EP0377691A1 - Transformateur matriciel a isolation dielectrique elevee - Google Patents
Transformateur matriciel a isolation dielectrique eleveeInfo
- Publication number
- EP0377691A1 EP0377691A1 EP89905315A EP89905315A EP0377691A1 EP 0377691 A1 EP0377691 A1 EP 0377691A1 EP 89905315 A EP89905315 A EP 89905315A EP 89905315 A EP89905315 A EP 89905315A EP 0377691 A1 EP0377691 A1 EP 0377691A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- primary
- matrix transformer
- transformer
- matrix
- winding
- Prior art date
- 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.)
- Withdrawn
Links
- 239000011159 matrix material Substances 0.000 title claims abstract description 51
- 238000002955 isolation Methods 0.000 title abstract description 11
- 238000004804 winding Methods 0.000 claims abstract description 49
- 238000009413 insulation Methods 0.000 claims description 39
- 239000012212 insulator Substances 0.000 claims description 9
- 239000004020 conductor Substances 0.000 claims description 5
- 239000004809 Teflon Substances 0.000 description 4
- 229920006362 Teflon® Polymers 0.000 description 4
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 2
- 235000008429 bread Nutrition 0.000 description 2
- 230000006698 induction Effects 0.000 description 2
- 239000000696 magnetic material Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 229910000859 α-Fe Inorganic materials 0.000 description 2
- WYTGDNHDOZPMIW-RCBQFDQVSA-N alstonine Natural products C1=CC2=C3C=CC=CC3=NC2=C2N1C[C@H]1[C@H](C)OC=C(C(=O)OC)[C@H]1C2 WYTGDNHDOZPMIW-RCBQFDQVSA-N 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 239000003985 ceramic capacitor Substances 0.000 description 1
- 230000009977 dual effect Effects 0.000 description 1
- 230000005669 field effect Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- 230000035939 shock Effects 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
- 239000002966 varnish Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F17/00—Fixed inductances of the signal type
- H01F17/04—Fixed inductances of the signal type with magnetic core
- H01F17/06—Fixed inductances of the signal type with magnetic core with core substantially closed in itself, e.g. toroid
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F38/00—Adaptations of transformers or inductances for specific applications or functions
- H01F2038/006—Adaptations of transformers or inductances for specific applications or functions matrix transformer consisting of several interconnected individual transformers working as a whole
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F38/00—Adaptations of transformers or inductances for specific applications or functions
- H01F38/20—Instruments transformers
- H01F38/22—Instruments transformers for single phase ac
- H01F38/28—Current transformers
- H01F38/30—Constructions
- H01F2038/305—Constructions with toroidal magnetic core
Definitions
- This invention relates to transformers, and in particular to transformers which have a requirement for high dielectric isolation, such as safety transformers.
- a matrix transformer comprises a plurality of interdependant magnetic elements, interwired as a transformer, as taught by U. S. Patent 4,665,357, "Plat Matrix Transformer", Herbert, May 12, 1987. Because of the small size of the interdependant magnetic elements, and the close proximity and intermingling of its windings, it is not apparent that the flat matrix transformer could have much dielectric isolating capability.
- Figure 1 shows a matrix transformer having high dielectric insulation.
- Figure 2 shows the transformer of figure 1, without the wiring, to more clearly show the insulating system.
- Figure 3 shows a section through one of the magnetic elements of figure 1.
- Pigure 4 shows a section through one magnetic element of a matrix transformer similar to the transformer of figure 1, but incorporating a safety shield.
- Figure 5 shows a matrix transformer having an intermediate, low voltage winding to further isolate the secondary circuit from the primary circuit.
- Figure 6 shows the a transformer similar to the one of figure 5, without the primary and secondary windings to more clearly show the intermediate low voltage winding. The ends of the low voltage intermediate winding are shown grounded.
- the matrix transformer is made of many magnetic elements, which are arranged and interwired to behave collectively as a transformer.
- the art of designing and manufacturing matrix transformers is adaptable to a very wide variety of shapes, sizes and configurations.
- Transformers belong to a broad family of static devices in which electric currents in conductors interact by means of magnetic induction with changing fluxes in magnetic cores. These include potential transformers, current transformers, flyback transformers, induction coils, “constant current output” transformers, multiple winding inductors and inductors. "Matrix transformer” is used herein as a generic term including any of these devices when they are built using an array of smaller interdependent magnetic elements interwired as a whole.
- the matrix transformer designed in this way functions as an ordinary transformer, but because of the manner in which the various elemental parts cooperate interdependently, it has some unique characteristics which can be used to advantage in many applications. Matrix transformers can also be designed which have characteristics which no single core device could have.
