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JP7404528B2 - Vehicle lamp module, vehicle headlamp and vehicle - Google Patents
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JP7404528B2 - Vehicle lamp module, vehicle headlamp and vehicle - Google Patents

Vehicle lamp module, vehicle headlamp and vehicle Download PDF

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JP7404528B2
JP7404528B2 JP2022525408A JP2022525408A JP7404528B2 JP 7404528 B2 JP7404528 B2 JP 7404528B2 JP 2022525408 A JP2022525408 A JP 2022525408A JP 2022525408 A JP2022525408 A JP 2022525408A JP 7404528 B2 JP7404528 B2 JP 7404528B2
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curvature
transverse line
aspherical lens
point
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JP2023501233A (en
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▲輝▼ 李
智平 仇
▲剣▼清 ▲陸▼
大攀 ▲張▼
▲賀▼ 祝
▲曉▼芬 ▲孫▼
文慧 桑
▲聰▼ 李
睿 ▲聶▼
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▲華▼域▲視▼▲覺▼科技(上▲海▼)有限公司
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21SNON-PORTABLE LIGHTING DEVICES; SYSTEMS THEREOF; VEHICLE LIGHTING DEVICES SPECIALLY ADAPTED FOR VEHICLE EXTERIORS
    • F21S41/00Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps
    • F21S41/20Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps characterised by refractors, transparent cover plates, light guides or filters
    • F21S41/25Projection lenses
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21SNON-PORTABLE LIGHTING DEVICES; SYSTEMS THEREOF; VEHICLE LIGHTING DEVICES SPECIALLY ADAPTED FOR VEHICLE EXTERIORS
    • F21S41/00Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps
    • F21S41/10Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps characterised by the light source
    • F21S41/19Attachment of light sources or lamp holders
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21WINDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO USES OR APPLICATIONS OF LIGHTING DEVICES OR SYSTEMS
    • F21W2102/00Exterior vehicle lighting devices for illuminating purposes
    • F21W2102/10Arrangement or contour of the emitted light
    • F21W2102/13Arrangement or contour of the emitted light for high-beam region or low-beam region
    • F21W2102/135Arrangement or contour of the emitted light for high-beam region or low-beam region the light having cut-off lines, i.e. clear borderlines between emitted regions and dark regions
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21WINDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO USES OR APPLICATIONS OF LIGHTING DEVICES OR SYSTEMS
    • F21W2107/00Use or application of lighting devices on or in particular types of vehicles
    • F21W2107/10Use or application of lighting devices on or in particular types of vehicles for land vehicles

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  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Non-Portable Lighting Devices Or Systems Thereof (AREA)

Description

[関連出願の相互参照]
本願は、2019年11月26日に提出された中国特許出願201911175135.0の権益を主張し、該出願の内容は引用により本明細書に組み込まれている。
[Cross reference to related applications]
This application claims the benefit of Chinese Patent Application No. 201911175135.0 filed on November 26, 2019, the contents of which are incorporated herein by reference.

本発明は、車両照明装置に関し、具体的には、車両ランプモジュールに関し、また、さらに車両ヘッドランプ及び車両に関する。 TECHNICAL FIELD The present invention relates to a vehicle lighting device, specifically to a vehicle lamp module, and further to a vehicle headlamp and a vehicle.

夜間運転では、自動車照明システム、特に自動車ヘッドランプの重要性は言うまでもないことである。自動車の高速走行中、眩しいハイビームは、ドライバーが自動車に対する制御を失うことを引き起こし、さらに予期せぬ危険が生じる可能性がある。従って、自動車ヘッドランプは、ドライバーに広い視覚範囲及び良好な視覚条件を提供するだけでなく、ほかの道路関与者を眩惑させないように、ほかの道路関与者に可能な限り影響を与えない必要がある。技術の発展に伴い、マトリックスLEDヘッドランプは自動車ランプの将来の発展方向の1つとなっており、マトリックスLEDヘッドランプの光源は複数のLEDからなり、これらのLEDは所定の方式で配列されてアレイパターンを形成し、車両の前方視野における車両、歩行者の位置に応じて、マトリックスLEDヘッドランプは対応する領域のLEDを消灯することで、歩行者又は対向ドライバーの眩惑を回避することができる。 When driving at night, it goes without saying that vehicle lighting systems, especially vehicle headlamps, are important. When a car is driving at high speeds, the dazzling high beams can cause the driver to lose control of the car, which can even lead to unexpected danger. Therefore, automobile headlamps must not only provide the driver with a wide visual range and good visual conditions, but also have as little impact on other road participants as possible so as not to dazzle them. be. With the development of technology, matrix LED headlamps have become one of the future development directions of automobile lamps.The light source of matrix LED headlamps consists of multiple LEDs, and these LEDs are arranged in a predetermined manner to form an array. By forming a pattern and turning off the LEDs in the corresponding area according to the positions of the vehicle and pedestrians in the front field of view of the vehicle, the matrix LED headlamp can avoid dazzling pedestrians or oncoming drivers.

従来技術では、一般的なマトリックス車両ランプモジュールはいずれもマトリックス状に配列された光源及び光源に対応する集光素子を使用してハイビームによるドライバーの眩惑という技術的課題を解決する。出願日が2018年4月13日の特許文献1は光学モジュール及び車両ランプを開示しており、該光学モジュールに使用される集光器は複数の光ガイド部材を備え、各光ガイド部材の光入射端は各光源に1対1で対応して設けられ、光出射端は互いに収束して弧状の光出射部を形成し、該集光器は光源から発する光に対する収束作用を有し、且つ隣接する光源から発する光を集光器の光出射面である程度融合させることで、各光源から発する光によって形成されるスポット間がより均一に繋がるが、該集光器は構造が非常に複雑で、各光ガイド部材間の相対的な位置の精度を確保する必要があり、集光器の加工精度を確保することが非常に困難であり、また、該集光器は取り付け構造も非常に複雑で、取り付け累積誤差が非常に大きく、その結果、光学モジュールの光学システムの精度が低く、車両ランプの光形状効果を損なってしまう。 In the prior art, a general matrix vehicle lamp module uses light sources arranged in a matrix and condensing elements corresponding to the light sources to solve the technical problem of dazzling a driver due to high beams. Patent Document 1, filed on April 13, 2018, discloses an optical module and a vehicle lamp, and a condenser used in the optical module includes a plurality of light guide members, and the light of each light guide member is The input end is provided in one-to-one correspondence with each light source, the light output end converges with each other to form an arc-shaped light output part, and the condenser has a convergence effect on the light emitted from the light source, and By merging the light emitted from adjacent light sources to some extent on the light output surface of the condenser, the spots formed by the light emitted from each light source are connected more uniformly, but the condenser has a very complicated structure. , it is necessary to ensure the accuracy of the relative position between each light guide member, and it is very difficult to ensure the processing accuracy of the condenser, and the mounting structure of the condenser is also very complicated. In this case, the installation cumulative error is very large, resulting in low precision of the optical system of the optical module, which impairs the light shape effect of the vehicle lamp.

自動車産業の発展に伴い、マトリックス車両ランプはADBアダプティブハイビーム機能の実現を必要とするだけでなく、これに基づいて、車両ランプの光形状の均一性をさらに向上し、車両ランプの放熱性能を高め、車両ランプの重量や寸法を減らす必要がある。 With the development of the automobile industry, matrix vehicle lamps not only require the realization of ADB adaptive high beam function, but also based on this, further improve the uniformity of the light shape of the vehicle lamps, and enhance the heat dissipation performance of the vehicle lamps. , there is a need to reduce the weight and dimensions of vehicle lamps.

従来技術の上記欠陥に鑑みて、新型車両ランプモジュールを設計する必要がある。 In view of the above deficiencies of the prior art, there is a need to design a new type of vehicle lamp module.

中国実用新案第201820529985.0号China Utility Model No. 201820529985.0

本発明が解決しようとする第1の技術的課題は、構造が簡単で、光形状が均一である車両ランプモジュールを提供することである。 A first technical problem to be solved by the present invention is to provide a vehicle lamp module that has a simple structure and a uniform light shape.

本発明が解決しようとする第2の技術的課題は、構造が簡単で、光形状が均一である車両ヘッドランプを提供することである。 A second technical problem to be solved by the present invention is to provide a vehicle headlamp that has a simple structure and a uniform light shape.

本発明が解決しようとする第3の技術的課題は、光形状が均一で、コストが低い車両を提供することである。 The third technical problem to be solved by the present invention is to provide a vehicle with a uniform light shape and low cost.

上記目的を実現するために、本発明の第1態様は、光出射方向に沿って順に設置される光源、集光部及び光出射素子を備え、前記光出射素子は非球面レンズであり、前記集光部は少なくとも1つの集光素子を備え、前記光源は対応する前記に対応して、前記光源から発する光は前記集光素子によって収束されて前記非球面レンズの光入射面に入射して、前記非球面レンズの光出射面から出射することがができる車両ランプモジュールを提供する。 In order to achieve the above object, a first aspect of the present invention includes a light source, a condensing section, and a light emitting element installed in order along the light emitting direction, the light emitting element being an aspherical lens, and the light emitting element being an aspherical lens. The light condensing unit includes at least one condensing element, and the light source is configured such that the light emitted from the light source is converged by the condensing element and enters the light incident surface of the aspherical lens. , provides a vehicle lamp module capable of emitting light from a light emitting surface of the aspherical lens.

