Pulse transformers for propagating pulses with rapid rise times and fall times are well known, and are described, for example, in the text Pulse, digital and switching waveforms, by Milman & Taub, published in 1965 by McGraw-Hill Publishing Company. Pulse transformers utilizing conventional cores and winding techniques, may not provide the necessary coupling and low leakage characteristics required for ultra narrow pulsewidth and high frequency operation with high voltage isolation, as for example isolation to voltages exceeding 10 kV. The difficulty in achieving good coupling and low leakage inductance is compounded by the additional insulation required to stand off the voltage between the transformer primary side at ground potential and the secondary side at the high voltage potential.
To optimize a transformer for passing low distortion rectangular electrical pulse shapes (pulses with fast rise and fall times at relatively constant amplitude), the transformer needs to have low values of leakage inductance and distributed capacitance, together with high open-circuit inductance. Good transient response is needed to maintain the pulse shape at the secondary winding(s) because slow rise times tend to cause switching losses in power transistors and excessive leakage inductance can generate transient ringing.
Leakage inductance is caused by the imperfect coupling of the primary and secondary windings, which in turn generates a leakage flux which does not link with all turns of the windings. The leakage flux acts as another magnetic component, storing and discharging magnetic energy with each frequency cycle of the electrical signal. The leakage flux acts as an inductor in series with each of the primary and secondary windings. This series inductive reactance then causes a frequency sensitive voltage drop (voltage reduction) that increases with frequency, hence constitutes a severe detriment to high-frequency, wide-bandwidth capability.
The physical design of the magnetic core and of the windings of a pulse transformer contribute to the leakage inductance. For high voltage applications, high insulation resistance and high breakdown voltage are required, and in general require even more separation of the windings, which potentially allows more leakage flux to occur. The more the exposure of the windings outside of the core's magnetic flux circuit and the less the proximity of the primary windings to the secondary windings, the more potential exists for leakage flux and the resultant series inductance.
In general, attempting to achieve low leakage inductance is addressed in the prior art by using either flat wide winding materials with minimal insulation or by using interleaved and twisted windings otherwise known as bifilar windings. For windings with a large number of turns, another method is to sectionalize or break up the winding into smaller alternating sections between primary and secondary windings. Neither approach achieves the required coupling since either the magnetic circuit is not sufficiently enveloped or the number of turns is too low for sectionalizing.
The existing design of twisting the primary and secondary windings together in a bifilar fashion on a toroidal magnetic core, as described for example by Milman & Taub, may compromise system performance, as the coupling may be less than desired, and leakage inductance may be excessive for the required performance at the frequencies and pulse shapes required.
Improved pulse transformers are desired.
A transformer comprises a magnetic core defining first and second apertures which extend therethrough. An electrical first conductor has a tubular shape, and extends through the first and second apertures. A twisted pair of insulated second and third conductors extends through the first conductor. The first conductor may be insulated where it passes through the core.
A transformer comprises a magnetic core defining first and second apertures extending therethrough. The first aperture defines first and second ends, and the second aperture defines first and second ends. The transformer further includes an electrical first conductor defining at least a local axis of elongation and also defining first and second ends. The first conductor extends through the first and second apertures in such a manner that the first end of the first conductor lies adjacent to the second end of the first conductor. The first conductor may be insulated at locations near where it passes through the first and second apertures. The first conductor has a generally tubular shape defining an opening extending generally parallel with the axis of elongation from the first to the second end of the first conductor. The transformer also includes a twisted pair of first and second insulated conductors, longer than the length of the first conductor. The twisted pair extends through the opening of the first conductor, at least from the first end to the second end of the opening of the first conductor. Each end of the first insulated conductor lacks, or is stripped of, insulation, and each end of the second insulated conductor lacks, or is stripped of, insulation at a location without the opening of the first conductor. In a particular embodiment, the apertures extending through the core are mutually parallel, and the first aperture defines first and second ends, and the second aperture defines first and second ends. The first ends of the first and second apertures are mutually adjacent, and the second ends of the first and second apertures being mutually adjacent. In one version, the magnetic core defines mutually parallel first and second planes, with the first apertures being defined in the first plane and the second apertures being defined in the second plane. The first and second ends of the first conductor may be physically and electrically connected to connection leads, and the connection leads may be, when the first conductor is a braided conductor, extensions of the braid of the braided conductor. In another version, the aperture extending through the first conductor may contain a plurality, greater than two, of electrical conductors twisted together.
