TW432143B - Modified construction method for interior wall form - Google Patents

Modified construction method for interior wall form Download PDF

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Publication number
TW432143B
TW432143B TW88107320A TW88107320A TW432143B TW 432143 B TW432143 B TW 432143B TW 88107320 A TW88107320 A TW 88107320A TW 88107320 A TW88107320 A TW 88107320A TW 432143 B TW432143 B TW 432143B
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TW
Taiwan
Prior art keywords
light
incident surface
grid structures
light incident
area
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TW88107320A
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Chinese (zh)
Inventor
Ming-Jr Chen
Original Assignee
Chen Ming Jr
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Priority to TW88107320A priority Critical patent/TW432143B/en
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Publication of TW432143B publication Critical patent/TW432143B/en

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Abstract

The modified construction method for interior wall form of this invention includes the following procedures: (1) to prepare multiple end boards with least one lean surface and one fix part on each end board; (2) to fix multiple end boards onto two end sides of one of the walls which are next to the target interior wall, and let lean surfaces of the multiple end board parallel to the target interior wall surfaces to make a reference level for form construction; (3) to connect and position one of the ends of multiple forms onto the lean surfaces of the multiple end boards to layout the interior form; (4) then to complete form construction by fixing forms.

Description

M432143 TW M432143U1M432143 TW M432143U1

1 · · ·本體 10 · · ·入光面 100 · · ·第一發散點 12 · · ·出光面 14 · · ·光學曲面 140 · · ·多區域反射 結構 1401 · · ·網格結構 2···中央軸心線 第1圖 五 、新型說明: 【新型所屬之技術領域】 本創作係屬於發先- 叱一極體透鏡領域,特別是指 一種將中央集中之弁 寸⑺疋^ 避免直視時產生亮區之 域反町 之發先二極體透鏡改良結構。 【先前技術】1 · · · Body 10 · · · Light entrance surface 100 · · · First divergence point 12 · · · Light exit surface 14 · · · Optical curved surface 140 · · · Multi-area reflective structure 1401 · · · Grid structure 2 · · · Central axis line Figure 1 V. Description of the new type: [Technical field to which the new type belongs] This creation belongs to the field of 先-polar lens, especially refers to a kind of 弁 inch that concentrates the center ⑺ 疋 Avoid to look directly Improved structure of the first diode lens in the field of anti-machi that produces bright areas. [Prior art]

