AU2001260837A1 - Partial core, low frequency transformer - Google Patents

Partial core, low frequency transformer

Info

Publication number
AU2001260837A1
AU2001260837A1 AU2001260837A AU6083701A AU2001260837A1 AU 2001260837 A1 AU2001260837 A1 AU 2001260837A1 AU 2001260837 A AU2001260837 A AU 2001260837A AU 6083701 A AU6083701 A AU 6083701A AU 2001260837 A1 AU2001260837 A1 AU 2001260837A1
Authority
AU
Australia
Prior art keywords
transformer
core
windings
winding
primary
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.)
Abandoned
Application number
AU2001260837A
Inventor
Patrick Selwyn Bodger
Wade Grant Enricht
Ming Chuen Liew
Mathew Bryan O'Neil
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Canterbury Tx Ltd
Original Assignee
Canterprise Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Canterprise Ltd filed Critical Canterprise Ltd
Publication of AU2001260837A1 publication Critical patent/AU2001260837A1/en
Assigned to Canterbury TX Limited reassignment Canterbury TX Limited Request for Assignment Assignors: CANTERPRISE LIMITED
Abandoned legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F36/00Transformers with superconductive windings or with windings operating at cryogenic temperature
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/24Magnetic cores
    • H01F27/245Magnetic cores made from sheets, e.g. grain-oriented
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Description

