The present invention relates generally to the field of thermal management structures for power electronic circuits and the like. More particularly, the invention relates to the cooling of resistors, such as brake resistors used in inverters and other power electronic devices.
Resistors are used in power electronic devices for a range of reasons. Firstly, such resistors may operatively figure as part of the overall power signal conditioning or control scheme. However, other resistors are used to dissipate energy, such as in the case of motor drives, power converters, and so forth. Such brake resistors may be associated, for example, with a DC bus extending between a rectifier and a converter (e.g., an inverter). The resistors may be switched into the circuit when necessary to dissipate energy, such as for braking an inertial load. Because resistors develop significant heat due to their internal resistance and the current flowing through them during operation, heat dissipation is often a challenge for their use.
Conventional approaches to cooling resistors, particularly brake resistors, having included the use of monolithic heat spreaders, radiant and convective thermal transfer, and transfer to a circulated cooling medium, such as water. However, in many settings, the resistors may generate more heat than can be adequately transmitted to the environment by conventional means. Water circulating systems are often undesirable due to their complexity and the potential for leaks. Many conventional cooling schemes also fail adequately to reduce temperature differences or gradients in structures surrounding the resistor.
There is a need, therefore, for improved approaches to thermal management of resistive structures, such as brake resistors. There is particular need for a technique which would allow for heat to be extracted from a brake resistor in a packaged or modular structure, and that would render the structure and the overall circuitry more isothermal than conventional arrangements.
The present invention provides an approach to resistive element cooling designed to respond to such needs. The approach may be used in a variety of applications and settings. It is particularly well suited to cooling large resistors from which substantial quantities of heat should be extracted. A particular setting for the approach is in cooling brake resistors, such as those used in motor drive, vehicle drive, and similar applications.
In accordance with aspects of the invention, a phase change heat spreader or cooling device is disposed adjacent to a resistor to be cooled. The resistor may take any suitable form. However, a planar resistor arrangement is particularly attractive insomuch as it may be placed in closer proximity to the heat spreader. The resistor may be placed in a modular enclosure, and the heat spreader either disposed adjacent to a side of the enclosure, or incorporated directly therein (e.g., as one side of the device. Moreover, such heat spreaders may be associated with more than one side of the enclosure.
In operation, the resistor generates heat due to current flowing through it, and heat is drawn from the resistor by a continuous phase change cycle that occurs within the phase change heat spreader. Because the phase change occurs over a large area within the heat spreader, heat within structures surrounding the resistor, such as the enclosure surfaces, is distributed more evenly, rendering the structures more isothermal.
These and other features, aspects, and advantages of the present invention will become better understood when the following detailed description is read with reference to the accompanying drawings in which like characters represent like parts throughout the drawings, wherein:
Turning now to the drawings, and referring first to
In the embodiment illustrated in
A range of other components may be included in the circuitry illustrated in
Circuitry such as that illustrated in
Certain locations, components, modules or subsystems of the power electronic circuitry 10 may make use of a phase change heat spreader or cooling device in accordance with aspects of the invention. In general, such devices may be employed to improve heat transfer from heat sources, such as switched components, un-switched components, busses and conductors, connection points, and any other source of heat. As will be appreciated by those skilled in the art, during operation many of the components of such circuitry may produce heat generally by conduction losses in the component, or between components. Such heat will generally form hot spots, which may be thought of as regions of high thermal gradient. Conventional approaches to extracting heat to reduce the temperature of such sources include extracting heat by conduction in copper or other conductive elements, circulation of air or other fluids, such a water, and so forth. The present approach makes use of phase change devices that not only improve the extraction of heat from such sources, but aid in distributing the heat to render the heat sources and neighboring areas of the circuitry more isothermal.
In the embodiment illustrated in
A phase change heat spreader or cooling device, in accordance with the present invention, is used to extract heat from one or more resistive devices, such as brake resistors of the type discussed above with reference to
As shown in
Within the enclosure, the resistive element 58 is disposed on a dielectric material or insulator 60. The insulator is, in turn, thermally bonded to the base 66, such as by means of a solder, thermal grease or the like. The leads of the resistive element 58 (see,
In operation, the resistive element may be switched in and out of the circuit as desired, and dissipates energy through resistive losses. The resulting energy is easily transmitted through the insulating layer 60 and thermal bonding layer 68 to the phase change heat spreader or cooling device 66. While locations immediately below the resistive element will typically be hotter than other locations in the enclosure, the phase change heat spreader will aid in distributing this heat over a larger area, rendering the entire device more isothermal, and lowering the overall operating temperature.
