|Publication number||US20060196651 A1|
|Application number||US 10/517,907|
|Publication date||Sep 7, 2006|
|Filing date||Jun 5, 2003|
|Priority date||Jun 13, 2002|
|Also published as||EP1516371A2, WO2003107440A2, WO2003107440A3|
|Publication number||10517907, 517907, PCT/2003/2431, PCT/GB/2003/002431, PCT/GB/2003/02431, PCT/GB/3/002431, PCT/GB/3/02431, PCT/GB2003/002431, PCT/GB2003/02431, PCT/GB2003002431, PCT/GB200302431, PCT/GB3/002431, PCT/GB3/02431, PCT/GB3002431, PCT/GB302431, US 2006/0196651 A1, US 2006/196651 A1, US 20060196651 A1, US 20060196651A1, US 2006196651 A1, US 2006196651A1, US-A1-20060196651, US-A1-2006196651, US2006/0196651A1, US2006/196651A1, US20060196651 A1, US20060196651A1, US2006196651 A1, US2006196651A1|
|Inventors||Kenneth Board, Gareth Evans, Gareth Jones|
|Original Assignee||Kenneth Board, Evans Gareth P, Gareth Jones|
|Export Citation||BiBTeX, EndNote, RefMan|
|Referenced by (8), Classifications (12), Legal Events (1)|
|External Links: USPTO, USPTO Assignment, Espacenet|
This invention relates to optoelectronic devices, such as light emitting diodes and other semiconductor light sources.
There are several known types of semiconductor light sources. For example, a p-n junction diode, when forward biassed, can be made to emit visible light by application of an energy source, and is known as a light emitting diode or LED. The radiation has a broad spectrum and is spontaneous and non-coherent, and is due to the recombination of electrons and holes which occur when conduction band electrons are captured by valence band holes.
The production of light in semiconductor devices, such as an LED, usually requires an efficient optical system to provide for maximum extraction of light from the active region within the semiconductor, and it is well known to provide, for example, an optical coupling system consisting of a bundle of optical fibres, one end of which is placed in close proximity to the active region or light emitting surface of the device to extract light therefrom.
The efficiency and operation of such semiconductor light sources is adversely affected by an increase in temperature, i.e. it is desirable to maintain the temperature rise of the active device below a critical temperature. However, the application of an electrical energy source to the active device leads to an inevitable rise in temperature of that device. In other words, the physical process of light production is accompanied by the electrical energy which is dissipated as heat, and this heat must be removed effectively in order to avoid the device overheating which would result the efficiency of the light generation process being degraded and possibly the reduction of the operating lifetime of the device due to some heat-related failure mechanism.
It is well known to mount the active device on a heat sink formed of a highly thermally conductive material, such that heat flows down from the active device into the heat sink, thereby drawing unwanted heat away from the active device to cool it and maintain its temperature within design limits.
However, there are two primary disadvantages associated with this method of heat removal, which limit the amount of heat that may be safely removed from the active device. Firstly, the thermal resistance of the overall arrangement is relatively high because heat is required to flow from the active region of the device (which is generally provided at the upper surface of the device, through the substrate on which the active region is formed to the heat sink, the thermal conductivity of the substrate material generally being substantially lower than that of the heat sink material, which is usually copper. Secondly, the transient response is low (i.e. there is a considerable delay between the heat being generated and that heat being drawn away from the device). This low transient response is not only due to the above-mentioned relatively high thermal resistance, but also due to the high thermal capacities of the substrate and the heat sink in combination.
A cooling mechanism that has, in recent years, been introduced to the field of cooling semiconductor devices is the heat pipe. In a heat pipe heat may be applied at a localised area, or evaporator, where the working fluid in the chamber is vaporised absorbing the latent heat of vaporisation. The vapour then flows due to a small pressure gradient, to the opposite side where it condenses and gives up the latent heat of vaporisation. A wick structure along the wall of the heat pipe provides capillary pumping for the liquid to return to the evaporator region thus completing the cycle. This phase change process will cause the condenser side to be nearly isothermal while spreading the energy from the heat source uniformly over the base of the heat sink. Heat pipes have superior heat transfer characteristics compared to more conventional heat removal arrangements, and have been found to be an excellent means to remove unwanted heat from semiconductor devices generally. However, known heat pipes are obviously not suitable for use on the light output side of semiconductor light sources, because they are opaque and would block the light output.
Thus, there are two primary considerations in respect of semiconductor light sources, that of efficient light extraction and that of effective heat removal from (or cooling of) the active device.
We have now devised an arrangement which overcomes the problems outlined above and achieves the object of the invention which is to provide a semiconductor light source in which efficient light extraction and effective heat removal is achieved. Thus in accordance with the present invention, there is provided a heat pipe for use in extracting heat from a semiconductor light source having an active region, the heat pipe comprising a transparent or translucent member of thermally conductive material and defining an optical transmission path therethrough, the heat pipe being adapted to be located proximate to the active region of the semiconductor device to extract heat, when in use.
The present invention extends to a semiconductor light source including an active region and having a heat pipe as defined above located proximate to said active region.
Thus, the heat pipe of the present invention is made of a transparent or translucent material, and has a refractive index or refractive index combination which facilitates the passage of light from the active region where it is generated.
