The present invention relates to light emitting diodes (LEDs) and other high power density devices such as laser and computer chips. In particular, it relates to a cooling mechanism for LED lights.
Although light emitting diodes (LEDs) hold great promise for application ranging from telecommunications to general illumination, the cost per-lumen still hinders LED's penetration of the markets. Currently, the lighting market is dominated by compact fluorescent lamp (CFL). The cost per-lumen for LED luminaires must rapidly decreases to compete with CFLs.
One way to realize the price-reduction objectives for LED lights without significantly changing the device manufacturing cost is to increase the injection current density, for example by a factor of 2 to 4, from an order of tens of A/cm2 to hundreds of A/cm2. However, increasing the light-power output of devices through increasing the drive-current of LEDs could lead to two problems due to increased heat generation. One is the effect of “efficiency droop” and the other one is the effect of “thermal runaway”. If the heat cannot be dissipated properly, the higher junction temperature will lead to lower EQE (external quantum efficiency) of the LED device, which will lead to an even higher temperature and eventually lead the LED devices to thermal failure. Therefore, the thermal management of the LEDs is a key issue to decreasing the cost of LED lights without significantly changing the manufacturing cost of LED chips. Additionally, keeping the junction temperature as low as possible is also beneficial to the lifetime of LEDs. In summary, LED thermal management is critical to lowering junction temperature, increasing light power output and lifetime.
Heat transfer process follows the following rule:
Q=hAΔT
where Q is the heat transfer power (W), h is the heat transfer coefficient (W/(m2·K)), A is the area of thermal pass, and ΔT is the temperature gradient or difference. The heat transfer coefficients of different heat transfer mechanisms are different. Because of the considerable difference of h between different heat transfer mechanisms, it is necessary to evenly spread the heat to different thermal pass area to achieve an effective cooling system.
The thermal model of a common LED system is depicted in
Comparing with the typical values of Rinner and Rinter, Rexter based on passive heat sink according to conventional technologies often cannot satisfy the application demands for LEDs driven by high injection currents. The thermal resistance of passive heat sink is caused by its poor heat match or spreading. Phase change cooling systems, which conduct heat away through phase change at a high temperature region and reverse phase change at a low temperature region, can improve the heat spreading significantly.
1-D heat pipe and 2-D vapor chamber are two widely used phase change cooling systems. Both of them have been applied in thermal management of LEDs, for example, as described in Lan Kim et al., Thermal analysis of LED array system with heat pipe, Thermochimica Acta, 455, 21-25 (2007) (“Kim et al. 2007”); and H.-S. Huang et al., Experimental Investigation of Vapor Chamber Module Applied to High-Power Light-Emitting Diodes, Experimental Heat Transfer, 22, 26 (2009) (“Huang et al. 2009”). In such systems, the heat pipe and vapor chamber function as a heat spreader between the heat source and the lower temperature region. As shown in
The natural air convective heat transfer coefficient between a heat sink and the environmental atmosphere is typically 5 to 25 W/(m2K) while the heat transfer coefficient of phase change process is in the order of tens of thousands W/(m2K). This means that the heat spreader needs to transfer the heat from the heat source to a heat sink of 104-105 times the area of the heat source if natural air convective cooling is used to cool the heat sink. Therefore, a major bottleneck of the cooling system for high power LEDs is the insufficient heat transfer area between heat sink and atmospheric environment. The required heat sink surface areas (Ahs) to realize the target light-power output for various types of LED chips, such as current commercial chips, advanced MQW chips, advanced DH chips, etc., and at various output powers can be calculated. For example, for a 60 W-equivalent replacement LED luminaire, the required heat sink surface areas are on the order of a thousand cm2 using the assumptions as follows: natural air convective heat transfer coefficient is 10 W/(m2K), and the temperature difference between the heat sink and atmospheric environments is 10 K. Additionally, the required large surface area and thickness of solid heat sink also increases the cost of luminaires. For example, a typical cost of solid heat sink for high power electronics devices can be in the range of 0.5-10 dollars. If heat pipes (1-D or 2-D) are used in the cooling system, the cost of the cooling system may increase dramatically to 15-100 dollars (see Huaiyu Ye et al., A review of passive thermal management of LED module, J. Semicond., 32, 014008 (2011)). The cost at this level is not practical in the luminaire applications.
As discussed above, the heat spreader in an LED cooling system needs to transfer the heat from the chip to a 104-105 times larger area. If the thermal match is carried out by the present 1-D heat pipe or 2-D vapor chamber, the cost burden will be too heavy to apply in luminaires. Therefore, these cooling systems based on heat pipe or vapor chamber need a secondary active cooling system in addition to the heat sink because of its insufficient heat spreading. Otherwise, there will be a temperature difference between the top of the heat sink and the environment ranging from tens to one hundred Ks.