- the magnetic elements can be small cores of ordinary design, such as C cores, E-I cores, pot cores or toroids, but alternatively can be one of several new geometries having multiple magnetic return paths such as two parallel plates bridged by a multitude of posts, a plurality of modified cross cores, or a plate of magnetic material having a plurality of holes therein.
- Different types of interdependent magnetic elements can be inter ⁇ mixed in an interdependent matrix array as long as the rules of transformers are followed.
- the matrix transformer can be very flat, and the electrical circuits can be made using printed wiring board techniques.
- matrix transformers There is a high degree of flexibility and discretion in the design of matrix transformers, including, but not limited to, the number of magnetic elements, the detailed design of the elements, and the physical arrangements of the elements. Also, the windings of the matrix transformer can be arranged in different ways, and there is flexibility in choosing how and where a particular winding enters and exits the transformer. The voltages and the currents in the matrix transformer have a definite relationship, one to another, and this information can be exploited to optimize the design.
- Pigure 1 shows a matrix transformer which has been built incorporating several features for high dielectric isolation. Typical requirements for high dielectric isolation will include a creep distance for the primary, a creep distance for the secondary, a creep distance between the primary and the secondary, a required number of layers of insulation, a distance through the insulation, and a dielectric test requirement.
- the transformer. of figure 1 comprises ten interdependant magnetic elements, shown a toroids 101a, - j.
- a primary winding 102 shown as a push pull (centertapped) winding, five parallel secondary windings 103a,b, (etc. ) , also shown as push pull (centertapped) windings.
- Primary insulation 105a,b encloses the primary winding 102, and extends entirely through the matrix transformer, uninterrupted, and extends beyond it on both ends. The amount that it extends on each end is determined by the creepage distance requirements to the secondary.
- Secondary insulation 104a,b-j encloses the secondary winding where it passes through the magnetic elements, and extends beyond each magnetic element on each side. The amount that it extends is determined by the creepage distance of the secondary to the core.
- the primary and secondary insulation can be insulating tubing, such as Teflon.
- Figure 2 shows the transformer of figure 1 without the primary and secondary wires.
- Primary insulation 205a,b could be one continuous piece of insulation, and would not have to extend beyond the transformer on the closed end. This would be preferred if it were important to minimize primary leakage inductance.
- the path of the primary winding is quite serpentine. For this, a flexible insulation would be preferred, and it would probably be easier to pull the primary wires through the insulation prior to installing it in the matrix transformer.
- Figure 3 shows a section through one of the magnetic elements of the transformer of figure 1. All of the are similar.
- 301 is the magnetic element, illustrated as a toroid, though it could be any type of magnetic core such as a U-I core, one side of an E core, a pot core or a specialized core structure for matrix transformers.
- the primary winding 302 preferably comprises a winding of insulated wire (preferably not just a film or varnish insulation) such as ordinary Teflon type E hook up wire.
- the secondary winding 303 is similar to the primary, and can be the same gauge, the currents being equal to the primary as is the nature of matrix transformers. In some applications or embodiments of the invention the secondary might not require the same amount of insulation Secondary and primary insulation 305 and 305 enclose each winding.
- the dielectric isolation criteria are fulfilled as follows: The primary creepage distance to the core and to the secondary is satisfied by the amount that the primary insulation 104 extends beyond the ends of the matrix transformer. The secondary creepage distance to the core is satisfied by the amount that the secondary insulation 105 extends beyond each magnetic element 101.
- the spacing through the insulation for the primary winding to the core is satisfied by the combined thickness of the insulation of the primary winding wire 102 and the primary insulation 104.
- the spacing through the insulation for the secondary winding to the core is satisfied by the combined thickness of the insulation of the secondary winding wire 103 and the secondary insulation 105.
- the spacing through the insulation from primary to secondary is satisfied by the thickness of the wire insulation of both windings and the thickness of both the primary and the secondary insulations.
- the insulation system would be preferred for various applications. If either the primary or the secondary, or both, were a single wire winding, the use of a wire having sufficient insulation of itself would be consistent with the teachings of this invention. Such an insulation would probably have at least two layers, and its total insulation thickness would be greater than " the specification requirements. In some cases this would be preferred even with windings having more than one wire, particularly if the primary wires followed different paths through the transformer, or if it were interrupted, as for switching elements or other components or the like.
- a second layer of insulation around the primary or the secondary or both might be used. This might be the case where there were more than one wire in a winding, and the winding factor could be improved by using a wire with insufficient insulation to meet the minimum requirements as a layer.
- Some magnetic materials are very good insulators, such as nickel ferrites.
- some magnetic cores are encapsulated or otherwise insulated. In either case, the insulation system, particularly the secondary, might be reduced, or even eliminated, and still provide sufficient dielectric isolation.
