WO2018004221A1 - Led lens - Google Patents

Led lens Download PDF

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Publication number
WO2018004221A1
WO2018004221A1 PCT/KR2017/006736 KR2017006736W WO2018004221A1 WO 2018004221 A1 WO2018004221 A1 WO 2018004221A1 KR 2017006736 W KR2017006736 W KR 2017006736W WO 2018004221 A1 WO2018004221 A1 WO 2018004221A1
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WO
WIPO (PCT)
Prior art keywords
led
lens
convex portion
light
exit surface
Prior art date
Application number
PCT/KR2017/006736
Other languages
French (fr)
Korean (ko)
Inventor
김성빈
김병욱
Original Assignee
주식회사 애니캐스팅
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Publication date
Application filed by 주식회사 애니캐스팅 filed Critical 주식회사 애니캐스팅
Priority to JP2018523407A priority Critical patent/JP6530864B2/en
Publication of WO2018004221A1 publication Critical patent/WO2018004221A1/en

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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B19/00Condensers, e.g. light collectors or similar non-imaging optics
    • G02B19/0033Condensers, e.g. light collectors or similar non-imaging optics characterised by the use
    • G02B19/0047Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with a light source
    • G02B19/0061Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with a light source the light source comprising a LED
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B19/00Condensers, e.g. light collectors or similar non-imaging optics
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B3/00Simple or compound lenses
    • G02B3/02Simple or compound lenses with non-spherical faces
    • G02B3/08Simple or compound lenses with non-spherical faces with discontinuous faces, e.g. Fresnel lens
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/48Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor body packages
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/48Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor body packages
    • H01L33/483Containers
    • H01L33/486Containers adapted for surface mounting
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/48Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor body packages
    • H01L33/58Optical field-shaping elements

Definitions

  • the present invention relates to an LED lens capable of evenly spreading the light from the LED.
  • LED Light Emitting Diode
  • LED Light Emitting Diode
  • the light tends to diverge to a narrow area, and in order to apply it to the lighting device, it is necessary to distribute the light evenly over a wide area.
  • the LED lens according to the prior art has a problem in that a circular band-shaped dark portion (darker portion than the periphery) occurs near the LED optical axis, and a hot spot (lighter portion than the periphery) occurs in the LED optical axis region. .
  • the present invention is to solve the above problems, and provides an LED lens that can improve the phenomenon that a circular band-shaped dark portion occurs near the LED optical axis, and the phenomenon that a hot spot occurs in the LED optical axis region.
  • the incident surface from which the light emitted from the LED is incident into the lens and the inside of the lens through the incident surface An emission surface for emitting light incident to the outside of the lens, the emission surface having a first exit surface forming a convex curved shape on the side of the LED on a vertical cross section, and positioned around the first exit surface;
  • the convex portion may be formed in a circular band shape surrounding an inflection point existing in a circular shape about the optical axis of the LED on a plane. Can be.
  • the emission surface has a convex shape upward in the vertical cross-section, the first convex portion and the second convex portion having a planar circular band shape is further formed,
  • the first block portion is formed on the first exit surface with a predetermined distance spaced from the convex portion to the first exit surface side, and the second convex portion is spaced a predetermined distance from the convex portion to the second exit surface side. It may be formed on the second exit surface.
  • the first convex portion and the second convex portion may be symmetric with each other based on the convex portion on a vertical cross section.
  • the LED lens according to the embodiment of the present invention having the above configuration, the effect of improving the phenomenon that the circular band-shaped dark portion near the LED optical axis, and the phenomenon that the hot spot occurs in the LED optical axis region There is.
  • FIG. 1 is a vertical cross-sectional view showing an LED lens according to an embodiment of the present invention
  • FIG. 2 is a schematic plan view of FIG. 1;
  • FIG. 3 is a view showing a result of simulating the light distribution of light emitted through the lens of FIG.
  • FIG. 4 is an enlarged view of a portion 'B' of FIG. 3,
  • FIG. 5 is an enlarged view of a region 'A' of FIG. 1,
  • FIG. 6 is a vertical sectional view showing the LED lens according to another embodiment of the present invention.
  • FIG. 7 is an enlarged view of region 'A' of FIG. 6.
  • FIG. 8 is a schematic plan view of FIG. 6;
  • FIG. 9 is a vertical sectional view showing the LED lens according to another embodiment of the present invention.
  • FIG. 10 is a schematic plan view of FIG. 9;
  • FIG. 11 is a diagram illustrating a result of simulating a light distribution of light emitted through the lens of FIG. 9.
  • FIG. 12 is an enlarged view of a portion 'B' of FIG. 11.
  • FIG. 1 is a vertical cross-sectional view showing an LED lens according to an embodiment of the present invention.
  • an LED lens 10 according to an embodiment of the present invention has an incident surface 20 in which light L1 emitted from the LED 11 is incident into the lens 10. And an emission surface 30 for emitting the light L2 incident into the lens 10 through the incident surface 20 to the outside of the lens 10.
  • the LED lens 10 is formed in the center of the bottom 13, the bottom 13, receiving groove 14, the bottom 13 and the exit surface for accommodating the LED 11 And a flange 17 connecting the 30 and protruding outward from the exit surface 30, and a leg 17 provided below the flange 15.
  • the incident surface 20 may be made of the inner surface of the receiving groove (14).
  • the light L1 emitted from the LED 11 accommodated in the accommodation groove 14 may be incident into the lens 10 through the entrance surface 20, which is the inner surface of the accommodation groove 14.
  • the exit surface 30 is positioned around the first exit surface 32 and the first exit surface 32 having a curved surface convex on the LED 11 side, that is, a downwardly convex curved surface, and the LED 11 is disposed.
  • a second exit surface 34 having a convex curved shape on the opposite side, that is, a convex upward curved shape, and an inflection point 37 is present at the connection portion between the first exit surface 32 and the second exit surface 34. do.
  • the emission surface 30 includes the first emission surface 32 having the curved surface convex downward and the second emission surface 34 having the curved surface upward convex
  • the incident surface 20 The light L2 incident into the lens 10 may be emitted to the outside of the lens 10 through the emission surface 30 in an evenly diffused state.
  • FIG. 2 is a schematic plan view of FIG. 1.
  • the planar shape of the entrance face 20 and the exit face 30 may have a substantially circular shape around the LED 11 optical axis 12, and the flange 15 may have an exit face. It may protrude from both sides to 30.
  • the first exit surface 32 is a center region including the LED 11 optical axis 12 among the planar regions of the exit surface 30, and the second exit surface 34 is the planar region of the exit surface 30.
  • the inflection point 37 existing between the first exit surface 32 and the second exit surface 34 is an edge region surrounding the first exit surface 32 among the LED 11 and the optical axis 12 in plan view. It will exist in the form of a circle.