A transformer according to another aspect of the disclosure comprises a magnetic core defining first and second apertures extending therethrough. The first aperture defines first and second ends, and the second aperture defines first and second ends. The transformer includes an electrical first conductor defining an axis of elongation and also defining first and second ends. The first conductor extends into the first end of the first aperture and exits from the second end of the first aperture, and extends from the second end of the first aperture to the second end of the second aperture, and extends into or enters the second end of the second aperture, and exits from the first end of the second aperture. The first conductor has a generally tubular shape defining an opening extending generally parallel with the axis of elongation from the first to the second end of the first conductor. The first conductor may be insulated near the region in which it passes through the first and second apertures. The transformer also comprises a twisted conductor pair, longer than the length of the first conductor, of first and second insulated conductors. The twisted pair of conductors extends at least from the first end to the second end of the opening of the first conductor. Each end of the first and second insulated conductors lacks or is without insulation at a location without the first conductor.
Magnetic coupling can be varied through several parameters including transformer core material or size, winding material, number of winding turns or winding wire size and can be directly improved by the close proximity of the primary windings to the core, close proximity of the secondary windings to the core, and close proximity of the primary to secondary windings.
In order to improve the magnetic coupling on a low-turns-ratio, high-voltage-isolation pulse transformer, both primary and secondary windings require maximum envelopment by the core. A multi-aperture core was used which provided two openings into an elongated ferrite core. See
The next parameter requiring improvement is to maximize coupling between the primary and secondary windings. In order to accomplish maximum coupling, a coaxial winding technique was used. Coaxial cable is primarily used to eliminate magnetic fields around the cable by surrounding an inner conductor with current flowing in one direction with an outer conductor carrying the return current in the opposite direction. This creates magnetic fields that cancel each other due to the superior coupling of the inner to the outer conductors. If one of the currents is reversed such that both currents flow in the same direction and coupling is still the same, the magnetic fields now add in a near ideal condition.
To create a high voltage coaxial primary and secondary winding, a low voltage coaxial cable was used and the inner conductor and dielectric removed, and replaced with the properly rated high voltage wire. The modified coaxial cable was then routed through the multi-aperture core as shown in
An electrical conductor 20 defines first and second ends 201 and 202, respectively. Conductor 20 has a generally tubular form, so that it defines an opening or passage 26 which generally follows a local axis 22 of elongation of conductor 20. The term “local” axis allows for curvature of the axis to follow a bent or deviated course. Conductor 20 may be a braided conductor, as known in the art. Conductor 20 is surrounded, over at least a portion of its length, by a layer 21 of electrical insulation or dielectric material.
The position of conductor 20 (and its insulation 21) in the apertures of core 20 as illustrated in
Conductor 20 of
As an alternative to directly using the braid of a braided conductor 20 of
According to an aspect of the disclosure, an insulated twisted conductor pair 30 extends through opening 26, which extends through the “center” of winding conductor 20. The twisting tends to improve the coupling between the wires of the twisted pair and to reduce the distributed capacitance between the inside of conductor 20 and the wires of the twisted pair.
It should be noted that the terms “between,” “across,” and other terms such as “parallel” have meanings in an electrical context which differ from their meanings in the field of mechanics or in ordinary parlance. More particularly, the term “between” in the context of signal or electrical flow relating to two separate devices, apparatuses or entities does not relate to physical location, but instead refers to the identities of the source and destination of the flow. Thus, flow of signal “between” A and B refers to source and destination, and the flow itself may be by way of a path which is nowhere physically located between the locations of A and B. The term “between” can also define the end points of the electrical field extending “across” or to points of differing voltage or potential, and the electrical conductors making the connection need not necessarily lie physically between the terminals of the source. Similarly, the term “parallel” in an electrical context can mean, for digital signals, the simultaneous generation on separate signal or conductive paths of plural individual signals, which taken together constitute the entire signal. For the case of current, the term “parallel” means that the flow of a current is divided to flow in a plurality of separated conductors, all of which are physically connected together at disparate, spatially separated locations, so that the current travels from one such location to the other by plural paths, which need not be physically parallel.
In addition, discussions of circuits necessarily describe one element at a time, as language is understood in serial time. Consequently, a description of two interconnected elements may describe them as being in “series” or in “parallel,” which will be true for the two elements described. However, further description of the circuit may implicate other interconnected devices, which when connected to the first two devices may result in current flows which contradict the “series” or “parallel” description of the original two devices. This is an unfortunate result of the limitations of language, and all descriptions herein should be understood in that context.
Also, the term “coupled” as used herein includes electrical activity extending from one element to another element either by way of one or more intermediary elements or in the absence of any intermediary element.
