TWI531843B - Light emitting module and backlight module using the same - Google Patents
Light emitting module and backlight module using the same Download PDFInfo
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- TWI531843B TWI531843B TW103111749A TW103111749A TWI531843B TW I531843 B TWI531843 B TW I531843B TW 103111749 A TW103111749 A TW 103111749A TW 103111749 A TW103111749 A TW 103111749A TW I531843 B TWI531843 B TW I531843B
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Description
本發明是有關於一種發光模組,且特別是有關於一種側向出光之發光模組及其背光模組應用。 The invention relates to a light-emitting module, and in particular to a light-emitting module with lateral light-emitting and a backlight module application thereof.
目前的發光模組所使用的元件為點光源,例如發光二極體燈條,然而發光二極體正向出光時,會因為發光二極體的亮度過度集中而產生光苞(hotspot),而兩相鄰之發光二極體燈條之間的區域會因為亮度不均勻而出現光暈(mura)或暗區,影響發光模組的光均勻性以及發光範圍。此外,當燈條之間的間距加長時,會有光強度不足的問題,必須增加更多數量的發光二極體,造成成本過高。因此,傳統的發光模組的缺陷有待改善。 The components used in the current light-emitting module are point light sources, such as light-emitting diode strips. However, when the light-emitting diodes emit light in the forward direction, hotspots are generated due to excessive concentration of the light-emitting diodes. The area between the two adjacent light-emitting diode strips may have a halo or dark area due to uneven brightness, which affects the light uniformity and the range of illumination of the light-emitting module. In addition, when the spacing between the light bars is lengthened, there is a problem that the light intensity is insufficient, and a larger number of light-emitting diodes must be added, resulting in an excessive cost. Therefore, the defects of the conventional light-emitting module need to be improved.
本發明係有關於一種發光模組及其背光模組的應用,其出光方向相對於發光元件的光軸為側向出光。 The invention relates to an application of a light-emitting module and a backlight module thereof, wherein the light-emitting direction is laterally emitted with respect to the optical axis of the light-emitting element.
根據本發明之一方面,提出一種發光模組,包括一電路板、一發光元件以及一長條透鏡。發光元件配置於電路板上,發光元件具有一垂直發光元件且通過一位在發光元件的光源 中心點的光軸。長條透鏡配置於發光元件上方。長條透鏡包括一上表面、一下表面以及二外側表面。上表面及下表面彼此位在長條透鏡相異側,其中上表面包括一彼此對稱且交會於一谷線的第一、第二曲面。下表面包括一可容納發光元件的凹穴,且凹穴表面具有一面向發光元件的入光面。下表面包括一彼此對稱且交會於一稜線的第三、第四曲面,及二內側表面分別延伸自第三、第四曲面之末端,且谷線與稜線的垂直投影彼此重合。此二外側表面位在長條透鏡兩側,分別連接上、下表面,長條透鏡的厚度於二外側表面處具有一最大值,且長條透鏡的厚度於谷線與稜線之間具有一最小值。其中,第一、第二曲面上具有一點P以及一位在與點P相同的曲面且趨近於點P之點P’,點P與光源中心點O的距離定義為RP,點P’與光源中心點O的距離定義為RP’,其中絕對差|RP’-RP|定義為△R,點P與光源中心點O之間的一連線與光軸之間的夾角定義為θP,點P’與光源中心點之間的一連線與光軸之間的夾角定義為θP’,其中絕對差|θP’-θP|定義為△θ,其中發光元件之光線於點P產生全反射時的入射角定義為θR,並滿足下列的方程式:,n為長條透鏡的折射率。 According to an aspect of the invention, a lighting module is provided, comprising a circuit board, a light emitting component and a long lens. The light emitting element is disposed on the circuit board, and the light emitting element has a vertical light emitting element and passes through an optical axis at a center point of the light source of the light emitting element. The elongated lens is disposed above the light emitting element. The elongated lens includes an upper surface, a lower surface, and two outer surfaces. The upper surface and the lower surface are located on opposite sides of the elongated lens, wherein the upper surface includes first and second curved surfaces that are symmetrical to each other and intersect with a valley line. The lower surface includes a recess for receiving the light-emitting element, and the recess surface has a light-incident surface facing the light-emitting element. The lower surface includes a third and fourth curved surface that are symmetrical to each other and intersect with a ridge line, and the two inner side surfaces extend from the ends of the third and fourth curved surfaces, respectively, and the vertical projections of the valley lines and the ridge lines coincide with each other. The two outer side surfaces are located on both sides of the elongated lens, respectively connected to the upper and lower surfaces, the thickness of the elongated lens has a maximum at the two outer side surfaces, and the thickness of the long lens has a minimum between the valley line and the ridge line. value. Wherein, the first and second curved surfaces have a point P and a point P' which is at the same curved surface as the point P and approaches the point P, and the distance between the point P and the center point O of the light source is defined as RP, and the point P' is The distance between the center point O of the light source is defined as RP', where the absolute difference |RP'-RP| is defined as ΔR, and the angle between the line between the point P and the center point O of the light source and the optical axis is defined as θP, The angle between a line connecting P' and the center point of the light source and the optical axis is defined as θP', where the absolute difference |θP'-θP| is defined as Δθ, where the light of the light-emitting element is totally reflected at point P. The angle of incidence is defined as θR and satisfies the following equation: , n is the refractive index of the elongated lens.