The present technique is thus based upon the use of a phase change cooling device which can be closely associated with or integrated into a package with the resistive element. The resistive element itself may be generally conventional in structure or, as discussed above, may be designed specifically to provide a more planar profile for packaging. It should be noted that similar phase change heat spreaders may be disposed adjacent to multiple sides of the enclosure in which the resistive element is positioned. On the one or more sides from which heat is to be dissipated, the phase change cooling device or devices allow for evaporation and recondensation of an internal cooling fluid. The change in phase extracts heat from the resistive element package. The cooling device may extend over an expanded area of the package to render the overall package more isothermal than conventional devices. The resulting heat extraction reduces the temperature of the package, and particularly the maximum temperature reached by the resistive element, allowing for extended life, high power ratings, and higher power density.
It should be noted that various alternative packaging arrangements may be designed for cooling resistive elements. For example, in the foregoing arrangement, the resistive element is disposed at least partially in an enclosure. Such enclosures may be preferred to reduce the exposure of the elements to the environment and to personnel. Alternatively one or more resistive elements may be similarly completely encased in an enclosure. Still further, cooled resistive structures may be designed that are not individually enclosed, but that are placed in a housing or enclosure with other components, such as in a converter or drive package.
It should also be noted that in the embodiment described above, and in various presently contemplated alternative arrangements, the “base” of the structure is not intended to be limited. That is, the base on which the resistive element is ultimately disposed (e.g., with or without intervening layers or materials) may be an integral part of an enclosure. However, this need not be the case. More generally, the base is simply one or more underlying structures between the resistive element and the phase change heat spreader. The base itself may even be part of the heat spreader itself, such as the evaporator plate of the arrangement described below with respect to
An exemplary phase change heat spreader is illustrated in section in
The various materials of construction for a suitable phase change cooling device may vary by application, but will generally include materials that exhibit excellent thermal transfer properties, such as copper and its alloys. The wick structures may be formed of a similar material, and provide spaces, interstices or sufficient porosity to permit condensate to be drawn through the wick structures and brought into proximity of the evaporator plate. Presently contemplated materials include metal meshes, sintered metals, such as copper, and so forth. In operation, a cooling fluid, such as water, is sealingly contained in the inner volume 80 of the device and the partial pressure reigning in the internal volume allows for evaporation of the cooling fluid from the primary wick structure due to heating of the evaporator plate. Vapor released by the resulting phase change will condense on the secondary wick structure and the condenser plate, resulting in significant release of heat to the condenser plate. To complete the cycle, the condensate, indicated generally by reference numeral 86 in
It should be noted that, as mentioned above, and in further embodiments described below, the phase change heat spreader may be designed as an “add-on” device, or may be integrated into the design of the resistive element module (typically as a support or substrate). Similarly, the fins on the various structures may be integral to the heat spreader, such as with the condenser plate. Also, the cooling media used within the heat spreader may include various suitable fluids, and water-based fluids are one example only. Finally, the ultimate heat removal, such as via the fins or other heat dissipating structures, may be to gasses, liquids, or both, through natural of forced convection, or a combination of such heat transfer modes. More generally, the fins described herein represent one form of heat dissipation structure, while others may be used instead or in conjunction with such fins.
While only certain features of the invention have been illustrated and described herein, many modifications and changes will occur to those skilled in the art. It is, therefore, to be understood that the appended claims are intended to cover all such modifications and changes as fall within the true spirit of the invention.
Number | Name | Date | Kind |
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4716396 | Kneifel | Dec 1987 | A |
5990780 | Caddock, Jr. | Nov 1999 | A |
6166937 | Yamamura et al. | Dec 2000 | A |
6490159 | Goenka et al. | Dec 2002 | B1 |
6522239 | Peschl | Feb 2003 | B1 |
6979843 | Nakajima et al. | Dec 2005 | B2 |
Number | Date | Country | |
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20080266046 A1 | Oct 2008 | US |