The present invention relates to a lens for an LED.
Light emitting diodes (LEDs) have many advantages over fluorescent tubes. LEDs are more efficient, last longer, and are less sensitive to vibrations and low temperatures. To take advantage of the benefits of LEDs, LEDs are being included in lights of various shapes, such as in the shape of fluorescent tubes. However, known LEDs are constrained by the directional light output of the LEDs in contrast to, for example, the uniform non-directional light output of fluorescent tubes. One way of spreading the directional light output from an LED is to direct the light through a diffuser.
Known LEDs provide directional light output that may result in the appearance of bright spots of light. Thus, known lights in the shape of fluorescent tubes including LEDs, for example, may appear different from fluorescent tubes, which are characterized by their uniform light distribution.
A light modifier for an LED which produces light about a central axis is described herein. The light modifier can reduce the appearance of bright spots resulting from the directional light output of the LED. In one example of such a light modifier, a lens defines an indentation. The indentation is angled relative to the central axis by an amount less than a complementary angle of a critical angle of the lens along the indentation.
In another embodiment, a replacement light for a fluorescent tube usable in a fluorescent fixture is provided. The replacement light includes a support structure having a longitudinal axis. At least one LED is connected to the support structure, and the at least one LED produces light about respective central axes. At least one lens is positioned along the central axis of the at least one LED, and the lens defines an indentation angled relative to the central axis by an amount less than a complementary angle of a critical angle of the lens along the indentation. At least one electrical connector at a longitudinal end of the support structure is in electrical communication with the at least one LED.
In another embodiment, a method of forming a lens defining an indentation angled by an amount less than a complementary angle of a critical angle of the lens along the indentation relative to a central axis of light produced by an LED is provided. The method includes extruding material in an extrusion direction to form a sheet of greater width than the lens. The sheet has a same profile as the lens. The method also includes sectioning the sheet to form the lens.
In another embodiment, a replacement light for a fluorescent tube usable in a fluorescent fixture is provided. The replacement includes a support structure having a longitudinal axis. Multiple LEDs connected to the support structure, and the LEDs producing light about respective central axes. At least one light pipe is positioned along the central axis of one of the LEDs, and the light pipe has a reflector positioned over at least a portion of the LED such that the light initially emitted from the LED strikes the reflector. At least one electrical connector at a longitudinal end of the support structure is in electrical communication with the multiple LEDs.
These and other embodiments will be described in additional detail hereinafter.
The description herein makes reference to the accompanying drawings wherein like reference numerals refer to like parts throughout the several views, and wherein:
Examples of lenses for use with LEDs are discussed below with reference to
A diffuser can be placed in the path of light produced by an LED to reduce the appearance of bright spots. However, as shown by line 104 in
The LED 16 can produce light in a Lambertian distribution centered about a central axis 17, which can extend normally to the LED 16. However, the LED 16 may also exhibit a different distribution of light, in which case the axis 17 can still represent at least one of a center point of the distribution of light and an axis normal to the LED 16. The LED 16 can be an LED of any power rating, e.g. 0.05 W, 0.10 W, 0.25 W, or a high power LED, such as a surface-mount LED of the type available from Nichia. Electrical connectors other than the illustrated leads 12 and 14 can be included depending on the type of LED 16 used. The LED 16 can produce a variety of wavelengths of light, such as white light, red light, blue light, or ultra-violet light.
The lens 18 can encase the LED 16 and can also encase portions of the leads 12 and 14 as shown in
As best shown in FIG, 4, the lens 18 can define a conical indentation 20. The conical indentation 20 can be centered over the axis 17 of the LED 16, and the indentation 20 can have a diameter large enough to cover the bright spot of light produced by the LED 16. (Given that the term “bright spot” is subjective, the bright spot does not necessarily have a definite diameter. However, the size of the bright spot can be determined based on, for example, consumer opinion or a standardized objective consideration, e.g., an area through which a certain percentage of the light produced by the LED 16 passes.) While the indentation 20 should be large enough to cover the bright spot produced by the LED 16, the indentation 20 can itself produce a dark spot since light can be totally internally reflected by a continuous sidewall 21 of the conical indentation 20. As a result, the indentation 20 should not be greatly larger than the bright spot. Thus, a trade-off can exist in determining the size of the indentation 20 between reflecting light that would otherwise produce the bright spot and not creating too large of a dark spot. A way of mitigating the dark spot created by the indentation 20 is discussed below.