- the primary insulations system might be upgraded.
- a matrix transformer similar to the one in figure 1 can be made with ferrite cores such as Pair-rite (tm) part no. 2677006301, which are about 3/8" outside diameter.
- the primary and secondary windings can be made with awg 22 Teflon hook up wire. If the primary and secondary windings are each inside a number 12 Teflon sleeving, the transformer will meet very high dielectric isolation requirements. (In test, there was no dielectric failure to the limit of the available test equipment: 40,000 VDC) .
- a transformer similar to the transformer of figure 1 was installed in a bread board of a push-pull pulse width modulated switch mode power supply.
- the input voltage was 40 to 60 volts, with 5 volts out.
- the primary was driven with a Unitrode (tm) part no. 3825 integrated circuit, buffered to improve the output fall time.
- the primary switches were n-channel power MOSFET's (metal- oxide-silicon field effect transistors).
- the individual secondaries were rectified with dual Schottky rectifiers.
- the individual secondary centertaps were connected to ground through small inductors.
- the anodes of each pair of rectifiers were connected together and to small ceramic capacitors, which was returned to ground, the whole being kept very tight. The outputs were then paralleled.
- Figure 4 shows a section of a magnetic element of a transformer similar to the transformer of figure 1, except that a safety shield 406 has been added. All other features are the same as the corresponding features of figure 3.
- the safety shield would preferably be terminated to a ground plane (which could also be a heat sink) immediately when it left the core.
- the shield could more fully, or completely enclose the primary or the secondary, or both, (but preferably not both together in one shield) .
- Figure 5 teaches an embodiment of the matrix transformer having an intermediate low voltage winding to further isolate the primary from the secondary.
- a primary winding 502 couples a first set of ten interdependant magnetic elements 501k-u.
- a primary insulator 503a,b extends through the transformer. Pairs of magnetic elements 501k-u couple a pairs of a second set-of magnetic elements 501a-j through intermediate low voltage windings 506a-e.
- the second set of magnetic elements 501a-j can have any suitable matrix transformer secondary, shown here as five parallel secondaries 503a-e.
- Figure 6 shows the intermediate low voltage windings more clearly, and shows that they are preferably grounded to a ground plane at both ends. In this manner, it can be seen that no dielectric failure will allow primary voltage to appear on the secondary as long as the ground plane can carry fault currents away.
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Coils Or Transformers For Communication (AREA)
- Insulating Of Coils (AREA)
Abstract
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US18725388A | 1988-04-28 | 1988-04-28 | |
US187253 | 1988-04-28 |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0377691A1 true EP0377691A1 (fr) | 1990-07-18 |
EP0377691A4 EP0377691A4 (en) | 1990-10-10 |
Family
ID=22688219
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP19890905315 Withdrawn EP0377691A4 (en) | 1988-04-28 | 1989-04-21 | Matrix transformer having high dielectric isolation |
Country Status (6)
Country | Link |
---|---|
EP (1) | EP0377691A4 (fr) |
JP (1) | JPH03500948A (fr) |
KR (1) | KR900701021A (fr) |
AU (1) | AU3537589A (fr) |
BR (1) | BR8906934A (fr) |
WO (1) | WO1989010621A1 (fr) |
Families Citing this family (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2307795A (en) * | 1995-12-01 | 1997-06-04 | Metron Designs Ltd | Isolation transformer with plural magnetic circuits coupled by a winding |
DE29716058U1 (de) * | 1997-09-06 | 1997-10-23 | Wollnitzke, Helmut, 95100 Selb | Magnetisierbares elektrisches Bauelement |
DE10218455A1 (de) * | 2002-04-25 | 2003-11-06 | Abb Patent Gmbh | Sperrwandleranordnung |
JP2004335885A (ja) | 2003-05-09 | 2004-11-25 | Canon Inc | 電子部品およびその製造方法 |
JP2004335886A (ja) * | 2003-05-09 | 2004-11-25 | Canon Inc | トランス集合体、それを用いた電力変換装置及び太陽光発電装置 |
WO2016036420A1 (fr) | 2014-09-05 | 2016-03-10 | PICHKUR, Dmytro | Transformateur |
Family Cites Families (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CA474473A (fr) * | 1951-06-12 | C. Wentz Edward | Isolateurs de conducteurs a haute tension | |
