end connected to the primaryside switching device 2 and the other end connected to an external circuit (not shown), and acapacitance 4 is formed between the primary side transmission ordistribution line 3 and ground. A secondaryside switching device 5 is connected to the secondary winding lb, a secondary side transmission ordistribution line 6 has one end connected to the secondaryside switching device 5 and the other end connected to an external circuit (not snown), and acapacitance 7 is formed between the secondary side transmission ordistribution line 6 and ground. A tertiaryside switching device 8 is connected to the tertiary winding lc, and ashunt reactor 9 has one end connected to the tertiaryside switching device 8 and the other end grounded or which is star- or delta-connected in three phases. Theflows 10 and 11 of "leading" reactive powers are supplied from theshunt reactor 9 to therespective capacitances switching devices - Next, the operation of the substation furnished with the prior-art electromagnetic induction apparatus will be explained.
- Usually, the
switching devices shunt reactor 9 through the transformer 1 to thecapacitance 4 of the primary side transmission or' distribution line 3 and thecapacitance 7 of the secondary side transmission ordistribution line 6 respectively as indicated by thearrows 10 and 11. - In a case where the transformer 1 and
tne shunt reactor 9 have become unnecessary for the power system or where an accident has occurred, theswitching devices shunt reactor 9 are separated from the power system. - In addition. Fig. 22 is a circuit diagram showing the single-line connection state of another prior-art example, wnile Fig. 23 is a perspective view showing a practical construction in the case where the circuit in Fig. 22 is used in three phases. Symbols 2 - 7 denote the same constituents as those shown in Figs. 20 and 21.
- A
transformer 20 has a primary winding 20a and asecondary winding 20b, aswitching device 12 on the primary side is connected to the primary side transmission ordistribution line 3, and ashunt reactor 13 on the primary side has one end connected to theswitching device 12 and the other end grounded or which is star- or delta-connected in three phases. Aswitching device 14 on the secondary side is connected to the secondary side transmission ordistribution line 6, and ashunt reactor 15 on the secondary side has one end connected to theswitching device 14 and the other end grounded or which is star-or delta-connected in three phases. - The
flows shunt reactors switching devices tne capacitances switching devices - Next, tne operation will be explained. Usually, the
switching devices shunt reactors distribution lines respective capacitances tne arrows transformer 20 and thesnunt reactors switching devices transformer 20 and theshunt reactors - In general, in a case where the transmission or
distribution lines great capacitances distribution lines lines shunt reactor 9 orshunt reactors - Fig. 24 is an equivalent circuit diagram of the
transformer 20 having the two windings as shown in Fig. 22, and Fig. 26 is a horizontal partial sectional view of thetransformer 20. In these figures, 21 indicates the primary side terminal of thetransformer transformer 20, 23 a magnetic space defined between the primary winding 20a and thesecondary winding 20b, 24 a leakage flux generated in thespace 23 by the primary winding 20a and thesecondary winding 20b, X the leakage reactance of thetransformer 20 induced by theleakage flux 24, r the winding resistance of thetransformer 20, and Zm the excitation impedance of thetransformer 20. - Usually, the following inequalities hold:
transformer 20 is expressed by only the leakage reactance X as shown in Fig. 25, so that the connection of the respective transmission ordistribution lines terminals - Likewise, the equivalent circuit of the transformer 1 with the three windings as shown in Fig. 20 is expressed as shown in Fig. 27, and it involves the following:
- X12: leakage reactance caused by a leakage flux flowing through a magnetic space defined between the primary winding la and the secondary winding lb,
- X13: leakage reactance caused by a leakage flux flowing through a magnetic space defined between the primary winding la and the tertiary winding lc,
- X23: leakage reactance caused by a leakage flux flowing through a magnetic space defined between the secondary winding lb and the tertiary winding lc,
- where X12 = X1 + X2 X13 = X 1 + X 3 X23 = X 2 + X 3
- In Fig. 27, 25 indicates the primary side terminal of the
transformer 1, 26 the secondary side terminal thereof, and 27 the tertiary side terminal thereof. The connection of the primary side transmission ordistribution line 3, the secondary side transmission ordistribution line 6 and the tertiary side transmission or distribution line to theprimary side terminal 25, thesecondary side terminal 26 and thetertiary side terminal 27 respectively corresponds to connecting "reactors whose reactsances have magnitudes X1, X2 and X3 respectively" in series with the power transmission or distribution system. Accordingly, as in Fig. 25, no reactance connected in parallel with the power transmission or distribution system exists with the transformer 1 only, and thesnunt reactor 9 needs to be separately disposed. - As stated above, the prior-art electromagnetic induction apparatus in the substation is equipped with the
shunt reactor 9 orshunt reactors capacitances distribution lines - (i) A large installation space for the shunt reactor(s) 9 or 13, 15 is required as shown in Fig. 21 or Fig. 23. Moreover, expenses necessary for subsidiary installations such as foundamental fire-prevention devices for the shunt reactor(s) 9 or 13, 15 become enormous.
