This application is based upon and claims the benefit of priority from the prior Japanese Patent Application No. 2013-166916, filed on Aug. 9, 2013, the entire contents of which are incorporated herein by reference.
Embodiments described herein relate generally to lighting devices.
Lighting devices using light-emitting diodes (LEDs) show superior environmental performance (long lifespan, low power consumption, non-use of mercury, etc.) to incandescent lamps and fluorescent lamps, and are therefore expected to replace these prevailing types of lighting devices. Various new types of lighting devices using LEDs are also proposed. Thus, expectations for such lighting devices are rising. Lighting devices using LEDs are heat-sensitive due to their containing semiconductors, whose typical maximum rating junction temperature is in the range of 100° C. to 150° C. LEDs virtually emit no infrared, and about 70% of the power consumed by LEDs is converted into heat. Therefore, a design for heat dissipation that allows heat to be conducted to a heatsink and dissipated is important.
Conventional LED light bulbs are designed to convey most of the heat generated by LEDs to a heatsink by heat conduction through a base connected to the LEDs, the heat then being dissipated into the environment by natural convection and radiation. In order to improve heat conductivity, the base member and the heatsink arranged on the outer side of the globe are made of a metal or ceramic of a high thermal conductivity. Furthermore, the heat transfer is improved by increasing the surface area of the heatsink by, for example, employing a fin structure to enhance natural convection, or by employing a special coating for improved emissivity. The dependency of such structures on heat dissipation from the outer surface of the LED light bulb, however, leads to increased dimensions if a higher output is to be achieved. This causes problems of compatibility with devices and light output, and of the appearance.
In order to solve the above problems, a structure is proposed to form an opening in an LED light bulb to use the inner surface thereof as a heat dissipation surface. In the proposed LED light bulb, the LEDs are arranged between fins to convey light emitted from the LEDs to a wide area of the globe, for a wide distribution of light. However, the fins also act as screens, and increasing the number of fins and employing complex fin structures to improve the heat dissipation performance leads to a degradation of device efficiency. Thus, it is a trade-off between light and heat dissipation efficiency.
In addition, since the diameter of a cylindrical body located at the center of the LED light bulb needs to be increased to ensure a space for a plurality of LEDs, the inner space of the LED light bulb decreases. For this reason, the interior of the LED light bulb cannot be used effectively as a heat dissipation region.
Furthermore, in order to efficiently convey the heat of the LEDs to the cylindrical body, the section of the cylindrical body should be such that the cylindrical body is in surface contact with the LEDs or substrate.
Moreover, since the LEDs are positioned between the fins, the number of LEDs should exceed the number of fins to prevent shadow formation. This raises the problem that a single light source of large output cannot be employed.
Since the LEDs are positioned inside of air flow, the light source is easily affected by dust, etc. This blocks light and decreases the lighting efficiency of the device.
Also, the spatial positioning of LEDs puts a great strain on manufacturing processes.
Due to the foregoing reasons, the dissipation surface area inside the LED light bulb cannot be sufficiently obtained. Therefore, in order to achieve a high output, the dissipation surface area, i.e., the size, of the LED light bulb increases.
a) and 9(b) are cross-sectional views of a lighting device according to a second embodiment.
a) and 12(b) are cross-sectional views of a lighting device according to a third embodiment.
A lighting device according to an embodiment includes: a light-emitting element having a light-emitting surface; an optical lens positioned on a positive direction side of an axis that is perpendicular to the light-emitting surface of the light-emitting element with a point of origin being set on a center of the light-emitting surface, a positive direction of the axis being determined as a direction in which light is emitted; a plurality of heat dissipation fins arranged on a negative direction side of the axis and around the axis that serves as a central axis, the heat dissipation fins being arranged so as not to be present within a range of a 1/2 light distribution angle of light emitted from the optical lens in the positive direction, and the heat dissipation fins being thermally connected to the light-emitting element; a cover housing the heat dissipation fins, being shaped like a body of rotation with the axis serving as a rotation axis, and having at least one opening in each of the positive direction side and the negative direction side of the axis; and a base member positioned along the axis and thermally connected to the light-emitting element and the heat dissipation fins.
Embodiments will now be explained with reference to the accompanying drawings. In the descriptions of the drawings, the same or similar elements are denoted by the same or similar reference codes.