  • FIG. 3 is a diagram illustrating a result of simulating a light distribution of light emitted through the lens of FIG. 1, and FIG. 4 is an enlarged view of a portion 'B' of FIG. 3.
  • the light distribution of the LED lens 10 according to FIG. 1 generates a dark portion b that is darker than the periphery of a substantially circular band near the optical axis 12 of the LED 11.
  • the LED (11) optical axis 12 can be confirmed that the hot spot (h), which is a brighter part than the surroundings, but the light uniformity by the dark portion (b) and hot spot (h) as described above. The problem of falling.
  • FIG. 5 is an enlarged view of an inflection point and an enlarged area 'A' of FIG. 1.
  • the dark region C causes a substantially circular band-shaped dark region b to occur near the optical axis 12 on the light distribution. do.
  • first exit surface 32 and the second exit surface 34 This is the shape of the first exit surface 32 and the second exit surface 34, that is, the first exit surface 32 has a curved surface convex downwards, while the second exit surface 34 has a curved surface upwardly convex It is because of the phenomenon.
  • the first exit surface 32 has a curved surface convex downward, and the second exit surface 34 has a curved surface convex upward, the first exit surface 32
  • the refraction angle of the light (L4) emitted to the outside of the lens 10 through the difference occurs, thereby Since the angle of refraction of the light exiting the lens 10 is rapidly changed with respect to the inflection point 37 connected between the first exit surface 32 and the second exit surface 34, the region substantially above the inflection point 37.
  • the light emitted to the remarkably decreases, whereby the dark region C is formed.
  • Fresnel reflection is a reflection generated when light passes through an interface between materials having different refractive indices. Some of the light exiting through the exit surface 30 by the Fresnel reflection is the bottom surface 20. The light reflected by the bottom surface 20 is reflected back from the bottom surface 20 and is directed toward the optical axis 12 portion. The hot spot h is generated at the optical axis 12 portion by the light. Will be done.
  • FIG. 6 is a vertical cross-sectional view illustrating an LED lens according to another exemplary embodiment.
  • FIG. 7 is an enlarged view of an inflection point of FIG. 6 and is an enlarged view of region 'A' of FIG. 6. 6 is a schematic plan view.
  • a problem occurs in the light distribution distribution of the lens 10 according to FIG. 1, that is, a circular band-shaped dark portion b occurs near the LED 11 optical axis 12.
  • the detailed description of the other components and the reference numerals refer to the detailed description and reference numerals of the lens 10 according to FIG.
  • the LED lens 40 according to the present exemplary embodiment includes a convex portion 42 formed at a portion of the inflection point 37 and having a convex shape on the vertical cross section.
  • the convex portion 37 when the convex portion 37 is formed at the inflection point 37, the light L5 emitted to the outside of the lens 40 through the inflection point 37 is convex portion 37. By being emitted through), it is refracted in the direction of the dark portion region C generated when there is no convex portion 37, and is emitted. Accordingly, a circular band shape in the light distribution distribution generated by the dark portion region C is produced. It is possible to improve the dark portion (b) of the.
  • the convex portion 42 formed at the inflection point 37 scatters the light reflected by the Fresnel at the exit surface 30 from the bottom surface 13 to the LED optical axis 12.
  • the convex portion 42 formed at the inflection point 37 scatters the light reflected by the Fresnel at the exit surface 30 from the bottom surface 13 to the LED optical axis 12.
  • the convex portion 42 is formed to surround the inflection point 37, that is, the inflection point 37, whereby the convex portion 42 has an optical axis 12 of the LED 11 in plan view. It may be formed in a circular band shape surrounding the inflection point (37) existing in the form of a circle around the center.
  • the convex portions 42 may not be formed in a circular band shape, but may be formed in a plurality of states spaced apart at predetermined intervals in the circumferential direction of the inflection point 37 present in a planar circular form. .
  • the convex portion 42 is formed in a circular band shape surrounding the inflection point 37, and the light is more evenly diffused than a plurality of convex portions are formed at predetermined intervals in the circumferential direction. It is preferable to make it possible.
  • FIG. 9 is a vertical cross-sectional view showing the LED lens according to another embodiment of the present invention
  • Figure 10 is a schematic plan view of FIG.
  • the LED lens 40 may include the first convex portion 43 and the first convex portion 43 having a convex shape on the vertical cross section in the same manner as the convex portion 42 in addition to the convex portion 42.
  • the convex portion 44 may further include.
  • the first convex portion 43 may be formed on the first exit surface 32 in a state spaced apart from the convex portion 42 toward the first exit surface 32 by a predetermined distance
  • the second convex portion 44 may be It may be formed on the second exit surface 34 in a state spaced apart from the convex portion 42 toward the second exit surface 34.
  • the first convex portion 43 and the second convex portion 44 have a circular band around the optical axis 12 of the LED 11 in a plane like the convex portion 42. It may be formed in a shape.
  • the first convex portion 43 and the second convex portion 44 are further formed in addition to the convex portion 42, the light reflected by the Fresnel from the exit surface 30 is reflected back from the bottom surface 13, thereby causing the LEDs. Since the light directed to the optical axis 12 can be further dispersed, the phenomenon in which the hot spot h is generated at the optical axis 12 portion as in the lens 10 according to FIG. 1 can be further improved.
  • first convex portion 43 and the second convex portion 44 may be formed to be symmetrical with each other based on the convex portion 42 on the vertical section. Then, the phenomenon in which the dark portion b occurs near the optical axis 12 and the hot spot h in the optical axis 12 may be further improved.
  • FIG. 11 is a diagram illustrating a result of a light distribution distribution of light emitted through the lens of FIG. 9, and FIG. 12 is an enlarged view of a portion 'B' of FIG.
  • the light distribution of the lens 40 according to the present embodiment is closer to the optical axis 12 than in FIGS. 3 and 4 showing the light distribution of the lens 10 according to FIG. 1. It can be seen that the development of the dark portion (b) and the occurrence of the hot spot (h) in the optical axis 12 region in the.
  • the dark portion b of a circular band is generated near the optical axis 12 on the screens of FIGS. 3 and 4.
  • the dark portion b is hardly distinguished from the surroundings. It can be confirmed that the improvement.
  • the shoulder shape is generated on both sides of the optical axis 12.
  • the shoulder shape almost disappears.
  • the shoulder shape is generated. Since it means that the dark portion (b) is darker than the surroundings, the disappearance of the shoulder shape in the graphs of Figs. 11 and 12 indicates that the occurrence of the dark portion (b) is improved.
  • the brightness of the optical axis 12 portion on the screen of FIGS. 11 and 12 is less bright than the brightness of the optical axis 12 portion on the screens of FIGS.
  • the hot spot (h) of the phenomenon is improved.