The conical indentation 20 can include sidewalls 21 angled relative to the central axis 17 such that light produced by the LED 16 that contacts the sidewall 21 is totally internally reflected, Since the critical angle for light contacting the sidewall 21 is measured from a line normal to the sidewall 21, the angle θ1 between the axis 17 and the sidewall 21 should be less than a complementary angle of the critical angle of the sidewall 21. For example, if the lens 18 is made from polycarbonate and air surrounds the LED package 10, the critical angle for light striking the sidewall 21 is approximately forty degrees. That is, if light strikes the sidewall 21 at an angle greater than forty degrees from a line normal to the lens 18, then the light will be totally internally reflected. Since the angle θ1 shown in
While the angle θ1 can be up to, in the example above, fifty degrees, the specific angle θ1 actually used can be selected based on the desired distribution of light. As the angle θ1 increases, the indentation 20 distributes light over a greater area radial of the axis 17, which may reduce the amount of light directed to an area to be illuminated. However, as the angle θ1 decreases, a greater amount of light is produced in the vicinity around the indentation 20, which can create the appearance of a bright halo of light around the indentation 20. Angling the sidewall 21 to produce a bright halo of light may allow a large amount of light to be directed toward a space to be illuminated while still reducing the appearance of bright spots.
Another consideration in selecting both the diameter of the indentation 20 and the angle θ1 is the depth of the indentation 20, since the depth is a function of the diameter and angle θ1. For example, the depth of the indentation 20 can be selected such that a tip of the indentation is near the LED 16 to reduce the distance light has to travel from the LED 16 before contacting the indentation 20, thereby reducing the likelihood that the light will be refracted by an imperfection in the lens 18 prior to contacting the indentation 20.
One way of determining an optimal indentation 20 diameter, sidewall 21 angle θ1, and indentation 20 depth is objectively through experimentation or calculation, with the size, angle θ1, and depth selected to obtain as even a distribution of light as possible (or some other distribution of light, if desired). For example, as shown in
As discussed earlier, diffusion is generally inefficient when the angle of incidence is large. However, the halo of light that can be produced around the indentation 20 can have a small angle of incidence relative to an annular portion of the lens 18 circumscribing the indentation 20. As a result, providing the lens 18 with a diffusing surface 22 around the indentation 20 can efficiently diffuse the bright halo of light. The diffusing surface 22 as shown includes surface roughening, though other diffusers such as a diffusing film can be used to produce diffusion. Alternatively, other portions of the lens 18 can include a diffusing surface. For example, the entire lens 18 other than the indentation 20 can include a diffuser.
Diffusing the halo of light can reduce the appearance of a dark spot created by the indentation 20, and it can also lower the brightness of the halo to be more inline with the brightness of other portions of the lens 18. For example, as shown in
Thus, unlike many known LEDs which produce a blight spot represented by the spike shaped distribution indicated by line 102 in
Also, while the angle θ1 of the sidewall 21 relative to the axis 17 is described above as designed to achieve TIR, this is not intended to mean that every photon of light that contacts the sidewall 21 is reflected. Current manufacturing limitations make achieving 100% TIR difficult, as the sidewall 21 may not be perfectly smooth. Instead, the angle θ1 can be such that theoretically, without such imperfections, TIR is achieved. Also, the sidewall 21 can be made substantially smooth such that enough light is reflected that the light distribution of the light 10 meets consumer preferences. The sidewall 21 can be made substantially smooth by, as examples, forming the indentation 20 with higher tolerances than normal or polishing the indentation 20, while forming an uneven texture in the indentation 20 to diffuse light may prevent the sidewall 21 from being substantially smooth. Alternatively, a reflector can be placed in the indentation 20 to reflect light that refracts through the sidewall 21. However, since reflectors can be less efficient than TIR, the lens 18 can be designed such that a large portion of light is reflected by TIR when contacting the sidewall 21.