To summarize, the inventors of the present invention realized that to keep junction temperature low when the LED device is driven by a high forward current, the system level thermal resistance of packaged LED luminaires needs to be reduced as far as possible, and that Rexter is the major bottleneck in the thermal management of LED luminaires. Therefore, a luminaire-level advanced cooling strategy is need for the LED luminaires with higher powers. As explained above, the key point in developing the advanced cooling strategy is how to spread the heat from a relatively small heat pass area (approximately 1 mm2) to a much bigger one (approximately 0.1 m2).
This invention is intended to provide an effective heat spreading strategy for thermal management in LED luminaires to enhance its light power output and life span performance while reducing the cost of the cooling system for high power LED luminaires significantly. Furthermore, this invention can be applied to other similar high power density devices, including computer main engine chips, laser diodes, etc.
A novel 3-D “phase change heat exchange” structure is used to dissipate heat from the high power LED chips and other high power density devices to the atmosphere.
Additional features and advantages of the invention will be set forth in the descriptions that follow and in part will be apparent from the description, or may be learned by practice of the invention. The objectives and other advantages of the invention will be realized and attained by the structure particularly pointed out in the written description and claims thereof as well as the appended drawings.
To achieve these and other advantages and in accordance with the purpose of the present invention, as embodied and broadly described, the present invention provides a light emitting diode (LED) light which includes: an enclosure structure defining a chamber, wherein the enclosure structure includes a plurality of hollow fins disposed substantially in parallel with each other, each fin enclosing a hollow space which is connected to the chamber, the hollow spaces and the chamber forming a sealed space, wherein a flat part of the enclosure structure forms an evaporator, a plurality of LED chips mounted on the evaporator and in thermal contact with the evaporator; and a liquid to vapor phase change material (L-V PCM) disposed inside the chamber.
It is understood that the examples and embodiments described herein are for illustrative purposes only and that various modifications or changes in light thereof will be suggested to persons skilled in the art and are to be included within the spirit and purview of this application and scope of the appended claims.
In embodiments of the present invention, the LED luminaire employs a fin structure with hollow fins to dissipate heat to the environment. The hollow space inside the fins is connected to a chamber, where a liquid to vapor phase change material (L-V PCM) is provided to transfer heat from the LED chips to the surfaces of the fins.
In some embodiments, LED chips are mounted on different evaporators, including chip-area evaporators and mounting and thermal block evaporators. Chip-area evaporators use the back surface of chips mosaicked in a mounting block as the evaporator surface. Mounting and thermal block evaporators are made of a copper sheet with a thickness of about 1-5 mm and the LED chips are mounted on the copper sheet. The copper sheet spread the heat from a chip area (about 1 mm2) to a relatively larger area (about 1 to 2 cm2). Both of these two kinds of evaporator surface are treated to be a hydrophilic surface. The evaporator with LED chips is packaged in a 3-D vacuum-sealed enclosure which forms a chamber. The sealed chamber can have a high vacuum, medium vacuum, or low vacuum.
In all embodiments, a liquid to vapor phase change materials (L-V PCMs) with a desired boiling temperatures (e.g., room temperature to 100° C.) is used to wet the evaporator surfaces during LED luminaire operation. The L-V PCM may be stored in a reservoir integrated with the 3-D enclosure. Additional wick structure or fiber materials can also be implemented to use capillary force effect to transport the L-V PCM from the reservoir to the evaporator surface. The hydrophilic surface of the evaporator spreads L-V PCM uniformly to keep the surface wet. During the high power LED chip operation, as the evaporator surface temperature rises, which can exceed the boiling temperature of the liquid, the L-V PCM liquid layer evaporates and carries away the heat from the evaporator surfaces. The heat carried by the vapor is transferred to the cold surfaces of the 3-D enclosure and the vapor condensed back into the liquid. The liquid then is transferred back to the L-V PCM reservoir or the evaporator surface by gravitational force or other methods to continue the cycle.
In some embodiments, the cold surfaces are the surfaces of containers which contain a solid to liquid PCM (S-L PCM) with a melting temperature slightly lower than the desired maximum operating temperature of the LED chips. The S-L PCM containers are packaged in the chamber or another 3-D enclosure with their surfaces spaced away from each other with small gaps. The surfaces of the S-L PCM container can be coated with a hydrophobic thin film to increase heat exchange coefficient of vapor to liquid phase change. The S-L PCM containers can have a geometry of flat plate or cylindrical shape, preferably with a thin thickness or small diameter. In this way, the evaporator surface and the S-L PCM container surfaces are thermally “short circuited” with negligible temperature difference. The heat on the evaporator surface is then transferred on the surface of the S-L PCM containers and thermally stored in the S-L PCM materials as the S-L PCM materials melt into a liquid. After the LED luminaire is turned off, the heat stored in S-L PCM is dissipated into the environment by natural air convection.