It is assumed that there is an axis 10 with the point of origin set on the center of the light-emitting surface of the light-emitting element 2 including LEDs, the axis 10 being perpendicular to the light-emitting surface and the direction in which light is emitted being set as a positive direction. The optical lens 3 is located on the positive direction side of the axis 10. The optical lens 3 is made of a material having a high transmittance such as poly-methyl-methacrylate (PMMA), and widely distributes light emitted from the light-emitting element 2 with high directivity. The first embodiment has an advantage in that the light source is unlikely to be affected by dust since the light-emitting surface of the light-emitting element 2 does not face the main stream of air flow.
The optical lens 3 is coupled to the light-emitting element 2.
The heat dissipation fins 4 are thermally connected with the light-emitting element 2, and arranged on the negative direction side of the axis 10 so as to radiate from the axis 10. The light-emitting element 2 is fixed to the heat dissipation fins 4 via the base member 4a. The fixing may use screws as shown in
A high device efficiency can be achieved by not arranging the heat dissipation fins 4 in the range of 1/2 light distribution angle of light emitted from the optical lens 3. Specifically, the light distribution angle a can be represented, based on the Etendue rule, by
θ=sin−1(A/B)1/2
where A denotes light-emitting area, and B denotes the light-emitting area of the lens. In this embodiment, a wide light distribution can be achieved by, for example, cutting outer corner portions of the heat dissipation fins 4. With such a structure, the positive direction side of the axis 10 can be treated as light region, and the negative direction side can be treated separately as dissipation region. As a result, the number of the light-emitting elements 2 and the number of the heat dissipation fins 4 can be determined independently of each other. Furthermore, this embodiment can be compatible with a single, high-output light source. Since the heat dissipation fins 4 do not block light, the shape of each fin can be complicated. Thus, the degree of freedom in design is improved. The heat dissipation fins 4 are made of a material with a high thermal conductivity, such as aluminum. The reflectivity of the heat dissipation fins 4 can be improved by mirror-finishing the surfaces thereof. The emissivity of the heat dissipation fins 4 can be improved by coating the surfaces thereof with an appropriate material. Openings such as holes can be formed through the heat dissipation fins 4. With such a structure, the lighting device may be installed so that the axis 10 extends in the horizontal direction. Specifically, air that rises due to natural convection passes through the openings of the heat dissipation fins, which prevents degradation of radiation performance.
The base member 6 is a body of rotation with the axis 10 serving as a rotation axis. The heat dissipation fins 4 are arranged and fixed around the base member 6. The heat dissipation fins 4 and the light-emitting element 2 are thermally connected with each other via the base member 6. Specifically, the heat dissipation fins 4 are directly connected to the base member 6, and the light-emitting element 2 is directly connected to the base member 6 and also indirectly connected to the base member 6 via the base member 4a and the heat dissipation fins 4. Therefore, it is important to reduce the thermal resistance from the light-emitting element 2 to the heat dissipation fins 4. From this point, the diameter of the base member 6 is preferably as great as possible. However, as the diameter of the base member 6 increases, the size of the heat dissipation fins 4 decreases. Therefore, the diameter of the base member 6 is set such that the temperature gradient does not increase too much in the direction of the axis 10. The base member 6 may be solid to reduce the thermal resistance. Alternatively, the base member 6 may be hollow to house wiring connecting the power supply unit 7 and the light-emitting element 2. A thermal interface material (TIM) such as thermal grease or heat conductive double-sided tape may be provided between the base member 6 and the light-emitting element 2 to reduce the contact thermal resistance. The base member 6 is made of a material with a high thermal conductivity such as aluminum. The base member 6 and the fins 4 may be integrally formed to reduce the base-fin contact thermal resistance. Alternatively, the base material 6 and the fins 4 may be separately formed to improve the productivity.
As shown in
The light emitted from the light-emitting element 2 is distributed by the optical lens 3. Therefore, the cover 5 is not necessarily made of a material having a sufficiently high refractive index, such as polycarbonate (PC), PMMA, or glass. For example, the cover 5 may be replaced with a madreporic body formed of paper such as Japanese paper or kite string. Thus, an application-customized design can be made. The heat dissipation performance can further be improved by having a portion outside the range of the 1/2 light distribution angle of the light emitted from the optical lens 3 to be made of a material with a high thermal conductivity such as a metal or ceramic, or material with a high emissivity. With the openings 9, air can be introduced into the cover 5, which exchanges heat with the heat dissipation fins 4. The position and the size of each opening 9 are not limited. If the openings are formed near the heat dissipation fins 4, the internal structure can be made unlikely to be seen, which allows a good design. The openings may be formed in a wide range to improve the heat dissipation performance.