根據本發明之一方面,提出一種背光模組,包括:一燈箱;至少一上述之發光模組,呈條狀排列,並配置於燈箱中;以及一擴散板,覆蓋上述之發光模組。 According to an aspect of the present invention, a backlight module includes: a light box; at least one of the above-mentioned light emitting modules arranged in a strip shape and disposed in the light box; and a diffusing plate covering the light emitting module.
為了對本發明之上述及其他方面有更佳的瞭解,下文特舉較佳實施例,並配合所附圖式,於後詳細說明。 In order to provide a better understanding of the above and other aspects of the present invention, the preferred embodiments of the present invention will be described in detail below.
100‧‧‧發光模組 100‧‧‧Lighting module
101‧‧‧背光模組 101‧‧‧Backlight module
110‧‧‧電路板 110‧‧‧Circuit board
120‧‧‧發光元件 120‧‧‧Lighting elements
130‧‧‧長條透鏡 130‧‧‧Large lens
130a‧‧‧上表面 130a‧‧‧ upper surface
130b‧‧‧下表面 130b‧‧‧ lower surface
131‧‧‧第一曲面 131‧‧‧First surface
132‧‧‧第二曲面 132‧‧‧Second surface
133‧‧‧第三曲面 133‧‧‧ Third surface
134‧‧‧第四曲面 134‧‧‧fourth surface
135‧‧‧外側表面 135‧‧‧ outside surface
136‧‧‧內側表面 136‧‧‧ inside surface
140‧‧‧燈箱 140‧‧‧Lightbox
150‧‧‧擴散板 150‧‧‧Diffuser
V‧‧‧谷線 V‧‧‧ Valley
A‧‧‧稜線 A‧‧‧ ridgeline
C‧‧‧凹穴 C‧‧‧ recess
L‧‧‧光軸 L‧‧‧ optical axis
O‧‧‧光源中心點 O‧‧‧Light source center point
S1、S2‧‧‧左右兩側 S1, S2‧‧‧ left and right sides
P、P’、P1~P6‧‧‧點 P, P’, P1~P6‧‧ points
θR、θP、θP’、θS、△R、△θ、θ1、θ2‧‧‧角度 θR, θP, θP', θS, ΔR, Δθ, θ1, θ2‧‧‧ angle
T‧‧‧切線 T‧‧‧ tangent
RP、RP’、△R‧‧‧距離 RP, RP', △R‧‧‧ distance
θ’‧‧‧餘角 ’’‧‧‧ 角角
S‧‧‧全反射臨界點 S‧‧‧ total reflection critical point
W1、W2‧‧‧水平寬度 W1, W2‧‧‧ horizontal width
H1、H2、h1、h2‧‧‧垂直高度 H1, H2, h1, h2‧‧‧ vertical height
第1A及1B圖繪示依照本發明一實施例之發光模組的立體圖及側視圖。 1A and 1B are a perspective view and a side view of a light emitting module according to an embodiment of the invention.
第2圖繪示由光源中心點發出之光線產生全反射時第一曲面的曲率設計。 Figure 2 is a diagram showing the curvature design of the first curved surface when the light emitted from the center point of the light source is totally reflected.