  • the present invention by forming a convex portion at the inflection point, the LED lens that can improve the phenomenon that the circular band-shaped dark portion near the LED optical axis, and the phenomenon that hot spots occur in the LED optical axis region
  • the embodiments may be modified in various forms. Therefore, the present invention is not limited to the embodiments disclosed in the present specification, and all forms changeable by those skilled in the art to which the present invention pertains will belong to the scope of the present invention.

Abstract

The present invention relates to an LED lens capable of uniformly dispersing light emitted from an LED. The LED lens according to one embodiment of the present invention, which is an LED lens for uniformly dispersing light emitted from an LED, comprises: an incident surface through which light emitted from the LED is incident on the inside of the lens; and a light-emitting surface for emitting the light, incident on the inside of the lens through the incident surface, to the outside of the lens, wherein the light-emitting surface comprises: a first light-emitting surface that forms a convex curved shape on the LED side in a vertical cross-section; and a second light-emitting surface that is located around the first light-emitting surface, and forms a convex curved shape on the opposite side of the LED. A convex portion having an upwardly convex shape in the vertical cross-section is formed in a region of an inflection point existing at a portion where the first light-emitting surface and the second light-emitting surface are connected, and the convex portion can be formed in a circular band shape which surrounds the inflection points existing in a circular shape about the optical axis of the LED in a plane.

Description

엘이디 렌즈LED lens
본 발명은 엘이디에서 나오는 빛을 고르게 확산시킬 수 있는 엘이디 렌즈에 관한 것이다.The present invention relates to an LED lens capable of evenly spreading the light from the LED.
일반적으로 엘이디(Light Emitting Diode, LED)는 광 변환 효율이 높으므로 소비전력이 상대적으로 매우 낮으며, 응답 속도가 빠르고, 점등회로가 간단하며, 안전성이 우수한 장점 때문에 실내외 조명용 광원으로 널리 사용되고 있다.In general, LED (Light Emitting Diode, LED) is widely used as a light source for indoor and outdoor lighting because of the high light conversion efficiency, the power consumption is relatively low, the response speed is fast, the lighting circuit is simple, and the safety is excellent.
그러나 광원으로 엘이디를 사용하는 경우에는 빛이 좁은 영역으로 집중하여 발산하는 경향이 있어서, 이를 조명장치에 적용하기 위해서는 빛을 넓은 영역에 고르게 분포되도록 할 필요가 있다. However, in the case of using the LED as a light source, the light tends to diverge to a narrow area, and in order to apply it to the lighting device, it is necessary to distribute the light evenly over a wide area.
이러한 기능을 수행하는 엘이디 렌즈에 대한 대표적인 선행기술로는 미국등록특허 제7348723호가 있다.Representative prior art for the LED lens performing this function is US Patent No. 7348723.
그러나 상기 선행기술에 따른 엘이디 렌즈는 엘이디 광축 근처에서 원형의 띠 모양의 암부(주변보다 어두운 부분)가 발생하는 문제가 있으며, 또한 엘이디 광축 부위에서 핫스팟(주변보다 밝은 부분)이 발생하는 문제가 있다.However, the LED lens according to the prior art has a problem in that a circular band-shaped dark portion (darker portion than the periphery) occurs near the LED optical axis, and a hot spot (lighter portion than the periphery) occurs in the LED optical axis region. .
본 발명은 상기와 같은 문제점을 해결하기 위한 것으로서, 엘이디 광축 근처에서 원형의 띠 모양의 암부가 발생하는 현상과, 엘이디 광축 부위에서의 핫스팟이 발생하는 현상을 개선할 수 있는 엘이디 렌즈를 제공한다.The present invention is to solve the above problems, and provides an LED lens that can improve the phenomenon that a circular band-shaped dark portion occurs near the LED optical axis, and the phenomenon that a hot spot occurs in the LED optical axis region.
본 발명의 일실시 예에 따른 엘이디 렌즈는, 엘이디에서 나오는 빛을 고르게 확산시키기 위한 엘이디 렌즈에 있어서, 상기 엘이디에서 나오는 빛이 상기 렌즈 내부로 입사하는 입사면과, 상기 입사면을 통해 상기 렌즈 내부로 입사한 빛을 상기 렌즈 외부로 출사시키는 출사면을 포함하고, 상기 출사면은 수직단면상 상기 엘이디 측에 볼록한 곡면 형상을 형성하는 제1출사면과, 상기 제1출사면의 주위에 위치하고 상기 엘이디 반대측에 볼록한 곡면 형상을 형성하는 제2출사면을 포함하고, 상기 제1출사면과 상기 제2출사면의 접속부분에 존재하는 변곡점 부위에는 수직단면상 상방으로 볼록한 형상을 가지는 볼록부가 형성되고, 상기 볼록부는 평면상 상기 엘이디의 광축을 중심으로 원형의 형태로 존재하는 변곡점을 감싸는 원형의 띠 형상으로 형성될 수 있다. In the LED lens according to an embodiment of the present invention, in the LED lens for evenly spreading the light emitted from the LED, the incident surface from which the light emitted from the LED is incident into the lens and the inside of the lens through the incident surface An emission surface for emitting light incident to the outside of the lens, the emission surface having a first exit surface forming a convex curved shape on the side of the LED on a vertical cross section, and positioned around the first exit surface; A convex portion having a convex portion having a convex shape upwardly in a vertical section, including a second exit surface forming a convex curved shape on an opposite side, and having an inflection point portion present at a connection portion between the first exit surface and the second exit surface; The convex portion may be formed in a circular band shape surrounding an inflection point existing in a circular shape about the optical axis of the LED on a plane. Can be.
또한, 본 발명의 일실시 예에 따른 엘이디 렌즈는, 상기 출사면에는 수직단면상 상방으로 볼록한 형상을 가지며, 평면상 원형의 띠 형상을 가지는 제1볼록부와 제2볼록부가 더 형성되고, 상기 제1블록부는 상기 볼록부로부터 상기 제1출사면 측으로 소정거리 이격된 상태로 상기 제1출사면 상에 형성되고, 상기 제2볼록부는 상기 볼록부로부터 상기 제2출사면 측으로 소정거리 이격된 상태로 상기 제2출사면 상에 형성될 수 있다. In addition, the LED lens according to an embodiment of the present invention, the emission surface has a convex shape upward in the vertical cross-section, the first convex portion and the second convex portion having a planar circular band shape is further formed, The first block portion is formed on the first exit surface with a predetermined distance spaced from the convex portion to the first exit surface side, and the second convex portion is spaced a predetermined distance from the convex portion to the second exit surface side. It may be formed on the second exit surface.
또한, 본 발명의 일실시 예에 따른 엘이디 렌즈는, 상기 제1볼록부와 상기 제2볼록부는 수직단면상 상기 볼록부를 기준으로 서로 대칭을 이룰 수 있다.In addition, in the LED lens according to an embodiment of the present invention, the first convex portion and the second convex portion may be symmetric with each other based on the convex portion on a vertical cross section.