The openings 9 may be slits to make the internal structure unlikely to be seen, as in a lighting device according to a first modification shown in
Depending on the positions of the openings 9, the air introduced may hit the optical lens 3. If the openings 9 are present in the positive direction side on the axis 10 relative to the optical lens 3, the flow resistance may be reduced by forming the optical lens 3 in a projecting shape or curved shape so that air can be easily introduced. The first modification has an advantage in that the light source is not affected by dust easily since the light-emitting surface of the light-emitting element 2 does not face the mainstream of air flow.
In contrast, the lighting device according to the first embodiment is capable of releasing heat within the cover 5 as shown in
The heat dissipation fins 4 housed in the cover 5 may be shaped such that they contact the cover 5 to convey heat to the cover 5 as shown in
The power supply unit 7 includes a power supply casing and a power supply circuit, and is positioned on the negative direction side of the axis 10. The power supply circuit is housed in the power supply casing connected to the base 8 for receiving a current from outside. The power supply unit 7 is screw-connected with the base member 6. Specifically, a male thread at the tip of the base member 6 on the side of the power supply unit 7 is screwed into a female thread hole in a corresponding recess of the power supply unit 7. In order to convey heat of the power supply circuit to the power supply casing, a resin or heat conduction grease may be filled into the power supply casing. The power supply unit 7 is preferably positioned so as not to contact the base member 6, the heat dissipation fins 4, and the cover 5 as much as possible so that the power supply circuit is not affected by heat generated by the light-emitting element 2. The power supply casing may be shaped to match the shape of the power supply circuit so that air may easily flow into and out of the cover 5. If the power supply unit 7 is positioned within the cover 5, the shape of the power supply unit 7 may be rounded to decrease the flow resistance of air within the cover 5. The power supply unit 7 may be located outside the cover 5 as in a second modification of the first embodiment shown in
As described above, according to the first embodiment, a lighting device using LEDs capable of increasing the output without decreasing the lighting efficiency and increasing the size can be provided.
A lighting device using LEDs according to a second embodiment will be described with reference to
The lighting device 1A according to the second embodiment differs from the lighting device 1 shown in
where t denotes the thickness of the heat dissipation fins 4, La denotes the distance from the center of the base member 6 (axis 10) to a point 11 on each heat dissipation fin 4. The condition under which the product of the heat transfer coefficient and the heat dissipation area obtained from the above formulas becomes a maximum can be determined using the distance S between adjacent heat dissipation fins 4 after the branching as a design parameter. A condition is preferable under which the fin efficiency depending on the thickness t of the heat dissipation fins 4, and the product of the heat transfer coefficient depending on the distance S between the heat dissipation fins 4 and the heat dissipation area depending on the angle θa between the heat dissipation fins 4 before the branding become a maximum.
It is assumed that the height of the heat dissipation fins 4 is 25 mm for allowing the lighting device to be applied to an incandescent light bulb. Then, the relationship between the distance S and the heat transfer coefficient is obtained from the relational formula of natural convection between flat plates in vertical and parallel arrangement. As a result, the heat transfer coefficient reaches a value substantially corresponding to a convergence value when S is about 6 mm. It is known that natural convection between flat plates in a vertical and parallel arrangement at a temperature Tw that is higher than an ambient temperature Ta can be approximated by the following formula from BarCohen-Rohsenow:
where /h denotes average heat transfer coefficient, S denotes interval between the parallel plates, ka denotes thermal conductivity of air, RaS denotes Rayleigh number of a representative length S, and H denotes height of the plates.
The fin efficiency η of a rectangular fin can be expressed by the following formula:
where L denotes fin length, /h denotes heat transfer coefficient, kf denotes thermal conductivity of the fins, t denotes fin thickness, and H denotes fin width (height of the plates).
From
Like the first embodiment, a lighting device using LEDs according to the second embodiment is capable of increasing the output without decreasing the lighting efficiency and increasing the size.
A lighting device according to a third embodiment will be described with reference to
The lighting device 1B according to the third embodiment differs from the lighting device 1 shown in
The design parameters of the third embodiment are the distances between adjacent fins θa1, θa2, θa3, and the interval between the heatsinks Lb. Like the second embodiment, conditions under which the product of the heat transfer coefficient and the heat dissipation area becomes a maximum are determined. The distances between fins θa1, θa2, θa3 are not needed to be the same value.
Like the second embodiment, the heat dissipation from the heat dissipation fins 4 of the third embodiment can be increased.
Furthermore, like the first embodiment, a lighting device using LEDs according to the third embodiment is capable of increasing the output without decreasing the lighting efficiency and increasing the size.