第3圖繪示長條透鏡的尺寸示意圖。 Figure 3 is a schematic view showing the dimensions of the elongated lens.
第4圖繪示第三曲面的曲率設計。 Figure 4 shows the curvature design of the third curved surface.
第5圖繪示依照本發明一實施例之背光模組的元件分解圖。 FIG. 5 is an exploded view of a backlight module according to an embodiment of the invention.
第6圖繪示發光模組的光分佈圖。 Figure 6 is a diagram showing the light distribution of the light-emitting module.
以下係提出實施例進行詳細說明,實施例僅用以作為範例說明,並非用以限縮本發明欲保護之範圍。 The embodiments are described in detail below, and the embodiments are only intended to be illustrative and not intended to limit the scope of the invention.
請參照第1A及1B圖,其繪示依照本發明一實施例之發光模組100的立體圖及側視圖。發光模組100包括一電路板110、一發光元件120以及一長條透鏡130。發光元件120配置於電路板110上。長條透鏡130配置於發光元件120上方,用以導引發光元件120發出的光線往長條透鏡130的左右兩側S1、S2出光。在一實施例中,發光元件120可由複數個發光二極體沿著長條透鏡130的長軸方向排列而成,以做為一線性發光源。然而,在另一實施例中,發光元件120亦可為單一個長條形發光元件, 本發明對此不加以限制。 Please refer to FIGS. 1A and 1B , which are a perspective view and a side view of a light emitting module 100 according to an embodiment of the invention. The light emitting module 100 includes a circuit board 110, a light emitting component 120, and an elongated lens 130. The light emitting element 120 is disposed on the circuit board 110. The elongated lens 130 is disposed above the light emitting element 120 for guiding the light emitted by the light emitting element 120 to the left and right sides S1 and S2 of the elongated lens 130. In one embodiment, the light-emitting element 120 may be formed by arranging a plurality of light-emitting diodes along the long-axis direction of the elongated lens 130 as a linear light-emitting source. However, in another embodiment, the light emitting element 120 can also be a single elongated light emitting element. The invention is not limited thereto.
在第1A及1B圖中,長條透鏡130的上表面130a具有一沿著長軸方向延伸的谷線V。此谷線V由彼此對稱且向內凹陷的二曲面(即第1B圖所示之第一曲面131及第二曲面132)交會而成。此外,長條透鏡130的下表面130b具有一沿著長軸方向延伸的稜線A。此稜線A由彼此對稱且向內隆起的二曲面(即第1B圖所示之第三曲面133及第四曲面134)交會而成。在本實施例中,谷線V與稜線A的垂直投影彼此重合,且長條透鏡130的厚度於谷線V與稜線A之間具有一最小值,以H2表示。 In FIGS. 1A and 1B, the upper surface 130a of the elongated lens 130 has a valley line V extending in the long axis direction. The valley line V is formed by intersecting two curved surfaces that are symmetrical with each other and recessed inward (that is, the first curved surface 131 and the second curved surface 132 shown in FIG. 1B). Further, the lower surface 130b of the elongated lens 130 has a ridge line A extending along the long axis direction. The ridgeline A is formed by two curved surfaces that are symmetrical with each other and bulged inward (i.e., the third curved surface 133 and the fourth curved surface 134 shown in FIG. 1B). In the present embodiment, the vertical projections of the valley line V and the ridge line A coincide with each other, and the thickness of the elongated lens 130 has a minimum value between the valley line V and the ridge line A, denoted by H2.
如第1B圖所示,發光元件120具有一光軸L。此光軸L垂直發光元件120且通過發光元件120的光源中心點O。同時,光軸L也通過長條透鏡130的谷線V與稜線A。 As shown in FIG. 1B, the light-emitting element 120 has an optical axis L. This optical axis L is perpendicular to the light-emitting element 120 and passes through the light source center point O of the light-emitting element 120. At the same time, the optical axis L also passes through the valley line V and the ridge line A of the elongated lens 130.
