M326994 八、新型說明： 【新型所屬之技術領域】 變焦功能。 本創作是有關一種照明裝置，具有改變照明範圍的 【先前技術】 現今-般的照明技術中，利用反光杯來反射光源所發射的 光線，或許再配合透鏡的折射，最後在某範_形成所需的照 明。根據不同的使用需求，對於照明範圍A小的設計就有所不 同’有時需要集中的光束，將光傳播到極遠處，例如燈塔；有 時舄要擴政的光，照凴大範圍區域，例如室内照明、搜索燈。 具變焦功能賴明系統可依照需求來調整照明的範圍，使用同 -設備就可形成集中的光束，或是大範圍的照明。因此，可變 焦的照明設計節省了郎與成本，著實具有利用價值與研^ 需要。M326994 Eight, new description: [New technology field] Zoom function. The present invention relates to a lighting device with a prior art that changes the illumination range. In today's general lighting technology, a reflector is used to reflect the light emitted by the light source, perhaps in combination with the refraction of the lens, and finally in a certain form. Required lighting. According to different usage requirements, the design with a small illumination range A is different. 'Sometimes you need to concentrate the light beam and spread the light to a very distant place, such as a lighthouse. Sometimes you want to expand the light of the government, and take care of a wide area. Such as indoor lighting, search lights. With the zoom function, the Laiming system can adjust the range of illumination according to the needs, and use the same device to form a concentrated beam or a wide range of illumination. Therefore, the variable focus lighting design saves lang and cost, and it has the value of use and research.
基於此，Chang在美國專利號侧957提出變焦照明設計， 利用透鏡_移動來達成目的，可細在舞台燈，但是使用透 鏡組的缺點為重1太重，且體積太職大(圖―）。美國專利號 517刚6提出固定的拋物面反光杯’讓光源在光軸方向移動，達 成變焦照明的設計(圖二），齡大部分的㈣斯採肢方法。 然而在光源移_魏過財，_面之雜會使反射光線從 ，軸的另-半邊射出，域光軸間的角度越來越大，即光線將 通離絲*無法縣在巾央，目此照_範獅纽變，但中 央的亮度降低了’祕成空_情形。朗專機69酬中 M326994 • 的設計利用一個反光杯與一個透鏡，因透鏡的移動來改變光線 -· 折射的角度以及反光杯可控制的光量，而達成變焦的效果(圖 三），不過連接透鏡的機構卻會擋住光源發射的光線，因此大大 降低了照明的效率。 【新型内容】 • 本創作之主要目的，是提供一種照明設計，可達成照明調 焦功能，且具有良好的效率，及低製造成本。本創作包含一内 反光杯、一外反光杯、一光源。内反光杯與外反光杯可以為塑 • 膠、金屬或其他可支撐反光面之材料製成。光源可以為led、 白熾燈、螢光燈或其他形式之光源。光源置於内反光杯之光軸 上，外反光杯可套於内反光杯之外部，且外反光杯之光軸與内 反光杯相同。藉由光源及反光杯在光軸上的移動，可調整光線 反射的角度，以及兩個反光杯所控制光的比例，而達成變焦效 果。 内反光杯為具有發散功能的曲面，光由光源所發射，透過 Φ 内反光杯反射射出之後，結合由光源直接射出的光，可形成均 ' 自的照明效果’在匕為泛光。移動光源向前，在内反光面同一位 置上之光線入射角變小，反射角也隨著變小，因而射出的光線 與水平的夾角變小。當光源移動一定距離後，透過内反光杯反 射的光線將大部分水平射出，此為聚光。如此便達成了照明變 焦的效果，並且藉由本創作的特殊設計之反光面，反射後之光 線，在隨光源移動的過程中，光線將不會從光軸的另一半邊射 出，而是在同-半邊且漸趨近水平的角度射出，即光線將聚集 M326994 ^ 在中央，因此整個過程中將不會產生中央空洞的情形；相較於 … 先前技藝中，使用拋物面反光杯之設計而產生之空洞，本創作 具有更優秀之效果。 然而本創作不僅滿足於此變焦效果，期望更提高效率。當 光源向前移動，透過内反光杯反射之光可水平射出，但另一部 分光，即由光源直接射出者，其所佔的比例也隨之增加，此部 分的光形成了更大範圍的泛光，但對於某些使用時機，例如探 照燈’要求盡量聚光’而不需要如此大範圍的泛光。因此提出 > 加入一外反光杯的設計，目的在於反射直接射出的光而使之聚 集。當外反光杯在光軸上向前移動，通過内反光杯邊緣且直接 射出的光，將有越來越多的光打到外反光杯，再透過外反光杯 之特殊形狀，使光若打在此反光面上將會以接近水平的角度射 出。由此可知，當外反光杯向前移動，越多直接射出的光將會 受到外反光杯的反射而變成水平射出，因此泛光照明的範圍逐 漸減小，聚光的情形增加。 > 本創作的優點在於，使用極少的元件而達成高品質的照明 效果，可調整的照明範圍相當大，同時具有均勻、聚集、高效 率的照明效果。並且在實際生產時，不像透鏡的設計需要高成 本的材料費用和成形費用，且需透過研磨、拋光的程序才能達 到良好的透光性，因此本創作在節省成本上具有極大的優勢。 本創作可細在車燈、手電筒、細燈與其他的照明器具等。 【實施方式】 參考第四圖，光源⑴可為LED、白熾燈或其他不同類型的 7 M326994 光源’内反光杯(2)置於光源前方，其具有反光功能的特殊曲面 (201)，例如雙曲面或其他曲面。外反光杯⑶具有反光功能的特 殊曲面(301)，例如雙曲面或其他曲面。外反光杯之小開口大於 内反光杯之最大外徑，因此外反光杯可套於内反光杯。由光源 (1)所發射’光線(4)交曲面(201)於(p)點，在曲面(201)上發生反 射而射出。此時曲面(201)為發散功能，因此光線⑷與其他射向 曲面(201)之光線，被反射後其與水平的夾角皆大於零度。光線 (5)為光源所發射，不受内反光杯(2)反射的光，其與内反光杯(2) 反射之光結合後後，可在前方形成大面積且均勻的照明。 當光源(1)向前移動，如第五圖所示，由光源所發射，光 線⑹交曲面(201)於(P)點，在曲面(2〇1)上發生反射而射出，相對 於圖一’此時由於入射角減小，反射角也跟著減小，因此所有 透過曲面(201)反射的光線與水平之夾角將趨近於零度，即發揮 光集中的效果。光線(7)定義為剛好掠過内反光杯(2)之最外緣， 不受内反光杯(2)反射之光線’因此光線(7)與水平的夾角可定義 最大的光線射出角度。在光源(1)移動之前光線(7)與水平的夾角 為第四圖中標號a，光源(1)移動之後夾角為第五圖中標號^^，且 b大於a,即光直接射出的角度增加，因此最大照明的範圍也增 大了。然而有些場合下，並不需要如此大的照明範圍，例如探 照燈，因此本創作再提出進一步縮小照明範圍且增加效率的設 計。 當外反光杯(3)向前移動，如第六圖所示，外反光杯(3)具有 特殊曲面(301)將光源(1)發射至此的光，透過反射將之射出，且 M326994 • _ 與水平的夾角極小。掠過内反光杯(2)外緣的光線(7)，將受到外 _ 、 反光杯(3)之反射而水平射出，定義光線(8)為剛好掠過外反光杯 ⑶外緣之光線’此時光線⑻與水平之夾角定義最大的光線射出 角度，標號為(：，且(：小於第二圖中標號b。因此，當外反光杯 (3)向前移動’原本直接射出的光線(7)至光線(8)之區間内之光 • 線，將受外反光杯(2)之反射而水平射出，在前方形成聚集之照 〜 明，即收集了邊緣的光而形成集中的光束，縮小了前方的照明 _ 範圍’提南了聚光的效率。 移動外反光杯(3)來收集邊緣射出的光，在光源(1)移動變焦 的過程中皆可發揮作用。如第七圖所示，光源(1)在變焦過程的 任意位置’掠過内光杯(2)的光線(7)，將受到外反光杯(3)之反射 而水平射出，光線(8)為剛好掠過外反光杯(2)外緣之光線。