While the indentation 20 described above is conically shaped, an indentation can have an alternative shape and still provide TIR. For example,
The lens 38 can provide a more even distribution of light than a known LED, though the distribution of light provided by the lens 38 can differ from the distribution of light provided by the lens 18. For example, when the angle θ2 is slightly greater or smaller than twenty degrees (e.g., between approximately fifteen and twenty five degrees), the indentation 40 produces two bright lines of light, one along each of its edges. Thus, the V-shaped indentation 40 can tend to create two bright lines separated by a dark line instead of the bright halo circumscribing a dark spot created by the conical indentation 20. However, to reduce the appearance of the dark line, the lens 38 can include a diffusing surface 44 on each side of the indentation 40 to diffuse some of the light that would otherwise contribute to the brightness of the bright lines. The diffusing surface 44 can direct light into the area above the indentation 40, which can reduce the appearance of the dark line. Also, other indentations can have other shapes not illustrated, such as an inverted pyramid shape or an asymmetrical shape.
While the above described lenses 18 and 38 are parts of stand-alone LED packages 10 and 30, respectively, lights can include LEDs having lenses to reduce the appearance of bright spots. For example,
One of the bi-pin end caps 52 can be disposed at each longitudinal end of the housing 56 for physically and electrically connecting the light 50 to a fluorescent fixture. The end caps 52 can be electrically connected to the circuit board 54 to provide power to the LEDs 58. Each end cap 52 can include two pins, though two of the total four pins can be “dummy pins” that do not provide an electrical connection. Alternatively, other types of end caps can be used, such as single pin end caps. Also, while the end caps 52 are shown as including cup-shaped bodies, the end caps 52 can have a different configuration (e.g., the end caps 52 can be shaped to be press fit into the housing 56).
The circuit board 54 as illustrated in
The housing 56 as shown in
The LEDs 58 can each produce light in a Lambertian distribution centered on a central axis 59, which can extend normally to its respective LED 58 as shown in
The lens 60 can extend over multiple LEDs 58 as shown in
Each hemispherical portion 61 can define an indentation 62 and a diffusing surface 64. The indentation 62 can be conical with a continuous sidewall 66 angled at an angle θ3 relative to the respective axis 59. Each indentation 62 can be centered over one of the axes 59, and the indentation 62 can have a diameter sufficient in diameter to reduce a bright spot of light produced by its respective LED 58. The specific geometry of the indentation 62 can be based on the same considerations discussed above in reference to the indentation 20.
Further, as shown in
The lens 60 additionally includes connecting portions 63. Each connecting portion 63 can include a Fresnel type lens 68 approximately midway between adjacent hemispherical portions 61. A portion of light produced by the LEDs 58 may not enter the hemispherical portions 61 of the lens 60. Instead, this light may enter one of the connecting portions 63. The connecting portion 63 can act as a light pipe, directing light to the Fresnel lens 68. The Fresnel lens 68 can direct the light outward, away from the circuit board 54. However, depending on the design of the connecting portion 63, some of the light may refract out of the connecting portion prior to reaching the Frensel lens 68. As a result, the lens 60 can reduce the appearance of dark spots between hemispherical portions 61.