상기와 같은 구성을 가지는 본 발명의 일실시 예에 따른 엘이디 렌즈에 의하면, 엘이디 광축 근처에서 원형의 띠 모양의 암부가 발생하는 현상과, 엘이디 광축 부위에서 핫스팟이 발생하는 현상을 개선할 수 있는 효과가 있다.According to the LED lens according to the embodiment of the present invention having the above configuration, the effect of improving the phenomenon that the circular band-shaped dark portion near the LED optical axis, and the phenomenon that the hot spot occurs in the LED optical axis region There is.
본 발명에 따른 효과들은 이상에서 언급된 효과들로 제한되지 않으며, 언급되지 않은 또 다른 효과들은 청구범위와 상세한 설명의 기재로부터 본 발명이 속하는 기술분야에서 통상의 지식을 가진자에게 명확하게 이해될 수 있을 것이다.Effects according to the present invention are not limited to the above-mentioned effects, and other effects not mentioned above will be clearly understood by those skilled in the art from the claims and the detailed description. Could be.
도 1은 본 발명의 일실시 예에 따른 엘이디 렌즈를 나타내는 수직단면도이고, 1 is a vertical cross-sectional view showing an LED lens according to an embodiment of the present invention,
도 2는 도 1의 개략적인 평면도이고,FIG. 2 is a schematic plan view of FIG. 1;
도 3은 도 1에 따른 렌즈를 통해 출사하는 빛의 배광분포를 시뮬레이션한 결과를 나타내는 도면이고, 3 is a view showing a result of simulating the light distribution of light emitted through the lens of FIG.
도 4는 도 3의 'B' 부분을 확대한 도면이고,4 is an enlarged view of a portion 'B' of FIG. 3,
도 5는 도 1의 'A' 영역을 확대한 도면이고, 5 is an enlarged view of a region 'A' of FIG. 1,
도 6은 본 발명의 다른 실시 예에 따른 엘이디 렌즈를 나타내는 수직단면도이고, 6 is a vertical sectional view showing the LED lens according to another embodiment of the present invention,
도 7은 도 6의 'A' 영역을 확대한 도면이고, FIG. 7 is an enlarged view of region 'A' of FIG. 6.
도 8은 도 6의 개략적인 평면도이고, FIG. 8 is a schematic plan view of FIG. 6;
도 9는 본 발명의 또 다른 실시 예에 따른 엘이디 렌즈를 나타내는 수직단면도이고, 9 is a vertical sectional view showing the LED lens according to another embodiment of the present invention,
도 10은 도 9의 개략적인 평면도이고, 10 is a schematic plan view of FIG. 9;
도 11은 도 9에 따른 렌즈를 통해 출사하는 빛의 배광분포를 시뮬레이션한 결과를 나타내는 도면이고, FIG. 11 is a diagram illustrating a result of simulating a light distribution of light emitted through the lens of FIG. 9.
도 12는 도 11의 'B' 부분을 확대한 도면이다.FIG. 12 is an enlarged view of a portion 'B' of FIG. 11.
이하, 첨부된 도면을 참조하여 본 발명에 따른 실시 예들에 대하여 본 발명이 속하는 기술 분야에서 통상의 지식을 가진 자가 용이하게 실시할 수 있도록 상세히 설명한다.DETAILED DESCRIPTION Hereinafter, exemplary embodiments of the present invention will be described in detail with reference to the accompanying drawings so that those skilled in the art may easily implement the present invention.
본 발명이 여러 가지 수정 및 변형을 허용하면서도, 그 특정 실시 예들이 도면들로 예시되어 나타내어지며, 이하에서 상세히 설명될 것이다. 그러나 본 발명을 개시된 특별한 형태로 한정하려는 의도는 아니며, 오히려 본 발명은 청구항들에 의해 정의된 본 발명의 사상과 합치되는 모든 수정, 균등 및 대용을 포함한다. While the invention allows for various modifications and variations, specific embodiments thereof are illustrated by way of example in the drawings and will be described in detail below. However, it is not intended to be exhaustive or to limit the invention to the precise forms disclosed, but rather the invention includes all modifications, equivalents, and alternatives consistent with the spirit of the invention as defined by the claims.
한편, 첨부 도면에서, 두께 및 크기는 명세서의 명확성을 위해 과장되어진 것이며, 따라서 본 발명은 첨부도면에 도시된 상대적인 크기나 두께에 의해 제한되지 않는다. On the other hand, in the accompanying drawings, the thickness and size are exaggerated for clarity of the specification, and thus the present invention is not limited by the relative size or thickness shown in the accompanying drawings.
도 1은 본 발명의 일실시 예에 따른 엘이디 렌즈를 나타내는 수직단면도이다.1 is a vertical cross-sectional view showing an LED lens according to an embodiment of the present invention.
도 1을 참조하면, 본 발명의 일실시 예에 따른 엘이디(Light Emitting Diode, LED) 렌즈(10)는 엘이디(11)에서 나오는 빛(L1)이 렌즈(10) 내부로 입사하는 입사면(20)과, 입사면(20)을 통해 렌즈(10) 내부로 입사한 빛(L2)을 렌즈(10) 외부로 출사시키는 출사면(30)을 포함한다.Referring to FIG. 1, an LED lens 10 according to an embodiment of the present invention has an incident surface 20 in which light L1 emitted from the LED 11 is incident into the lens 10. And an emission surface 30 for emitting the light L2 incident into the lens 10 through the incident surface 20 to the outside of the lens 10.
또한, 본 발명의 일실시 예에 따른 엘이디 렌즈(10)는 밑면(13), 밑면(13)의 중심부에 형성되어 엘이디(11)를 수용하는 수용홈(14), 밑면(13)과 출사면(30)을 연결하며 출사면(30)으로부터 외측으로 돌출되는 플랜지(15), 플랜지(15) 하부에 구비되는 레그(17)를 포함한다.In addition, the LED lens 10 according to an embodiment of the present invention is formed in the center of the bottom 13, the bottom 13, receiving groove 14, the bottom 13 and the exit surface for accommodating the LED 11 And a flange 17 connecting the 30 and protruding outward from the exit surface 30, and a leg 17 provided below the flange 15.
여기서, 입사면(20)은 수용홈(14)의 내면으로 이루어질 수 있다. Here, the incident surface 20 may be made of the inner surface of the receiving groove (14).
즉, 수용홈(14)에 수용된 엘이디(11)에서 나오는 빛(L1)은 수용홈(14)의 내면인 입사면(20)을 통해 렌즈(10) 내부로 입사할 수 있다.That is, the light L1 emitted from the LED 11 accommodated in the accommodation groove 14 may be incident into the lens 10 through the entrance surface 20, which is the inner surface of the accommodation groove 14.