- (ii) In a case where the shunt reactor(s) 9 or 13, 15 operate(s) as the phase modifying means, current flow through tne shunt reactor(s) 9 or 13, 15. Power loss to be incurred in the winding(s), electromagnetic shield(s) etc. of the shunt reactor(s) 9 or 13, 15 by the current cannot be neglected, either.
- (iii) When the
shunt reactor 9 is connected to the tertiary winding lc as shown in Fig. 20, not only theshunt reactor 9 but also the tertiary winding lc undergoes power loss. On the other hand, when theshunt reactors distribution lines shunt reactors - This invention has been made in crder to solve all the problems as mentioned above, and has for its object the provision of an electromagnetic induction apparatus which is so constructed as to have the function of supplying "leading" reactive powers without the installation of a shunt reactor, thereby to reduce the space and to lower the power loss.
- Another ooject of this invention is to make the capacity of an equivalent shunt reactor which functions to supply "leading" reactive powers variable.
- An electromagnetic induction apparatus according to this invention comprises a short-circuit winding which is electromagnetically coupled to at least two windings.
- An electromagnetic induction apparatus in another aspect of performance of this invention comprises a reactor winding which is electromagnetically coupled to at least two windings including a tap winding and which is inserted between one end of the tap winding and a tap.
- In this invention, two windings operate as an ordinary transformer, while a leakage flux appears in the magnetic space between the two windings and a short-circuit winding, and it equivalently functions as a shunt reactor, to supply "leading" reactive powers to transmission or distribution lines and capacitances.
- In another aspect of performance of this invention, a tap voltage whicn is lower than tne open-circuit voltage of a reactor winding is forcibly applied from a tap to the reactor winding, to generate a desired magnitude of leakage flux between the reactor winding and a tap winding.
-
- Fig. 1 is a circuit diagram showing an embodlment- of this invention,
- Fig. 2 is a perspective view showing an embodiment in which a transformer in Fig. 1 is constructed of a shell type transformer,
- Fig. 3 is a horizontal partial sectional view corresponding to Fig. 2,
- Fig. 4 is a circuit diagram showing in a single-line connection state a case where the transformer in Fig.l is used as the electromagnetic induction apparatus of a substation,
- Fig. 5 is a perspective view showing a case where the circuit in Fig. 4 is used in three phases,
- Fig. 6 is an equivalent circuit diagram corresponding to Fig. 1,
- Fig. 7 is a perspective view showing an embodiment in which the transformer in Fig. 1 is constructed of a core type transformer,
- Fig. 8 is a horizontal partial sectional view showing an embodiment in which the magnetic space of the transformer in Fig. 3 is formed of a gapped core,
- Fig. 9 is a circuit diagram showing in a single-line connection state an example where in an embodiment in which a switching device is added to a short-circuit winding in Fig. 1 is used as the electromagnetic induction apparatus of a substation,
- Fig. 10 is a perspective view showing a case where the circuit in Fig. 9 is used in three phases,
- Figs. 11 and 12 are horizontal partial sectional views respectively showing the states in which the switching device of the transformer in Fig. 9 is opened and closed,
- Fig. 13 is a circuit diagram showing another aspect of performance of this invention,
- Pic. 14 is a perspective view showing an embodiment in which a transformer in Fig. 13 is constructed of a shell type transformer,
- Figs. 15 and 16 are horizontal partial sectional, views respectively showing the states in which the tertiary winding of the transformer in Fig. 14 is opened and is connected to a tap,
- Fig. 17 is a circuit diagram showing an embodiment in which a changer is added to the taps of the transformer in Fig. 13,
- Fig. 18 is a horizontal partial sectional view showing an embodiment in which the magnetic space of a transformer in Fig. 15 is formed of a gapped core,
- Fig. 19 is a horizontal partial sectional view showing and embodiment in which the transformer in Fig. 13 is constructed of a core type transformer,
- Fig. 20 is a circuit diagram showing the single-line connection state of a substation in a prior art,
- Fig. 21 is-a perspective view showing a case where the circuit in Fig. 20 is used in three phases,
- Fig. 22 is a circuit diagram showing another substation in a prior art under a single-line connection state,
- Fig. 23 is a perspective view showing a case where the circuit in Fig. 22 is used in three phases,
- Fig. 24 is an equivalent circuit diagram corresponding to Fig. 22,
- Fig. 25 is an equivalent circuit diagram corresponding to Fig. 24,
- Fig. 26 is a horizontal partial sectional view of a transformer in Fig. 22, and
- Fig. 27 is an equivalent circuit diagram of a transformer in Fig. 20.