按’發光二極體作A 股作為先源已然成為照明產業 發展趨勢,而將發井-权触 呆 —阁 先—極體之點光源轉換成為較大 範圍而均勻之出光,目丨丨失 _ 、J為發二極體照明發展之重 研究方向。將發光二極體與透鏡結合是一種可提古 照明效率且能有效轉換出光效果的方法,利用光: 折射、反射之基本原理,將發光二極體高功率之點 光源出光轉變成為柔和而均勾 J < ,,、'叨。—般使 發光二極體透鏡,大多可分成杯形、或半球體 形式’光線從發光二極體發射後’經過兩次 透鏡發射而出。杯形之發光二極體透鏡,係: 體側邊之全反射效應,使得光線往上方聚集形 勻之照明範圍,而半球體之發光二 句 U組遇鏡,則系 利用球體曲率造成光線折射效果,使得光線朝上’、 聚集’亦得到均勻之照明範圍。 方 此些設計雖能有效改變發光二極體之出光 光線能夠均勻照設於固定範圍之照明區域,伸== 去避免中心區域較明亮而越外圈越昭 ··'、 ,、、、π效果, M432143 使得人眼直視仍可辨識出下方之發光二極體光源。 除此之外’杯體側面曲面以及半球體曲面多為平滑 設計’但造成在同樣的視角下人眼直視時,僅有一 固定區域之光線照射該視角方向而造成視覺上之亮 塊出現。此等缺失使得現有之發光二極體透鏡雖能 提供均勻之出光及照明,但仍無法使得發光二極體 成為人眼可直視之照明燈具。請參考美國公告號 US201 1/01 57898A1之專利,係提供一種改變出光方 向使得光線涵蓋360度出光方向之透鏡,以及台灣 公告號1 262604之專利,係提供一種將出光導向側 面或背面之透鏡。此兩種透鏡之設計皆能將中央出 光之光線導向側面或是其它角度,而產生均勻散光 之光學效果,由於其入光面與光線行徑方向皆近乎 垂直’故往正面方向之光源近無改變方向仍然直射 至出光面,方經過出光面之折射而改變方向,但由 於入光角度會影響產生拼糾μ θ 王斫射與反射之光量,故其光 學效果仍受到極大之侷限。 、 柯喂。此外,該等設計仍無法 改善肉眼直視時,同—鉬β α 視角所見透鏡提供之光線仍 為一亮區及其它暗區。 是故,有鑑於上述 &缺失’本創作係提供一種能According to the 'light-emitting diodes' A-shares as the first source has become the development trend of the lighting industry, and the hair well-right touch-Gexian-polar point light source is converted into a large range and uniform light, eyes _ And J are the major research directions for the development of diode lighting. Combining a light-emitting diode with a lens is a method that can improve the efficiency of ancient lighting and effectively convert the light effect. Using the basic principles of light: refraction and reflection, the light from the high-power point light source of the light-emitting diode is transformed into a soft and uniform light. Check J < ,,, '叨. Generally, most of the light-emitting diode lenses can be divided into a cup shape or a hemispherical form. 'Light is emitted from the light-emitting diode' and emitted through the lens twice. The cup-shaped light-emitting diode lens is: the total reflection effect on the side of the body, which makes the light gather upward to form a uniform illumination range, while the light-emitting two-line U group of the hemisphere meets the mirror, the light is refracted by the curvature of the sphere The effect is that the light is directed upward, and the light is gathered to obtain a uniform illumination range. Although these designs can effectively change the light output of the light-emitting diodes, they can evenly illuminate the lighting area in a fixed range, and extend == to avoid the center area is brighter and the outer circle is more visible ... ', ,,,, π Effect, M432143 enables the human eye to directly recognize the light emitting diode light source below. In addition, 'the side surface of the cup and the surface of the hemisphere are mostly smooth designs', but when the human eye is looking directly at the same angle of view, only a fixed area of light illuminates the direction of the angle of view, causing visually bright blocks to appear. These defects make the existing light-emitting diode lens capable of providing uniform light output and illumination, but still cannot make the light-emitting diode into a lighting fixture that can be directly seen by human eyes. Please refer to U.S. Bulletin No. US201 1/01 57898A1, which provides a lens that changes the direction of light output so that the light covers the 360-degree light output direction, and Taiwan Bulletin No. 1 262604, which provides a lens that guides light to the side or back. The design of these two lenses can direct the light from the central light to the side or other angles to produce an optical effect of uniform astigmatism. Because the light incident surface and the direction of the light path are nearly vertical, the light source in the front direction is almost unchanged. The direction is still straight to the light-emitting surface, and the direction is changed by the refraction of the light-emitting surface. However, because the angle of incident light will affect the amount of light that is emitted and reflected by the μ θ king, the optical effect is still greatly limited. Ke feed. In addition, these designs are still unable to improve the direct vision of the naked eye, the light provided by the lens at the same view angle of molybdenum β α is still a bright area and other dark areas. That ’s why, in light of the above &

