This invention relates to a structure for removing heat from a generally bulb-shaped solid state lamp, such as a high power light emitting diode (LED) lamp, and, in particular, to a fin design and cavity structure for the lamp.
A huge market for LEDs is in replacement lamps for standard, screw-in incandescent light bulbs, commonly referred to as A19 bulbs. The letter “A” refers to the general shape of the bulb, including its base, and the number 19 refers to the maximum diameter of the bulb. Such a form factor is also specified in ANSI C78-20-2003. Therefore, it is desirable to provide an LED lamp that has the same screw-in base as a standard light bulb and approximately the same size diameter or less. Additional markets exist for replacing other types of standard incandescent bulbs with longer lasting and more energy efficient solid state lamps.
LEDs are only about 1 mm2, so heat removal from high power LEDs is a difficult problem when the LED lamp has to adapt to a preexisting form factor. About 80%-90% of the LED power consumption is translated to heat. The temperature of an LED die should be kept relatively low (e.g., under 120° C.) to ensure the LED remains efficient and has a long life.
For a desirable LED lamp implementation, there are a few basic components: a standard (e.g., E26 or E27) base, an electronic driver (if needed) to convert the mains voltage into the required LED drive voltage, a heat sink, one or more LEDs to generate at least 600 lumens, and secondary optics to create a desired emission pattern, all contained within the A19 form factor or other standard form factor.
The current LED efficacy of 80-120˜lm/W translates to an LED lamp power of 7.5 W. Additionally, the driver internal to the lamp may add about 2-2.5 W to the system. For an Energy Star requirement or a TC-L70 35,000 hrs requirement, the die junction temperature should be maintained preferably below 120° C. High power LED lamps greater than about 7.5 W that can directly replace 40 W and 60 W incandescent light bulbs need innovative heat removal techniques to dissipate up to 10 W of heat without any active cooling.
It is known to provide metal fins extending from a bulb-shaped body to dissipate heat from an LED lamp. The fins are symmetrical around the body. The symmetrical fins on such known prior art solid state lamps are typically arranged vertically. A symmetrical pattern of fins causes the rising air flow around a vertically oriented lamp to be symmetrical and only in a plane parallel to the lamp's center axis. As a result, the temperature pattern is symmetrical around the lamp. When a bulb-shaped solid state lamp is used in a light fixture, such as a ceiling can, that orients the lamp so that its base is above the LEDs, there is generally some air flow obstruction above the lamp due to the design of the fixture. In such a case, the heated air builds up and air flow velocity around the lamp is reduced due to there being symmetrical air flow resistance around the lamp. As a result, the LEDs get much hotter, limiting the lumens output of a lamp that can be used with the fixture.
What is needed is a new approach to remove adequate heat from a high power LED lamp, or other solid state lamp, using only passive techniques, where the size of the lamp is constrained to, for example, an A19 form factor.
In one embodiment, a solid state lamp has a generally bulb shape, such as a standard A19 shape. Many other form factors are envisioned. The light source may be an array of LEDs. The section of the lamp between the LEDs and the screw-in base is a heat sink having the A19 form factor. The heat sink may be formed of molded aluminum or other thermally conductive material. Metal fins extend from a central shaft portion of the heat sink or other support structure in the heat sink. The fins are asymmetrically arranged with respect to the support such that, when the lamp's center axis is oriented vertically and the lamp is generating heat, the fins create an asymmetric air flow that moves through (across) a plane that is parallel to the center axis, wherein the air flow pattern is peripherally monoperiodic around the periphery of the lamp. The peripherally monoperiodic flow pattern means that there is no pattern of air flow that repeats around the center axis of the lamp. The lamp may have a generally circular shape around its center axis (like a bulb), or the lamp may have a non-circular shape.
In one embodiment, the fins are angled with respect to the center axis between an LED support platform and the lamp base. In one embodiment, if the heat sink is bisected vertically, the fin patterns on the two halves would be mirror images of each other (the fin angles are opposite on opposite sides of the lamp). Therefore, when looking down at the lamp along the center axis, the angled fins on both sides of the lamp are generally pointing toward the same side of the lamp. This results in an asymmetrical air flow pattern around the lamp's periphery. In contrast, if the fins were symmetrical around the heat sink (all have same angle around the periphery), the air flow would be symmetrical around the heat sink.
Many other asymmetrical arrangements of the fins are possible to create an asymmetrical air flow pattern, including vertical and angled arrangements of fins.