Additionally, while the above described embodiments describe lenses that are integral with an LED package (i.e., the lenses function as casings for LEDs), this need not be the case. For example,
The lower cover 76 can be made from a polymer such as polycarbonate or ABS, and lower cover 76 can be generally U-shaped and engaged with the heat sink 74. For example, the lower cover 76 can be sized to slidably receive the heat sink 74, though the cover 76 can alternatively be bonded or otherwise adhered to the heat sink 74. Further, the lower cover 76 can be configured to secure the upper cover 80 in place. For example, the lower cover 76 can define grooves for slidably receiving the upper cover 80. Since little light is directed toward the lower cover 76 as shown in
The LEDs 78 can be similar to the LEDs 58, with each LED 78 producing light in a Lambertian distribution about a central axis 79 as shown in
The upper cover 80 can function as a lens to provide a more even distribution of light than known LED lights shaped as fluorescent tubes, though the distribution of light provided by the cover 80 can differ from the distribution of light provided by the lens 60 described above in reference to
Also as shown in
However, the orientation of the indentations 94 causes the light 90 to have a different appearance compared to the light 70. While the light 70 can result in two bright lines extending longitudinally the length of the light 70, the light 90 can result in a series of bright lines extending perpendicular to the longitudinal axis of the light 90. More specifically, each indentation 94 can result in two bright lines extending perpendicularly to the longitudinal axis of the light 90 due to the orientation of the indentations 94. A dark line created by the indentation 94 can separate the two lines. The darkness of this line can be mitigated by, for example, including a diffusing surface on each side of the indentation 94. An additional dark line can exist between adjacent indentations 92, though the exact distribution of light between the indentations 92 can vary depending on the spacing of the LEDs 78 and the geometries of the indentations 92. Alternatively, a cover can be formed to include conical indentations, pyramid shaped indentations, or other indentation shapes.
The cover 92 shown in
While the above described lights 50, 70, and 90 are shaped to replace fluorescent tubes, a lens as described herein can also be used in other types of lights, such as flashlights and lights shaped to replace incandescent bulbs.
Each light pipe 131 can be adjacent to another light pipe 131 so that a space 129 exists between adjacent light tubes. The light pipe 131 can be made of any suitable light transmitting material such as acrylic. The light pipe 131 can have a generally rectangular cross section and a level surface although other suitably shaped light pipes are also available. Further, the light pipe 131 may be of any sufficient size to provide an even distribution of light in the light tube 120, as discussed in more detail below, across the length and width thereof.
The space 129 can be of any suitable dimension as desired or required. Alternatively, in other embodiments, no space can exist between adjacent light pipes 131 (i.e. light pipes are physically touching), a single light pipe can extend over all or most of the LEDs 128 or a single light pipe can be positioned over more than one LED 128.
Each light pipe 131 can define a conical indentation 132 with a continuous sidewall 136 angled at an angle θ5 relative to a central axis 135. The indentation 132 can be shaped to provide TIR and reflect light down the light pipe 131. Each indentation 132 can be centered over one of the axes 135, and the indentation 132 can have a diameter sufficient in size to reduce a bright spot of light produced by its respective LED 128. The specific geometry of the indentation 132 can be determined using the same considerations (i.e., the width and depth of the indentation 132 and the angle θ5) described above in reference to the indentation 20. For example, the angle θ5 can be approximately twenty degrees, and the indentation 132 can extend to adjacent its respective LED 128. Further, the conical indentation 132 is illustrated as having a planar surface, in other embodiments the conical indentation can have a curved surface.
The light pipe 131 permits the light L to be transported across the surface thereof through TIR. The light is extracted at multiple points P1-P4, as discussed in more detail below by a diffusing surface 134. Further, the light L diminishes at, for example, points P1 and P4 (i.e. points that are further from the light source LED 128) as the light is transported down the length of the pipe. The indication of points P1-P4 and illustration of the light L are provided in order to allow easy understanding of the invention and do not limit the scope of embodiments of the invention. Other embodiments may have more or less points where the light is emanated and reflected and may have a different distribution of light L.
The diffusing surface 134 disrupts the TIR to permit light to emanate at points P1-P4. The diffusing surface 134 can be, for example, grooves, pits, bumps or any other type of extraction elements and be any combination thereof. Each extraction element of diffusing surface 134 may be of varying size and at the same or different distances from other extraction elements. The diffusing surface may be printed, formed as a part of or otherwise adhered to a top surface 131c of the light pipe 131. Alternatively the diffusing surface maybe printed, formed as a part of or otherwise adhered on a bottom surface 131d of the light pipe 131. The light L emanating at points P1-P4 may strike diffusing surface 134 and be diffused thereby. The emitted light may emanate from the light pipe 131 in a variety of directions. The light L may also be emanated in a direction back within the light pipe 131.