有效避免光線集中於中奂F 一 为&域,以及人眼直視時造 成亮區之發光二極體透鐘 兄改良結構,使得燈具提供 使用時肉眼直視時光線更 不尺加舒適均勻。 4 M432143 【新型内容】 本創作之主要目的,旨在提供一種壁面光線集 中於中央而照度均勻,且人眼直視時避免產生亮區 之發光二極體透鏡改良結構。 為達上述目的,本創作之發光二極體透鏡改良 結構,供以與一發光二極體光源結合以改善出光效 果’該發光二極體透鏡改良結構具有一本體,係為 截頂圓錐狀體並以一中央軸心線呈現軸對稱,該本 體之錐頂凹設形成有一入光面,該本體之錐底形成 有一出光面,該本體之側壁則形成有一光學曲面, 該發光二極體透鏡改良結構,其特徵在於:該本體 之該入光面係收束成形於一第一發散點,且該第一 發散點係位於該中央軸心線位置,又該光學曲面上 係形成一多區域反射結構,據以將從入光面進入該 本體之光線均勻分佈由該出光面射出,以避免整片 之亮區造成視覺效果上之不平均,該多區域反射結 構係為複數個網格結構,且各該網格結構之側剖面 為直線或平滑曲線,邊框則分別呈四邊形或六邊 形。而為了加強反射之功效,該發光二極體透鏡改 良結構更包含一反射層.,係設於該本體外側並僅包 覆該光學曲面及該等網格結構。 為了加強分散中央區域光線之效果,該出光面 係收束成形於一第二發散點’且該第二發散點係位 於該中央軸心線位置而相對該第一發散點位置設 5 置’使得光線分佈更加平均。 而為使該發光二極體透鏡改良結構便於使用, 其更包含至少一安裝構件’設於該本體之錐頂、錐 底' 或兩者兼具。 為前述之目的’本創作亦提供一種發光二極體 透鏡改良結構’供以與一發光二極體光源結合以改 善出光效果,該發光二極體透鏡改良結構具有一本 體’係為截頂圓錐狀體並以一中央軸心線呈現軸對 稱’該本體之錐頂凹設形成有一入光面,該本體之 錐底形成有一出光面’該本體之側壁則形成有一光 學曲面’該發光二極體透鏡改良結構,其特徵在於: 該本體之該出光面係收束成形於一第二發散點,且 該第二發散點係位於該中央轴心線位置,又該光學 曲面上係形成一多區域反射結構’據以將從入光面 進入該本體之光線均勻分佈由該出光面射出,以避 免整片之売區造成視覺效果上之不平均,該多區域 反射結構係為複數個網格結構,且各該網格結構之 側剖面為直線或平滑曲線。而為了加強反射之功 效’該發光二極體透鏡改良結構更包含一反射層, 係設於該本體外側並僅包覆該光學曲面及該等網格 結構。 為達前述目的,本創作更提供一種發光二極體 透鏡改良結構’供以與一發光二極體光源結合以改 善出光效果,該發光二極體透鏡改良結構具有一本 6 狀:並"央……對 錐底形成有一出:°又:成有-入光面,該本體之 學曲面,节發朵 本體之側壁則形成有-光 該光學曲面上=體透㈣良結構,其特徵在於: 形成一多區域反射結構,據以將從 /入該本體之光線均勻分佈由該出光面射 =避免整片之亮區造成視覺效果上之不平均, 二夕£域反射結構係為複數個網格結構,且各該網 結構之側剖面為直線或平滑曲線,邊框則分別呈 四邊形。而為了加強反射之功效,該發光二極體透 文良、。構更包含_反射層,係設於該本體外側並 僅包覆該光學曲面及該等網格結構。 透過上述之設計,可將中央區域直射之光線經 由入光面而折射往不同角度’而有效避免光線集中 於中央區$,使得點光源之發光二極體經由透鏡轉 換後,變成均勻之照度分佈。同時該多區域反射結 構能將光線分散由不同區域之結構反射至同一視 角,避免人眼直視時因為平滑之反光區域產生整片 之亮區而不舒適,進而使得燈具提供使用時肉眼直 視時光線更加舒適均勻。. 【實施方式】 為使貴審查委員能清楚了解本創作之内容,謹 以下列說明搭配圖式,敬請參閱。Effectively avoiding the concentration of light in the mid-F-field, and the light-emitting diode transparent clock that creates a bright area when the human eye is looking directly. The improved structure makes the lamp more comfortable and even when the light is directly looking at the naked eye. 4 M432143 [New content] The main purpose of this creation is to provide an improved structure of a light-emitting diode lens with wall light concentrated in the center and uniform illumination, and avoiding bright areas when the human eye is looking directly. In order to achieve the above purpose, the light-emitting diode lens improved structure of this creation is provided to be combined with a light-emitting diode light source to improve the light output effect. The light-emitting diode lens improved structure has a body, which is a truncated cone. A central axis line is used to present the axis symmetry. The cone top of the body is concavely formed with a light incident surface. The light cone of the body is formed with a light emitting surface. The side wall of the body is formed with an optical curved surface. The light-emitting diode lens The improved structure is characterized in that the light incident surface of the body is formed at a first divergence point, and the first divergence point is located at the central axis line position, and a multi-region is formed on the optical curved surface Reflective structure, according to which the light entering the body from the light incident surface is evenly distributed and emitted from the light emitting surface to avoid unevenness in visual effects caused by the bright area of the whole piece. The multi-region reflective structure is a plurality of grid structures Each side of the grid structure is a straight line or a smooth curve, and the frame is a quadrangle or a hexagon, respectively. In order to enhance the effect of reflection, the improved structure of the light-emitting diode lens further includes a reflective layer, which is disposed outside the body and only covers the optical curved surface and the grid structures. In order to enhance the effect of dispersing the light in the central area, the light emitting surface is converged and formed at a second divergence point, and the second divergence point is located at the