Due to the asymmetric air flow pattern around the center axis of the lamp, there are different air pressures and temperatures around the periphery of the lamp, so there are asymmetrical air flow resistances around the lamp. As a result of the asymmetric air flow resistances, the maximum air flow velocity at locations around the periphery increases compared to the maximum air flow velocities around lamp heat sinks with symmetrical vertical fins. The increased air flow velocity results in more volume of ambient air per unit time removing heat from the heat sink. Hence, there is greater overall cooling of the LEDs (or other solid state light source) than had the fins been arranged symmetrically.
The asymmetrical air flow and temperature pattern is particularly beneficial when the lamp is mounted “upside down” such as in a ceiling can which restricts upward air movement. The asymmetric air flow and asymmetric air temperature pattern tends to stir the air inside the ceiling can for increased cooling of the heat sink.
Computer simulations have proven that the maximum air flow velocity using the asymmetrical fin design is greater than the maximum air flow velocity using a symmetrical fin design, resulting in increased cooling. Computer simulations have also proven that the heat sink and LED temperatures using the asymmetrical fin design are lower than the temperatures using a symmetrical fin design.
Additionally, conventional vertical fins that symmetrically taper toward a base have a smaller and smaller air flow channel between the fins as the fins approach the base. This restricts the air flow between the fins. Various designs of fins are described herein, such as angled fins with a substantially constant gap between the fins, that result in substantially no air flow restrictions along the length of the lamp, causing greater cooling of the heat sink.
In one embodiment, there is an open area of the heat sink around the center axis of the lamp between the fins. An air vent is formed through the metal support platform that supports the LEDs to allow air to enter the area of the heat sink where the fins are located. This is particularly beneficial when the lamp is mounted in a cylindrical ceiling can and there is only a small air gap between the sides of the lamp and the ceiling can wall.
In one embodiment, the fins comprise a set of asymmetrically arranged angled fins and one or more vertical fins, where the vertical fins extend from a bottom surface of the LED support platform and intersect a plurality of the angled fins. The vertical fins conduct heat from the support to the plurality of the angled fins. The vertical fins also extend from the central shaft to conduct heat from the central shaft to the plurality of angled fins.
In one embodiment, the periphery of the bottom surface of the LED support platform is rounded to provide a reduction in air flow resistance as heated air flows from the heat sink and around a periphery of the lamp.
A novel cavity of the heat sink is also described. In some applications, it is desirable for the heat sink to have a central metal shaft to house a driver and wires and to conduct the LED heat along the length of the shaft so it can be better cooled by the fins. The hollow space for the driver and the wires that connect the driver to the LED module is a relatively poor conductor of heat. In one embodiment, the driver is located at the bottom of the heat sink near the base, so the base can conduct heat from the driver to the socket, and the driver is a maximum distance from the LEDs to limit heating of the LEDs by the driver. Additionally, since the LED module (comprising a metal circuit board populated with LEDs) typically has a power supply wire connection on only one edge of the module, the hole through the heat sink's shaft for the wire can be asymmetrical. The side of the shaft with the hole will have the highest thermal resistance, so the hole is positioned to be on the side of the heat sink where the cool ambient air enters the fin channels.
Elements that are the same or similar in the various figures are identified with the same numeral.
The heat sink 12 has angled fins 22 extending from a central shaft of the heat sink 12.
The lamp 10 has a translucent cover 24 to diffuse the light from the LEDs mounted on the heat sink 12. In one embodiment, there are gaps between the cover 24 and the heat sink 12 to allow heated air to escape.
As seen in the view of
In the example, the fins 22 extend a maximum of about 2-2.5 cm from a central shaft of the heat sink 12. The maximum width of the fins 22 depends on the width of the central shaft. A central shaft is not necessary for the invention.
The asymmetrical arrangement of the fins 22 causes an asymmetrical air flow to occur. If it is assumed the lamp 10 is oriented vertically in a fixture so that its base 14 is at the lowest point, the air heated between the fins 22 will flow upward in the angled direction of the fins 22, relative to the lamp's center line 25, as shown by the air flow lines 26 in
The velocity of the rising air is related to the temperature of the air, air flow restrictions, and other factors. The gaps between the fins 22 are generally constant along the length of the lamp, so there is reduced air flow resistance between the fins 22, compared to prior art vertical fins having gaps that taper toward the narrow base. Further, since the air flows are all directed toward the same side, there is a reduction of opposing air flow forces around the periphery of the lamp compared to symmetrical air flows around prior art lamps. For at least these reasons, the heated air has a maximum velocity that is greater than the maximum velocity of air moving through prior art symmetrical vertical fins.