The pattern of the diffusing surface 134 can be, for example, selected to provide a substantially uniform distribution of light across the length and width of the light pipe 131. The diffusing surface 134 can be evenly spread across each light pipe 131 or, as illustrated in
While the indentation 132 is conically shaped, an indentation can have an alternative shape and still provide TIR. For example,
While the light pipes 131 and 161 have a generally rectangular cross section and a level top surface, a light pipe can have an alternative shape. For example,
The reflector 218 can cover the LED 218. Specifically, the reflector 218 can be positioned such that the light L emitted directly from the LED 128 would strike the reflector 218 and experience TIR. As such, the reflector can additionally cover an area slightly surrounding the LED 218 as desired or required.
After the light L strikes the reflector 218, the light can be transported through the light pipe 211 similar to the manner described in
Although the light pipes 131, 161, 181 and 211 illustrate light L emitted through the top surface thereof, in other embodiments, light may be extracted and emitted in any direction such the top, bottom, sides or ends of the light pipes. For example, in one embodiment, a light tube can include light pipes that extract and emit light in all directions (i.e. 360°). Further, as discussed previously, the LEDs 128, 158, 188 and 218 may be any suitable LED white or colored LED. If the LEDs 128, 158, 188 and 218 are colored LEDs, a wavelength-converting material may be included in, on or outside the light pipes 131, 161, 181 and 211, respectively. Alternatively, a wavelength-converting layer can be included between LEDs 128, 158, 188 and 218 and the light pipes 131, 161, 181 and 211, respectively.
As discussed previously, LED packages containing conical indentation 20 and V-shaped indentation 40 can create the appearance of a bright halo of light circumscribing a dark spot. A way of mitigating the dark spot is to provide, for example a diffusing surface around the indentations such that the bright halo of light is diffused. Other light tubes are available having a double-coned LED package and or a double-coned lens to obfuscate the bright spot created by the LED while also mitigating the dark spot by further spreading the light rays.
For example,
Each LED 308 produces light in a Lambertian distribution about a central axis 309 as shown in
The linear lens 311 also includes two flared outer walls 311c and 311d extending from edges 311e and 311f, respectively. Edge 311e is formed by an intersection of sidewall 311a and outer wall 311c and edge 311f is formed by an intersection of sidewall 311b and outer wall 311d. Two base walls 311g and 311h vertically extend to the circuit board 304 from edges 311i and 311k. Edge 311i is formed by an intersection of outer wall 311c and base wall 311g and edge 311k is formed by an intersection of outer wall 311d and base wall 311h.
Outer walls 311c and 311d can be angled relative to a horizontal axis 320 to receive the totally internally reflected light from sidewalls 311a and 311b and to redirect the light into an external path parallel and/or substantially parallel to a central axis 309. In other words, the primary light rays L1 are redirected to produce light rays L2 in this manner by, for example, angling outer walls 311c and 311d at suitable angles θ8. Angle θ8 is the angled between outer walls 311c and 311d and horizontal axis 320. As illustrated in
Additionally, linear lens 311 can also include an optional reflector 315 on end surfaces 311k (only one end surface shown in
While the double-coned concept is implemented within a linear lens and is described above as extending through the light tube, other embodiments may include the double-coned concept as part of an LED package. For example,
Lens 408 includes a V-shaped indentation 440 having two angled sidewalls 441 and 442. The indentation 440 can have a width sufficient to block a bright spot produce by the LED 416. The sidewalls 441 and 442 can be angled to produce TIR, with the angles θ9 between the sidewalls 441 and 442 and the axis 417 less than a complementary angle of a critical angle of the sidewalls 41 and 42. The geometry of the indentation 440 (i.e., the width and depth of the indentation 440 and the angle θ9) can be determined with the same considerations as used to determine the geometry of the indentation 20 described above. As illustrated in
The lens 408 also includes a circumferentially flared outer wall 450 extending from points (or edges) 452 and 454, respectively. Point 452 is formed by an intersection of sidewall 441 and outer wall 450 and point 454 is formed by an intersection of side wall 442 and outer wall 450. A circumferentially extending base wall 456 vertically extends from an edge 458. Edge 458 is formed by an intersection of outer wall 450 and base wall 456.