central axis line position and is set to 5 relative to the first divergence point position so that The light distribution is more even. In order to make the improved structure of the light-emitting diode lens easy to use, the light-emitting diode lens further includes at least one mounting member 'cone top, cone bottom' or both. For the foregoing purpose, 'this creation also provides a light-emitting diode lens improved structure' for combining with a light-emitting diode light source to improve the light output effect. The light-emitting diode lens improved structure has a body 'is a truncated cone The shape of the body is axisymmetric with a central axis line. The cone top of the body is concavely formed with a light incident surface. The light cone of the body is formed with a light emitting surface. The side wall of the body is formed with an optical curved surface. The light emitting diode The improved body lens structure is characterized in that: the light emitting surface of the body is formed at a second divergence point, and the second divergence point is located at the central axis line position, and a plurality of optical surfaces are formed on the optical curved surface. The area reflection structure is based on the uniform distribution of the light that enters the body from the light entrance surface and is emitted from the light exit surface to avoid the unevenness of the visual effect caused by the whole area of the entire area. The multi-area reflection structure is a plurality of grids. Structure, and the side section of each grid structure is a straight line or a smooth curve. In order to enhance the effect of reflection, the improved structure of the light-emitting diode lens further includes a reflective layer, which is disposed outside the body and only covers the optical curved surface and the grid structures. In order to achieve the foregoing object, the present invention further provides an improved structure of a light-emitting diode lens for combining with a light-emitting diode light source to improve the light output effect. The improved structure of the light-emitting diode lens has a shape of 6: and " The central part of the cone is formed with an output: ° and: Chengyou-light-entering surface, the body's academic surface, and the side wall of the nodular body is formed with -light on the optical surface = body through a good structure, its characteristics The reason is: forming a multi-area reflective structure, according to which the light from / into the body is evenly distributed from the light emitting surface = to avoid unevenness in visual effects caused by the bright area of the entire film, and the domain reflective structure is plural Grid structure, and the side profile of each grid structure is a straight line or a smooth curve, and the frame is a quadrangle. In order to enhance the effect of reflection, the light emitting diode is transparent. The structure further includes a reflective layer, which is disposed outside the body and only covers the optical curved surface and the grid structures. Through the above design, the direct rays of light in the central area can be refracted to different angles through the light incident surface, thereby effectively preventing the light from being concentrated in the central area. . At the same time, the multi-area reflective structure can reflect light from different areas of the structure to the same angle of view, avoiding the uncomfortable appearance of the entire bright area caused by the smooth reflective area when the human eye is directly looking, thereby making the lamp provide the light when the human eye is looking directly More comfortable and even. [Implementation] In order for your review committee to understand the content of this creation clearly, I would like to refer to the following descriptions and drawings.