A lighting device according to a fourth embodiment will be described with reference to
In the fourth embodiment, a rotation member 18 rotating around the axis 10 is provided inside the cover 5. The rotation member 18 generates forced convection, by which boundary layers of the heat dissipation fins 4 can be decreased. As a result, the heat transfer coefficient is increased, and the temperature of air near the heat dissipation fins 4 is lowered by increasing the mass flow rate of air inside the cover 5.
If the rotation member 18 is formed separately from the heat dissipation fins 4, any impediment placed in the rotation direction of the rotation member 18 should be removed to avoid any interference from the heat dissipation fins 4. Providing extra space may help avoiding any interference due to dimensional tolerance.
The heat dissipation fins 4 themselves may rotate to act as the rotation member 18. For example, the heat dissipation fins 4 can be rotated by rotating the base member 6. If a rotating mechanism is housed in the base member 6, the base member 6 should be made hollow. If the diameter of an opening to make it hollow is large, thermal resistance between the light-emitting element 2 and the heat dissipation fins 4 may be increased.
If the light-emitting element 2 is not rotated together, attention should be paid to twisting and entanglement of wiring. From the foregoing, if a rotating mechanism is housed in the base member 6 to rotate the heat dissipation fins 4, and the light-emitting element 2 is not rotated together, heat generated by the light-emitting element 2 may not be conveyed satisfactorily to the rotating heat dissipation fins 4.
In order to deal with this problem, a rotating mechanism is positioned on the side of the power supply unit 7 of the base member 6 and the rotation member 18 is positioned near openings 9 located on the negative direction side of the axis 10 in the lighting device according to the fourth embodiment shown in
The rotation member 18 preferably has a shape to guide, by its rotations, air flow to the normal line in the direction of angular velocity, i.e., the direction of the openings 9. The heat dissipation from the rotation member 18 can be increased by forming the rotation member 18 of a material having a high thermal conductivity such as aluminum. The reliability of the rotation member 18 can be improved by forming it of a material having a high rigidity. The weight of the rotation member 18 can be decreased by forming it of a material having a low density. Noise generated by the rotation member 18 can be prevented by lowering the number of revolutions thereof.
Like the first embodiment, the lighting device using LEDs according to the fourth embodiment is capable of increasing the output without decreasing the lighting efficiency and increasing the size.
As described above, an embodiment has the following effects.
Heat dissipation performance can be improved without disturbing the roles conventionally held by globes, diffusion and light guide, by positioning an optical lens to face the light-emitting surface of LEDs, and arranging heat dissipation fins inside the globe so as not to block light. As a result, LEDs can be positioned near the top portion of the globe, i.e., near openings. Accordingly, the trade-off between light and heat dissipation can be solved.
Specifically, a positive direction side of an axis that is perpendicular to the light-emitting surface of the LEDs with the center of the light-emitting surface being set as the point of origin and with a direction in which light is emitted being set as a positive direction is defined as a light-emitting side, and a negative direction side is defined as a heat dissipation side. Since the light-emitting side and the heat dissipation side can be separated from each other, the number of LEDs and the number of fins can be determined separately from each other. Furthermore, embodiments can be applied to a single light source with a high output. Moreover, the shape of fins can be complicated, which allows a higher freedom in design. A high device efficiency can be achieved if no shield is provided within a 1/2 light distribution angle of the optical lens in the heat dissipation side.
Further, an effect can be expected that no shadow may be produced by the heat dissipation fins etc. since the distance between a point of the optical lens from which light is emitted and a point at which the light hits the globe is long. The reason for this is that light emitted from the optical lens are widely dispersed before they reach the globe.
In the described structures, the light-emitting surface of the LEDs does not face the mainstream of air flow. Therefore, the light source is not affected by dust etc.
Since light is distributed by the optical lens, the globe may be made of a material of which the refractive index may not be sufficiently high, such as PC, PMMA, and glass. For example, the globe may be made of Japanese paper. If the housing portion conventionally made of metal is made of the same material as the globe, the appearance may become closer to that of an incandescent light bulb. If portions outside the 1/2 light distribution angle of the optical lens are formed of a material having a high thermal conductivity such as a metal or ceramic, or having a high emissivity, the heat dissipation performance can be improved further.
The heat dissipation may be improved by increasing the globe temperature by shaping the fins in accordance with the shape of the cover so that the fins are in contact with the cover. The shadows of the fins may become unlikely to be seen easily by forming a space between the globe and the fins.
While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel methods and systems described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the methods and systems described herein may be made without departing from the spirit of the inventions. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the inventions.
Number | Date | Country | Kind |
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2013-166916 | Aug 2013 | JP | national |