The heat pipe of the present invention has a number of advantages. Firstly, the effective thermal conductivity of a heat pipe is very large and significantly greater than that of a copper (or similar) heat sink, such that temperature rises are substantially lower than in conventional semiconductor light sources. Secondly, the heat generated in the active region of the device can be removed directly from the surface that is emitting light, in addition (or as an alternative to) heat removal through the substrate. Thirdly, the transient response of the overall system including the heat pipe of the present invention is substantially improved because the heat transport function is dependent on the rate of vapour movement and not on the rate at which heat flows through the substrate and heat sink combination of the prior art. Finally, the heat pipe of the present invention has the significant advantage of permitting the passage of light therethrough such that it is suitable for use with a semiconductor light source.
The optical transmission path is preferably provided by means of a channel which runs through the heat pipe. In one preferred embodiment of the invention, the channel is arranged to receive optical transmission means.
The transparent or translucent member preferably comprises a hollow pipe (which can be any closed shape, not necessarily cylindrical) with sealed ends and is made of any suitable thermally conductive transparent or translucent material having the required mechanical strength for the application. A heat pipe is generally at least partially filled with a cooling fluid, such as water, deionised water, or any other suitable working fluid (which may be placed under a partial vacuum so as to lower the boiling point of the liquid). In use, the water in the end of the heat pipe which is closest to the active region is heated by the heat produced by the active region during operation of the device, until it is vaporised, at which point it rises to the cool side of the heat pipe (thus the heat is transported away from the active region as latent heat within the vapour), where it condenses and returns to the hot end of the heat pipe. The condensed liquid may be carried back to the hot end of the heat pipe by gravity. Alternatively or in addition, a wick or similar material which transports liquid by capillary action may be provided, in which case the condensed liquid is carried back to the hot end of the heat pipe by capillary forces in the wick.
In one preferred embodiment of the invention, the heat pipe defines a channel therethrough, in which is disposed a bundle of optical fibres or the like, said optical fibres being substantially circular in cross-section, the gaps between said optical fibres defining capillary channels by means of which heated coolant fluid (whether liquid or vaporised) can be transported towards the cool end of the heat pipe, and by means of which the condensed liquid can be transported from the cool end of the heat pipe back to the hot end (closest to the active region of the device). Thus, in one embodiment of the invention, a bundle of optical fibres placed in close proximity to the light emitting surface of a semiconductor light source would not only act as a light guide but, if made part of the heat pipe system, would allow (or at least aid) swift and effective heat removal when the coolant fluid (which is beneficially transparent) contained in the heat pipe is vaporised, and also return of the condensed fluid back to the cool end of the heat pipe. In another embodiment, a conventional wick structure of transparent material could be used.
An embodiment of the present invention will now be described by way of example only and with reference to the accompanying drawings, in which:
The heat pipe 18 is partially filled with a liquid (preferably transparent, such as water or deionised water or the like).
In use, light can be extracted from the active region of the device 10 via the heat pipe 18, which is transparent (or at least translucent) in nature. At the same time, heat generated by the active region (because of the continuous or intermittent electrical energy applied thereto) is transmitted to the heat pipe 18 (via the upper surface 12 of the device 10), which heats the liquid in the heat pipe 18. The liquid is vaporised and rises toward the top of the heat pipe 18 (which is relatively cool), where it condenses and returns by means of gravity (and the wick 20) to the lower (hot) end of the heat pipe 18. In one embodiment of the present invention, a condenser 22 is provided at the upper (cool) end of the heat pipe 18 to speed up the process of condensing the coolant fluid within the heat pipe 18. However, in another embodiment, heat may simply be removed by convection from the surface of the heat pipe.
Thus the heat pipe of the present invention provides an optical coupling system which also removes heat directly from the surface of the device close to the active region using a transparent heat pipe.
In a preferred embodiment of the present invention, and referring to
Embodiments of the present invention have been described above by way of examples only, and it will be apparent to a person skilled in the art that modifications and variations can be made to the described embodiments, without departing from the scope of the invention as defined by the appended claims.
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|US8292463||Jul 27, 2007||Oct 23, 2012||Koninklijke Philips Electronics N.V.||Illumination module with similar heat and light propagation directions|
|US8378559 *||Aug 20, 2010||Feb 19, 2013||Progressive Cooling Solutions, Inc.||LED bulb for high intensity discharge bulb replacement|
|US8731139||Aug 10, 2011||May 20, 2014||Media Lario S.R.L.||Evaporative thermal management of grazing incidence collectors for EUV lithography|
|US8746975||Jan 23, 2012||Jun 10, 2014||Media Lario S.R.L.||Thermal management systems, assemblies and methods for grazing incidence collectors for EUV lithography|
|US8845137 *||Sep 21, 2010||Sep 30, 2014||Cree, Inc.||Lighting device having heat dissipation element|
|US20100212871 *||Jun 30, 2009||Aug 26, 2010||Furui Precise Component (Kunshan) Co., Ltd.||Heat pipe and manufacturing method thereof|
|US20110043092 *||Aug 20, 2010||Feb 24, 2011||Progressive Cooling Solutions, Inc.||Led bulb for high intensity discharge bulb replacement|
|US20110074270 *||Mar 31, 2011||Cree, Inc.||Lighting device having heat dissipation element|
|International Classification||F21V29/00, F28F1/00, F28D15/02, H01L33/64|
|Cooperative Classification||F21V29/006, H01L33/648, F21Y2101/02, F28D15/02, F21V29/004|
|European Classification||H01L33/64H, F28D15/02|
|Jun 15, 2006||AS||Assignment|
Owner name: ENFIS LIMITED, UNITED KINGDOM
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:BOARD, KENNETH;EVANS, GARETH PETER;JONES, GARETH;REEL/FRAME:017787/0270;SIGNING DATES FROM 20051101 TO 20051204