- Now, an embodiment of this invention will be described with reference to the drawings. Fig. 1 is a circuit diagram in a single-line connection state showing the embodiment of this invention as a transformer which has, for example, three windings, Fig. 2 is a perspective view showing a practical construction corresponding to Fig. 1, Fig. 3 is a horizontal partial sectional view corresponding to Fig. 2, Fig. 4 is a circuit diagram showing in a single-line connection state a case where the transformer in Fig. 1 is applied to a substation, Fig. 5 is a perspective view showing a case where tne circuit in Fig. 4 is used in three phases, Fig. 6 is an equivalent circuit diagram corresponding to Fig. 1, Fig. 7 is a perspective view showing an embodiment in which the transformer is constructed of a core type transformer, Fig. 8 is a horizontal partial sectional view showing an embodiment in which a magnetic space is formed of a gapped core, Fig. 9 is a circuit diagram showing a single-line connection state in the case wnere an embodiment having a switching device added to a short-circuit winding is applied to a substation, Fig. 10 is a perspective view showing a case where the circuit in Fig. 9 is used in three phases, and Figs. 11 and 12 are horizontal partial sectional views respectively showing the states in which the switching device in Fig. 9 is opened and closed. In Figs. 1-12, la-lc, 2-7, 10 and 11 indicate the same portions as in the prior art examples stated before, and 1A indicates a transformer corresponding to the transformer 1.
- The core of the transformer 1A is denoted by ld and S is a short-circuit line which short-circuits both the ends of the tertiary winding lc and due to which the tertiary winding lc becomes a short-circuit winding.
- A
leakage flux 18 is induced between the tertiary winding lc and the primary winding la or secondary winding lb by the short-circuit current of the tertiary winding lc, and tnougn not shown, such a leakage flux is also generated between the primary winding la and the secondary winding lb. Theleakage flux 18 passes through amagnetic space 19 which is illustrated only between the secondary winding lb and the tertiary winding lc nere. - A switching
device 29 added to the short-circuit line S. In actuality, the switching device may well be connected between one end of the tertiary winding lc and ground by leading the terminal of the tertiary winding lc out of the transformer 1A as shown in Fig. 9, or between the lines of the tertiary winding connected in three phases. A power source V0 such as a power station (not shown) or the like is connected to the primary winding la, and amagnetic flux 18A is generated in the core ld by the power source V0 when theswitching device 29 has been opened. Thus, when theswitching device 29 shown in Figs. 9 to 12 is opened as depicted in Fig. 11, the tertiary winding lc falls into an unshorted state, and a snunt reactor function vanishes. When theswitcning device 29 is closed as depicted in Fig. 12, the tertiary winding lc serves as the short-circuit winding and gives rise to the shunt reactor function, quite similarly to the state in which the short-circuit line S is provided as illustrated in Figs. 1 and 2. That is, the supply of the "leading"reactive powers 10, 11 can be on-off-controlled as is necessary by means of theswitching device 29. - Now, the operation of the embodiment of this invention will be described. First, with the switching
device 29 opened as shown in Fig. 11, the power source V0 of the power station (not shown) is connected to the primary winding la to excite the transformer lA. Then, themagnetic flux 18A is generated in the core ld and interlinks with the primary winding la, secondary winding 1b and tertiary winding lc in common. Under the electromagnetic induction action of themagnetic flux 18A, voltages proportional, to the numbers of turns of the respective windings are generated across the primary winding la, secondary winding lb and tertiary winding lc. That is, in the state of Fig. 11, the output terminals of the secondary winding lb are connected to the external circuit (not shown), thereby to operate as the output terminals of the ordinary transformer. Besides, since the tertiary winding lc is in the open state, it is merely generating the voltage. Accordingly, no current flows through the tertiary winding lc, and the tertiary winding lc is not supplying electric power externally. - On the other hand, in the state in which both the ends of the tertiary winding lc are short-circuited by the short-circuit line S or by the closure of the