또한, 출사면(30)은 엘이디(11) 측에 볼록한 곡면 형상 즉, 하방으로 볼록한 곡면 형상을 가지는 제1출사면(32)과, 제1출사면(32)의 주위에 위치하고 엘이디(11) 반대측에 볼록한 곡면 형상 즉, 상방으로 볼록한 곡면 형상을 가지는 제2출사면(34)을 포함하며, 제1출사면(32)과 제2출사면(34)의 접속부분에는 변곡점(37)이 존재한다.In addition, the exit surface 30 is positioned around the first exit surface 32 and the first exit surface 32 having a curved surface convex on the LED 11 side, that is, a downwardly convex curved surface, and the LED 11 is disposed. A second exit surface 34 having a convex curved shape on the opposite side, that is, a convex upward curved shape, and an inflection point 37 is present at the connection portion between the first exit surface 32 and the second exit surface 34. do.
이와 같이, 출사면(30)이 하방으로 볼록한 곡면 형상을 가지는 제1출사면(32)과, 상방으로 볼록한 곡면 형상을 가지는 제2출사면(34)을 포함하면, 입사면(20)을 통해 렌즈(10) 내부로 입사한 빛(L2)은 고르게 확산된 상태로 출사면(30)을 통해 렌즈(10) 외부로 출사할 수 있게 된다. As such, when the emission surface 30 includes the first emission surface 32 having the curved surface convex downward and the second emission surface 34 having the curved surface upward convex, the incident surface 20 The light L2 incident into the lens 10 may be emitted to the outside of the lens 10 through the emission surface 30 in an evenly diffused state.
도 2는 도 1의 개략적인 평면도이다.FIG. 2 is a schematic plan view of FIG. 1.
도 2에서 보이는 바와 같이, 입사면(20)과 출사면(30)의 평면상 형상은 엘이디(11) 광축(12)을 중심으로 대략 원형의 형상을 가질 수 있으며, 플랜지(15)는 출사면(30)으로부터 양측으로 돌출될 수 있다.As shown in FIG. 2, the planar shape of the entrance face 20 and the exit face 30 may have a substantially circular shape around the LED 11 optical axis 12, and the flange 15 may have an exit face. It may protrude from both sides to 30.
제1출사면(32)은 출사면(30)의 평면상 영역 중 엘이디(11) 광축(12)을 포함하는 중심영역이고, 제2출사면(34)은 출사면(30)의 평면상 영역 중 제1출사면(32)을 감싸는 가장자리 영역으로서, 제1출사면(32)과 제2출사면(34) 사이에 존재하는 변곡점(37)은 평면상 엘이디(11) 광축(12)을 중심으로 하는 원형의 형태로 존재하게 된다. The first exit surface 32 is a center region including the LED 11 optical axis 12 among the planar regions of the exit surface 30, and the second exit surface 34 is the planar region of the exit surface 30. The inflection point 37 existing between the first exit surface 32 and the second exit surface 34 is an edge region surrounding the first exit surface 32 among the LED 11 and the optical axis 12 in plan view. It will exist in the form of a circle.
도 3은 도 1에 따른 렌즈를 통해 출사하는 빛의 배광분포를 시뮬레이션한 결과를 나타내는 도면이고, 도 4는 도 3의 'B' 부분을 확대한 도면이다.3 is a diagram illustrating a result of simulating a light distribution of light emitted through the lens of FIG. 1, and FIG. 4 is an enlarged view of a portion 'B' of FIG. 3.
도 3 및 도 4를 참조하면, 도 1에 따른 엘이디 렌즈(10)에 의한 배광분포는 엘이디(11) 광축(12) 근처에서 대략 원형의 띠 모양의 주변보다 어두운 부분인 암부(b)가 발생하는 것을 확인할 수 있으며, 또한 엘이디(11) 광축(12) 부위에서는 주변보다 밝은 부분인 핫스팟(h)이 발생하는 것을 확인할 수 있는데, 위와 같은 암부(b)와 핫스팟(h)에 의해 빛의 균일도가 떨어지는 문제가 발생하게 된다.Referring to FIGS. 3 and 4, the light distribution of the LED lens 10 according to FIG. 1 generates a dark portion b that is darker than the periphery of a substantially circular band near the optical axis 12 of the LED 11. In addition, the LED (11) optical axis 12 can be confirmed that the hot spot (h), which is a brighter part than the surroundings, but the light uniformity by the dark portion (b) and hot spot (h) as described above. The problem of falling.
도 5는 변곡점 부위를 확대한 도면으로서, 도 1의 'A' 영역을 확대한 도면이다.5 is an enlarged view of an inflection point and an enlarged area 'A' of FIG. 1.
도 5에서 보이는 바와 같이, 제1출사면(32)을 통해 렌즈(10) 외부로 출사하는 빛(L3)과, 제2출사면(34)을 통해 렌즈(10) 외부로 출사하는 빛(L4)은 대략 변곡점(37) 상부 영역에서 암부영역(C)를 형성하게 되는데, 이러한 암부영역(C)에 의해 배광분포상에서 대략 원형의 띠 모양의 암부(b)가 광축(12) 근처에 발생하게 된다.As shown in FIG. 5, light L3 exiting the lens 10 through the first exit surface 32, and light L4 exiting the lens 10 through the second exit surface 34. ) Forms a dark region C at the upper region of the inflection point 37. The dark region C causes a substantially circular band-shaped dark region b to occur near the optical axis 12 on the light distribution. do.
이는 제1출사면(32)과 제2출사면(34)의 형상 즉, 제1출사면(32)은 하방으로 볼록한 곡면 형상을 가지는 반면, 제2출사면(34)은 상방으로 볼록한 곡면 형상을 가지기 때문에 발생하는 현상이다.This is the shape of the first exit surface 32 and the second exit surface 34, that is, the first exit surface 32 has a curved surface convex downwards, while the second exit surface 34 has a curved surface upwardly convex It is because of the phenomenon.
상세히 설명하면, 도면에서 보이는 바와 같이, 제1출사면(32)은 하방으로 볼록한 곡면 형상을 가지고, 제2출사면(34)은 상방으로 볼록한 곡면 형상을 가지기 때문에, 제1출사면(32)을 통해 렌즈(10) 외부로 출사하는 빛(L3)의 굴절각과, 제2출사면(32)을 통해 렌즈(10) 외부로 출사하는 빛(L4)의 굴절각이 차이가 발생하게 되는데, 이로 인하여 제1출사면(32)과 제2출사면(34)이 접속하는 변곡점(37)을 기준으로 렌즈(10) 외부로 출사하는 빛의 굴절각이 급격하게 변하게 되기 때문에, 대략 변곡점(37) 상방 영역으로 출사하는 빛은 현저히 감소하게 되고, 그에 따라 암부영역(C)이 형성되는 것이다.In detail, as shown in the drawing, since the first exit surface 32 has a curved surface convex downward, and the second exit surface 34 has a curved surface convex upward, the first exit surface 32 Through the refraction angle of the light (L3) emitted to the outside of the lens 10 through the second exit surface 32, the refraction angle of the light (L4) emitted to the outside of the lens 10 through the difference occurs, thereby Since the angle of refraction of the light exiting the lens 10 is rapidly changed with respect to the inflection point 37 connected between the first exit surface 32 and the second exit surface 34, the region substantially above the inflection point 37. The light emitted to the remarkably decreases, whereby the dark region C is formed.