US2600057A (en) * | 1949-05-18 | 1952-06-10 | Quentin A Kerns | High-voltage multiple core transformer |
NL229257A (fr) * | 1957-07-24 | |||
US2945961A (en) * | 1958-05-05 | 1960-07-19 | Ite Circuit Breaker Ltd | Current balancing reactors for diodes |
US3577110A (en) * | 1969-05-09 | 1971-05-04 | Dominion Electric Corp | Transformer having a wound core around linear conductors |
US3725741A (en) * | 1971-06-30 | 1973-04-03 | Westinghouse Electric Corp | Differential transformer mounting arrangement particulary for ground fault interrupter apparatus |
US3961292A (en) * | 1974-01-02 | 1976-06-01 | Ross Alan Davis | Radio frequency transformer |
US3996513A (en) * | 1975-04-24 | 1976-12-07 | Butler Fred C | Differential microampere current sensor |
US4021729A (en) * | 1975-12-03 | 1977-05-03 | I-T-E Imperial Corporation | Cross-field ground fault sensor |
US4414543A (en) * | 1980-09-25 | 1983-11-08 | Schweitzer Edmund O Jun | Ground fault indicator |
US4510478A (en) * | 1981-08-17 | 1985-04-09 | Mid-West Transformer Company | Coil body |
US4617543A (en) * | 1984-01-26 | 1986-10-14 | Tdk Corporation | Coil bobbin |
-
1989
- 1989-04-21 EP EP19890905315 patent/EP0377691A4/en not_active Withdrawn
- 1989-04-21 AU AU35375/89A patent/AU3537589A/en not_active Abandoned
- 1989-04-21 BR BR898906934A patent/BR8906934A/pt unknown
- 1989-04-21 KR KR1019890702473A patent/KR900701021A/ko not_active Application Discontinuation
- 1989-04-21 WO PCT/US1989/001714 patent/WO1989010621A1/fr not_active Application Discontinuation
- 1989-04-21 JP JP1505064A patent/JPH03500948A/ja active Pending
Non-Patent Citations (2)
Title |
---|
No relevant documents have been disclosed. * |
See also references of WO8910621A1 * |
Also Published As
Publication number | Publication date |
---|---|
KR900701021A (ko) | 1990-08-17 |
AU3537589A (en) | 1989-11-24 |
EP0377691A4 (en) | 1990-10-10 |
BR8906934A (pt) | 1990-09-11 |
WO1989010621A1 (fr) | 1989-11-02 |
JPH03500948A (ja) | 1991-02-28 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US6181231B1 (en) | Diamond-based transformers and power convertors | |
US4845606A (en) | High frequency matrix transformer | |
US6486765B1 (en) | Transformer | |
US7218199B1 (en) | Structure of transformer | |
US7482905B2 (en) | Method and apparatus for transferring energy in a power converter circuit | |
JP5813320B2 (ja) | 高電圧用途のための高周波変圧器 | |
EP3425650B1 (fr) | Module et circuit de conversion de courant continu-continu | |
KR20010049159A (ko) | 전력 트랜스포머/인덕터 | |
GB2531348A (en) | Embedded magnetic component transformer device | |
GB2331853A (en) | Transformer | |
US5631815A (en) | High voltage power supply | |
US5168440A (en) | Transformer/rectifier assembly with a figure eight secondary structure | |
EP0370102A1 (fr) | Transformateur de matrices a haute frequence | |
EP0377691A1 (fr) | Transformateur matriciel a isolation dielectrique elevee | |
EP0989717A2 (fr) | Dispositif d'alimentation pour système de communication sous-marin | |
KR20010049160A (ko) | 전력 트랜스포머/인덕터 | |
FI82341C (fi) | Hoegspaenningstransformator foer en videoaotergivningsanordning. | |
US11735357B2 (en) | Transformer with improved insulation structure | |
US4754390A (en) | Conductively cooled switching regulator | |
EP0864165B1 (fr) | Transformateur de puissance a forte isolation | |
US6822549B2 (en) | Method for increased coupling coefficient in a pulse type transformer through coil configuration and varied core area | |
WO2002103725A1 (fr) | Appareil electrique possedant un dispositif electromagnetique actionnable a des valeurs d'inductance multiples | |
AU613211C (en) | High frequency matrix transformer | |
WO2004021375A1 (fr) | Transformateur electrique | |
KR900019075A (ko) | 대칭형 푸시-풀 권선을 지니는 트랜스포머 |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
17P | Request for examination filed |
Effective date: 19900424 |
|
AK | Designated contracting states |
Kind code of ref document: A1 Designated state(s): AT BE CH DE FR GB IT LI LU NL SE |
|
RAP1 | Party data changed (applicant data changed or rights of an application transferred) |
Owner name: FMTT, INC. |
|
A4 | Supplementary search report drawn up and despatched |
Effective date: 19900822 |
|
AK | Designated contracting states |
Kind code of ref document: A4 Designated state(s): AT BE CH DE FR GB IT LI LU NL SE |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN |
|
18D | Application deemed to be withdrawn |
Effective date: 19921103 |