好ましくは、前記非球面レンズの光出射面は、前記非球面レンズの中央横方向横断面と前記非球面レンズの光出射面が交差して中央横方向横断線を形成するように構成され、前記中央横方向横断線は第1曲率境界点及び第2曲率境界点を有し、前記第1曲率境界点は前記中央横方向横断線の中点から左端点までの間の任意の一点であり、前記第2曲率境界点は前記中央横方向横断線の中点から右端点までの間の任意の一点であり、前記中央横方向横断線の第1曲率境界点から第2曲率境界点までの曲率は等しく、前記中央横方向横断線の第1曲率境界点から左端点までの曲率、及び前記中央横方向横断線の第2曲率境界点から右端点までの曲率はいずれも最初に増加し、次に減少する。 Preferably, the light exit surface of the aspherical lens is configured such that a central lateral cross section of the aspherical lens intersects with the light exit surface of the aspherical lens to form a central lateral transverse line; The central lateral transverse line has a first curvature boundary point and a second curvature boundary point, the first curvature boundary point being an arbitrary point between the midpoint and the left end point of the central lateral transverse line, The second curvature boundary point is an arbitrary point between the midpoint and the right end point of the central lateral transverse line, and the curvature of the central lateral transverse line from the first curvature boundary point to the second curvature boundary point. are equal, the curvature from the first curvature boundary point of the central transverse transverse line to the left end point, and the curvature from the second curvature boundary point of the central transverse transverse line to the right end point both initially increase, and then decreases to

好ましくは、前記中央横方向横断線の左端点の曲率及び/又は前記中央横方向横断線の右端点の曲率は前記中央横方向横断線の第1曲率境界点から第2曲率境界点までの曲率に等しい。 Preferably, the curvature of the left end point of said central lateral transverse line and/or the curvature of the right end point of said central lateral transverse line is the curvature of said central lateral transverse line from a first curvature boundary point to a second curvature boundary point. be equivalent to.

好ましい構造形態として、前記非球面レンズの光出射面は前方に向かって突出した曲面であり、前記非球面レンズの光出射面はさらに、前記非球面レンズのいずれか1つの縦方向横断面と前記非球面レンズの光出射面が交差して1本の縦方向横断線を形成するように構成され、前記縦方向横断線は、前記縦方向横断線の中点から上端点までの間の任意の一点である曲率変化境界点を有し、前記縦方向横断線の曲率変化境界点から下端点までの曲率は等しく、前記縦方向横断線の曲率変化境界点から上端点までの曲率は等しく、且つ前記縦方向横断線の上端点の曲率は前記縦方向横断線の下端点の曲率よりも小さい。 In a preferred structural form, the light exit surface of the aspherical lens is a curved surface protruding forward, and the light exit surface of the aspherical lens further includes a longitudinal cross section of any one of the aspherical lenses and the The light exit surfaces of the aspherical lenses are configured to intersect to form one longitudinal transverse line, and the longitudinal transverse line is an arbitrary point between the midpoint and the upper end point of the longitudinal transverse line. has a curvature change boundary point that is one point, the curvatures of the longitudinal transverse line from the curvature change boundary point to the lower end point are equal, and the curvatures of the longitudinal transverse line from the curvature change boundary point to the upper end point are equal; The curvature of the upper end point of the longitudinal transverse line is smaller than the curvature of the lower end point of the longitudinal transverse line.

別の好ましい構造形態として、前記非球面レンズの光出射面は前方に向かって突出した曲面であり、前記非球面レンズの光出射面はさらに、前記非球面レンズのいずれか1つの縦方向横断面と前記非球面レンズの光出射面が交差して1本の縦方向横断線を形成するように構成され、前記縦方向横断線は、前記縦方向横断線の中点から上端点までの間の任意の一点である曲率変化境界点を有し、前記縦方向横断線の曲率変化境界点から下端点までの曲率は等しく、前記縦方向横断線の曲率変化境界点から上端点までの曲率は徐々に減少する。 In another preferred structural form, the light exit surface of the aspherical lens is a curved surface protruding forward, and the light exit surface of the aspherical lens further includes a longitudinal cross section of any one of the aspherical lenses. and the light exit surface of the aspherical lens intersect to form one longitudinal transverse line, and the longitudinal transverse line is a line between the midpoint and the upper end point of the longitudinal transverse line. The curvature change boundary point is an arbitrary point, and the curvature of the longitudinal transverse line from the curvature change boundary point to the lower end point is equal, and the curvature of the longitudinal transverse line from the curvature change boundary point to the upper end point is gradually decreases to

好ましくは、前記非球面レンズの光入射面は前記非球面レンズの光軸方向に沿って後方に向かって突出する。 Preferably, the light entrance surface of the aspherical lens projects rearward along the optical axis direction of the aspherical lens.

好ましくは、前記集光部は複数の集光素子を備え、前記集光素子は1行複数列のマトリックス状に配置され得るか、又は複数行複数列のマトリックス状に配置され得る。 Preferably, the light condensing unit includes a plurality of light condensing elements, and the light condensing elements may be arranged in a matrix of one row and multiple columns, or may be arranged in a matrix of multiple rows and multiple columns.

より好ましくは、前記集光素子は平凸レンズであり、前記集光素子の光入射面は平面であり、前記集光素子の光出射面は前方に向かって突出した曲面である。 More preferably, the light condensing element is a plano-convex lens, the light incidence surface of the light condensing element is a flat surface, and the light exit surface of the light condensing element is a curved surface protruding forward.

具体的には、前記車両ランプモジュールは、前記集光部を取り付けるための取り付けブラケットをさらに備え、前記取り付けブラケットに位置決めピン及び取り付け孔が設けられ、前記取り付けブラケットの周囲にフランジが設けられ、前記集光部と前記取り付けブラケットは一体に成形されるか、又は組み立てて接続される。 Specifically, the vehicle lamp module further includes a mounting bracket for mounting the light condensing part, the mounting bracket is provided with a positioning pin and a mounting hole, a flange is provided around the mounting bracket, and the mounting bracket is provided with a locating pin and a mounting hole. The light collecting part and the mounting bracket may be integrally molded or assembled together.

好ましくは、前記光源は前記集光素子の焦点の前方に設けられる。 Preferably, the light source is provided in front of the focal point of the condensing element.

より好ましくは、前記光源は前記非球面レンズの焦点面に設けられる。 More preferably, the light source is provided at the focal plane of the aspheric lens.

本発明の第2態様は、第1態様の技術案のいずれか1項に記載の車両ランプモジュールを備え、前記車両ランプモジュールは縦方向、横方向、又は斜めに配列して分布する車両ヘッドランプを提供する。 A second aspect of the present invention includes the vehicle lamp module according to any one of the technical solutions of the first aspect, wherein the vehicle headlamps are arranged and distributed in a vertical direction, a horizontal direction, or an oblique direction. I will provide a.

本発明の第3態様は、第2態様の技術案に記載の車両ヘッドランプを備える車両を提供する。 A third aspect of the invention provides a vehicle comprising the vehicle headlamp according to the technical solution of the second aspect.

本発明の基本的な技術案では、光源から発する光は集光部によって収束されて非球面レンズの光入射面に入射し、さらに非球面レンズの光出射面から出射し、該集光部は少なくとも1つの集光素子が設けられることで、従来技術の複数の光ガイド部材を備えた集光器に比べて、車両ランプモジュールは構造が簡単であるだけでなく、寸法や重量がさらに小さくなり、また、本発明の非球面レンズの中央から縁までの曲率は連続的に変化することで、光形状の拡散角度を変更し、所望の光形状を得ることができる。 In the basic technical scheme of the present invention, the light emitted from the light source is converged by a condensing part, enters the light incident surface of the aspherical lens, and then exits from the light exiting surface of the aspherical lens, and the condensing part By providing at least one concentrating element, the vehicle lamp module is not only simpler in structure, but also smaller in size and weight compared to concentrators with multiple light guide elements in the prior art. Furthermore, by continuously changing the curvature from the center to the edge of the aspherical lens of the present invention, it is possible to change the diffusion angle of the light shape and obtain a desired light shape.

本発明のほかの利点及び好ましい実施形態の技術的効果について、以下の具体的な実施形態ではさらに詳しく説明する。 Other advantages of the present invention and technical effects of the preferred embodiments will be explained in more detail in the following specific embodiments.