한편, 도면에는 도시되지 않지만, 엘이디(11) 광축(12) 부위에서 핫스팟(h)이 발생하는 이유는, 출사면(30)을 통해 렌즈(10) 외부로 출사할 때 발생하는 프레넬 반사(Fresnel reflection)에 의한 것이다. On the other hand, although not shown in the figure, the reason that the hot spot (h) occurs in the LED 11 optical axis 12, the reason, the Fresnel reflections generated when exiting the lens 10 through the exit surface 30 ( Fresnel reflection).
즉, 프레넬 반사(Fresnel reflection)는 굴절률이 다른 물질 사이에서 빛이 경계면을 통과할 때 생기는 반사인데, 이러한 프레넬 반사에 의하여 출사면(30)을 통해 출사하는 빛 중 일부는 밑면(20)으로 반사하게 되며, 이와 같이 밑면(20)으로 반사된 빛은 다시 밑면(20)에서 반사되어 대략 광축(12) 부위로 향하게 되는데, 이러한 빛에 의해 광축(12) 부위에서 핫스팟(h)이 발생하게 되는 것이다.In other words, Fresnel reflection is a reflection generated when light passes through an interface between materials having different refractive indices. Some of the light exiting through the exit surface 30 by the Fresnel reflection is the bottom surface 20. The light reflected by the bottom surface 20 is reflected back from the bottom surface 20 and is directed toward the optical axis 12 portion. The hot spot h is generated at the optical axis 12 portion by the light. Will be done.
도 6은 본 발명의 다른 실시 예에 따른 엘이디 렌즈를 나타내는 수직단면도이고, 도 7은 도 6의 변곡점 부위를 확대한 도면으로서, 도 6의 'A' 영역을 확대한 도면이고, 도 8은 도 6의 개략적인 평면도이다. FIG. 6 is a vertical cross-sectional view illustrating an LED lens according to another exemplary embodiment. FIG. 7 is an enlarged view of an inflection point of FIG. 6 and is an enlarged view of region 'A' of FIG. 6. 6 is a schematic plan view.
본 실시 예에 따른 엘이디 렌즈(40)는 도 1에 따른 렌즈(10)의 배광분포상 발생하는 문제점 즉, 엘이디(11) 광축(12) 근처에서 원형의 띠 모양의 암부(b)가 발생하는 현상과, 광축(12) 부위에서 핫스팟(h)이 발생하는 현상을 개선하기 위한 것으로서, 도 1에 따른 렌즈(10)와 비교하여 변곡점(37)을 제거하는 대신 변곡점(37) 부위에 볼록부(42)를 형성시킨다는 점에서 차이가 있으므로, 기타 다른 구성에 대한 상세한 설명과 도면부호는 도 1에 따른 렌즈(10)에 대한 상세한 설명과 도면부호를 원용한다.In the LED lens 40 according to the present exemplary embodiment, a problem occurs in the light distribution distribution of the lens 10 according to FIG. 1, that is, a circular band-shaped dark portion b occurs near the LED 11 optical axis 12. And, to improve the phenomenon in which the hot spot (h) occurs in the optical axis 12, as compared to the lens 10 according to Figure 1, instead of removing the inflection point 37, the convex portion (37) 42), the detailed description of the other components and the reference numerals refer to the detailed description and reference numerals of the lens 10 according to FIG.
도 6 내지 도 8을 참조하면, 본 실시 예에 따른 엘이디 렌즈(40)는 변곡점(37) 부위에 형성되며 수직단면상 상방으로 볼록한 형상을 가지는 볼록부(42)를 포함한다. 6 to 8, the LED lens 40 according to the present exemplary embodiment includes a convex portion 42 formed at a portion of the inflection point 37 and having a convex shape on the vertical cross section.
이와 같이, 변곡점(37) 부위에 볼록부(42)를 형성하면, 도 3 및 도 4에서 보이는 바와 같은, 도 1에 따른 렌즈(10)의 배광분포상에서 발생하는 원형의 띠 모양의 암부(b)를 개선할 수 있다.As such, when the convex portion 42 is formed at the inflection point 37, a circular band-shaped dark portion b generated in the light distribution distribution of the lens 10 according to FIG. 1, as shown in FIGS. 3 and 4. ) Can be improved.
상세히 설명하면, 도 7에서 보이는 바와 같이, 변곡점(37) 부위에 볼록부(37)를 형성하면, 변곡점(37) 부위를 통해 렌즈(40) 외부로 출사하는 빛(L5)은 볼록부(37)를 통해 출사하게 됨으로써, 볼록부(37)가 없는 경우에 발생하는 암부영역(C) 방향으로 굴절되어 출사하게 되며, 그에 따라 암부영역(C)에 의해 발생하는 배광분포상에서의 원형의 띠 모양의 암부(b)를 개선할 수 있게 된다. In detail, as shown in FIG. 7, when the convex portion 37 is formed at the inflection point 37, the light L5 emitted to the outside of the lens 40 through the inflection point 37 is convex portion 37. By being emitted through), it is refracted in the direction of the dark portion region C generated when there is no convex portion 37, and is emitted. Accordingly, a circular band shape in the light distribution distribution generated by the dark portion region C is produced. It is possible to improve the dark portion (b) of the.
나아가, 변곡점(37)에 형성된 볼록부(42)는, 출사면(30)에서 프레넬 반사된 빛이 밑면(13)에서 다시 반사되어 엘이디 광축(12)으로 향하는 빛을 분산시키거나(scattering) 변곡점(37) 상방으로 모이게 함으로써, 도 3 및 도 4에서 보이는 바와 같은, 도 1에 따른 렌즈(10)의 배광분포상에서 발생하는 광축(12) 부위에서의 핫스팟(h)을 개선할 수 있게 된다.Furthermore, the convex portion 42 formed at the inflection point 37 scatters the light reflected by the Fresnel at the exit surface 30 from the bottom surface 13 to the LED optical axis 12. By converging above the inflection point 37, it is possible to improve the hot spot h at the optical axis 12 portion generated in the light distribution distribution of the lens 10 according to FIG. 1 as shown in FIGS. 3 and 4. .