Title Partial Core, Low Frequency Transformer
Technical Field
The present invention relates to an improved transformer design by combining a previously unexplored combination of design parameters.
Background Art
As is well known, a transformer is designed to connect independent alternating current (AC) electrical networks at different voltages and typically comprises two or more electrically isolated windings. An AC voltage applied to one winding induces a voltage in the other winding via the intermediary of a magnetic field. There has been extensive research in transformer design and applications, such that the key performance characteristics such as frequency, voltage and operating temperature extend over a wide spectrum, whilst the transformer may utilize either a full-core, a partial core, or be completely core-less.
The design of the transformer is greatly affected by the nature of its intended use. The present invention relates to a power transformer and utilizes a particular combination of design parameters which surprisingly has hitherto been unexplored.
The intended operating temperature also affects the transformer design, configuration and constituent materials and may be generally classified as follows:-
- high temperatures exceeding those tolerable by humans, typically created in artificial environments,
- the ambient temperatures encompassing the range of naturally encountered climatic conditions, e.g. frost/ice to high-temperature deserts. The internal heat generated by the operation of transformers may cause the actual operating temperature to exceed ambient,
- high temperature super-conducting temperatures provided by operations in a liquid nitrogen environment,
- to low temperature super-conducting temperatures provided by operations in a liquid helium environment.
Whilst frequency and voltage may seem at face value to be a performance parameter, the physical design and configuration of the transformer directly effect the operational range of both these parameters. High frequency transformers designs differ significantly from low frequency designs, particularly due to the need to accommodate the capacitance effects generated at high frequencies.
The present invention is primarily intended to operate in the frequency range classified as 'extremely low frequency' (30Hz to 300Hz), which covers the mains frequency (50- 60Hz) of the majority of land-based power systems. However, the present invention is equally adaptable for use with signals in the adjacent 300Hz-3000Hz range which covers harmonic frequency multiples of the mains frequencies and aircraft power system frequencies. Generically, all the aforesaid frequencies are considered as 'low frequency' and are typically associated with energy or power transfer in contrast to 'high frequencies' typically involved in information transfer, e.g. radio, microwave and so forth.
In a complimentary manner, the transformer application voltage is a design parameter which affects the physical configuration and size of the transformer. A high voltage transformer would require different insulation and winding configuration than a low voltage design. Typically, power transformers are designed for high voltage usage as they operate from the mains supply (typically 110V or 230V or above) or the distribution/transmission voltages of a national power system. As used herein, the term 'high voltage' is used to mean equal to or greater than a voltage of about 100V.
In a conventional 2 winding transformer, the flux linkage between windings is a function of core permeability, the number of turns in the winding, the primary/secondary winding separation, the core length and cross-sectional area. The core of a transformer is the medium through which the magnetic field propagates in linking the windings and its configuration and constituent material are critical transformer design parameters that can be broadly classified into three categories:- full core, core-less and partial core.
A full-core forms a continuous and closed magnetic path, around which the windings are wound. A power transformer designed for high efficiency power transfer would typically employ a high permeability full core, confining the magnetic flux to the core material instead of passing through the air. The use of a full core allows magnetic flux to develop without requiring a large magnetization current. This aids both the efficiency and regulation of the transformer. The core would usually be formed from a ferromagnetic material to give a high volts per turn ratio, minimizing the quantity of winding material used and therefore reducing losses. The windings usually are made of low resistivity materials (e.g. copper or aluminium), whilst the core material is usually laminated into high resistance paths (to reduce eddy current losses) and formed from materials with low hysteresis and high permeability values. Full-core transformers typically are used for low frequency applications, particularly in the power industry.
A core-less transformer has no ferromagnetic material passing through the windings. A conceptual core-less transformer would have a primary winding wound about the central non-conducting, non-magnetic former with a secondary winding wound about the primary winding, though the winding arrangement may be reversed or two windings may be wound together to reduce flux leakage. The absence of a core theoretically implies no hysteresis or eddy current losses (commonly referred to as core losses) and consequently the device should exhibit a linear magnetization curve.
However, a significant disadvantage of core-less transformers is that the magnetizing current drawn from the supply may be a significant percentage of the total on-load current due to a low magnetizing reactance, which is itself in direct proportion to the operational frequency. The combination of low frequency with a core-less design would render the transformer extremely ineffective. Consequently, practical core-less transformers usually are employed in high frequency applications.
One method of overcoming this problem is to increase the number of winding turns, though this naturally increases the quantity of winding material. Thus, although there are no core losses, the increase in winding losses and increased flux leakage due to the increased spatial displacement of the windings (with a corresponding reduction in efficiency) restricts the practical applications of such core-less transformer designs.
A partial core, normally formed from ferromagnetic or ferrite laminated material addresses some of the deficiencies of a core-less transformer. The core material typically is present only within the internal space of the windings and forms a non- closed, discontinuous magnetic path. Part of the coupling magnetic field of the transformer propagates through non-magnetic material, e.g. air.
In comparison to a full core, the reduced size of the partial core reduces core and magnetization losses, whilst significant savings are possible in the core and winding material volumes. Partial core transformers have typically been used in high frequency applications.
However, despite the substantial prior art relating to all aspects of transformer design and operation a transformer incorporating the combination of low frequency, high voltage and a partial core (operating in either ambient or superconducting temperature conditions) has not been explored.
Disclosure of Invention
It is therefore an object of the present invention to substantially ameliorate the aforesaid disadvantages by the provision of a partially cored transformer capable of operating at low frequency and high voltages.
It is a further object of the present invention to provide a power transformer capable of operating under ambient or superconducting temperature conditions.
The present invention provides a transformer designed to operate in the low frequency range of 30-3000 Hz at a primary voltage of the order of 100V or above, wherein said transformer includes a primary winding and a secondary winding both of electrically conductive material and configured to at least partially surround a partial core; the primary winding and secondary winding are electrically insulated from each other and from the partial core, and are arranged such that a magnetic flux generated by the application of an alternating current to one of said windings links the other of said windings to induce a voltage therein; and wherein said partial core is made of ferromagnetic material and does not form a closed, continuous magnetic path.
Preferably, said core may be formed from a laminated construction.
Preferably, at least one of said windings is formed from high-temperature superconducting tape.
The said transformer may be capable of immersion in a cryogenic liquid to permit superconducting operation
Brief Description of Drawings
By way of example only, preferred embodiments of the present invention are described in detail with reference to the accompanying drawings, in which: Fig 1. shows a perspective view of a partial longitudinal section of a first embodiment of the present invention,
Fig 2. shows an end view of a second embodiment of the present invention.
Best Mode for Carrying out the Invention
Fig 1 shows a longitudinal section through the core and winding assembly of a power transformer according to a preferred embodiment of the present invention. The transformer 1 consists of a partial core 2, a primary winding 3 and a secondary winding 4. In this embodiment, the partial core 2 may be made of a metallic, ferromagnetic material, formed as a solid elongated element with a constant rectangular cross-section and laminated to reduce eddy current losses. The partial core 2 is enveloped about its longitudinal length by a central former 5 with a longitudinal slit, formed from a non-magnetic non-conducting or conducting material.
The secondary low voltage winding 4 is wound directly about the exterior surface of the former 5 in the series of concentric layers and is connected to a suitable AC power outlet (not shown). The outer layer of the secondary windings 4 is covered by an insulating layer 6 about which the primary winding 3 is directly wound in a corresponding series of concentric layers. The ends of the primary winding 3 are connected to a single or three phase input AC power supply with a frequency between 30Hz to 3000Hz. The winding 3,4 materials will typically be copper or aluminium wire to minimize the effects of winding heating losses.
As will be appreciated by those versed in the art, the position of the primary and secondary windings 3,4 may be reversed, or be wound concurrently.
Although the partial core may extend beyond the volume enclosed by the turns of the windings 3,4 it does not form a complete, continuous closed magnetic path.
In either of the aforesaid embodiments, the windings 3,4 or the entire transformer unit 1 may be immersed in a cryogenic liquid such as liquid nitrogen. This permits a sufficient reduction in the operating temperature of the transformer 1 to enable superconduction, effectively creating zero resistance and thus generating zero heat losses in the windings.
In the case of a transformer specifically designed for operation at superconducting temperatures, the material used to form one or both of the windings 3,4 can be high- temperature superconducting tape.
Naturally, the transformer need not be square/rectangular in cross-section and Fig 2 shows a corresponding cross-section of an alternative embodiment with a circular configuration.
In this embodiment, the partial core 2, former 5 and insulating layer 6 all are as described with reference to Fig. 1 , apart from being of circular, rather than rectangular, cross-section.
However, the primary winding 3a is wound on the former 5, and the secondary winding 4a is wound over the insulating layer 6, surrounding the primary.
In all other respects, the Fig. 2 embodiment is constructed and operates as the Fig. 1 embodiment.
The type of transformer described with reference to Fig. 2 (but of rectangular cross- section) has been found to be suitable for incorporation into an arc welder.
This arc welder is designed to operate off the mains supply, with an operational frequency of 50 Hz and a primary voltage of 230V rms.
The partial core 2 is made of laminated ferromagnetic material, with the laminations 0.5 mm thick, forming a partial core 195 mm long with a rectangular cross-section of 38 x 43 mm. The laminations are enclosed in a tube 5 of insulation material to hold them together. The tube 5 also provides electrical insulating between the core 2 and the primary winding 3a, and acts as a former for the primary winding.
The primary winding 3a consists of 836 turns of 1.9 mm diameter copper wire, wound in ten layers around the tube 5.
An insulating layer 6 insulates the primary winding 3a from the secondary winding 4a, which consists of 158 turns of 4 mm copper wire, wound in four layers.
The external diameter of the welder is 130 mm, with a weight of approximately 14 kg.
In operation, the secondary winding was terminated with one connection to the metal to be welded and the other connection to an appropriately - sized welding rod (e.g. 2.5 mm diameter) of a metal similar to that to be welded. Arc welding is then achieved in the usual manner, by striking an arc between the welding rod and the metal to be welded.
The striking or open circuit secondary voltage is 44V. Under these conditions, the primary current is 11 A. Under arcing conditions, the secondary voltage is 24V, with a secondary current of 95A and a primary current of 22A. The supply power factor is 0.98 lagging. The duty cycle for the welder is estimated to be approximately 25%.
the above-described performance can be compared to that of a commercially available full core transformer based welder, with name plate readings for a 50 Hz, 230V, 10A supply, duty cycle of 25% and a nominal welding rod current of 105A for a 2.5 mm diameter welding rod. The transformer core dimensions are 155 x 135 x 90 mm, with windings of the order of 35 x 35 mm cross-sectional area. The transformer weighs 18 kg.
The transformer of the present invention is significantly simpler in design than a conventional (i.e. full-core) transformer, and as a result is simpler and thus cheaper to manufacture, but without any sacrifice of efficiency of operation.