switching device 29 as shown in Figs. 1 and 2 or in Fig. 12, a short-circuit current flows through the loop of the tertiary winding lc. Since the voltage across the tertiary winding 1c is forcibly rendered zero by the short-circuit current, tnemagnetic flux 18A in Fig. 11 flows through themagnetic space 19 between the tertiary winding lc and the secondary winding 1b as well as the primary winding la. That is, theleakage flux 18 appears in themagnetic space 19 as shown in Fig. 3 or Fig. 12. - At this time, magnetic energy Q is generated in the
magnetic space 19, and the value thereof is expressed by"magnetic space 19 and V the volume of themagnetic space 19. Simultaneously, a short-circuit current 13 of a magnitude establishing a magnetic field of the flux density B in themagnetic space 19 flows through the tertiary winding lc. In addition, currents I1 and I2 satisfying the following flow through the primary winding la and the secondary winding 2b in accordance with a transformer operation: - N2: number of turns of the secondary winding lb,
- N3: number of turns of the tertiary winding lc,
- The
leakage flux 18 functions equally to the shunt reactor(s) 9 or 13, 15 in tne prior-art examples shown in Figs. 20 to 23 and supplies the "leading"reactive powers 10, 11 to thecapacitances distribution lines - Now, there will be explained the equivalence between the
leakage flux 18 shown in Figs. 3 and 12 the shunt reactor(s) 9 or 13, 15 in the prior art. - As elucidated in conjunction with Figs. 24 to 27, the
leakage flux 24 appears also in the two-windingtransformer 20 or three-winding transformer 1 of the prior-art construction. As illustrated in the equivalent circuit of Fig. 25 or 27, however, the leakage reactance functions as the series reactance which is connected in series with the circuit. - Meanwhile, tne equivalent circuit of the transformer 1A with tne tertiary winding lc short-circuited is expressed as in Fig. 6. In the figure, 25-27 and X1-X3 are the same as in Fig. 27. By short-circuiting the tertiary winding lc to ground, the reactance X3 on the tertiary side functions as a parallel reactance which is connected in parallel with the circuit. That is, connecting the primary side transmission or
distribution line 3 and the secondary side transmission ordistribution line 6 to theprimary side terminal 25 and tnesecondary side terminal 26 respectively corresponds to connecting "a shunt reactor whose reactance has the magnitude 13" in parallel with the power transmission or distribution system. This signifies nothing but the fact that themagnetic space 19 shown in Figs. 3 and 12 functions physically as the magnetic space of the shunt reactor in the prior art. - Moreover, in the case of the two-winding transformer, when it is further provided with the tertiary winding lc which is electromagnetically coupled to the primary winding la and the secondary winding lb, it becomes identical to the construction of the three-winding transformer 1A and can also be operated similarly to the shunt reactor.
- In this manner, the three-winding transformer 1A with both the ends of the tertiary winding lc short-circuited functions also as the shunt reactor whose reactance has the magnitude X3, without spoiling the original voltage transformation function of the transformer and can supply the "leading" reactive powers to the
capacitances distribution lines cr distribution line 3 and the secondary transmission ordistribution line 6. Therefore, when the voltage across the tertiary winding lc is rendered sufficiently low, the transformer 1A need not be especially enlarged. - Although the above embodiment has been explained as to the case wnen the transformer 1A is constructed as a shell type, the transformer may also be constructed with a core type one as shown in Fig. 7.