詳言之,長條透鏡130包括一上表面130a、一下表面130b以及二外側表面135。上表面130a及下表面130b彼此位在長條透鏡130相異側(即上、下兩側),且此二外側表面135位在長條透鏡130兩側(即左、右兩側)。此二外側表面135分別連接上、下表面130b,且長條透鏡130的厚度於此二外側表面135處具有一最大值,以H1表示。 In detail, the elongated lens 130 includes an upper surface 130a, a lower surface 130b, and two outer side surfaces 135. The upper surface 130a and the lower surface 130b are located on opposite sides of the elongated lens 130 (ie, the upper and lower sides), and the two outer side surfaces 135 are located on both sides of the elongated lens 130 (ie, the left and right sides). The two outer side surfaces 135 are respectively connected to the upper and lower surfaces 130b, and the thickness of the elongated lens 130 has a maximum value at the two outer side surfaces 135, denoted by H1.
在一實施例中,此二外側表面135大致上平行於光軸L的軸向延伸。 In an embodiment, the two outer side surfaces 135 extend substantially parallel to the axial direction of the optical axis L.
上表面130a包括彼此對稱且交會於谷線V的第一曲面131及第二曲面132。下表面130b包括一可容納發光元件 120的凹穴C,且此凹穴C表面具有一面向發光元件120的入光面。此外,下表面130b包括彼此對稱且交會於稜線A的第三曲面133及第四曲面134。也就是說,第三曲面133及第四曲面134的頂端交會於凹穴C的頂端。 The upper surface 130a includes a first curved surface 131 and a second curved surface 132 that are symmetrical to each other and intersect the valley line V. The lower surface 130b includes a light-emitting element A recess C of 120, and the surface of the recess C has a light incident surface facing the light emitting element 120. Further, the lower surface 130b includes a third curved surface 133 and a fourth curved surface 134 that are symmetrical to each other and intersect the ridgeline A. That is, the top ends of the third curved surface 133 and the fourth curved surface 134 intersect at the top end of the pocket C.
另外,下表面130b還包括二內側表面136,分別延伸自第三曲面133及第四曲面134的末端。在一實施例中,此二內側表面136大致上平行於光軸L的軸向延伸。 In addition, the lower surface 130b further includes two inner side surfaces 136 extending from the ends of the third curved surface 133 and the fourth curved surface 134, respectively. In an embodiment, the two inner side surfaces 136 extend substantially parallel to the axial direction of the optical axis L.
以下針對長條透鏡130的外觀結構性設計,進一步闡述,以期達到發光模組100具有側向出光的目的。請參照第2~4圖,其中第2圖繪示由光源中心點O發出之光線產生全反射時第一曲面131的曲率設計,第3圖繪示長條透鏡130的尺寸示意圖,第4圖繪示第三曲面133的曲率設計。在下列圖中,由於長條透鏡130為左右對稱的結構,僅示意長條透鏡130的右半側,左半側與右半側的結構相對稱,因此不再贅述。 The structural design of the appearance of the elongated lens 130 is further described below in order to achieve the purpose of the lateral light output of the light-emitting module 100. Please refer to FIGS. 2~4, wherein FIG. 2 is a view showing the curvature design of the first curved surface 131 when the light emitted from the center point O of the light source is totally reflected, and FIG. 3 is a schematic view showing the size of the elongated lens 130, FIG. The curvature design of the third curved surface 133 is illustrated. In the following figures, since the elongated lens 130 is a bilaterally symmetrical structure, only the right half of the elongated lens 130 is illustrated, and the structures of the left half and the right half are symmetrical, and therefore will not be described again.
請參照第2圖,第一曲面131上具有一點P以及一位在與點P相同的曲面且趨近於點P之點P’,點P與光源中心點O的距離定義為RP,點P’與光源中心點O的距離定義為RP’,其中絕對差|RP’-RP|定義為△R,點P與光源中心點O之間的一連線與光軸L之間的夾角定義為θP,點P’與光源中心點O之間的一連線與光軸L之間的夾角定義為θP’,其中絕對差|θP’-θP|定義為△θ。在本實施例中,發光元件120之光線於點P產生全反射時的入射角定義為θR,並滿足下列的方程式(1): ,n為長條透鏡130的折射 率。 Referring to FIG. 2, the first curved surface 131 has a point P and a point P' which is on the same curved surface as the point P and approaches the point P. The distance between the point P and the center point O of the light source is defined as RP, point P. 'The distance from the center point O of the light source is defined as RP', where the absolute difference |RP'-RP| is defined as ΔR, and the angle between the line between the point P and the center point O of the light source and the optical axis L is defined as θP, the angle between a line between the point P' and the center point O of the light source and the optical axis L is defined as θP', where the absolute difference |θP'-θP| is defined as Δθ. In the present embodiment, the incident angle when the light of the light-emitting element 120 is totally reflected at the point P is defined as θR, and satisfies the following equation (1): , n is the refractive index of the elongated lens 130.