또한, 도 8에서 보이는 바와 같이, 볼록부(42)는 변곡점(37) 부위 즉, 변곡점(37)을 감싸도록 형성되는데, 그에 따라 볼록부(42)는 평면상 엘이디(11)의 광축(12)을 중심으로 하는 원형의 형태로 존재하는 변곡점(37)을 감싸는 원형의 띠 형상으로 형성될 수 있다.In addition, as shown in FIG. 8, the convex portion 42 is formed to surround the inflection point 37, that is, the inflection point 37, whereby the convex portion 42 has an optical axis 12 of the LED 11 in plan view. It may be formed in a circular band shape surrounding the inflection point (37) existing in the form of a circle around the center.
물론, 도면에는 도시되지 않지만, 볼록부(42)는 원형의 띠 형상으로 형성되지 않고, 평면상 원형의 형태로 존재하는 변곡점(37)의 원주방향으로 소정간격 이격된 상태로 복수개 형성될 수도 있다.Of course, although not shown in the drawings, the convex portions 42 may not be formed in a circular band shape, but may be formed in a plurality of states spaced apart at predetermined intervals in the circumferential direction of the inflection point 37 present in a planar circular form. .
그러나, 도 8에서 보이는 바와 같이, 볼록부(42)는 변곡점(37)을 감싸는 원형의 띠 형상으로 형성되는 것이, 원주방향으로 소정간격 이격된 상태로 복수개 형성되는 것보다, 빛을 더욱 고르게 확산시킬 수 있어서 바람직하다.However, as shown in FIG. 8, the convex portion 42 is formed in a circular band shape surrounding the inflection point 37, and the light is more evenly diffused than a plurality of convex portions are formed at predetermined intervals in the circumferential direction. It is preferable to make it possible.
도 9는 본 발명의 또 다른 실시 예에 따른 엘이디 렌즈를 나타내는 수직단면도이고, 도 10은 도 9의 개략적인 평면도이다.9 is a vertical cross-sectional view showing the LED lens according to another embodiment of the present invention, Figure 10 is a schematic plan view of FIG.
도 9 및 도 10을 참조하면, 본 실시 예에 따른 엘이디 렌즈(40)는 볼록부(42) 외에 볼록부(42)와 마찬가지로 수직단면상 상방으로 볼록한 형상을 가지는 제1볼록부(43)와 제2볼록부(44)를 더 포함할 수 있다.9 and 10, the LED lens 40 according to the present exemplary embodiment may include the first convex portion 43 and the first convex portion 43 having a convex shape on the vertical cross section in the same manner as the convex portion 42 in addition to the convex portion 42. The convex portion 44 may further include.
제1볼록부(43)는 볼록부(42)로부터 제1출사면(32) 측으로 소정거리 이격된 상태로 제1출사면(32) 상에 형성될 수 있으며, 제2볼록부(44)는 볼록부(42)로부터 제2출사면(34) 측으로 소정거리 이격된 상태로 제2출사면(34) 상에 형성될 수 있다.The first convex portion 43 may be formed on the first exit surface 32 in a state spaced apart from the convex portion 42 toward the first exit surface 32 by a predetermined distance, and the second convex portion 44 may be It may be formed on the second exit surface 34 in a state spaced apart from the convex portion 42 toward the second exit surface 34.
또한, 도 10에서 보이는 바와 같이, 제1볼록부(43)와 제2볼록부(44)는 볼록부(42)와 마찬가지로 평면상 엘이디(11)의 광축(12)을 중심으로 하는 원형의 띠 형상으로 형성될 수 있다.As shown in FIG. 10, the first convex portion 43 and the second convex portion 44 have a circular band around the optical axis 12 of the LED 11 in a plane like the convex portion 42. It may be formed in a shape.
이와 같이, 볼록부(42) 외에 제1볼록부(43)와 제2볼록부(44)를 더 형성하면, 도 1에 따른 렌즈(10)에서와 같이 광축(12) 근처에서 원형의 띠 모양의 암부(b)가 발생하는 현상을 더욱 개선할 수 있게 된다. As such, when the first convex portion 43 and the second convex portion 44 are further formed in addition to the convex portion 42, as in the lens 10 of FIG. 1, a circular band is formed near the optical axis 12. It is possible to further improve the phenomenon that the dark portion (b) of the occurs.
특히, 볼록부(42) 외에 제1볼록부(43)와 제2볼록부(44)를 더 형성하게 되면, 출사면(30)에서 프레넬 반사된 빛이 밑면(13)에서 다시 반사되어 엘이디 광축(12)으로 향하는 빛을 더욱 분산시킬 수 있어서, 도 1에 따른 렌즈(10)에서와 같이 광축(12) 부위에서 핫스팟(h)이 발생하는 현상을 더욱 개선할 수 있게 된다.In particular, when the first convex portion 43 and the second convex portion 44 are further formed in addition to the convex portion 42, the light reflected by the Fresnel from the exit surface 30 is reflected back from the bottom surface 13, thereby causing the LEDs. Since the light directed to the optical axis 12 can be further dispersed, the phenomenon in which the hot spot h is generated at the optical axis 12 portion as in the lens 10 according to FIG. 1 can be further improved.
또한, 제1볼록부(43)와 제2볼록부(44)는 수직단면상 볼록부(42)를 기준으로 서로 대칭을 이루도록 형성될 수 있다. 그러면, 광축(12) 근처에서 암부(b)가 발생하는 현상과 광축(12) 부위에서 핫스팟(h)이 발생하는 현상을 더욱더 개선할 수 있게 된다.In addition, the first convex portion 43 and the second convex portion 44 may be formed to be symmetrical with each other based on the convex portion 42 on the vertical section. Then, the phenomenon in which the dark portion b occurs near the optical axis 12 and the hot spot h in the optical axis 12 may be further improved.
도 11은 도 9에 따른 렌즈를 통해 출사하는 빛의 배광분포를 시뮬레이션한 결과를 나타내는 도면이고, 도 12는 도 11의 'B' 부분을 확대한 도면이다.FIG. 11 is a diagram illustrating a result of a light distribution distribution of light emitted through the lens of FIG. 9, and FIG. 12 is an enlarged view of a portion 'B' of FIG.
도 11 및 도 12에서 보이는 바와 같이, 본 실시 예에 따른 렌즈(40)의 배광분포는 도 1에 따른 렌즈(10)의 배광분포를 나타내는 도 3 및 도 4와 비교하여, 광축(12) 근처에서의 암부(b) 발생 현상과, 광축(12) 부위에서의 핫스팟(h) 발생 현상이 개선되었음을 알 수 있다. As shown in FIGS. 11 and 12, the light distribution of the lens 40 according to the present embodiment is closer to the optical axis 12 than in FIGS. 3 and 4 showing the light distribution of the lens 10 according to FIG. 1. It can be seen that the development of the dark portion (b) and the occurrence of the hot spot (h) in the optical axis 12 region in the.