The increased air flow velocity results in more volume of ambient air per unit time removing heat from the heat sink 12. Hence, there is greater overall cooling of the LEDs (or other solid state light source) than had the fins been arranged symmetrically and vertically.
In a computer simulation, the maximum air flow velocity along a lamp with symmetrical and vertical fins, where the lamp was positioned vertically with its base at the lowest point, was 0.23 meters/second (m/s), while the maximum air flow velocity along the lamp 10 was 0.30 m/s.
In a computer simulation, for the lamp with symmetrical and vertical fins, where the lamp was positioned vertically with its base at the lowest point, the maximum heat sink temperature rise was 63.8° C., and the average LED junction temperature rise was 66.8° C. For the lamp 10, the maximum heat sink temperature rise was only 49.9° C., and the average LED junction temperature rise was only 53.6° C.
In a computer simulation, for the lamp with symmetrical and vertical fins, where the lamp was positioned vertically in a conventional four inch ceiling can with its base at the highest point, the maximum heat sink temperature rise was 78.4° C., and the average LED junction temperature rise was 81.9° C. For the lamp 10, the maximum heat sink temperature rise was only 69.9° C., and the average LED junction temperature rise was only 72.8° C.
The lamp 10 also has two vertical fins 31 (
Due to the radially asymmetrical pattern of air flow (i.e., peripherally monoperiodic air flow pattern), there is an asymmetrical temperature pattern around the heat sink 12, as described with respect to
In another embodiment, part of the metal support 46 is formed of a separate copper insert mounted within an indentation in the aluminum portion of the metal support 46. Since copper has a thermal conductivity much higher than that of aluminum, there is less thermal resistance in the resulting heat sink.
A central shaft 52 (
The driver 60 comprises components mounted on a metal core printed circuit board that is, in turn, mounted on a metal platform forming part of the molded aluminum heat sink 12. Much of the heat from the driver 60 is coupled to the socket via the screw-in base 14.
The heat coupled along the shaft 52 is coupled to the fins 22. The fins 22 have a larger surface area near the top (where the heat is greatest) due to the widening of the lamp 10 at the top.
The shaft 52 is asymmetrical, where the thermal resistance along the shaft 52 is less along the right side than along the left side due to the opening 54 for the wiring 56. The LED circuit board 42 is arranged so that its power connectors are near the edge of the board 42 nearest the opening 54.
If the lamp 10 is optimized for being vertically oriented in a fixture such that air flow will be from left to right across the heat sink, the opening 54 should be on the left side of the lamp 10 since cooler air enters the left side. The optimal position of the opening 54 will therefore depend on whether the lamp 10 is optimized for being vertically oriented with its base down or up.
In one embodiment, there are 18 fins 16 that extend from the cylindrical center shaft 52 to the outer periphery of the bulb form factor (e.g., A19 form factor). The angle of the fins is between 20-40 degrees relative to the centerline, and preferably about 30 degrees.
In another embodiment, the driver is deleted, and there are a sufficient number of LEDs connected in series so the LED currents are within an acceptable range.
In one embodiment, there is no central shaft that extends between the base and the LED support, or the central shaft is discontinuous. In such a case, the base is mechanically secured to the LED support by the fins. This allows the air to flow through the middle of the lamp, resulting in less air restriction and increased air velocity for better cooling.
Additionally, there are air vents 66 through the heat sink's LED support that lead to the open area above the portion 64.
Although a standard light bulb form factor has been used in the examples, other incandescent and fluorescent bulb form factors may also be used for the solid state lamp. The base may be a plug-in base or have other types of connectors. A list of standard bulb and socket form factors can be found at http://www.donsbulbs.com/cgi-bin/r/t.pl/socket.base.html, copyright 2009, incorporated herein by reference.
The asymmetrical arrangement of the fins to generate an asymmetrical air flow pattern may take many forms.
Having described the invention in detail, those skilled in the art will appreciate that given the present disclosure, modifications may be made to the invention without departing from the spirit and inventive concepts described herein. Therefore, it is not intended that the scope of the invention be limited to the specific embodiments illustrated and described.