本発明の車両ランプモジュールの一実施例の構造模式図1である。1 is a schematic structural diagram 1 of an embodiment of a vehicle lamp module of the present invention. FIG. 本発明の車両ランプモジュールの一実施例の構造模式図2である。FIG. 2 is a schematic structural diagram 2 of an embodiment of the vehicle lamp module of the present invention. 図2の中央縦方向横断面の模式図である。FIG. 3 is a schematic view of the center longitudinal cross section of FIG. 2; 図2の中央横方向横断面の模式図である。FIG. 3 is a schematic view of the central transverse cross section of FIG. 2; 本発明の集光部の一実施例の構造模式図1である。FIG. 1 is a schematic diagram 1 of a structure of an embodiment of a light condensing section of the present invention. 図5のA部の部分拡大図である。6 is a partially enlarged view of section A in FIG. 5. FIG. 本発明の集光部の一実施例の構造模式図2である。FIG. 2 is a schematic structural diagram 2 of an embodiment of the light condensing section of the present invention. 図5の縦方向横断面の模式図である。FIG. 6 is a schematic longitudinal cross-sectional view of FIG. 5; 図5の横方向横断面の模式図である。FIG. 6 is a schematic diagram of a lateral cross section of FIG. 5; 本発明の非球面レンズの一実施例の中央縦方向横断面の模式図である。1 is a schematic diagram of a central longitudinal cross section of an embodiment of an aspherical lens according to the present invention; FIG. 本発明の非球面レンズの一実施例の中央横方向横断面の模式図である。1 is a schematic view of a central transverse cross section of an embodiment of an aspheric lens of the present invention; FIG. 本発明の非球面レンズの別の実施例の構造模式図である。FIG. 3 is a schematic structural diagram of another embodiment of the aspherical lens of the present invention. 従来技術の車両ランプモジュールによって投射された光形状の模式図である。1 is a schematic illustration of a light shape projected by a prior art vehicle lamp module; FIG. 本発明の車両ランプモジュールによって投射された光形状の模式図である。FIG. 3 is a schematic diagram of a light shape projected by a vehicle lamp module of the present invention.

以下、図面を参照しながら本発明の具体的な実施形態を詳細に説明する。理解できるように、ここで説明される具体的な実施形態は単に本発明を説明及び解釈することに用いられ、本発明を限定するものではない。 Hereinafter, specific embodiments of the present invention will be described in detail with reference to the drawings. As can be understood, the specific embodiments described herein are merely used to explain and interpret the invention, and are not intended to limit the invention.

なお、本発明の説明では、特に明記及び限定されていない限り、「接続」、「設置」のような用語は広義に理解すべきであり、例えば、固定接続、取り外し可能な接続、又は一体接続であってもよく、直接接続、又は中間媒体を介する間接接続であってもよく、2つの素子の内部が連通すること、又は2つの素子の相互作用関係であってもよい。当業者であれば、場合によって本発明における上記用語の具体的な意味を理解することができる。 In the description of the present invention, unless otherwise specified and limited, terms such as "connection" and "installation" should be understood in a broad sense, such as fixed connection, removable connection, or integral connection. It may be a direct connection or an indirect connection via an intermediate medium, or it may be an internal communication between two elements, or an interaction relationship between two elements. Those skilled in the art can understand the specific meanings of the above terms in the present invention, as the case may be.

なお、光出射方向に沿って、「前」とは、非球面レンズ3が位置する端部であり、「後」とは、光源1が位置する端部であり、「上」とは、車両ランプモジュールが正常に取り付けられている場合の光出射方向の上方であり、「下」とは、車両ランプモジュールが正常に取り付けられている場合の光出射方向の下方であり、「左」とは、車両ランプモジュールが正常に取り付けられている場合の光出射方向の左側であり、「右」とは、車両ランプモジュールが正常に取り付けられている場合の光出射方向の右側であり、「縦方向横断面」は、非球面レンズ3の光軸35に平行で、非球面レンズ3の上縁から下縁に垂直に延びているいずれか1つの横断面であり、「縦方向横断線33」は、該縦方向横断面と非球面レンズ3の光出射面32が交差して形成される曲線であり、「横方向横断面」は、前記縦方向横断面に垂直であり、「横方向横断線」は、該横方向横断面と非球面レンズ3の光出射面32が交差して形成される曲線であり、「中央縦方向横断面」は、非球面レンズ3の光軸35を通る縦方向横断面であり、「中央横方向横断面」は、非球面レンズ3の光軸35を通る横方向横断面であり、「中央縦方向横断線」は中央縦方向横断面と非球面レンズ3の光出射面32が交差して形成される曲線であり、「中央横方向横断線34」は、中央横方向横断面と非球面レンズ3の光出射面32が交差して形成される曲線であり、「中央横方向横断線34の中点」は、中央横方向横断線34と光軸35との交点であり、光軸35は非球面レンズ3の焦点を通り且つ前後方向に沿って延びている軸線である。用語は、図に示される方位又は位置関係に基づくものであり、係る装置又は素子が必ずしも特定の方位を有するか、特定の方位で構成及び操作することを指示又は暗示するのではなく、単に本発明を説明し説明を簡略化することに用いられ、従って、本発明を限定するものではないと理解すべきである。 In addition, along the light emission direction, the "front" is the end where the aspherical lens 3 is located, the "rear" is the end where the light source 1 is located, and the "top" is the end where the aspherical lens 3 is located, and the "top" is the end where the aspherical lens 3 is located. ``Bottom'' refers to the upper side of the light output direction when the lamp module is installed correctly, ``bottom'' refers to the lower side of the light output direction when the vehicle lamp module is installed correctly, and ``left'' refers to the lower side of the light output direction when the vehicle lamp module is installed correctly. , "Right" is the left side of the light output direction when the vehicle lamp module is installed normally, "right" is the right side of the light output direction when the vehicle lamp module is installed normally, and "vertical direction" The "transverse section" is any one transverse section that is parallel to the optical axis 35 of the aspherical lens 3 and extends perpendicularly from the upper edge to the lower edge of the aspherical lens 3, and the "vertical transverse line 33" is , is a curve formed by the intersection of the longitudinal cross section and the light exit surface 32 of the aspherical lens 3, and the "horizontal cross section" is perpendicular to the longitudinal cross section, ” is a curve formed by the intersection of the horizontal cross section and the light exit surface 32 of the aspherical lens 3, and the “central longitudinal cross section” is a curve formed by the intersection of the horizontal cross section and the light exit surface 32 of the aspherical lens 3, and the “center longitudinal cross section” is a curve formed by the intersection of the horizontal cross section and the light exit surface 32 of the aspherical lens 3. The "central transverse cross section" is a transverse cross section passing through the optical axis 35 of the aspherical lens 3, and the "central longitudinal transverse line" is a cross section between the central longitudinal cross section and the aspheric lens 3. It is a curve formed by intersecting the light exit surface 32, and the "central lateral transverse line 34" is a curve formed by intersecting the central lateral cross section and the light exit surface 32 of the aspherical lens 3. , "the midpoint of the central transverse transverse line 34" is the intersection of the central transverse transverse line 34 and the optical axis 35, and the optical axis 35 passes through the focal point of the aspherical lens 3 and extends along the front-rear direction. This is the axis line. Terminology is based on the orientation or positional relationships depicted in the drawings, and is not intended to indicate or imply that the device or element necessarily has a particular orientation or is to be constructed or operated in a particular orientation. They are used to describe and simplify the description of the invention, and should therefore not be construed as limiting the invention.

図1~図4に示すように、本発明の基本的な解決手段における車両ランプモジュールは、光源1の出射方向に沿って順に設置される光源1、集光部2及び光出射素子を備え、光源1はLED発光チップ、OLED発光チップ、又はレーザー光源に基づく発光チップであってもよく、集光部2は少なくとも1つの集光素子21を備えてもよく、各集光素子21の後方に1つの光源1が対応して設けられ、光出射素子は非球面レンズ3を使用する。光源1から発する発散光は集光素子21によって収束されて前記非球面レンズ3の光入射面31に入射し、該非球面レンズ3の光出射面32から出射する。非球面レンズ3の光出射面32の表面曲率を調整することで、非球面レンズ3の屈折力を変更でき、それにより光スクリーンに所望のハイビーム配光パターンが投射される。集光部2が1つの集光素子21のみを備える場合、該車両ランプモジュールは基本的なハイビーム機能を実現し、法規制を満たすハイビーム光形状を得ることができ、集光部2が複数の集光素子21を備える場合、各集光素子21の後方に対応する光源1は個別アドレッシング可能であり、ハイビーム照明領域を複数の照明領域に細分化し、車載センシングシステムは対向車線の対向車を検出すると、対応する領域の光源1をオフにすることで、ハイビームによる眩惑を効果的に防止するとともに、路面のほかの領域で優れた照明効果を示し、アダプティブハイビーム機能を実現する。 As shown in FIGS. 1 to 4, the vehicle lamp module according to the basic solution of the present invention includes a light source 1, a light condensing part 2, and a light emitting element, which are installed in order along the emission direction of the light source 1. The light source 1 may be an LED light emitting chip, an OLED light emitting chip, or a light emitting chip based on a laser light source, and the light collecting unit 2 may include at least one light collecting element 21 , and behind each light collecting element 21 One light source 1 is correspondingly provided, and the light emitting element uses an aspherical lens 3. The diverging light emitted from the light source 1 is converged by the condensing element 21, enters the light entrance surface 31 of the aspherical lens 3, and exits from the light exit surface 32 of the aspherical lens 3. By adjusting the surface curvature of the light exit surface 32 of the aspherical lens 3, the refractive power of the aspherical lens 3 can be changed, thereby projecting a desired high beam light distribution pattern onto the optical screen. When the light condensing section 2 includes only one condensing element 21, the vehicle lamp module can realize a basic high beam function and obtain a high beam light shape that satisfies the legal regulations. When the light condensing element 21 is provided, the light source 1 corresponding to the rear of each condensing element 21 can be individually addressed, and the high beam illumination area is subdivided into a plurality of illumination areas, and the on-vehicle sensing system detects oncoming vehicles in the oncoming lane. Then, by turning off the light source 1 in the corresponding area, it effectively prevents dazzling caused by the high beam, and provides excellent lighting effects in other areas of the road surface, realizing the adaptive high beam function.