즉, 도 3 및 도 4의 화면상에서 광축(12) 근처에 원형의 띠인 암부(b)가 발생하던 것이, 도 11 및 도 12의 화면상에서는 암부(b)가 주변과 비교하여 거의 구분이 가지 않을 정도로 개선되었음을 확인할 수 있다.That is, the dark portion b of a circular band is generated near the optical axis 12 on the screens of FIGS. 3 and 4. On the screens of FIGS. 11 and 12, the dark portion b is hardly distinguished from the surroundings. It can be confirmed that the improvement.
특히, 도 3 및 도 4의 그래프에서 광축(12) 양쪽에 어깨 형태가 발생하던 것이, 도 11 및 도 12의 그래프에서는 상기 어깨 형태가 거의 사라진 것을 확인할 수 있는데, 그래프에서 위와 같은 어깨 형태가 발생한다는 것은 주위보다 어두운 암부(b)가 발생한다는 것을 의미하기 때문에, 도 11 및 도 12의 그래프에서 상기 어깨 형태가 사라졌다는 것은 암부(b) 발생 현상이 개선되었음을 나타낸다.In particular, in the graphs of FIGS. 3 and 4, the shoulder shape is generated on both sides of the optical axis 12. In the graphs of FIGS. 11 and 12, the shoulder shape almost disappears. In the graph, the shoulder shape is generated. Since it means that the dark portion (b) is darker than the surroundings, the disappearance of the shoulder shape in the graphs of Figs. 11 and 12 indicates that the occurrence of the dark portion (b) is improved.
또한, 도 3 및 도 4의 화면상에서의 광축(12) 부위의 밝기보다 도 11 및 도 12의 화면상에서의 광축(12) 부위의 밝기가 덜 밝은 것을 확인할 수 있는데, 이는 광축(12) 부위에서의 핫스팟(h) 현상이 개선되었음을 나타낸다.In addition, it can be seen that the brightness of the optical axis 12 portion on the screen of FIGS. 11 and 12 is less bright than the brightness of the optical axis 12 portion on the screens of FIGS. The hot spot (h) of the phenomenon is improved.
특히, 도 3 및 도 4의 그래프에서 광축(12) 부위가 위로 뾰족한 형태였던 것이, 도 11 및 도 12의 그래프에서는 납작한 형태로 변경되었음을 확인할 수 있는데, 이는 광축(12) 부위에서의 핫스팟(h) 현상이 개선되었음을 나타낸다.In particular, in the graphs of FIGS. 3 and 4, the point of the optical axis 12 was pointed upward, and it can be seen that the graph of FIGS. 11 and 12 changed to the flat shape, which is a hot spot (h) at the area of the optical axis 12. ), The phenomenon is improved.
이상에서 살펴본 바와 같이, 본 발명은 변곡점 부위에 볼록부를 형성함으로써, 엘이디 광축 근처에서 원형의 띠 모양의 암부가 발생하는 현상과, 엘이디 광축 부위에서의 핫스팟이 발생하는 현상을 개선할 수 있는 엘이디 렌즈에 관한 것으로서, 그 실시 형태는 다양한 형태로 변경가능하다 할 것이다. 따라서 본 발명은 본 명세서에서 개시된 실시 예에 의해 한정되지 않으며, 본 발명이 속하는 기술분야에서 통상의 지식을 가진 자가 변경 가능한 모든 형태도 본 발명의 권리범위에 속한다 할 것이다.As described above, the present invention, by forming a convex portion at the inflection point, the LED lens that can improve the phenomenon that the circular band-shaped dark portion near the LED optical axis, and the phenomenon that hot spots occur in the LED optical axis region As related to the present invention, the embodiments may be modified in various forms. Therefore, the present invention is not limited to the embodiments disclosed in the present specification, and all forms changeable by those skilled in the art to which the present invention pertains will belong to the scope of the present invention.

Claims (3)

  1. 엘이디에서 나오는 빛을 고르게 확산시키기 위한 엘이디 렌즈에 있어서, In the LED lens for evenly spreading the light from the LED,
    상기 엘이디에서 나오는 빛이 상기 렌즈 내부로 입사하는 입사면과, 상기 입사면을 통해 상기 렌즈 내부로 입사한 빛을 상기 렌즈 외부로 출사시키는 출사면을 포함하고,And an entrance surface through which light emitted from the LED is incident into the lens, and an exit surface emitting light incident into the lens through the entrance surface to the outside of the lens.
    상기 출사면은 수직단면상 상기 엘이디 측에 볼록한 곡면 형상을 형성하는 제1출사면과, 상기 제1출사면의 주위에 위치하고 상기 엘이디 반대측에 볼록한 곡면 형상을 형성하는 제2출사면을 포함하고, The exit surface includes a first exit surface forming a convex curved shape on the LED side on a vertical cross section, and a second exit surface positioned around the first exit surface and forming a convex curved shape on the opposite side of the LED,
    상기 제1출사면과 상기 제2출사면의 접속부분에 존재하는 변곡점 부위에는 수직단면상 상방으로 볼록한 형상을 가지는 볼록부가 형성되고, A convex portion having a convex shape upward in a vertical section is formed at an inflection point portion existing at the connection portion between the first exit surface and the second exit surface.
    상기 볼록부는 평면상 상기 엘이디의 광축을 중심으로 원형의 형태로 존재하는 변곡점을 감싸는 원형의 띠 형상으로 형성되는 것을 특징으로 하는 엘이디 렌즈. The convex portion of the LED lens, characterized in that formed in a circular band shape surrounding the inflection point existing in a circular shape around the optical axis of the LED on a plane.
  2. 제 1 항에 있어서,The method of claim 1,
    상기 출사면에는 수직단면상 상방으로 볼록한 형상을 가지며, 평면상 원형의 띠 형상을 가지는 제1볼록부와 제2볼록부가 더 형성되고, The emission surface has a first convex portion and a second convex portion having a convex shape upwardly in a vertical section, and having a planar circular band shape,
    상기 제1블록부는 상기 볼록부로부터 상기 제1출사면 측으로 소정거리 이격된 상태로 상기 제1출사면 상에 형성되고, The first block portion is formed on the first exit surface in a state spaced apart a predetermined distance from the convex portion toward the first exit surface,
    상기 제2볼록부는 상기 볼록부로부터 상기 제2출사면 측으로 소정거리 이격된 상태로 상기 제2출사면 상에 형성되는 것을 특징으로 하는 엘이디 렌즈.And the second convex portion is formed on the second emission surface in a state spaced apart from the convex portion toward the second emission surface by a predetermined distance.
  3. 제 2 항에 있어서,The method of claim 2,
    상기 제1볼록부와 상기 제2볼록부는 수직단면상 상기 볼록부를 기준으로 서로 대칭을 이루는 것을 특징으로 하는 엘이디 렌즈.And the first convex portion and the second convex portion are symmetrical with respect to the convex portion on a vertical section.
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