- Also, while tne air-core structure has been adopted as the
magnetic space 19 through which theleakage flux 18 passes, a gapped-core structure may well be adopted by interposing agapped core 28 as shown in Fig. 8. - Further, while the transformer 1A of the three windings has been explained as an example, it is needless to say that, even when the invention is applied to a transformer of four or more windings not shown, an electromagnetic induction apparatus having the same functional effect as stated above can be realized by short-circuiting the tertiary winding.
- Next, another aspect of performance of this invention will be described. Fig. 13 is a circuit diagram showing the embodiment of another aspect of performance of this invention, Fig. 14 is a perspective view showing a practical construction corresponding to Fig. 13, and Figs. 15 and 16 are horizontal partial sectional views respectively showing the states in which a tertiary winding in Fig. 14 is opened and is connected to a tap. In the figures, ia-ld, 18 and 19 denote portions similar to those described before, and 1B denotes a transformer corresponding to the transformer lA.
- The secondary winding lb is provided with a plurality of
taps 30, and owing to wnich the secondary winding lt becomes a tap winding. In addition, the tertiary winding lc has one end connected tc one end of the secondary winding lb at a node P and has the other end connected to one of the plurality oftaps 30, thereby to become a reactor winding. - Next, the operation of the embodiment of another aspect of performance of this invention will now be described. First, it is assumed that the primary side transmission or distribution line, namely, the power source V0 of a power station or the like be connected to the primary winding la in the state in which the tertiary winding lc as the reactor winding is open as depicted in Fig. 15. Then, the
magnetic flux 18A of a magnitude φ0 is generated in the core ld and interlinks with the primary winding la, secondary winding lb and tertiary winding lc in common. This state is the same as in the case of Fig. 11. - At this time, a voltage equal to the supply voltage V0 is generated across the primary winding la, and voltages according to the numbers of turns Nl-N3 of the respective windings la-lc are generated across the secondary winding lb and tertiary winding lc. The voltages generated across the windings la-lc, denoted by V10-V30 respectively are expressed as follows:
- Subsequently, as depicted in Fig. 16, one end of the tertiary winding lc is connected to one end of the secondary winding lb through the node P, and the other end of the tertiary winding lc is connected to one of the
taps 30, whereby a tap voltage V3 lower than the open-circuit voltage V30 as evaluated with Eqs. (3) and (5) is forcibly applied to the tertiary winding lc. After the application of the tap voltage V3, the magnitude φ of themagnetic flux 18B interlinking with the tertiary winding lc becomes a value satisfying the equation: - On the other hand, the magnitude to of the
magnetic flux 18A in the open-circuit condition becomes:magnetic flux 18B upon being connected to the tap is expressed relative to the value φ0 of themagnetic flux 18A in the open-circuit condition as follows: -
- In this manner, upon being connected to the tap illustrated in Fig. 16, the
leakage flux 18C of the magnitude Δφ flows through themagnetic space 19, whereby predetermined magnetic energy is generated to effect the shunt reactor function. - Here, it is understood that, by altering the
tap 30 of the secondary winding lb to which the other end of the tertiary winding 1c is connected, to change the tap voltage V3 in Eq. (8), the value : of themagnetic flux 18B interlinking with the tertiary winding lc varies in proportion to the tap voltage V3. At this time, the value Δφ of theleakage flux 18C flowing through themagnetic space 19 changes simultaneously, so that the magnitude of the magnetic energy of themagnetic space 19 changes to change the capacity cf the shunt reactor. In particular, the state in which the tap voltage V3 is rendered zero is the same as tne case illustrated in Fig. 12. The value φ0 of themagnetic flux 18A in the open-circuit condition flows entirely to themagnetic space 19 upon being connected to the tap and the capacity of the shunt reactor becomes the maximum. - while the above embodiment has referred to the three-winding transformer by way of example, it is needless to say that, quite similarly to the case of tne three-winding transformer, an electromagnetic induction apparatus comprising a shunt reactor of variable capacity can be realized even with a transformer of four or more windings by using one of the windings as a reactor winding and another as a tap winding.
