1. Technical Field
The disclosure generally relates to illumination devices, and particularly to an illumination device having a base with a spherical surface.
2. Description of Related Art
Light emitting diodes (LEDs) have recently been extensively used as light sources for illumination devices due to their high luminous efficiency, low power consumption and long lifespan. A single LED generally has a limited radiating range. To achieve a large radiating range, some illumination devices employ a plurality of LEDs on a base. However, such illumination devices may not achieve uniform light output. Therefore the range of applications suitable for these illumination devices is limited.
Thus, what is needed is an illumination device that overcomes the described limitations.
Many aspects of the disclosure 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 disclosure. Moreover, in the drawings, like reference numerals designate corresponding parts throughout the several views.
Referring to
In this embodiment, the base 10 is solid and has a hemispherical shape. The base 10 has a spherical surface 12 for mounting the first and second solid-state light sources 20, 30 thereon. The spherical surface 12 has a spherical center O, and a base central axis M passing through the spherical center O. The spherical surface 12 is thus a hemispherical surface.
The first and second solid-state light sources 20, 30 may be LEDs or LED chips. In this embodiment, the first and second solid-state light sources 20, 30 are all LEDs. The first light source 20 has a first light source central axis M1. Each of the second light sources 30 has a second light source central axis M2.
Referring also to
The first, the second, the third, the fourth, the fifth, and the sixth imaginary circles 31-36 have different numbers of second solid-state light sources 30 arranged thereon. The number of second solid-state light sources 30 on each imaginary circle 31-36 increases with increasing radius of the imaginary circles 31-36. Thus, all the second solid-state light sources 30 cooperate with the first solid-state light source 20 to form an illuminating region 120, in which the first and second solid-state light sources 20, 30 are approximately evenly distributed. In this embodiment, the first imaginary circle 31 has four second solid-state light sources 30 arranged thereon. The second imaginary circle 32 has eight second solid-state light sources 30 arranged thereon. The third imaginary circle 33 has twelve second solid-state light sources 30 arranged thereon. The fourth imaginary circle 34 has fifteen second solid-state light sources 30 arranged thereon. The fifth imaginary circle 35 has eighteen second solid-state light sources 30 arranged thereon, and the sixth imaginary circle 35 has twenty second solid-state light sources 30 arranged thereon.
The second light source central axis M2 of each second solid-state light source 30 passes through the spherical center O of the spherical surface 12. An angle θ is defined between each second light source central axis M2 and the base central axis M. Since the center of each imaginary circle is at the base central axis M, the angle θ defined by the second light source central axis M2 of one second solid-state light source 30 on a given imaginary circle 31˜36 is equal to that of any other second solid-state light source 30 on the same imaginary circle 31˜36. In this embodiment, the angle θ between the second light source central axis M2 of any one of the second solid-state light sources 30 on the first imaginary circle 31 and the base central axis M is ten degrees. In addition, the angle θ defined by the second light source central axis M2 of any second solid-state light source 30 on any one of the imaginary circles 31˜36 (e.g., the second imaginary circle 32) is different from the angle θ defined by the second light source central axis M2 of any second solid-state light source 30 on either of the neighboring imaginary circles 31˜36 (e.g., the first imaginary circle 31 or the third imaginary circle 33). The difference between the two angles 0 is ten degrees.
The light intensities of the first solid-state light source 20 and each second solid-state light source 30 satisfy the formula: I=I0/cos3 θ, wherein I0 is the light intensity of the first solid-state light source 20, and I is the light intensity of each second solid-state light source 30.
In one example, the light intensity I0 of the first solid-state light source 20 is 0.00524 candelas (cd). In such case, the second solid-state light sources 30 should satisfy the following conditions in Table 1 in order that the illumination device 100 provides uniform illumination.
The base 10 can be made of insulating material, such as plastic. Alternatively, the base 10 can be made of metallic material with high thermal conductivity, such as aluminum, copper, aluminum-copper alloy, or other suitable metallic materials. When the base 10 is made of metallic material, heat dissipation from the first and second solid-state light sources 20, 30 is enhanced.
The provision of the cavity 140 in the base 10 reduces the amount of material needed for the base 10. The flexible circuit board 22 may be a Flexible Printed Circuit (FPC). A substrate of the flexible circuit board 22 may be made of, for example, a mixture of graphite and polyester (such as polyethylene terephthalate-PET), or a mixture of graphite and polyimide (PI). With this configuration, heat from the first and second solid-state light sources 20, 30 can be transferred to the base 10 via the flexible circuit board 22, and thence be dissipated to ambient air. Accordingly, the first and second solid-state light sources 20, 30 may operate continuously within an acceptable temperature range and thereby achieve stable optical performance. In particular, the brightness and the luminous efficiency of the first and second solid-state light sources 20, 30 can be stably maintained.
It is noted that in other embodiments, a larger number of second solid-state light sources 30 may be arranged on the spherical surface 12, as long as the light intensity I of each second solid-state light source 30 follows the formula: I=I0/cos3 θ. In such case, the first and second solid-state light sources 20, 30 may be distributed on the spherical surface 12 more evenly. Thereby, the illumination device 100, 200 can provide more uniform output light.
It is to be understood that the above-described embodiments are intended to illustrate rather than limit the disclosure. Variations may be made to the embodiments without departing from the spirit of the disclosure. The above-described embodiments illustrate the scope of the disclosure but do not restrict the scope of the disclosure.
Number | Date | Country | Kind |
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200910302263.7 | May 2009 | CN | national |