Other embodiments of the disclosed transformer will be apparent to those skilled in the art. For example, the hollow conductive winding, illustrated as 420 in
A transformer (10) according to an aspect of the disclosure comprises a magnetic core (12) defining first (14) and second (16) apertures extending therethrough. The first aperture (14) defines first (141) and second (142) ends, and the second (16) aperture defines first (161) and second (162) ends. The transformer (10) further includes an electrical first conductor (20) defining at least a local axis (22) of elongation and also defining first (201) and second (202) ends. The first conductor (20) may be electrically insulated over a portion of its length. The first conductor (20) extends through the first (14) and second (16) apertures in such a manner that the first (201) end of the first conductor (20) lies adjacent to the second end (202) of the first conductor (20). The first conductor (20) has a generally tubular shape defining an opening (26) extending generally parallel with the axis (22) of elongation from the first (241) to the second (242) end of the first conductor (20). The transformer (10) also includes a twisted pair (30) of first (301) and second (302) insulated conductors, longer than the length (L) of the first conductor (20). The twisted pair (30) extends through the opening (26) of the first conductor (20), at least from the first end (201) to the second end (202) of the opening (26) of the first conductor (20). Each end (401, 402) of the first (301) insulated conductor lacks, or is stripped of, insulation, and each end (411, 412) of the second (302) insulated conductor lacks, or is stripped of, insulation at a location without the opening (26) of the first conductor (20). In a particular embodiment, the apertures (14, 16) extending through the core (12) are mutually parallel, and the first (14) aperture defines first (141) and second (142) ends, and the second aperture (16) defines first (161) and second (162) ends. The first ends (141, 161) of the first (14) and second (16) apertures are mutually adjacent, and the second ends (142, 162) of the first and second apertures being mutually adjacent. In one version, the magnetic core (12) defines mutually parallel first (12ps1) and second (12ps2) planes, with the first apertures (141 161) being defined in the first plane (12ps1) and the second apertures (142 162) being defined in the second plane (12ps2). The first (201) and second (202) ends of the first conductor may be physically and electrically connected to connection leads (501, 502; 270), and the connection leads may be, when the first conductor (20) is a braided conductor, extensions of the braid of the braided conductor. In another version, the aperture (26) extending through the first conductor (20) may contain a plurality, greater than two, of electrical conductors twisted together (430). Any of the windings may be viewed as being a primary winding and the others as secondary.
A transformer (10) according to another aspect of the disclosure comprises a magnetic core (12) defining first (14) and second (16) apertures extending therethrough. The first aperture (14) defines first (141) and second (142) ends, and the second (16) aperture defines first (161) and second (162) ends. The transformer includes an electrical first conductor (20) defining an axis (22) of elongation and also defining first (201) and second (202) ends. The first conductor (20) may be electrically insulated over at least a portion of its length. The first conductor (20) extends into the first end (141) of the first aperture (14) and exits from the second end (142) of the first aperture (14), and extends from the second end (142) of the first aperture (14) to the second end (162) of the second aperture (16), and extends into or enters the second end (162) of the second aperture (16), and exits from the first end (161) of the second aperture (16). The first conductor (20) has a generally tubular shape defining an opening (26) extending generally parallel with the axis (22) of elongation from the first (241) to the second (242) end of the first conductor (20). The transformer (10) also comprises a twisted conductor pair (30), longer than the length of the first conductor, of first (301) and second (302) insulated conductors. The twisted pair of conductors (30) extends at least from the first end (261) to the second end (262) of the opening (26) of the first conductor (20). Each end of the first (301) and second (302) insulated conductors lacks insulation, or is absent insulation, or is without insulation at a location without the first conductor (12).
Number | Name | Date | Kind |
---|---|---|---|
2865006 | Sabaroff | Dec 1958 | A |
3725741 | Misencik | Apr 1973 | A |
4052785 | Duncan | Oct 1977 | A |
4119914 | Duncan | Oct 1978 | A |
4222016 | Stock et al. | Sep 1980 | A |
4437019 | Chass | Mar 1984 | A |
4485361 | Bender | Nov 1984 | A |
4584551 | Burgher et al. | Apr 1986 | A |
4791262 | Ando et al. | Dec 1988 | A |
4868533 | Ehrenhalt et al. | Sep 1989 | A |
5216215 | Walker et al. | Jun 1993 | A |
5220297 | Crowhurst | Jun 1993 | A |
5309120 | Koontz | May 1994 | A |
5341281 | Skibinski | Aug 1994 | A |
5736854 | Zuger | Apr 1998 | A |
5841335 | Onishi et al. | Nov 1998 | A |
6040753 | Ramakrishnan et al. | Mar 2000 | A |
6087916 | Kutkut et al. | Jul 2000 | A |
6114924 | Cain et al. | Sep 2000 | A |
6679981 | Pan et al. | Jan 2004 | B1 |
6850142 | Saito et al. | Feb 2005 | B2 |
7061355 | Tanaka et al. | Jun 2006 | B2 |
7796005 | Blankenship et al. | Sep 2010 | B2 |