Outer wall 450 can be angled relative to a horizontal axis 467 to receive the totally internally reflected light from sidewalls 441 and 442 and, similar to the linear lens 311 of
In another example,
Rather than a V-shaped indentation as described in lens 408, lens 508 includes a conical indentation 540 having an angled sidewall. The indentation 440 can have a width sufficient to block a bright spot produce by the LED 416. Sidewall 541 can be angled to produce TIR, with the angles θ11 between the sidewall 541 and the axis 517 less than a complementary angle of a critical angle of the sidewall 541. The geometry of the indentation 540 (i.e., the width and depth of the indentation 540 and the angle θ11) can be determined with the same considerations as used to determine the geometry of the indentation 20 described above. As illustrated in
The lens 508 also includes a circumferentially flared outer wall 550 extending from an annular edge 542. Annular edge 542 is formed by an intersection of sidewall 541 and outer wall 550. A circumferentially extending base wall 556 vertically extends from an edge 558. Edge 558 is formed by an intersection of outer wall 550 and base wall 556.
Outer wall 550, similar to outer wall 450 of
While the above described lenses 408 and 508 are parts of stand-alone LED packages 400 and 500, respectively, lights can include LEDs having lenses incorporating the double-coned structure. For example,
Additionally, light tube 600 can include connecting portions 663 extending between adjacent double-coned portions 611. Connecting portions 663 can be similar to connecting portions 63 illustrated in
Each double-coned portion 611 can define a V-shaped indentation 612 having two angled sidewalls 611a and 611b. The indentation 612 can have a width sufficient to block a bright spot produce by the LED 608. The sidewalls 611a and 611b can be angled to produce TIR, with the angles θ13 between the sidewalls 611a and 611b and the axis 609 less than a complementary angle of a critical angle of the sidewalls 611a and 611b. The geometry of the indentation 612 (i.e., the width and depth of the indentation 612 and the angle θ13) can be determined with the same considerations as used to determine the geometry of the indentation 20 described above. As illustrated in
The double coned portion 611 also includes a circumferentially flared outer wall 650 extending from points (or edges) 652 and 654, respectively. Point 652 is formed by an intersection of sidewall 611a and outer wall 650 and point 654 is formed by an intersection of side wall 611b and outer wall 650. A circumferentially extending base wall 656 vertically extends from an edge 658. Edge 658 is formed by an intersection of outer wall 650 and base wall 656.
Outer wall 650 can be angled relative to a horizontal axis 620 to receive the totally internally reflected light from sidewalls 611a and 611b, similar to the linear lens 311 of
In another example,
Conical lens portions 711 extend over each LED 708 similar to double-coned portions 611. However, rather than a V-shaped indentation, each portion 711 includes a conical indentation 740 having an angled sidewall 711a. The indentation 740 can have a width sufficient to block a bright spot produce by the LED 708. Sidewall 711a can be angled to produce TIR, with the angles θ15 between the sidewall 711a and the axis 709 less than a complementary angle of a critical angle of the sidewall 711a. The geometry of the indentation 740 (i.e., the width and depth of the indentation 740 and the angle θ15) can be determined with the same considerations as used to determine the geometry of the indentation 20 described above. As illustrated in
Each portion 711 also includes a circumferentially flared outer wall 750 extending from an annular edge 742. Annular edge is 742 formed by an intersection of sidewall 711a and outer wall 750. A circumferentially extending base wall 756 vertically extends from an edge 758. Edge 758 is formed by an intersection of outer wall 750 and base wall 756.
Outer wall 750, similar to outer wall 450 of
The above-described embodiments have been described in order to allow easy understanding of the invention and do not limit the invention. On the contrary, the invention is intended to cover various modifications and equivalent arrangements included within the scope of the appended claims, which scope is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structure as is permitted under the law.
This application claims priority from U.S. Provisional Patent Application No. 61/144,853, filed Jan. 15, 2009, the entire contents of which is incorporated herein by reference.
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| Number | Date | Country | |
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| 20100177532 A1 | Jul 2010 | US |
| Number | Date | Country | |
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| 61144853 | Jan 2009 | US |