因 此’當外反光杯(3)向前移動，原本直接射出的光線(7)至光線(8) 之區間内之光線，將受到外反光杯(3)之反射而水平射出，在前 _ 方形成聚集之照明。 【圖式簡單說明】 第一圖係習知變焦照明設計 第二圖係習知變焦照明設計 第三圖係習知變焦照明設計 第四圖係本創作之第一剖面圖 第五圖係本創作之第二剖面圖 第六圖係本創作之第三剖面圖 第七圖係本創作之第四剖面圖 9 M326994 【主要元件符號說明】 [習知] 第圖丨7光源；12第一透鏡；5第二透鏡 第二圖28光源；2〇反光杯 第二圖1光源；22透鏡之平面；20透鏡之半球面；28反光杯 [本創作]Based on this, Chang proposed a zoom illumination design on the US Patent No. 957, which uses lens _ movement to achieve the purpose, and can be fine on the stage light, but the disadvantage of using the lens set is that the weight is too heavy and the volume is too large (Fig.). U.S. Patent No. 517 Just 6 proposes a fixed parabolic reflector. The light source is moved in the direction of the optical axis to achieve the design of the zoom illumination (Fig. 2), and most of the (four) s. However, when the light source moves _ Wei Guocai, the _ surface miscellaneous will cause the reflected light to be emitted from the other half of the axis, and the angle between the optical axes of the domain is getting larger and larger, that is, the light will pass through the wire. This photo _ Fan Lion New Change, but the central brightness reduced the 'mystery empty _ situation. Lang Plane 69 paid for M326994 • The design uses a reflector and a lens to change the light due to the movement of the lens - the angle of refraction and the amount of light that can be controlled by the reflector to achieve the zoom effect (Figure 3), but the lens is connected The mechanism will block the light emitted by the light source, thus greatly reducing the efficiency of the lighting. [New Content] • The main purpose of this creation is to provide a lighting design that achieves lighting and focusing functions with good efficiency and low manufacturing costs. The creation includes an inner reflector, an outer reflector, and a light source. The inner and outer reflectors can be made of plastic, metal or other material that supports the reflective surface. The light source can be a led, incandescent, fluorescent or other form of light source. The light source is placed on the optical axis of the inner reflector, and the outer reflector can be placed outside the inner reflector, and the optical axis of the outer reflector is the same as the inner reflector. By moving the light source and the reflector on the optical axis, the angle of the light reflection and the ratio of the light controlled by the two reflectors can be adjusted to achieve the zoom effect. The inner reflector is a curved surface with a diverging function. The light is emitted by the light source, and after being reflected by the Φ inner reflector, combined with the light directly emitted by the light source, the uniform illumination effect can be formed. When the moving light source is forward, the incident angle of the light at the same position on the inner reflecting surface becomes smaller, and the reflection angle also becomes smaller, so that the angle between the emitted light and the horizontal becomes smaller. When the light source moves a certain distance, the light reflected through the inner reflector will be emitted at a large level, which is concentrated. In this way, the effect of the illumination zoom is achieved, and with the specially designed reflective surface of the creation, the reflected light, during the movement with the light source, will not be emitted from the other half of the optical axis, but in the same - Half and gradually near horizontal angles, ie the light will accumulate M326994 ^ in the center, so there will be no central voids in the whole process; compared to... In the previous technique, the design of the parabolic reflector was used. Empty, this creation has a better effect. However, this creation not only satisfies this zoom effect, but also expects to improve efficiency. When the light