長條透鏡130的折射率例如介於1.45~1.6之間。 The refractive index of the elongated lens 130 is, for example, between 1.45 and 1.6.
在上述方程式(1)中,由第2圖可知,(i)入射角θR與餘角θ’的總和為90度,且(ii)通過P點之切線T與P點至P”點的線段之間的一夾角為θS,此夾角θS與餘角θ’的總和亦為90度。由上述(i)和(ii)之關係及利用三角形PP’P”的正切函數求角度θS,可推知入射角 In the above equation (1), as can be seen from Fig. 2, (i) the sum of the incident angle θR and the complementary angle θ' is 90 degrees, and (ii) the line passing through the tangent T of the point P and the point P to the point P" The angle between them is θS, and the sum of the angle θS and the residual angle θ' is also 90 degrees. It can be inferred from the relationship between (i) and (ii) above and the tangent function of the triangle PP'P". Incident angle
另外,在上述方程式(1)中,利用反射定律推導出發生全反射時的臨界角θc如下:n*sinθc=n2*sinθt,其中折射角θt等於90度時,入射角θR等於發生全反射時的臨界角θc。因此,只要入射角θR大於臨界角θc,光線會發生全反射。將n2=1及θt=90度代入上式,可得知 臨界角 Further, in the above equation (1), the critical angle θc at which total reflection occurs is derived using the law of reflection as follows: n *sin θ c = n 2*sin θt , where the incident angle θR is equal to the angle of refraction θt equal to 90 degrees The critical angle θc at which total reflection occurs. Therefore, as long as the incident angle θR is larger than the critical angle θc, the light is totally reflected. Substituting n2=1 and θt=90 degrees into the above equation, the critical angle can be known.
因此,綜合上述的式(2)及式(3),可得到上述方程式(1)。 Therefore, by integrating the above formulas (2) and (3), the above equation (1) can be obtained.
接著,請參照第3圖,長條透鏡130的尺寸設計如下:H1表示長條透鏡130的出射曲線(第一曲面131)的極大高 度;H2表示長條透鏡130的出射曲線(第一曲面131)的極小高度;W1表示長條透鏡130的出射曲線(第一曲面131)的極大寬度;W2表示長條透鏡130的入射曲線(第三曲面133)的極大寬度;h2表示長條透鏡130的入射曲線(第三曲面133)的極大高度;h1表示長條透鏡130的入射曲線(第三曲面133)的極小高度。 Next, referring to FIG. 3, the size of the elongated lens 130 is designed as follows: H1 represents the maximum height of the exit curve (first curved surface 131) of the elongated lens 130. H2 represents the minimum height of the exit curve (first curved surface 131) of the elongated lens 130; W1 represents the maximum width of the exit curve (first curved surface 131) of the elongated lens 130; W2 represents the incident curve of the elongated lens 130 ( The maximum width of the third curved surface 133); h2 represents the maximum height of the incident curve (third curved surface 133) of the elongated lens 130; h1 represents the minimum height of the incident curve (third curved surface 133) of the elongated lens 130.
在第3圖中,長條透鏡130於二外側表面135處的垂直高度(點P5至點P6的垂直距離)定義為H1,谷線V與光源中心點O之間的垂直高度(點P4至中心點O的垂直距離)定義為H2,其中H1/H2的比值較佳介於2.2~2.9之間。 In FIG. 3, the vertical height of the elongated lens 130 at the two outer side surfaces 135 (the vertical distance from the point P5 to the point P6) is defined as H1, the vertical height between the valley line V and the center point O of the light source (point P4 to The vertical distance of the center point O is defined as H2, and the ratio of H1/H2 is preferably between 2.2 and 2.9.