好ましくは、前記非球面レンズ3の中央横方向横断面と前記非球面レンズ3の光出射面32が交差して中央横方向横断線34を形成し、前記中央横方向横断線34は第1曲率境界点及び第2曲率境界点を有し、第1曲率境界点は中央横方向横断線34の中点から左端点までの間の任意の一点であり、第2曲率境界点は中央横方向横断線34の中点から右端点までの間の任意の一点であり、第1曲率境界点と第2曲率境界点の位置は左右対称に設定されてもよく、所要の光形状に応じて調整して非対称的に設定されてもよく、図11に示すように、いずれも中央横方向横断線34の中点に設定されてもよい。説明の便宜上、中央横方向横断線34の第1曲率境界点から第2曲率境界点までの間の曲線は中部曲線と呼ばれ、中央横方向横断線34の第1曲率境界点から左端点までの曲線は左部曲線と呼ばれ、中央横方向横断線34の第2曲率境界点から右端点までの曲線は右部曲線と呼ばれ、前記中部曲線の曲率は等しく、前記左部曲線の曲率、及び前記右部曲線の曲率はいずれも光軸35から離れる方向に沿って最初に増加し、次に減少するという法則に従って変化し、好ましくは、曲率は前記中部曲線の曲率に等しいまで減少可能である。より詳しくは、本発明の非球面レンズ3の光出射面32の曲率変化についての説明の便宜上、前記非球面レンズ3に基づいて1つの仮想球面レンズを構成し、該球面レンズはレンズの中央から縁まで一定の曲率を有し、且つ該球面レンズの光出射面の中央の曲率は前記非球面レンズ3の光出射面32の中央の曲率と同じであり、図10及び図11に示すように、図中の実線は非球面レンズ3の中央縦方向横断線33又は中央横方向横断線34であり、破線は球面レンズの対応する位置での縦方向横断線又は横方向横断線である。従来の球面レンズに比べて、該非球面レンズ3の中央横方向横断線34の中部曲線の曲率変化法則は球面レンズの対応する位置での横方向横断線の中部曲線の曲率変化法則と同じであるが、該非球面レンズ3の中央横方向横断線34の左部曲線及び右部曲線の曲率はいずれも球面レンズの対応する位置での横方向横断線の左部曲線及び右部曲線の曲率よりも大きいため、非球面レンズ3の左部及び右部の光出射方向は光軸35に接近する方向に出射することであり、非球面レンズ3の中央横方向横断線34の左部曲線及び右部曲線の曲率は光軸35から離れる方向に沿って最初に増加し、次に減少するため、非球面レンズ3の左部及び右部の出射光の光軸35に接近する振幅は最初に増加し、次に減少し、即ち、曲率が増加する場合、光は徐々に光軸35に接近する方向に投射する傾向を有し、曲率が減少する場合、光は徐々に光軸35に接近する方向から光軸35から離れる方向に投射する。上記中央横方向横断線34の曲率変化法則により、非球面レンズ3の光出射面の左右方向における出射光は全体として中部領域の輝度が高く且つ各スポット間の境界がぼやけ、光形状の均一性が向上するという効果を実現する。 Preferably, the central transverse cross section of the aspherical lens 3 and the light exit surface 32 of the aspherical lens 3 intersect to form a central transverse transverse line 34, and the central transverse transverse line 34 has a first curvature. a boundary point and a second curvature boundary point, the first curvature boundary point being any one point between the midpoint of the central lateral transverse line 34 and the left end point, and the second curvature boundary point being an arbitrary point between the central lateral transverse line 34 It is an arbitrary point between the midpoint of the line 34 and the right end point, and the positions of the first curvature boundary point and the second curvature boundary point may be set symmetrically, and can be adjusted according to the required light shape. They may be set asymmetrically, and both may be set at the midpoint of the central transverse transverse line 34, as shown in FIG. For convenience of explanation, the curve from the first curvature boundary point to the second curvature boundary point of the central lateral transverse line 34 is referred to as the middle curve; The curve from the second curvature boundary point of the central transverse transverse line 34 to the right end point is called the right curve, and the curvature of the middle curve is equal to the curvature of the left curve. , and the curvature of said right curve both change according to the law of first increasing and then decreasing along the direction away from the optical axis 35, preferably the curvature can decrease until equal to the curvature of said middle curve. It is. More specifically, for the convenience of explaining the change in curvature of the light exit surface 32 of the aspherical lens 3 of the present invention, one virtual spherical lens will be constructed based on the aspherical lens 3, and the spherical lens will extend from the center of the lens. It has a constant curvature up to the edge, and the curvature at the center of the light exit surface of the spherical lens is the same as the curvature at the center of the light exit surface 32 of the aspherical lens 3, as shown in FIGS. 10 and 11. , the solid line in the figure is the central longitudinal transverse line 33 or the central transverse transverse line 34 of the aspheric lens 3, and the broken line is the longitudinal transverse line or transverse transverse line at the corresponding position of the spherical lens. Compared with the traditional spherical lens, the curvature change law of the middle curve of the central transverse transverse line 34 of the aspherical lens 3 is the same as the curvature variation law of the middle curve of the transverse transverse line at the corresponding position of the spherical lens. However, the curvatures of the left and right curves of the central lateral transverse line 34 of the aspherical lens 3 are both greater than the curvatures of the left and right curves of the lateral transverse line at the corresponding positions of the spherical lens. Because of the large size, the light exit direction of the left and right parts of the aspherical lens 3 is to exit in the direction approaching the optical axis 35, and the left part curve and the right part of the central transverse transverse line 34 of the aspherical lens 3 Since the curvature of the curve first increases and then decreases along the direction away from the optical axis 35, the amplitude of the left and right output lights of the aspherical lens 3 approaching the optical axis 35 increases first. , then decreases, i.e., if the curvature increases, the light has a tendency to project in a direction gradually approaching the optical axis 35, and if the curvature decreases, the light has a tendency to project in a direction gradually approaching the optical axis 35. The light is projected in a direction away from the optical axis 35. Due to the law of curvature change of the central transverse transverse line 34, the light emitted in the left-right direction of the light exit surface of the aspherical lens 3 has a high brightness in the central region as a whole, and the boundaries between each spot are blurred, resulting in a uniform light shape. achieve the effect of improving