source moves forward, the light reflected through the inner reflector can be emitted horizontally, but the other part of the light, that is, directly emitted by the light source, also increases its proportion. This part of the light forms a wider range of pans. Light, but for some occasions, such as the searchlight 'requires to concentrate as much as possible' without the need for such a wide range of floodlights. Therefore, it is proposed to add an outer reflector design to reflect the directly emitted light and collect it. When the outer reflector moves forward on the optical axis, the light that passes through the edge of the inner reflector and directly emits light will hit more and more light to the outer reflector, and then through the special shape of the outer reflector, so that if the light is hit On this reflective surface will be emitted at a nearly horizontal angle. It can be seen that when the outer reflector moves forward, the more directly emitted light will be reflected by the outer reflector and become horizontally emitted, so the range of flood illumination gradually decreases, and the concentration of the light increases. > The advantage of this creation is that it achieves high-quality lighting with very few components, and the adjustable illumination range is quite large, with uniform, concentrated, and highly efficient lighting effects. Moreover, in actual production, unlike the design of the lens, high material cost and forming cost are required, and the polishing and polishing process is required to achieve good light transmittance, so the creation has great advantages in cost saving. This creation can be detailed in headlights, flashlights, light lamps and other lighting fixtures. [Embodiment] Referring to the fourth figure, the light source (1) can be an LED, an incandescent lamp or other different types of 7 M326994 light source 'inside reflector (2) placed in front of the light source, and has a special curved surface (201), such as double Surface or other surface. The outer reflector (3) has a special curved surface (301) with a reflective function, such as a hyperboloid or other curved surface. The small opening of the outer reflector is larger than the maximum outer diameter of the inner reflector, so the outer reflector can be placed over the inner reflector. The light (4) emitted by the light source (1) intersects the curved surface (201) at the point (p), and is reflected on the curved surface (201) to be emitted. At this time, the curved surface (201) is a diverging function, so the light (4) and other rays that are directed toward the curved surface (201) are reflected and their angles with the horizontal are greater than zero degrees. The light (5) is emitted by the light source and is not reflected by the inner reflector (2). When combined with the light reflected by the inner reflector (2), it can form a large area and uniform illumination in front. When the light source (1) moves forward, as shown in the fifth figure, it is emitted by the light source, and the light (6) intersects the curved surface (201) at the point (P), and is reflected on the curved surface (2〇1) to be emitted, as shown in the figure. At this time, as the incident angle decreases, the reflection angle also decreases. Therefore, the angle between the light reflected by the curved surface (201) and the horizontal level will approach zero, that is, the effect of light concentration. Light (7) is defined as the light that is just past the outermost edge of the inner reflector (2) and is not reflected by the inner reflector (2). Thus the angle between the light (7) and the horizontal defines the maximum angle of light emission. Before the light source (1) moves, the angle between the light (7) and the horizontal is the number a in the fourth