長條透鏡130於此二外側表面135之間的水平寬度(點P4至點P5的水平距離W1的兩倍)定義為2W1,且長條透鏡130於此二內側表面136之間的水平寬度(點P3至點P2的水平距離W2的兩倍)定義為2W2,其中W1/W2的比值較佳介於3.6~4.4之間。 The horizontal width of the elongated lens 130 between the two outer side surfaces 135 (twice the horizontal distance W1 of the point P4 to the point P5) is defined as 2W1, and the horizontal width of the elongated lens 130 between the two inner side surfaces 136 ( The horizontal distance W2 from point P3 to point P2 is defined as 2W2, and the ratio of W1/W2 is preferably between 3.6 and 4.4.
稜線A距光源中心點O的垂直高度(點P3至光源中心點O的距離)定義為h2,且內側表面136的垂直高度(點 P2至點P1的距離)定義為h1,其中h2/h1的比值較佳介於1.4~2.1之間。 The vertical height of the ridge line A from the center point O of the light source (the distance from the point P3 to the center point O of the light source) is defined as h2, and the vertical height of the inner side surface 136 (point The distance from P2 to point P1 is defined as h1, and the ratio of h2/h1 is preferably between 1.4 and 2.1.
在第3圖中,光線L1可由入射曲線(點P3至點P2)入射至長條透鏡130內,再經由第一曲面131全反射至外側表面135,並射出於長條透鏡130之外。此外,光線L2可由內側表面136(點P2至點P1)入射至長條透鏡130內,再經由外側表面135射出於長條透鏡130之外。 In FIG. 3, the light ray L1 is incident into the elongated lens 130 from the incident curve (point P3 to point P2), is totally reflected to the outer side surface 135 via the first curved surface 131, and is emitted outside the elongated lens 130. Further, the light ray L2 may be incident into the elongated lens 130 from the inner side surface 136 (point P2 to point P1) and out of the elongated lens 130 via the outer side surface 135.
接著,請參照第4圖,第三曲面133的曲率設計滿足下列方程式(4):y=-0.531x 5+1.958x 4-2.072x 3+0.329x 2-0.057x+h2 Next, referring to Fig. 4, the curvature of the third curved surface 133 is designed to satisfy the following equation (4): y = -0.531 x 5 +1.958 x 4 -2.072 x 3 +0.329 x 2 -0.057 x +h2
其中,y為位在第三曲面133上一座標點與該光源中心點O之間的垂直距離,x為第三曲面133上此座標點與該光源中心點O之間的水平距離,h2為長條透鏡130的入射曲線(第三曲面133)在x=0時的垂直高度。 Where y is the vertical distance between a punctuation point on the third curved surface 133 and the center point O of the light source, and x is the horizontal distance between the coordinate point of the third curved surface 133 and the center point O of the light source, and h2 is long. The incident curve of the strip lens 130 (the third curved surface 133) has a vertical height at x=0.
在一實施例中,第三曲面133具有一全反射臨界點S,此全反射臨界點S的垂直高度介於h1及h2之間。此臨界點具有負斜率變化之極大值,也就是說,第三曲面133的曲率變化為:由點P3開始斜率為0,往負斜率增加,直到臨界點S時為負斜率變化之極大值。 In one embodiment, the third curved surface 133 has a total reflection critical point S whose vertical height is between h1 and h2. This critical point has a maximum value of the negative slope change, that is, the curvature of the third curved surface 133 changes to: the slope from the point P3 is 0, and the negative slope increases until the critical point S is the maximum value of the negative slope change.
在一實施例中,全反射臨界點S與光源中心點O之間的一連線(線段O-S)與光軸L之間的夾角θ1較佳介於30~60度之間。此外,第三曲面133與內側表面136交會處具有一交 會點P2,此交會點P2與光源中心點O之間的一連線(線段O-P2)與該光軸L之間的夾角θ2較佳介於30~90度之間。 In one embodiment, the angle θ1 between the line connecting the total reflection critical point S and the center point O of the light source (the line segment O-S) and the optical axis L is preferably between 30 and 60 degrees. In addition, the intersection of the third curved surface 133 and the inner surface 136 has a cross The point P2 is set, and the angle θ2 between the line (the line segment O-P2) between the intersection point P2 and the center point O of the light source and the optical axis L is preferably between 30 and 90 degrees.