An LED light according to a first embodiment of the present invention is illustrated in
A number of LED chips 401 are located at the bottom end of the chamber 410. The chips 401 may be used as chip-area evaporators, shown in detail in
Alternatively, as shown in
In both kinds of evaporator structures (
The L-V PCM, which is preferably a liquid at room temperature, is placed inside an L-V PCM reservoir 404, which is located near the evaporator surface in the example shown in
During operation, as the evaporator surface temperature rises, which can exceed the boiling temperature of the L-V PCM, the thin liquid layer evaporates to carry away the heat from the evaporator surface. The vapor fills the chamber 410 and the hollow space inside the fins of the fin structure, and condenses back into a liquid on the cold inside surfaces of the 3-D enclosure 405, transferring the heat to the cold surface.
In
The LED light shown in the embodiment of
As seen above, a phase change thermal exchange method is used as a thermal transformer to match thermal impedance of a small area of the chip evaporator (
An LED light according to a second embodiment of the present invention is illustrated in
The S-L PCM containers 708 preferably have small sizes and are shaped as plates or cylinders to increase the contact area between them and the L-V PCM vapor. They can be placed inside the interior space 710 of the LED light as shown in
Using this structure, when the environmental temperature is higher than the melting temperature of the S-L PCM, the heat generated by the LED chips during operation is temporarily stored inside the S-L PCM, and then dissipated into the environment when the environmental temperature drops down during the night.
Four LED lights according to third to sixth embodiments of the present invention are shown in
The different overall geometries of the fin structures (3-D enclosures) 805/905/1005/1105 shown in
In the above embodiments, the fins of the fin structures are hollow inside. One advantage of such a structure, compared so the structure with solid fins such as that shown in
An example of a manufacturing process for the 3-D vacuum-sealed enclosure 405/705 of the first and second embodiment is schematically shown in
As shown in
The fin structure can be assembled by sequentially placing the sheets and the outer and/or inner rings on top of each other and adhering them together to form a stack. Compared to forming the entire fins structure form a metal, the above manufacturing method is more cost effective without compromising the heat dissipation performance.
The fin structures in the third to sixth embodiments (
To summarize, in traditional heat pipes or vapor chambers, the main material is copper. This leads to the high costs of the traditional heat pipes or vapor chambers. In embodiments of the present invention, aluminum sheets can be sealed successfully by using plastic rings. Because aluminum is a relatively cheap materials and because of the hollow structures, the estimated cost of such 3-D enclosures for the high power LEDs can be as low as 0.5 to 1.5 dollars. Comparing with solid heat sinks or 1-D/2-D heat pipes coupled with solid heat sinks, the 3-D enclosure according to embodiments of the present invention achieves a relatively low cost and a much better thermal matching performance.
It is understood that the examples and embodiments described herein are for illustrative purposes only and that various modifications or changes in light thereof will be suggested to persons skilled in the art and are to be included within the spirit and purview of this application and scope of the appended claims.
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/US2014/035371 | 4/24/2014 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2014/176465 | 10/30/2014 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
5865244 | Moser | Feb 1999 | A |
7628512 | Netzel et al. | Dec 2009 | B2 |
20070159833 | Netzel, Sr. | Jul 2007 | A1 |
20100263842 | Ast | Oct 2010 | A1 |
20110026251 | Liu | Feb 2011 | A1 |
20110043092 | Shuja | Feb 2011 | A1 |
20120026745 | Cheng | Feb 2012 | A1 |
20130186596 | Rubenstein | Jul 2013 | A1 |
20140160762 | Dudik | Jun 2014 | A1 |
Entry |
---|
International Search Report in the parent PCT application No. PCT/U52014/035371, dated Aug. 22, 2014. |
IPRP in the parent PCT application No. PCT/US2014/035371 dated Oct. 27, 2015. |
Kim et al., “Thermal analysis of LED array system with heat pipe”, Thermochimica Acta, vol. 455, 2007, pp. 21-25. |
Huang et al., “Experimental Investigation of Vapor Chamber Module Applied to High-Power Light-Emitting Diodes”, Experimental Heat Transfer, 22:26-38, 2009. |
Ye et al., “A review of passive thermal management of LED module”, Journal of Semiconductors, vol. 32, No. 1, pp. 014008-1-014008-4, Jan. 2011. |
Number | Date | Country | |
---|---|---|---|
20160102854 A1 | Apr 2016 | US |
Number | Date | Country | |
---|---|---|---|
61854428 | Apr 2013 | US |