さらに好ましくは、図10に示すように、非球面レンズ3のいずれか1つの縦方向横断面と前記非球面レンズ3の光出射面32が交差して1本の縦方向横断線33を形成し、縦方向横断線33は、縦方向横断線33の中点から上端点までの間の任意の一点である曲率変化境界点を有し、前記曲率変化境界点の位置は所要の光形状に応じて調整できる。説明の便宜上、前記縦方向横断線33の曲率境界点から上端点までの間の曲線は上部曲線と呼ばれ、前記縦方向横断線33の曲率境界点から下端点までの曲線は中下部曲線と呼ばれる。好ましい構造形態として、前記縦方向横断線33の中下部曲線の曲率は等しく、前記縦方向横断線33の上部曲線の曲率は等しく、且つ前記縦方向横断線33の上端点の曲率は前記縦方向横断線33の下端点の曲率よりも小さく、別の好ましい構造形態として、前記縦方向横断線33の中下部曲線の曲率は等しく、前記縦方向横断線33の上部曲線の曲率は光軸35から離れる方向に沿って徐々に小さくなる。より詳しくは、従来の球面レンズに比べて、前記非球面レンズ3のいずれか1つの縦方向横断線33の中下部の変化法則は球面レンズの対応する位置での縦方向横断線の中下部の変化法則と同じであり、前記非球面レンズ3の縦方向横断線33の上部曲線の曲率は球面レンズの対応する位置での縦方向横断線の上部曲線の曲率よりも小さい。従来の球面レンズを用いて光を投射する場合、光は該球面レンズの光軸35に略平行な方向に出射し、形成されたハイビーム光形状は図13に示され、ハイビームは水平0度線の上下付近領域内に対称的に分布しており、ハイビーム光形状の法規制要件を満たさない。図14に示すように、非球面レンズ3を用いて光を投射する場合、同じ光は、球面レンズの縦方向横断線の上部曲線から出射するよりも、該非球面レンズ3の縦方向横断線33の上部曲線から出射するほうが、出射方向がより光軸35から離れており、形成されたハイビーム光形状の大部分は水平0度線以上にあり且つ上方拡散角度が非常に大きく、光形状の範囲はハイビーム光形状の法規制要件を満たす。 More preferably, as shown in FIG. 10, the longitudinal cross section of any one of the aspherical lenses 3 and the light exit surface 32 of the aspherical lens 3 intersect to form one longitudinal transverse line 33. , the longitudinal transverse line 33 has a curvature change boundary point that is an arbitrary point between the midpoint and the upper end point of the longitudinal transverse line 33, and the position of the curvature change boundary point is determined according to the required light shape. can be adjusted. For convenience of explanation, the curve from the curvature boundary point of the longitudinal transverse line 33 to the upper end point is called the upper curve, and the curve from the curvature boundary point of the longitudinal transverse line 33 to the lower end point is called the lower middle curve. Called. In a preferred structural form, the middle and lower curves of the longitudinal transverse line 33 have equal curvatures, the upper curves of the longitudinal transverse line 33 have equal curvatures, and the curvature of the upper end point of the longitudinal transverse line 33 has the same curvature in the longitudinal direction. The curvature of the lower end point of the longitudinal transverse line 33 is smaller than the curvature of the lower end point of the transverse line 33, and as another preferred structure, the curvature of the middle and lower curves of the longitudinal transverse line 33 is equal, and the curvature of the upper curve of the longitudinal transverse line 33 is smaller than the curvature of the lower end point of the longitudinal transverse line 33. It gradually becomes smaller along the direction of separation. More specifically, compared to the conventional spherical lens, the law of change of the middle and lower part of the longitudinal transverse line 33 of any one of the aspherical lenses 3 is the lower middle part of the longitudinal transverse line 33 at the corresponding position of the spherical lens. It is the same as the law of variation, and the curvature of the upper curve of the longitudinal transverse line 33 of the aspherical lens 3 is smaller than the curvature of the upper curve of the longitudinal transverse line at the corresponding position of the spherical lens. When projecting light using a conventional spherical lens, the light is emitted in a direction approximately parallel to the optical axis 35 of the spherical lens, and the formed high beam shape is shown in FIG. They are distributed symmetrically in the area near the top and bottom of the beam, and do not meet the legal requirements for high beam light shape. As shown in FIG. 14, when using an aspherical lens 3 to project light, the same light exits from the longitudinal transverse line 33 of the aspherical lens 3 than from the upper curve of the longitudinal transverse line of the aspherical lens 3. When the light is emitted from the upper curve of meets regulatory requirements for high beam light shape.

好ましくは、非球面レンズ3は両凸レンズであり、光入射面31が前記非球面レンズ3の光軸35方向に沿って後方に向かって突出し、このように、太陽光が該非球面レンズ3に照射する時に形成される焦点はより該非球面レンズ3に接近し、ベゼルから離れており、それによりベゼルの焼損が回避される。勿論、該非球面レンズ3は平凸レンズ、凹凸レンズ等であってもよい。 Preferably, the aspherical lens 3 is a biconvex lens, and the light incident surface 31 protrudes toward the rear along the optical axis 35 direction of the aspherical lens 3, so that sunlight irradiates the aspherical lens 3. The focal point formed when doing so is closer to the aspherical lens 3 and further away from the bezel, thereby avoiding burnout of the bezel. Of course, the aspherical lens 3 may be a plano-convex lens, a concave-convex lens, or the like.

本発明の好ましい実施例における非球面レンズは、球面レンズに基づくものであり、該非球面レンズ3の光出射面32は、中央横方向横断線34の中部曲線の曲率が球面レンズの対応する位置での横方向横断線の曲率に等しく、該非球面レンズ3の中央横方向横断線34の左部曲線の曲率、中央横方向横断線34の右部曲線の曲率がいずれも光軸35から離れる方向に沿って最初に増加し、次に減少し、且つ、前記中部曲線の曲率に等しいまで減少し、即ち、左端点が球面レンズの対応する左端点に重なり、右端点が球面レンズの対応する右端点に重なり、そして、前記非球面レンズ3の縦方向横断線33の中下部曲線の曲率が球面レンズの曲率に等しく、該非球面レンズ3の縦方向横断線33の上部曲線の曲率が光軸35から離れる方向に沿って徐々に小さくなるように構成される。本発明の好ましい実施例における非球面レンズ3について、非球面レンズ3の中央縦方向横断線を輪郭線とし、非球面レンズ3の中央横方向横断線34をガイド線としてスイープして曲面を形成するか、又は、非球面レンズ3の中央横方向横断線34を複数のサブ線分に分割し、各サブ線分の分割点を通る非球面レンズ3の縦方向横断線33を輪郭線とし、それに対応する中央横方向横断線34のサブ線分をガイド線としてスイープし、複数のスイープ面を接続して光出射面32を形成することによって非球面レンズ3の光出射面32を構成するようにしてもよく、このように、光出射面32を複数のスイープ面に分けることができ、光出射面32の設計中、形成される光形状を微調整するように各スイープ面のパラメータを簡単に調整でき、このような形態では、輪郭線とする縦方向横断線33は複数本あり、縦方向横断線33の上部曲線の曲率が球面レンズの対応する位置での縦方向横断線の曲率よりも小さいという条件の下では、各縦方向横断線33の上部曲線の曲率は異なってもよく、各縦方向横断線33の曲率変化境界点の位置も所要の光形状に応じて調整可能である。 The aspherical lens in a preferred embodiment of the invention is based on a spherical lens, and the light exit surface 32 of the aspherical lens 3 is such that the curvature of the middle curve of the central transverse transverse line 34 is at the corresponding position of the spherical lens. The curvature of the left curve of the central transverse transverse line 34 of the aspherical lens 3 and the curvature of the right curve of the central transverse transverse line 34 of the aspherical lens 3 are both in the direction away from the optical axis 35. first increases, then decreases, and decreases until equal to the curvature of said middle curve, i.e. the left end point overlaps the corresponding left end point of the spherical lens, and the right end point overlaps the corresponding right end point of the spherical lens. , and the curvature of the lower middle curve of the longitudinal transverse line 33 of the aspherical lens 3 is equal to the curvature of the spherical lens, and the curvature of the upper curve of the longitudinal transverse line 33 of the aspherical lens 3 is from the optical axis 35. It is configured to gradually become smaller in the direction of separation. Regarding the aspherical lens 3 in the preferred embodiment of the present invention, a curved surface is formed by sweeping the central longitudinal transverse line of the aspherical lens 3 as a contour line and using the central transverse transverse line 34 of the aspherical lens 3 as a guide line. Alternatively, the central transverse transverse line 34 of the aspherical lens 3 is divided into a plurality of sub-line segments, and the longitudinal transverse line 33 of the aspherical lens 3 passing through the dividing point of each sub-line segment is defined as a contour line; The light exit surface 32 of the aspherical lens 3 is configured by sweeping the corresponding sub-line segment of the central horizontal transverse line 34 as a guide line and connecting a plurality of sweep surfaces to form the light exit surface 32. In this way, the light exit surface 32 can be divided into a plurality of sweep surfaces, and during the design of the light exit surface 32, the parameters of each sweep surface can be easily adjusted to finely adjust the formed light shape. In such a form, there are a plurality of longitudinal transverse lines 33 as contour lines, and the curvature of the upper curve of the longitudinal transverse line 33 is greater than the curvature of the longitudinal transverse line at the corresponding position of the spherical lens. Under the condition of being small, the curvature of the upper curve of each longitudinal transverse line 33 may be different, and the position of the curvature change boundary point of each longitudinal transverse line 33 can also be adjusted according to the required light shape.