請參照第5圖,其繪示依照本發明一實施例之背光模組101的元件分解圖。此背光模組101包括上述實施例之發光模組100(電路板110、發光元件120以及長條透鏡130)、一燈箱140以及一擴散板150。上述之發光模組100配置於燈箱140中,呈條狀排列。此外,擴散板150覆蓋發光模組100。在本實施例中,由於發光模組100為側向發光,其出光面並非朝向擴散板150,因此光線可均勻分佈在燈箱140中,之後,均勻分佈的光線再透過擴散板150射出燈箱140之外。因此,可避免傳統發光模組的出光面朝向擴散板時而容易發生光苞(hot spot)及亮度不均勻分佈的現象。 Please refer to FIG. 5, which is an exploded view of the backlight module 101 according to an embodiment of the invention. The backlight module 101 includes the light emitting module 100 (the circuit board 110, the light emitting element 120, and the elongated lens 130) of the above embodiment, a light box 140, and a diffusion plate 150. The above-described light emitting modules 100 are disposed in the light box 140 and arranged in a strip shape. In addition, the diffusion plate 150 covers the light emitting module 100. In this embodiment, since the light emitting module 100 is laterally illuminated, the light emitting surface thereof is not directed toward the diffusing plate 150, so the light can be uniformly distributed in the light box 140, and then the uniformly distributed light is transmitted through the diffusing plate 150 to the light box 140. outer. Therefore, it is possible to avoid a phenomenon in which hot spots and uneven brightness distribution are likely to occur when the light-emitting surface of the conventional light-emitting module faces the diffusion plate.
此外,請參照第6圖,其為發光模組100的光分佈圖,根據在光軸上(以0度表示)測得的光強度及在垂直光軸方向上(以正負90度表示)測得的光強度,可知上述的發光模組100應用在背光模組101中,因為側向出光的光強度相對大於正向出光的光強度,因此,當兩相鄰之發光模組100間的間距加大時,不會因間距加大而出現暗區的亮度不足的問題,故本實施例之背光模組101可應用數量較少且間距加大的發光模組,以減少背光模組101的成本。 In addition, please refer to FIG. 6 , which is a light distribution diagram of the light-emitting module 100, which is measured according to the light intensity measured on the optical axis (indicated by 0 degree) and in the direction of the vertical optical axis (indicated by plus or minus 90 degrees). The light intensity of the light-emitting module 100 is applied to the backlight module 101 because the light intensity of the lateral light is relatively greater than the light intensity of the forward light. Therefore, when the distance between the two adjacent light-emitting modules 100 is When the size is increased, the brightness of the dark area is not insufficient due to the increased spacing. Therefore, the backlight module 101 of the embodiment can apply a small number of light-emitting modules with increased spacing to reduce the backlight module 101. cost.
本發明上述實施例所揭露之發光模組及其背光模組的應用,因其出光方向相對於發光元件的光軸為側向出光,故可 避免傳統發光模組的出光面朝向擴散板時而容易發生光苞(hot spot)及亮度不均勻分佈的現象,以達到均勻出光的目的。 The application of the light-emitting module and the backlight module thereof disclosed in the above embodiments of the present invention, because the light-emitting direction is laterally emitted relative to the optical axis of the light-emitting element, When the light-emitting surface of the conventional light-emitting module is faced to the diffusing plate, the phenomenon of hot spot and uneven brightness distribution is likely to occur, so as to achieve uniform light output.
綜上所述,雖然本發明已以較佳實施例揭露如上,然其並非用以限定本發明。本發明所屬技術領域中具有通常知識者,在不脫離本發明之精神和範圍內,當可作各種之更動與潤飾。因此,本發明之保護範圍當視後附之申請專利範圍所界定者為準。 In conclusion, the present invention has been disclosed in the above preferred embodiments, and is not intended to limit the present invention. A person skilled in the art can make various changes and modifications without departing from the spirit and scope of the invention. Therefore, the scope of the invention is defined by the scope of the appended claims.
100‧‧‧發光模組 100‧‧‧Lighting module
110‧‧‧電路板 110‧‧‧Circuit board
120‧‧‧發光元件 120‧‧‧Lighting elements
130‧‧‧長條透鏡 130‧‧‧Large lens
S1、S2‧‧‧左右兩側 S1, S2‧‧‧ left and right sides
V‧‧‧谷線 V‧‧‧ Valley
Claims (10)
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