- Besides, while the other end of the tertiary winding lc has been connected to a proper one of the
taps 30, achanger 31 for changing thetaps 30 in an on-load condition may well be disposed between the other end of the tertiary winding lc and thetaps 30 as shown in a circuit diagram of Fig. 17. In this case, the change of thetaps 30, in other words, tne alteration cf the capacity of the shunt reactor can be performed in the energized state. In this way, when the respective tap voltages V3 at the plurality oftaps 30 are properly changed-over and applied to the tertiary winding lc, the capacities of the equivalent shunt reactor can be turned on and off stepwise, and hence, an instantaneous voltage fluctuation is not incurred in the power transmission or distribution system. - Besides, while the
magnetic space 19 through which theleakage flux 18C passes has been illustrated as the air-core structure as depicted in Fig. 16, it may well be a gapped-core structure with agap core 28 interposed therein as depicted in Fig. 18. - Further, while the transformer 1B as the electromagnetic induction apparatus has been illustrated as the shell type transformer, it may well be a core type one as shown in Fig. 19.
- As described above, according to this invention, a short-circuit winding which is electromagnetically coupled to at least two windings is disposed. This produces the effect that a transformer having also a shunt reactor function for supplying "leading" reactive powers required by transmission or distribution lines can be realized, and that an electromagnetic induction apparatus which dispenses with facilities for a shunt reactor and which can reduce the construction cost of a substation and power loss is provided.
- In another aspect of performance of this invention, a reactor winding whicn is electromagnetically coupled to at least two windings, one being a tap winding, and whicn is connected between one end of the tap winding and a tap is disposed, and the difference flux of respective magnetic fluxes appearing when tne reactor winding is opened and is connected to the tap is generated in a magnetic space. This produces the effect that an electromagnetic induction apparatus in which the capacity of an equivalent shunt reactor is variable is provided.
and the shunt reactor function of supplying the magnetic energy Q externally is effected.
Claims (11)
Applications Claiming Priority (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18048985 | 1985-08-19 | ||
JP180489/85 | 1985-08-19 | ||
JP58111/86 | 1986-03-18 | ||
JP5811186A JPS62122113A (en) | 1985-08-19 | 1986-03-18 | Electromagnetic induction apparatus |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0216500A1 true EP0216500A1 (en) | 1987-04-01 |
EP0216500B1 EP0216500B1 (en) | 1992-06-03 |
Family
ID=26399191
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP86306422A Expired - Lifetime EP0216500B1 (en) | 1985-08-19 | 1986-08-19 | Electromagnetic induction apparatus |
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EP (1) | EP0216500B1 (en) |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2827073A1 (en) * | 2001-07-06 | 2003-01-10 | Aristide Polisois | Industrial networks/information/remote control exchange transformer having two windings producing opposite fields/same intensity optimizing magnetic circuit/suppressing alternating currents with capacitive/short circuit windings. |
FR2881266A1 (en) * | 2005-01-27 | 2006-07-28 | Areva T & D Sa | Transformer for multisystem rail traction unit, has primary winding, pull-in secondary winding and additional secondary winding, where secondary windings cooperate to generate leakage inductor for smoothing waves affecting direct current |
WO2007133169A1 (en) * | 2006-05-12 | 2007-11-22 | Great Man Made River Co. For Reclamation And Construction | Description electro-ageeb electrical safety device |
EP3267444A1 (en) * | 2016-07-06 | 2018-01-10 | Tamura Corporation | Transformer and switched-mode power supply apparatus |
EP3267445A1 (en) * | 2016-07-06 | 2018-01-10 | Tamura Corporation | Transformer and switched-mode power supply apparatus |
US20180013350A1 (en) | 2016-07-05 | 2018-01-11 | Tamura Corporation | Transformer and switched-mode power supply apparatus |
US10262789B2 (en) | 2016-07-05 | 2019-04-16 | Tamura Corporation | Transformer and switched-mode power supply apparatus |
Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB191105190A (en) * | 1911-03-01 | 1912-02-29 | Arthur Francis Berry | Improvements in or relating to Electrical Transformers. |
FR488384A (en) * | 1917-01-26 | 1918-09-24 | Westinghouse Electric Corp | Tertiary coils for transformers |
FR45888E (en) * | 1935-03-04 | 1935-12-27 | Fr De Materiel Electr Soc | Improvements made to electrical transformer stations |
US2221619A (en) * | 1939-12-28 | 1940-11-12 | Westinghouse Electric & Mfg Co | Electrical induction apparatus |
FR891965A (en) * | 1942-03-09 | 1944-03-24 | Licentia Gmbh | High voltage transformer, choke coil or measuring transformer |
CH306155A (en) * | 1951-08-24 | 1955-03-31 | Bbc Brown Boveri & Cie | Power transformer with a device for reactive power compensation. |
GB1244219A (en) * | 1967-08-24 | 1971-08-25 | Licentia Gmbh | Inductive devices for compensating capacitive currents |
FR2290012A1 (en) * | 1974-10-25 | 1976-05-28 | Smit Nijmegen Bv | Adjustable polyphase transformer system for coupling networks - has three equal single phase transformers with tertiary and regulating windings |
EP0149169A2 (en) * | 1984-01-13 | 1985-07-24 | BBC Aktiengesellschaft Brown, Boveri & Cie. | Transformer-rectifier |
-
1986
- 1986-08-19 EP EP86306422A patent/EP0216500B1/en not_active Expired - Lifetime
Patent Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB191105190A (en) * | 1911-03-01 | 1912-02-29 | Arthur Francis Berry | Improvements in or relating to Electrical Transformers. |
FR488384A (en) * | 1917-01-26 | 1918-09-24 | Westinghouse Electric Corp | Tertiary coils for transformers |
FR45888E (en) * | 1935-03-04 | 1935-12-27 | Fr De Materiel Electr Soc | Improvements made to electrical transformer stations |
US2221619A (en) * | 1939-12-28 | 1940-11-12 | Westinghouse Electric & Mfg Co | Electrical induction apparatus |
FR891965A (en) * | 1942-03-09 | 1944-03-24 | Licentia Gmbh | High voltage transformer, choke coil or measuring transformer |
CH306155A (en) * | 1951-08-24 | 1955-03-31 | Bbc Brown Boveri & Cie | Power transformer with a device for reactive power compensation. |
GB1244219A (en) * | 1967-08-24 | 1971-08-25 | Licentia Gmbh | Inductive devices for compensating capacitive currents |
FR2290012A1 (en) * | 1974-10-25 | 1976-05-28 | Smit Nijmegen Bv | Adjustable polyphase transformer system for coupling networks - has three equal single phase transformers with tertiary and regulating windings |
EP0149169A2 (en) * | 1984-01-13 | 1985-07-24 | BBC Aktiengesellschaft Brown, Boveri & Cie. | Transformer-rectifier |
Cited By (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2827073A1 (en) * | 2001-07-06 | 2003-01-10 | Aristide Polisois | Industrial networks/information/remote control exchange transformer having two windings producing opposite fields/same intensity optimizing magnetic circuit/suppressing alternating currents with capacitive/short circuit windings. |
FR2881266A1 (en) * | 2005-01-27 | 2006-07-28 | Areva T & D Sa | Transformer for multisystem rail traction unit, has primary winding, pull-in secondary winding and additional secondary winding, where secondary windings cooperate to generate leakage inductor for smoothing waves affecting direct current |
WO2006079744A1 (en) * | 2005-01-27 | 2006-08-03 | Areva T & D Sa | Transformer for multicurrent motor vehicle |
EP1841616B1 (en) | 2005-01-27 | 2016-12-21 | Alstom Grid SAS | Transformer for multicurrent motor vehicle |
WO2007133169A1 (en) * | 2006-05-12 | 2007-11-22 | Great Man Made River Co. For Reclamation And Construction | Description electro-ageeb electrical safety device |
GB2452203A (en) * | 2006-05-12 | 2009-02-25 | Great Man Made River Co For Re | Description electro-ageeb electrical safety device |
US20180013350A1 (en) | 2016-07-05 | 2018-01-11 | Tamura Corporation | Transformer and switched-mode power supply apparatus |
US10249430B2 (en) | 2016-07-05 | 2019-04-02 | Tamura Corporation | Transformer and switched-mode power supply apparatus |
US10262789B2 (en) | 2016-07-05 | 2019-04-16 | Tamura Corporation | Transformer and switched-mode power supply apparatus |
EP3267444A1 (en) * | 2016-07-06 | 2018-01-10 | Tamura Corporation | Transformer and switched-mode power supply apparatus |
EP3267445A1 (en) * | 2016-07-06 | 2018-01-10 | Tamura Corporation | Transformer and switched-mode power supply apparatus |
Also Published As
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