Claims (10)

1. A transformer designed to operate in the low frequency range of 30-3000 Hz at a primary voltage of the order of 100V or above, wherein said transformer includes a primary winding and a secondary winding both of electrically conductive material and configured to at least partially surround a partial core; the primary winding and secondary winding are electrically insulated from each other and from the partial core, and are arranged such that a magnetic flux generated by the application of an alternating current to one of said windings links the other of said windings to induce a voltage therein; and wherein said partial core is made of ferromagnetic material and does not form a closed, continuous magnetic path.
2. The transformer as claimed in Claim 1 , wherein the primary winding surrounds the secondary winding.
The transformer as claimed in Claim 1 , wherein the secondary winding surrounds the primary winding.
4. The transformer as claimed in Claim 1 , wherein the primary and secondary windings are wound concurrently.
The transformer as claimed in any one of the preceding claims wherein the core is laminated.
6. The transformer as claimed in any one of the preceding claims wherein one of said windings is made of high-temperature super conducting tape.
7. The transformer as claimed in any one of Claims 1-5, wherein both of said windings are made of high-temperature superconducting tape.
8. An arc welder incorporating a transformer as claimed in any one of the preceding claims.
9. A method of operating a transformer as claimed in any one of claims 1-7, wherein said primary winding is connected to an alterating-current power supply having a frequency in the range 30-3000 Hz and a voltage of the order of 100V or greater.
10. A method of operating a transformer as claimed in Claim 6 or Claim 7, wherein said transformer is immersed in a cryogenic liquid.
AU2001260837A 2000-05-11 2001-05-11 Partial core, low frequency transformer Abandoned AU2001260837A1 (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
NZ504474 2000-05-11
NZ50447400 2000-05-11
PCT/NZ2001/000089 WO2001086667A1 (en) 2000-05-11 2001-05-11 Partial core, low frequency transformer