figure. After the light source (1) moves, the angle is the number ^^ in the fifth figure, and b is greater than a, that is, the angle at which the light is directly emitted. Increased, so the range of maximum illumination has also increased. However, in some cases, such a large illumination range, such as a searchlight, is not required, so the design proposes a design that further reduces the illumination range and increases efficiency. When the outer reflector (3) moves forward, as shown in the sixth figure, the outer reflector (3) has a special curved surface (301) that emits light to the light source (1), which is emitted by reflection, and M326994 • _ The angle with the horizontal is extremely small. The light (7) passing over the outer edge of the inner reflector (2) will be reflected horizontally by the reflection of the outer _ and the reflector (3), defining the light (8) as the light that just passes over the outer edge of the outer reflector (3). At this time, the angle between the light (8) and the horizontal defines the maximum angle of light emission, which is (:, and (: is smaller than the number b in the second figure. Therefore, when the outer reflector (3) moves forward, the light that was originally directly emitted ( 7) The light and the line in the interval of the light (8) will be horizontally emitted by the reflection of the outer reflector (2), and a concentrated illumination will be formed in the front, that is, the light of the edge is collected to form a concentrated beam. Reduces the illumination in front _ range' to increase the efficiency of collecting light. Move the outer reflector (3) to collect the light emitted from the edge, which can play a role in the process of moving the zoom of the light source (1). It is shown that the light source (1) passes through the light (7) of the inner light cup (2) at any position of the zooming process, and will be horizontally emitted by the reflection of the outer reflector (3), and the light (8) is just passed over. The light on the outer edge of the reflector (2). So 'when the outer reflector (3) moves forward, the light that was originally emitted directly (7) to the light (8) The light in the interval will be reflected horizontally by the reflection of the outer reflector (3), forming a concentrated illumination in the front _ square. [Simplified illustration] The first picture is the second figure of the conventional zoom illumination design. The third picture of the zoom illumination design is the first view of the zoom illumination design. The fifth picture is the first section of the creation. The fifth picture is the second section of the creation. The sixth picture is the third section of the creation. The fourth section of the creation is shown in Fig. 9 M326994 [Description of main component symbols] [Generally known] Fig. 7 light source; 12 first lens; 5 second lens second Fig. 28 light source; 2 〇 reflective cup second Fig. 1 light source; The plane of the lens; the hemispherical surface of 20 lenses; 28 reflective cups [this creation]
1光源 201内反光杯之特殊曲面 3〇1外反光杯之特殊曲面 5光源直接射出之光線 7剛好掠過内反光杯之光線 9變焦前光線最大射出角度 10光源移動後光線最大射出角度 2内反光杯 3外反光杯 4光源移動前p點反射之光線 6光源移動後P點反射之光線 8剛好掠過外反光杯之光線 11光源與外反光杯皆移動後最大射出角度1Special curved surface of the reflector inside the light source 201 3〇1 Special curved surface of the outer reflector 5 Light source directly emitted by the light source 7 just passing the light of the inner reflector cup 9 before the zoom maximum light exit angle 10 after the light source moves the maximum light exit angle 2 Reflector 3 External Reflector 4 Light source moves before p point reflects light 6 Light source moves P point reflects light 8 just passes over the outer reflector light 11 The maximum exit angle after the light source and the outer reflector are moved