本発明の好ましい実施例における非球面レンズ3の構造において、非球面レンズ3の焦点に1つの光源1が設けられ、該光源1から発する光と併せて該非球面レンズ3の屈折法則をより詳しく説明する。図10に示すように、非球面レンズ3の縦方向横断線33の中下部曲線の曲率が等しいため、非球面レンズ3の光出射面32の中部及び下部によって屈折された光L1は非球面レンズ3の光軸35方向に略平行であり、該非球面レンズ3の光出射面32の縦方向横断線33の上部曲線の曲率が光軸35から離れる方向に沿って徐々に減少するため、非球面レンズ3の光出射面32の上部によって屈折された光L2は光軸35方向に対して斜め上に出射し、図11に示すように、中央横方向横断線34の第1曲率境界点及び第2曲率境界点はいずれも中央横方向横断線34の中点に設定され、且つ中央横方向横断線34の左部曲線及び右部曲線の曲率はいずれも中央横方向横断線34の中点に対して光軸35から離れる方向に沿って最初に増加し、次に減少し、従って、L3の屈折点の位置の曲率が中点位置の曲率よりも大きいので、光L3は光軸35に接近する方向に出射し、光L4の屈折点の位置の曲率が光L3の屈折点の位置の曲率よりも大きいので、光L4は光L3よりも光軸35に接近する方向に出射し、光L5の屈折点の位置の曲率が光L4の屈折点の位置の曲率よりも小さいので、光L5は光L4よりも光軸35から離れる方向に出射し、光L6の屈折点の位置の曲率が光L5の屈折点の位置の曲率よりも小さいので、光L6は光L5よりも光軸35から離れる方向に出射し、即ち、光軸35に略平行な方向に沿って出射し、このようにして、非球面レンズ3は受けた光を上方に向かって拡散するとともに、中央領域が明るくより均一な光形状を投射して形成することができる。図10及び図11の光路図において光源1が非球面レンズ3に直射する光路であり、集光素子21によって集光されていないものであるが、光源1から発し集光素子21によって集光されて非球面レンズ3に入射した光も上記屈折法則に従うことになり、集光部2が1行の集光素子21を備える場合、それに対応して、各集光素子21の後方に1つの光源1が対応して設けられ、各光源1から発し集光素子21によって収束されて非球面レンズ3に入射した光も上記屈折法則に従うことになり、このように、非球面レンズ3で投射することで、各スポット間の境界がぼやけ、均一性が高いハイビーム光形状を形成できるとともに、形成されたハイビーム光形状の大部分は水平0度線以上にあり、且つ上方拡散角度が非常に大きい。 In the structure of the aspherical lens 3 in the preferred embodiment of the present invention, one light source 1 is provided at the focal point of the aspherical lens 3, and the refractive law of the aspherical lens 3 is explained in more detail in conjunction with the light emitted from the light source 1. do. As shown in FIG. 10, since the curvatures of the middle and lower curves of the vertical transverse line 33 of the aspherical lens 3 are equal, the light L1 refracted by the middle and lower parts of the light exit surface 32 of the aspherical lens 3 is reflected by the aspherical lens 3. 3, and the curvature of the upper curve of the longitudinal transverse line 33 of the light exit surface 32 of the aspherical lens 3 gradually decreases in the direction away from the optical axis 35. The light L2 refracted by the upper part of the light exit surface 32 of the lens 3 is emitted diagonally upward with respect to the direction of the optical axis 35, and as shown in FIG. The two curvature boundary points are both set at the midpoint of the central transverse transverse line 34, and the curvatures of the left and right curves of the central transverse transverse line 34 are both set at the midpoint of the central transverse transverse line 34. On the other hand, the light L3 first increases and then decreases along the direction away from the optical axis 35. Therefore, since the curvature at the refraction point of L3 is larger than the curvature at the midpoint, the light L3 approaches the optical axis 35. Since the curvature of the refraction point of the light L4 is larger than the curvature of the refraction point of the light L3, the light L4 is emitted in a direction closer to the optical axis 35 than the light L3, and the light L5 Since the curvature at the position of the refraction point of light L4 is smaller than the curvature at the position of the refraction point of light L4, light L5 is emitted in a direction farther away from the optical axis 35 than light L4, and the curvature of the position of the refraction point of light L6 is smaller than the curvature of the position of the refraction point of light L4. Since the curvature of the position of the refraction point of L5 is smaller, the light L6 is emitted in a direction farther from the optical axis 35 than the light L5, that is, emitted along a direction substantially parallel to the optical axis 35, and in this way, The aspherical lens 3 diffuses the received light upward, and can project and form a brighter and more uniform light shape in the central region. In the optical path diagrams of FIGS. 10 and 11, the light path is such that the light source 1 is directly incident on the aspherical lens 3 and is not focused by the condensing element 21, but the light is emitted from the light source 1 and is condensed by the condensing element 21. The light incident on the aspherical lens 3 also follows the above-mentioned refraction law, and when the condensing section 2 includes one row of condensing elements 21, correspondingly, one light source is provided behind each condensing element 21. 1 are provided correspondingly, and the light emitted from each light source 1, converged by the condensing element 21, and incident on the aspherical lens 3 also follows the above refraction law, and in this way, the light is projected by the aspherical lens 3. In this way, the boundaries between the spots are blurred, and a highly uniform high beam light shape can be formed, and most of the formed high beam light shape is located above the horizontal 0 degree line, and the upward diffusion angle is very large.

さらに好ましくは、図10~図12に示すように、非球面レンズ3は光入射面31及び光出射面3232を有し、該光出射面3232は非球面であり、表面に光をさらに拡散するための縦リブ状構造、横リブ状構造又は格子状構造が設けられる。より好ましくは、非球面レンズ3は両凸レンズであり、光入射面31が前記非球面レンズ3の光軸35方向に沿って後方に向かって突出し、このように、太陽光が該非球面レンズ3に照射する時に形成される焦点はより該非球面レンズ3に接近し、ベゼルから離れており、それによりベゼルの焼損が回避される。勿論、該非球面レンズ3は平凸レンズ、凹凸レンズ等であってもよい。 More preferably, as shown in FIGS. 10 to 12, the aspherical lens 3 has a light entrance surface 31 and a light exit surface 3232, and the light exit surface 3232 is an aspheric surface to further diffuse the light on the surface. A vertical rib-like structure, a horizontal rib-like structure or a lattice-like structure is provided for this purpose. More preferably, the aspherical lens 3 is a biconvex lens, and the light entrance surface 31 protrudes toward the rear along the optical axis 35 direction of the aspherical lens 3, so that sunlight enters the aspherical lens 3. The focal point formed when irradiating is closer to the aspherical lens 3 and away from the bezel, thereby avoiding bezel burnout. Of course, the aspherical lens 3 may be a plano-convex lens, a concave-convex lens, or the like.

好ましくは、図5及び図6に示すように、集光部2は複数の集光素子21を備えてもよく、前記集光素子21は1行複数列のマトリックス状に配置され得るか、又は複数行複数列のマトリックス状に配置され得て、各集光素子21の後方に対応する光源1は個別アドレッシング可能であり、ハイビーム照明領域を複数の照明領域に細分化し、車載センシングシステムは対向車を検出すると、対応する領域の光源1をオフにすることで、ダプティブハイビーム機能を実現する。 Preferably, as shown in FIGS. 5 and 6, the light collecting section 2 may include a plurality of light collecting elements 21, and the light collecting elements 21 may be arranged in a matrix of one row and a plurality of columns, or The light sources 1 can be arranged in a matrix of multiple rows and multiple columns, and the light sources 1 corresponding to the rear of each condensing element 21 can be individually addressed, subdividing the high beam illumination area into multiple illumination areas, and the in-vehicle sensing system can detect oncoming vehicles. When detected, the adaptive high beam function is realized by turning off the light source 1 in the corresponding area.

好ましくは、図8及び図9に示すように、集光素子21は平凸レンズであり、集光素子21の光入射面は平面であり、光出射面は前方に向かって突出した曲面である。勿論、集光素子21は平凸、両凸、凹凸又は平凹レンズを使用してもよい。集光素子21は好ましくは平凸レンズであり、従来技術の集光カップ構造を備えた集光器を用いて集光することに比べて、集光素子21は構造が簡単で、発光効率が高く、同じ光利用率の場合、光源1と集光素子21の光入射面との距離を適宜増加させることができることで、車両ランプモジュールの放熱効果を向上させ、光源1は集光素子21の光入射面の後方0.1mm~5mmに設けられ、該距離は好ましくは0.5mmであり、また、光入射面が凸面の集光素子21に比べて、集光素子21の光入射面が平面を使用することで、該光入射面に入射する光は全反射し難く、発光効率をさらに向上させる。 Preferably, as shown in FIGS. 8 and 9, the condensing element 21 is a plano-convex lens, the light incident surface of the condensing element 21 is a flat surface, and the light exiting surface is a curved surface protruding toward the front. Of course, the condensing element 21 may be a plano-convex, biconvex, concave-convex, or plano-concave lens. The condensing element 21 is preferably a plano-convex lens, and the condensing element 21 has a simple structure and high luminous efficiency compared to using a condenser with a conventional condensing cup structure to condense light. , in the case of the same light utilization rate, the distance between the light source 1 and the light incident surface of the condensing element 21 can be increased appropriately, thereby improving the heat dissipation effect of the vehicle lamp module, and the light source 1 It is provided 0.1 mm to 5 mm behind the incident surface, and the distance is preferably 0.5 mm, and the light incident surface of the light condensing element 21 is flat compared to the condensing element 21 having a convex light incident surface. By using this, the light incident on the light incident surface is less likely to be totally reflected, further improving the luminous efficiency.

具体的には、図7に示すように、本発明の車両ランプモジュールは集光部2を取り付けるための取り付けブラケット4をさらに備え、前記取り付けブラケット4に位置決めピン41及び取り付け孔42が設けられることで、集光部2を、例えば放熱器のようなほかの部材に位置決めして取り付け、前記取り付けブラケット4の周囲にフランジ43が設けられることで、取り付けブラケット4の強度を高め、前記集光部2と前記取り付けブラケット4は一体に成形されるか、又は組み立てて接続されるようにしてもよい。 Specifically, as shown in FIG. 7, the vehicle lamp module of the present invention further includes a mounting bracket 4 for mounting the light condensing part 2, and the mounting bracket 4 is provided with a positioning pin 41 and a mounting hole 42. Then, the light condensing section 2 is positioned and attached to another member such as a radiator, and a flange 43 is provided around the mounting bracket 4, so that the strength of the mounting bracket 4 is increased and the light condensing section 2 and the mounting bracket 4 may be integrally molded or assembled together.

