The present invention relates generally to a heat transfer apparatus, and more particularly to a heat pipe having a honeycombed wick structure.
It is well known that a heat pipe is generally a vacuum-sealed pipe. A porous wick structure is provided on an inner face of the pipe, and the pipe is filled with at least a phase changeable working media employed to carry heat. Generally, according to positions from which heat is input or output, the heat pipe has three sections, an evaporating section, a condensing section and an adiabatic section between the evaporating section and the condensing section.
In use, the heat pipe transfers heat from one place to another place mainly by virtue of phase change of the working media taking place therein. Generally, the working media is liquid such as alcohol, water and the like. When the working media in the evaporating section of the heat pipe is heated up, it evaporates, and a pressure difference is thus produced between the evaporating section and the condensing section in the heat pipe. As a result vapor with high enthalpy flows to the condensing section and condenses there. Then the condensed liquid reflows to the evaporating section along the wick structure. This evaporating/condensing cycle continues in the heat pipe; consequently, heat can be continuously transferred from the evaporating section to the condensing section. Due to the continual phase change of the working media, the evaporating section is kept at or near the same temperature as the condensing section of the heat pipe.
However, during the phase change of the working media, the resultant vapor and the condensed liquid flows along two opposite directions, which reduces the speed of the condensed liquid in returning back to the evaporating section and therefore limits the heat transfer performance of the heat pipe. As a result, a heat pipe often suffers from drying-out at the evaporating section as the condensed liquid cannot be timely sent back to the evaporating section of the heat pipe.
In general, movement of the working fluid from the condensing section to the evaporating section depends on capillary action of the wick structure. The wick structure currently available for the heat pipe includes fine grooves integrally formed at the inner walls of the casing, screen mesh or bundles of fiber inserted into the casing and held against the inner walls thereof, or sintered powder combined to the inner walls through a sintering process.
However it is hard to obtain consistent characters during mass production of these wicks. Porosity of the wicks is difficult to control, which leads to varying thermal performances among heat pipes. Furthermore, the porosity of the wicks is limited to a small range, whereby a thermal resistance of the heat pipe is high. This also affects the heat dissipating performance of the heat pipe.
Therefore, it is desirable to provide a heat pipe having a honeycombed wick structure which can over the shortcomings of the related art.
The present invention relates to a heat pipe. The heat pipe includes a hollow metal casing and a honeycombed wick structure arranged at an inner surface of the hollow metal casing. The wick structure includes a plurality of slices stacked together. Each of the slices has a plurality of pores therein and a plurality of protrusions formed thereon along a longitudinal direction of the heat pipe to form a plurality liquid channels between the protrusions. Each of the liquid channels has alternate large and small sections along a length of the liquid channel. The liquid channels are communicated with micro-channels between two neighboring ones of the slices. The design of the liquid channels helps condensed liquid in the heat pipe to accelerate to return to an evaporating section from a condensing section of the heat pipe via the micro-channels.
Other advantages and novel features of the present invention will become more apparent from the following detailed description of preferred embodiment when taken in conjunction with the accompanying drawings, in which:
Many aspects of the present device can be better understood with reference to the following drawings. The components in the drawings are not necessarily drawn to scale, the emphasis instead being placed upon clearly illustrating the principles of the present device. Moreover, in the drawings, like reference numerals designate corresponding parts throughout the several views.
The casing 100 includes an evaporating section 400 and a condensing section 600 at respective opposite ends thereof, and an adiabatic section 500 located between the evaporating section 40 and the condensing section 600. The casing 100 is typically made of highly thermally conductive materials such as copper or copper alloys. The honeycombed wick structure 200 is saturated with a working fluid (not shown), which acts as a heat carrier for carrying thermal energy from the evaporating section 400 toward the condensing section 600 when undergoing a phase transition from liquid state to vapor state. A vapor channel 300 is defined in the casing 100 along a lengthwise direction of the heat pipe.
Referring to
Each of the first slices 210 has a wave-shaped configuration when expanded, consisting of a plurality of triangular sections (not labeled) arranged along a circle. Each of the second slices 220 has a planar type configuration when expanded, and is wrapped into a circle sandwiched between two first slices 210. The first and second slices 210, 220 respectively define a plurality of pores (not shown) therein to form the honeycombed wick structure 200 with a plurality of micro-channels 211 therebetween for reflowing of the condensed liquid. The condensed liquid can flow from one micro-channel 211 to a neighboring micro-channel 211 via the pores. The first and second slices 210, 220 are made of metal sheets.
Referring to
Specifically, when the working fluid contained in the honeycombed wick structure 200 receives heat from a heat source in thermal connection with the evaporating section 400 of the heat pipe and turns into vapor, the vapor is quickly transferred toward the condensing section 600 via the vapor channel 300. At the condensing section 600, the vapor releases its heat and turns into liquid. Then, the condensed liquid is brought back, via the honeycombed wick structure 200, to the evaporating section 400 of the heat pipe where it is available again for evaporation.
Due to the honeycombed wick structure 200 being made of the first and second slices 210, 220 having the plurality of liquid channels 230 therein which have the plurality of narrow sections 231, the velocity of the liquid can be increased as flowing through the micro-channels 211 of the honeycombed wick structure 200. Moreover, porosity of the honeycombed wick structure 200 is relatively easy to control by regulating the configuration of the protrusions 222, and the number and size of the pores defined in the slices 210, 220; accordingly, heat transfer performance of the heat pipe can be further improved.
The protrusions of the previous embodiments of the invention can also be round in cross section shape, although other shapes such as triangular or crescent or the like may also be suitable, only if the protrusions allow the cross section of the liquid channel to vary along its extending direction.
It is known that porosity of the wick structure is an important parameter for the heat transfer capacity of the heat pipe. The honeycombed wick structure 200 of the invention is made of the plurality of first and second slices stacked together and having the plurality of protrusions thereon, whereby the porosity of the honeycombed wick structure 200 can be accurately controlled to improve the heat transfer performance of the heat pipe.
It is to be understood, however, that even though numerous characteristics and advantages of the present invention have been set forth in the foregoing description, together with details of the structure and function of the invention, the disclosure is illustrative only, and changes may be made in detail, especially in matters of shape, size, and arrangement of parts within the principles of the invention to the full extent indicated by the broad general meaning of the terms in which the appended claims are expressed.
Number | Name | Date | Kind |
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3018087 | Steele | Jan 1962 | A |
3532158 | Hiebert | Oct 1970 | A |
3613778 | Feldman, Jr. | Oct 1971 | A |
3735806 | Kirkpatrick | May 1973 | A |
4220195 | Borgoyn et al. | Sep 1980 | A |
6003591 | Campbell | Dec 1999 | A |
20050077030 | Wong | Apr 2005 | A1 |
Number | Date | Country |
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52024366 | Feb 1977 | JP |
55126788 | Sep 1980 | JP |
61093391 | May 1986 | JP |
Number | Date | Country | |
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20070277963 A1 | Dec 2007 | US |