Publications (1)

Publication Number Publication Date
AU2001260837A1 true AU2001260837A1 (en) 2001-11-20

Family

ID=19927875

Family Applications (1)

Application Number Title Priority Date Filing Date
AU2001260837A Abandoned AU2001260837A1 (en) 2000-05-11 2001-05-11 Partial core, low frequency transformer

Country Status (4)

Country Link
US (1) US20030174039A1 (en)
EP (1) EP1297541A1 (en)
AU (1) AU2001260837A1 (en)
WO (1) WO2001086667A1 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011161772A1 (en) * 2010-06-22 2011-12-29 住友電気工業株式会社 Reactor
JP6598084B2 (en) * 2017-02-22 2019-10-30 株式会社オートネットワーク技術研究所 Coil and reactor

Family Cites Families (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2764745A (en) * 1954-03-02 1956-09-25 Gen Electric Autotransformer
US3233154A (en) * 1962-12-17 1966-02-01 Nat Res Corp Solenoid coil wound with a continuous superconductive ribbon
US3499216A (en) * 1964-08-05 1970-03-10 Mini Ind Constructillor Manufacturing process for magnet steel strips with oriented grains
DE3017368A1 (en) * 1980-05-07 1981-11-12 Licentia Patent-Verwaltungs-Gmbh, 6000 Frankfurt LINE TRANSFORMER FOR A TELEVISION RECEIVER
JPS60172319U (en) * 1984-04-21 1985-11-15 株式会社村田製作所 flyback transformer
EP0303994B1 (en) * 1987-08-21 1993-05-05 Nippon Telegraph And Telephone Corporation Push-pull current-fed dc-dc converter
US5204650A (en) * 1990-04-27 1993-04-20 Railway Technical Research Institute Switch for controlling current flow in superconductors
JP2774672B2 (en) * 1990-06-28 1998-07-09 東京電力株式会社 Superconducting current limiter
DE19515226A1 (en) * 1995-04-28 1996-11-07 Thomson Brandt Gmbh High voltage transformer for a television receiver
DE19528185A1 (en) * 1995-08-01 1997-02-06 Thomson Brandt Gmbh transformer
SE9504650L (en) * 1995-12-27 1997-05-12 Asea Brown Boveri Transformer with superconducting windings

Also Published As

Publication number Publication date
WO2001086667A1 (en) 2001-11-15
EP1297541A1 (en) 2003-04-02
US20030174039A1 (en) 2003-09-18

Similar Documents

Publication Publication Date Title
RU2467445C2 (en) Short-circuit current limiter
US4520335A (en) Transformer with ferromagnetic circuits of unequal saturation inductions
AU717413B2 (en) Improved superconducting inductors
US5339061A (en) Iron-free transformer
US6914511B2 (en) Superconducting transformer
GB2211671A (en) Electromagnetic devices with superconducting windings
EP0900444B1 (en) A controllable inductor
AU2008318277A1 (en) High voltage saturated core fault current limiter
RU2320045C1 (en) Transformer
JPH0787134B2 (en) Electrical components with inductive and capacitive properties
US5334964A (en) Current limiting choke coil
FI107845B (en) Choke filter choke for high energy loss
KR101590922B1 (en) Arrangement having a superconductive cable
WO2003079379A1 (en) Composite core nonlinear reactor and induction power receiving circuit
US20030174039A1 (en) Partial core, low frequency transformer
US5539369A (en) Multiple-toroid induction device
US7019608B2 (en) Superconducting transformer
JPH1116751A (en) Transformer
US4213076A (en) Constant-current transformer for gas-discharge tubes
CA1158325A (en) Core for electromagnetic induction device
Rahimi-Kian et al. Minimum loss design of a 100 kHz inductor with litz wire
AU2001239019B2 (en) A superconducting transformer
Bodger et al. Towards a usable mains frequency partial core transformer
JPH08130134A (en) Superconducting coreless transformer
Denisov et al. The cascade transformer for the high-voltage electron cooling system for the NICA collider