The present invention pertains generally to inductors. More particularly, the present invention pertains to inductors designed for repetitively pulsed, high current applications. The present invention is particularly, but not exclusively, useful as an inductance coil for high current applications in which a relatively long service life is required.
Inductance coils are commonly used in various electrical, electronic and electromechanical applications. It is well known that the electrical characteristics of an inductance coil are dependent on the size and shape (e.g. the number of coil turns) of the coil, as well as a number of other factors. In practice, inductance coils are designed with a particular purpose in mind, and as a consequence, it is a basic design requirement that an inductance coil maintain its original electrical characteristics during its service life. This, in turn, implies that the inductance coil maintain its original shape (i.e. does not deform or fracture in service).
In use, inductance coils generate magnetic fields which are proportional in strength to the current that is passed through the coil. These magnetic fields, in turn, generate magnetic forces, the strength of which are proportional to the square of the magnitude of the magnetic fields. When relatively high currents are passed through single layer inductance coils, strong magnetic forces are generated that can deform the coil.
During high current flow, wires in single layer solenoid inductors are exposed to significant magnetic forces. Relative to a circular coil, these forces comprise or include two primary components. The first component is oriented perpendicular to the axis of the coil and produces a hoop stress in the wire. This hoop stress results from the magnetic pressure that is generated by the relatively high field inside the coil and the relatively low field outside the coil. In addition, there is a “turn to turn” force on the wires that causes the wires next to each other to be pulled together. This “turn to turn” force is most pronounced on the ends of the coil and causes the wires on the end of the coil to try to move toward the center of the coil. The forces balance near the center of the inductor and these axial forces are less of a concern at the center of the coil. On the other hand, because the forces are strong near the coil ends, the termination of the coil ends must withstand relatively strong forces.
The above-described axial forces can also cause unrestrained cyclic deformations (which are typically more pronounced when pulsed currents are used) that can lead to fatigue failure and result in a relatively short inductor service life. In addition, another factor that must be considered is the heating (i.e. ohmic heating) that occurs during current flow through the inductor. Prior art devices in which the coil is completely embedded in a dielectric structure (e.g. fiberglass) are prone to overheating. Overheating of the inductance coil can alter the electrical characteristics of an inductance coil and decrease fatigue cycles to failure. Although the problem of overheating may be overcome by using a hollow, tubular conductor as an inductor coil and passing a cooling fluid therethrough, this solution is overly complicated and typically requires cooling lines, pumps and controllers.
In light of the above, it is an object of the present invention to provide an inductor that has a relatively long service life when used with relatively high currents that are repetitively pulsed. It is another object of the present invention to provide a high pulsed current inductor which maintains a suitable service temperature and does not overheat in use. Yet another object of the present invention is to provide a high pulsed current inductor and a method for manufacturing a high pulsed current inductor which are easy to use, relatively simple to implement, and comparatively cost effective.
The present invention is directed to an inductor for use in applications in which a relatively high current is passed through the inductor. In some applications, a repetitively pulsed, high current is passed through the inductor. For the present invention, the inductor includes a nonconductive, tubular form which is typically made of a glass—epoxy composite material. Within this tubular shape, the form defines a tube axis and has an outer surface which is typically cylindrically shaped. For the inductor envisioned by the present invention, the outer surface is formed with a groove that extends substantially helically about the tube axis.
For the present invention, the inductor also includes a coiled, conductive wire that is formed with a plurality of turns. The wire is wound around the outer surface of the form with at least a portion of the wire disposed in the groove. With this interactive cooperation of structure, the form maintains a predetermined separation between adjacent turns of the coil. More specifically, the form prevents deformation of the coil wire by the strong magnetic forces that are generated when high electrical currents are passed through the wire.
In another aspect of the present invention, a mechanism is provided to clamp the ends of the wire to the form. More specifically, the ends of the wire are clamped into a conductive terminal (e.g. copper) with stainless steel clamps that are positioned outside the tubular form where the magnetic fields generated by the high currents are relatively low. The conductive terminal, in turn, includes provisions for electrical connections to bus bars which connect to other circuit elements.
Structurally, the inductor can include a pair of saddles that are made of a nonmagnetic material such as stainless steel. For the inductor of the present invention, a saddle is positioned at each end of the form. Each saddle includes an inner saddle member that is located inside the form, and is positioned against the inner surface of the tubular form. In addition, each saddle includes an outer saddle member that is located outside the form, and is positioned against the outer surface of the tubular form. A fastening system (e.g. one or more high strength stainless steel bolts) is provided for each saddle that extends through the tubular form to attach the inner saddle member to the outer saddle member. Each conductive clamp, between the inductor and the conductive terminal, is then mounted on a respective outer saddle member. This cooperation of structure allows only high strength, nonmagnetic portions of the saddle/clamp system to be located within the tubular form where relatively strong magnetic fields are generated.
In a particular embodiment of the present invention, the inductor is designed to be mounted on a flat mounting plate together with various other components. For this purpose, the inductor can include a pair of insulating members, with each insulating member affixed to a respective outer saddle member. Each insulating member, in turn, is attached to the mounting plate. In another aspect of the present invention, a shroud can be mounted on the mounting plate and used to partially cover the form and coil wire. A fan is then activated to pass air through a volume defined by the shroud to cool the partially exposed wire.
The novel features of this invention, as well as the invention itself, both as to its structure and its operation, will be best understood from the accompanying drawings, taken in conjunction with the accompanying description, in which similar reference characters refer to similar parts, and in which:
Referring to
A more detailed understanding of the form 12 used in the inductor 10 can be obtained with cross-reference to
Continuing with cross-reference to
With the wire coil 14 disposed in the groove 20 as shown in
Turning now to
Referring back to
This structure of the saddles 32a,b results in only high strength, nonmagnetic portions of the saddle/clamp system to be located within the tubular form 12 where relatively strong magnetic fields are generated. Specifically, the saddles 32a,b allow the conductive terminals 24a,b and bus bar 30 to be positioned outside the tubular form 12 where the magnetic field generated by the wire coil 14 is relatively small. In particular, as seen with cross-reference to
While the particular high current, long life inductor as herein shown and disclosed in detail is fully capable of obtaining the objects and providing the advantages herein before stated, it is to be understood that it is merely illustrative of the presently preferred embodiments of the invention and that no limitations are intended to the details of construction or design herein shown other than as described in the appended claims.
This application is a divisional of application Ser. No. 10/728,075, filed Dec. 4, 2003 now U.S. Pat No. 7,005,954, which is currently pending. The contents of application Ser. No. 10/728,075 are incorporated herein by reference.
Number | Name | Date | Kind |
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2591408 | Crankshaw | Apr 1952 | A |
3243746 | Doggart et al. | Mar 1966 | A |
3353040 | Abbott | Nov 1967 | A |
6842101 | Maguire et al. | Jan 2005 | B2 |
Number | Date | Country | |
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20060080829 A1 | Apr 2006 | US |
Number | Date | Country | |
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Parent | 10728075 | Dec 2003 | US |
Child | 11293952 | US |