具体的には、光源1は前記集光素子21の焦点の前方に設けられ、距離は好ましくは0.5mmであり、光源1が集光素子21の焦点に設けられることに比べて、光は集光素子21の光出射面によって屈折された後に、周囲に拡散し、非球面レンズ3によって屈折されることで、最終的なハイビーム光形状を形成することに有利であり、また、光源1が集光素子21の焦点の前方に設けられることで、発光効率をさらに向上させることができる。 Specifically, the light source 1 is provided in front of the focal point of the condensing element 21, and the distance is preferably 0.5 mm. After being refracted by the light output surface of the condensing element 21, it is diffused into the surroundings and refracted by the aspherical lens 3, which is advantageous in forming the final high beam shape. By providing it in front of the focal point of the light condensing element 21, the light emission efficiency can be further improved.

より具体的には、光源1は前記非球面レンズ3の焦点面に設けられることで、光スクリーンに投射された配光パターンをより鮮明にする。 More specifically, the light source 1 is provided on the focal plane of the aspherical lens 3 to make the light distribution pattern projected on the optical screen clearer.

本発明の好ましい実施例における車両ランプモジュールは、光出射方向に沿って順に設置される光源1、集光部2及び光出射素子を備え、集光部2は1行のマトリックス状に分布する集光素子21を備え、該集光素子21は平凸レンズであり、光源1は集光素子21の後方に設けられ、且つ各集光素子21に1対1で対応しており、光出射素子は上記好ましい実施例における非球面レンズ3である。該車両ランプモジュールは前記集光部2を取り付けるための取り付けブラケット4をさらに備え、取り付けブラケット4に位置決めピン41及び取り付け孔42が設けられことで、放熱器等の部材に接続され、取り付けブラケット4の周囲にフランジ43が設けられることで、取り付けブラケット4の強度を高め、集光部2と取り付けブラケット4は組み立てて接続されるか、又は該集光部2と取り付けブラケット4は直接一体に成形される。該車両ランプモジュールを取り付ける際に、光源1を集光素子21の焦点の前方0.5mmに設けるようにしてもよい。光源1をオンにし、光源1から発する光は集光部2によって収束されて非球面レンズ3に入射し、非球面レンズ3は受けた光を上方に拡散するとともに、中央領域が明るくより均一な光形状を投射して形成することができ、また、該車両ランプモジュールの各集光素子21の後方に対応する光源1は個別アドレッシング可能であり、ハイビーム照明領域を複数の照明領域に細分化し、車載センシングシステムは対向車線の対向車を検出すると、対応する領域の光源1をオフにすることで、ハイビームによる眩惑を効果的に防止するとともに、路面のほかの領域で優れた照明効果を示し、アダプティブハイビーム機能を実現する。本発明の好ましい実施例における車両ランプモジュールは、アダプティブハイビーム機能を実現可能な限りでなく、集光素子21を集光部2とすることで、従来技術の集光器に比べて、発光効率がさらに高く、占有空間が小さく、構造が簡単で、寸法が小さく、軽量であり、集光素子21と取り付けブラケットが一体に成形されることで、車両ランプモジュールの取り付け精度をさらに向上させ、調光時、集光部2と非球面レンズ3との相対的な位置を調整するだけでよく、それにより車両ランプモジュールの光学精度を向上させ、また、光出射面32の曲率が変化する非球面レンズ3を光出射素子とすることで、中央領域の輝度が高く、均一性がより高いハイビーム光形状を形成でき、さらに、非球面レンズ3の光出射面32の曲率を調整することによって、様々な光形状を柔軟に得ることができる。 A vehicle lamp module according to a preferred embodiment of the present invention includes a light source 1, a light condensing section 2, and a light emitting element, which are installed in order along the light emission direction, and the light condensing section 2 is a concentrator distributed in a matrix of one row. It is equipped with an optical element 21, the condensing element 21 is a plano-convex lens, the light source 1 is provided behind the condensing element 21, and corresponds to each condensing element 21 on a one-to-one basis, and the light emitting element is This is the aspherical lens 3 in the above preferred embodiment. The vehicle lamp module further includes a mounting bracket 4 for mounting the light condensing section 2, and the mounting bracket 4 is provided with a positioning pin 41 and a mounting hole 42, so that it is connected to a member such as a radiator. A flange 43 is provided around the periphery of the mounting bracket 4 to increase the strength of the mounting bracket 4, and the light collecting part 2 and the mounting bracket 4 can be assembled and connected, or the light collecting part 2 and the mounting bracket 4 can be directly molded into one piece. be done. When installing the vehicle lamp module, the light source 1 may be provided 0.5 mm in front of the focal point of the condensing element 21. When the light source 1 is turned on, the light emitted from the light source 1 is converged by the condenser 2 and enters the aspherical lens 3, and the aspherical lens 3 diffuses the received light upward and makes the central area brighter and more uniform. The light shape can be projected and formed, and the light source 1 corresponding to the rear of each condensing element 21 of the vehicle lamp module is individually addressable, subdividing the high beam illumination area into a plurality of illumination areas, When the in-vehicle sensing system detects an oncoming vehicle in the oncoming lane, it turns off the light source 1 in the corresponding area, effectively preventing dazzling caused by high beams, and providing excellent lighting effects on other areas of the road surface. Realizes adaptive high beam function. The vehicle lamp module according to the preferred embodiment of the present invention is not only capable of realizing an adaptive high beam function, but also has light emitting efficiency by using the light collecting element 21 as the light collecting part 2 compared to the light collecting device of the prior art. The height is higher, occupies less space, the structure is simple, the dimensions are small, and the mounting bracket is integrally molded, which further improves the installation precision of the vehicle lamp module and allows dimming. At the time, it is only necessary to adjust the relative position between the condensing part 2 and the aspherical lens 3, thereby improving the optical precision of the vehicle lamp module, and the aspherical lens whose curvature of the light exit surface 32 changes. By using 3 as a light emitting element, it is possible to form a high beam light shape with high brightness in the central region and high uniformity.Furthermore, by adjusting the curvature of the light emitting surface 32 of the aspherical lens 3, various Light shapes can be obtained flexibly.

本発明の車両ヘッドランプの実施例は、少なくとも1つの上記技術案のいずれか1項に記載の車両ランプモジュールを備え、前記車両ランプモジュールは垂直に分布するか、水平に分布するか、又は斜めに配列して分布する。本発明の車両ヘッドランプの実施例は上記すべての実施例に記載の車両ランプモジュールを備えてもよく、従って、少なくとも上記車両ランプモジュールの実施例によるすべての有益な効果を持つ。 An embodiment of the vehicle headlamp of the present invention comprises at least one vehicle lamp module according to any one of the above technical solutions, wherein the vehicle lamp module is vertically distributed, horizontally distributed or diagonally distributed. It is arranged and distributed as follows. Embodiments of the vehicle headlamp according to the invention may comprise a vehicle lamp module as described in all the embodiments described above and thus have at least all the beneficial effects of the embodiments of the vehicle lamp module described above.

本発明の車両の実施例は上記実施例に記載の車両ヘッドランプを備えてもよく、従って、少なくとも上記車両ヘッドランプの実施例によるすべての有益な効果を持つ。 Vehicle embodiments of the invention may be equipped with a vehicle headlamp as described in the above embodiments and thus have at least all the beneficial effects of the above vehicle headlamp embodiments.

以上、図面を参照しながら本発明の好ましい実施形態を詳細に説明したが、本発明はこれに限定されない。本発明の技術的的概念の範囲を逸脱せずに、本発明の技術案に対して、各具体的な技術的特徴を任意の適切な方式で組み合わせることを含む様々な簡単な変形を行うことができる。不必要な繰り返しを避けるために、本発明は様々な可能な組み合わせ方式を別途に説明しない。それにもかかわらず、これらの簡単な変形や組合せも本発明に開示されている内容としてみなされ、本発明の特許範囲に属する。 Although preferred embodiments of the present invention have been described above in detail with reference to the drawings, the present invention is not limited thereto. Without departing from the scope of the technical concept of the present invention, various simple modifications may be made to the technical solution of the present invention, including combining each specific technical feature in any appropriate manner. Can be done. To avoid unnecessary repetition, the present invention does not separately describe various possible combination schemes. Nevertheless, these simple variations and combinations are also considered to be disclosed in the present invention and fall within the patentable scope of the present invention.