Claims (1)

M432143 接佈設裏該本體1之錐底,使得該等網格結構ΐ4〇ι 之邊緣形成從該本體1之錐頂延伸至錐底之轄射 線,及以該中央軸心線2為圓心之複數個同心圓交 又而成之大小漸增之方格,且該等網格結構14〇1中 之側剖面為直線或平滑曲線,以提供不同之光線反 射效果。 請參閲第2a〜2d圖,係為本創作第一實施例之 不同態樣之剖面圖。如圖中所示,該等網格結構ΐ4〇ι 之側剖面為朝外凸出之平滑曲線,彼此相連而形成 整體為波浪狀之該多區域反射結構14〇。該入光面 10之曲率及外觀係與該光學曲面14互相搭配輔 助,以提供最佳之照明效果,由於光之性質,由光 疏之介質進入光密之介質時,不會發生全反射現 象,故於此端進行設計能軚為有效而容易提升折射 光線之效果,而不會因為光線反射而增加光學設計 上之複雜度。以直射進入透鏡之光線路徑討論之, 如2a圖所示,該入光面1〇之斜率變化使得直射進 入該本體1.之光線在該入光面1〇中央區域產生大角 度之偏折,而在該入光.面1〇邊緣區域則產生較小角 度之偏折,因而使得照射到該光學曲面14之光量提 升如2b圖所不,該入光面10之斜率固定使得直 射進入該本體1之光線均勻朝向固定角度產生偏 折L較2a圖中之中央區域之光線偏折角度較小,對 於亮度較低之光源可避免該入光面1〇中央區域光 9 線過度發散而造成暗區。 ZC圖所不,該入光面 1 0係以兩段不同之斜率所 ^ ^ 傅风〒央區域之光線偏 折角度較2b圖中更小,而々k 丨> , 而外側之光線偏折角度則較 大’使得該入光面10中本F Y夹區域直射光線之折射效果 較輕微而邊緣區域之折射齡或 _ 外耵1乂為明顯。此外如2d圖所 示’該入光面1 0係以—段田— 丰又固疋斜率以及一段曲面所 形成’使得進入該本體1 之光線折射產生局部性更 加細微之變化,使得光學寺罢 T兀子效果更加精緻。除了上述 之實施樣態,該入光面10之形狀以及光學設計更可 細分成多段曲率、或者是各部分產生高低'凹凸之 局部結構’增加或是降低光之折射效果,搭配該光 學曲面14之設計以達成最佳之照明功效以及視覺 感受。 請一併參閱第3a ' 3b圖,係為本創作多區域反 射結構之兩種示意圖。如圖中所示,該多區域反射 結構140係為複數個網格結構14〇1 ’各該網格結構 1401之側剖面均為平滑之曲面,如第圖所示, 該等網格結構1401之側剖面係為朝外凸出之平滑 曲面,由於每個該等網格結構14〇1皆有相似之曲 面,故當肉眼在與該出光面12垂直方向正視該出光 面1 2時’光線分別由該等網格結構14 〇 1之一邊反 射至同一視角,如圖中「」之光線示意。故在人 眼'上並非呈現整片之亮面,而是分別置於該等網格 結構1401 —部份之小亮面。應注意的是,由於該等 10M432143 is connected to the cone bottom of the body 1 in the arrangement, so that the edges of the grid structures ΐ400m form a ray extending from the cone top of the body 1 to the bottom of the cone, and the central axis line 2 is a plurality of circles. Concentric circles intersect gradually increasing squares, and the side sections of the grid structures 1401 are straight or smooth curves to provide different light reflection effects. Please refer to Figs. 2a to 2d, which are sectional views of different aspects of the first embodiment of the present invention. As shown in the figure, the side sections of the grid structures 40m are smooth curves that project outward, and are connected to each other to form the multi-area reflective structure 14 that is wavy as a whole. The curvature and appearance of the light incident surface 10 are matched with the optical curved surface 14 to provide the best lighting effect. Due to the nature of light, when a light-sparse medium enters a light-dense medium, total reflection will not occur. Therefore, designing at this end can be effective and easily improve the effect of refracting light without increasing the complexity of optical design due to light reflection. As discussed in the light path of direct light entering the lens, as shown in Figure 2a, the change in the slope of the light incident surface 10 causes the light entering the body 1 to produce a large-angle deflection in the central area of the light incident surface 10. In the edge area of the light incident surface 10, a smaller angle deflection occurs, so that the amount of light shining on the optical curved surface 14 is increased as shown in FIG. 2b. The slope of the light incident surface 10 is fixed so that direct light enters the body. The light of 1 is deflected evenly toward a fixed angle. L is smaller than the light deflection of the central area in 2a. For light sources with lower brightness, the light incident surface of the central area can be avoided. Area. The ZC chart does not show that the light incident surface 10 is at two different slopes ^ ^ The angle of deflection of the light in the Fu Fengyang central area is smaller than in 2b, and 々k 丨 > The angle of refraction is relatively large ', so that the refraction effect of the direct rays of the FY clip region in the light incident surface 10 is slight, and the refraction age of the edge region or outer diameter 1 is obvious. In addition, as shown in Figure 2d, 'the light incident surface 10 is formed by-Duan Tian-Feng You solid slope and a curved surface', which makes the refraction of the light entering the body 1 produce local more subtle changes, making the optical temple Wuzi effect is more refined. In addition to the above-mentioned implementation, the shape and optical design of the light incident surface 10 can be further subdivided into multiple curvatures, or the local structure of the unevenness of each part increases or decreases the refraction effect of light, with the optical curved surface 14 Designed to achieve the best lighting effect and visual experience. Please also refer to Figures 3a '3b, which are two schematic diagrams of the multi-region reflective structure of this creation. As shown in the figure, the multi-area reflective structure 140 is a plurality of grid structures 1401. The side sections of the grid structures 1401 are all smooth curved surfaces. As shown in the figure, the grid structures 1401 The side profile is a smooth curved surface protruding outward. Since each of these grid structures 1401 has similar curved surfaces, when the naked eye faces the light emitting surface 12 perpendicularly to the light emitting surface 12, the light One side of these grid structures 14 01 is reflected to the same perspective, as shown by the light rays "" in the figure. Therefore, the human eye 'does not show the bright surface of the whole piece, but is placed on the small bright surfaces of these grid structures 1401-parts. It should be noted that since these 10
TW88107320A 1999-05-05 1999-05-05 Modified construction method for interior wall form TW432143B (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112270025A (en) * 2020-09-30 2021-01-26 晟通科技集团有限公司 Template combination design method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112270025A (en) * 2020-09-30 2021-01-26 晟通科技集团有限公司 Template combination design method

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