1 光源
2 集光部
21 集光素子
3 非球面レンズ
31 光入射面
32 光出射面
33 縦方向横断線
34 中央横方向横断線
35 光軸
4 取り付けブラケット
41 位置決めピン
42 取り付け孔
43 フランジ
1 Light source 2 Light condensing unit 21 Condensing element 3 Aspherical lens 31 Light entrance surface 32 Light exit surface 33 Vertical transverse line 34 Central horizontal transverse line 35 Optical axis 4 Mounting bracket 41 Positioning pin 42 Mounting hole 43 Flange

Claims (10)

車両ランプモジュールであって、光出射方向に沿って順に設置される光源(1)、集光部(2)及び光出射素子を備え、前記光出射素子は非球面レンズ(3)であり、前記集光部(2)は少なくとも1つの集光素子(21)を備え、前記光源(1)は対応する前記集光素子(21)に対応し、前記光源(1)から発する光は前記集光素子(21)によって収束されて前記非球面レンズ(3)の光入射面(31)に入射して、前記非球面レンズ(3)の光出射面(32)から出射することができ、前記非球面レンズ(3)の光出射面(32)は、前記非球面レンズ(3)の中央横方向横断面と前記非球面レンズ(3)の光出射面(32)が交差して中央横方向横断線(34)を形成するように構成され、前記中央横方向横断線(34)は第1曲率境界点及び第2曲率境界点を有し、前記第1曲率境界点は前記中央横方向横断線(34)の中点から左端点までの間の任意の一点であり、前記第2曲率境界点は前記中央横方向横断線(34)の中点から右端点までの間の任意の一点であり、前記中央横方向横断線(34)の第1曲率境界点から第2曲率境界点までの曲率は等しく、前記中央横方向横断線(34)の第1曲率境界点から左端点までの曲率、及び前記中央横方向横断線(34)の第2曲率境界点から右端点までの曲率はいずれも最初に増加し、次に減少することを特徴とする車両ランプモジュール。 A vehicle lamp module, comprising a light source (1), a condensing part (2), and a light emitting element, which are installed in order along the light emitting direction, the light emitting element being an aspherical lens (3), and the light emitting element being an aspherical lens (3); The light collecting section (2) includes at least one light collecting element (21), the light source (1) corresponds to the corresponding light collecting element (21), and the light emitted from the light source (1) is connected to the light collecting element (21). The light can be converged by the element (21), enter the light entrance surface (31) of the aspherical lens (3), and exit from the light exit surface (32) of the aspherical lens (3). The light exit surface (32) of the spherical lens (3) is formed by intersecting the central lateral cross section of the aspherical lens (3) and the light exit surface (32) of the aspherical lens (3). the central lateral transverse line (34) having a first curvature boundary point and a second curvature boundary point, the first curvature boundary point being configured to form a central lateral transverse line (34); The second curvature boundary point is an arbitrary point between the midpoint of (34) and the left end point, and the second curvature boundary point is an arbitrary point between the midpoint of the central horizontal transverse line (34) and the right end point. , the curvature from the first curvature boundary point to the second curvature boundary point of the central lateral transverse line (34) is equal, and the curvature from the first curvature boundary point to the left end point of the central lateral transverse line (34) is equal; and the curvature of the central lateral transverse line (34) from the second curvature boundary point to the right end point first increases and then decreases. 前記中央横方向横断線(34)の左端点の曲率及び/又は前記中央横方向横断線(34)の右端点の曲率は前記中央横方向横断線(34)の第1曲率境界点から第2曲率境界点までの曲率に等しいことを特徴とする請求項1に記載の車両ランプモジュール。 The curvature of the left end point of said central lateral transverse line (34) and/or the curvature of the right end point of said central lateral transverse line (34) varies from a first curvature boundary point of said central lateral transverse line (34) to a second curvature boundary point of said central lateral transverse line (34). Vehicle lamp module according to claim 1, characterized in that the curvature is equal to the curvature boundary point. 前記非球面レンズ(3)の光出射面(32)は前方に向かって突出した曲面であり、前記非球面レンズ(3)の光出射面(32)はさらに、前記非球面レンズ(3)のいずれか1つの縦方向横断面と前記非球面レンズ(3)の光出射面(32)が交差して1本の縦方向横断線(33)を形成するように構成され、前記縦方向横断線(33)は、前記縦方向横断線(33)の中点から上端点までの間の任意の一点である曲率変化境界点を有し、前記縦方向横断線(33)の曲率変化境界点から下端点までの曲率は等しく、前記縦方向横断線(33)の曲率変化境界点から上端点までの曲率は等しく、且つ前記縦方向横断線(33)の上端点の曲率は前記縦方向横断線(33)の下端点の曲率よりも小さい、又は、 前記非球面レンズ(3)の光出射面(32)は前方に向かって突出した曲面であり、前記非球面レンズ(3)の光出射面(32)はさらに、前記非球面レンズ(3)のいずれか1つの縦方向横断面と前記非球面レンズ(3)の光出射面(32)が交差して1本の縦方向横断線(33)を形成するように構成され、前記縦方向横断線(33)は、前記縦方向横断線(33)の中点から上端点までの間の任意の一点である曲率変化境界点を有し、前記縦方向横断線(33)の曲率変化境界点から下端点までの曲率は等しく、前記縦方向横断線(33)の曲率変化境界点から上端点までの曲率は徐々に減少することを特徴とする請求項2に記載の車両ランプモジュール。 The light exit surface (32) of the aspherical lens (3) is a curved surface that protrudes forward, and the light exit surface (32) of the aspherical lens (3) further extends toward the front. Any one longitudinal transverse cross section and the light exit surface (32) of the aspherical lens (3) are configured to intersect to form one longitudinal transverse line (33), and the longitudinal transverse line (33) has a curvature change boundary point that is any one point between the midpoint and the upper end point of the longitudinal transverse line (33), and from the curvature change boundary point of the longitudinal transverse line (33). The curvatures from the curvature change boundary point to the upper end point of the longitudinal transverse line (33) are equal, and the curvature of the upper end point of the longitudinal transverse line (33) is equal to that of the longitudinal transverse line (33). (33) smaller than the curvature of the lower end point , or the light exit surface (32) of the aspherical lens (3) is a curved surface protruding forward, and the light exit surface of the aspherical lens (3) (32) further includes one longitudinal transverse line (33 ), the longitudinal transverse line (33) has a curvature change boundary point that is any one point between the midpoint and the upper end point of the longitudinal transverse line (33), The curvature of the longitudinal transverse line (33) from the curvature change boundary point to the lower end point is equal, and the curvature of the longitudinal transverse line (33) from the curvature change boundary point to the upper end point gradually decreases. The vehicle lamp module according to claim 2. 前記非球面レンズ(3)の光入射面(31)は前記非球面レンズ(3)の光軸(35)方向に沿って後方に向かって突出することを特徴とする請求項1~のいずれか1項に記載の車両ランプモジュール。 Any one of claims 1 to 3 , wherein the light entrance surface (31) of the aspherical lens (3) projects rearward along the optical axis (35) direction of the aspherical lens (3). The vehicle lamp module according to item 1. 前記集光部(2)は複数の集光素子(21)を備え、前記集光素子(21)は1行複数列のマトリックス状に配置され得るか、又は複数行複数列のマトリックス状に配置され得ることを特徴とする請求項1~4のいずれか1項に記載の車両ランプモジュール。 The light collecting section (2) includes a plurality of light collecting elements (21), and the light collecting elements (21) may be arranged in a matrix of one row and a plurality of columns, or arranged in a matrix of a plurality of rows and a plurality of columns. The vehicle lamp module according to any one of claims 1 to 4, characterized in that it can be 前記集光素子(21)は平凸レンズであり、前記集光素子(21)の光入射面は平面であり、前記集光素子(21)の光出射面は前方に向かって突出した曲面であることを特徴とする請求項1~のいずれか1項に記載の車両ランプモジュール。 The light condensing element (21) is a plano-convex lens, the light incidence surface of the light condensing element (21) is a flat surface, and the light exit surface of the light condensing element (21) is a curved surface protruding forward. The vehicle lamp module according to any one of claims 1 to 5 , characterized in that: 前記集光部(2)を取り付けるための取り付けブラケット(4)をさらに備え、前記取り付けブラケット(4)に位置決めピン(41)及び取り付け孔(42)が設けられ、前記取り付けブラケット(4)の周囲にフランジ(43)が設けられ、前記集光部(2)と前記取り付けブラケット(4)は一体に成形されるか、又は組み立てて接続されることを特徴とする請求項1~のいずれか1項に記載の車両ランプモジュール。 The mounting bracket (4) is further provided with a mounting bracket (4) for mounting the light condensing section (2), and the mounting bracket (4) is provided with a positioning pin (41) and a mounting hole (42), and the mounting bracket (4) is provided with a 7. A flange (43) is provided on the light collecting part (2) and the mounting bracket ( 4 ) are integrally molded or assembled and connected. The vehicle lamp module according to item 1. 前記光源(1)は前記集光素子(21)の焦点の前方に設けられる、かつ/又は、前記光源(1)は前記非球面レンズ(3)の焦点面に設けられることを特徴とする請求項1~7のいずれか1項に記載の車両ランプモジュール。 The light source (1) is provided in front of the focal point of the condensing element (21) , and/or the light source (1) is provided in the focal plane of the aspherical lens (3). The vehicle lamp module according to any one of items 1 to 7. 車両ヘッドランプであって、少なくとも1つの請求項1~のいずれか1項に記載の車両ランプモジュールを備え、前記車両ランプモジュールは縦方向、横方向、又は斜めに配列して分布することを特徴とする車両ヘッドランプ。 A vehicle headlamp comprising at least one vehicle lamp module according to any one of claims 1 to 8 , wherein the vehicle lamp modules are distributed in a longitudinal, transverse or diagonal arrangement. Characteristic vehicle headlamps. 請求項に記載の車両ヘッドランプを備えることを特徴とする車両。 A vehicle comprising the vehicle headlamp according to claim 9 .
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