CN201310816Y - Planar Fresnel LED optical lens and LED assembly consisting same - Google Patents

Abstract

The utility model relates to a planar Fresnel LED optical lens which is adapted to orderly arraying LED assemblies comprising LED chips, adhesive layers and optical lenses from a light source side to an image side along a central axis. In each optical lens, the image side optical surface is a planar Fresnel optical surface, and a ring surface of the Fresnel optical surface is formed by transferring a light concentrating curved surface and is provided with vertical ring teeth so that the light ray emitted by a light emitting diode chip passes through the adhesive layer and the optical lens and then forms a light shape with an oval-shaped illumination angle. The optical lens satisfies the following conditions: Fs/rn is larger than or equal to 0.7 and is smaller than or equal to 2.2, and the product of the multiplication of Nd2-1 and fs is larger than or equal to 0.1 and is smaller than or equal to 1.25, wherein fs is the effective focus of the optical lens, rn is the last ring radius of the Fresnel optical surface, d2 is the thickness of a central axis optical lens, and Nd2 is the reflection rate of the optical lens. The simple use of the optical lens can concentrate the light ray emitted by the LED so as to form a predetermined light shape and meets the requirement that the luminous flux ratio is greater than 85 percent. The planar Fresnel LED optical lens can be used for illumination, cell phone flashlight or camera flashlight.

Description

Plane Fresnel LED optical mirror slip and the LED assembly that is constituted thereof

Technical field

The utility model is relevant a kind of light bar led optical mirror slip and the light-emitting diode component that constituted thereof, especially refer to that a kind of luminous intensity (peak intensity) that produces is oval Fresnel optical mirror slip according to angle light type (Elliptic angulardistribution pattern), supply is used for the light-emitting diode component of mat LED light emitting source with generation light type, and can be applicable to the flash lamp of LED illumination, mobile phone or camera.

Background technology

Light emitting diode (light emitting diode is called for short LED) has low-voltage, low power consumption, long advantage of life-span, has been widely used in display unit (indicator), lighting device fields such as (illuminator).But light color is simple because LED has more, the miniaturization planar package, has used on the flash lamp of mobile phone camera.Yet because the light that led chip sends has the characteristic of spot light, brightness irregularities, existing researcher carries out multinomial research for the gathering of light, as dwindles outside chip, the raising luminous efficiency, and using optical mirror slip also is important techniques exploitation direction.

In the design of LED optical mirror slip, can be divided into an optical mirror slip (primary optical lens) and secondary optics eyeglass (secondary optical lens); An optical mirror slip is the lens that directly encapsulate on led chip, generally to assemble (concentrate) light; The secondary optics eyeglass is for using at single or number LEDs array (Array), based on dispersed light beam.On an existing optics design, be to use the non-spherical lens of symmetry as ES2157829; Japan Patent JP3032069, JP2002-111068, JP2005-203499, U.S. Pat 2006/187653, Chinese patent CN101013193 etc. is to use spherical lens; JP2002-221658 uses spherical lens etc. to Bulk type LED.In the utilization for high-order, an optical mirror slip is except that wanting the energy collected light, more can be in the specific light type (distribution pattern) of luminous intensity (peak intensity) generation uniformly, special light types such as wide-angle, low-angle, circle, ellipse for example, use with the collocation led array, to produce best optical effect.The utilization of an optical mirror slip is covered with lens 23 on led chip 21 shown in Figure 1A, 1B, when led chip 21 emits beam, via sending predetermined light type light after lens 23 gatherings, or on optical mirror slip, add one deck secondary optics eyeglass, in the hope of the effect of homogenising.This optical mirror slip has various design, and wherein optical mirror slip adopts the optical surface of Fresnel (Fresnel) formula, on prior art, as Deutsche Bundespatent WO/2003/083943; Japan Patent JP2005-049367 etc.; U.S. Pat 6,726,859, publication number US2007/0275344, US2008/0158854; European patent EP 1091167; And Taiwan patent TW200711186 etc.; Yet above-mentioned prior art mainly is to be covered in that several LED go up or for being the secondary optics eyeglass (secondary lens) of grenade instrumentation (projector) usefulness with Fresnel formula eyeglass.But with the fast development of LED luminous efficacy, the utilization of single LEDs is day by day important.The light source that led array or plurality of LEDs are formed can be thoroughly compensated and is become uniform light by crosslights scioptics to each other; But single LEDs is on lens design, and the light source of forming far beyond led array or plurality of LEDs be complicated, the light gathering efficiency that must an optical mirror slip of consideration (primary lens) and the homogenising of luminous intensity; Be to use the Fresnel lenses on single face or two sides to be positioned over LED illuminator top as Japan Patent JP2005-257953, U.S. Pat 2006/0027828, to produce uniform light, as Figure 1A, 1B; Patent TW560085 in Taiwan utilizes parabolic bowl-type side and Fresnel Lenses to reduce beam divergence and to constitute the uniform light type of light beam for another example; And for example Korean Patent 1020070096368 is made optical mirror slip of LED with Taiwan patent I261654 with Fresnel formula eyeglass, but its light type shines the angle based on circle, for the single LEDs assembly of the ellipse with practical application, still be difficult to the expansion utilization according to angle light type.

Progress along with science and technology, electronic product constantly develops towards compact and multi-functional direction, and in the electronic product as: digital camera (Digital Still Camera), camera computer (PC camera), network cameras (Network camera), mobile phone (mobile phone) etc. have possessed outside the camera lens, even personal digital assistance devices such as (PDA) also has the demand that adds camera lens; Therefore the LED flash lamp or the illuminating LED light fixture that are used for this series products, Chang Yidan or plurality of LEDs assembly composition array; And for easy to carry and meet the demand of hommization, LED flash lamp or illuminating LED light fixture not only need suitable luminous flux, arrange in pairs or groups mutually with the type LED assembly of not sharing the same light, and also need smaller volume and lower cost simultaneously.Fresnel Lenses is provided with one group of irregular Fresnel ring (Fresnel zone plate) at lens surface, its ring spacing becomes big (ring spacing (pitch) change) from inside to outside or from outside to inside gradually, because Fresnel Lenses is except having leaded light and the ability of collecting light, also have light, thin, plasticization and characteristic cheaply concurrently, be well suited for the system that is used for throwing light on; But use for the LED illumination that multiple spot is luminous, then will consider the uniformity of illumination and luminous intensity.On prior art, normal a certain proportion of ring spacing (zone pitch) and the ring spacing that encircles the degree of depth (zone height) or gradual change and the ring degree of depth of adopting, especially the illuminator that constitutes with plurality of LEDs can meet illumination and the uniform practical requirement of luminous intensity then with the ring spacing method of gradual change; But, then to arrange in pairs or groups mutually with the optical characteristics of optical mirror slip for optical mirror slip of single LED.Though Fresnel Lenses has complicated external form surface, and manufacturing cost is higher, and the good light efficient and the effect of homogenising are arranged, use with the illumination of single LEDs assembly especially and more noted.For the light that single LEDs is sent reaches peak efficiency, the utility model is promptly under this active demand, utilize Fresnel Lenses to make optical mirror slip to produce specific elliptical light type and to use the LED assembly of formation, under suitable formation of the present utility model, can be assembled and be produced even luminous intensity (peak intensity) and oval-shaped smooth type to the light that led chip sent of surface light emitting.

Summary of the invention

The utility model main purpose is to be the light-emitting diode component that a kind of plane Fresnel light emitting diode (LED) light eyeglass is provided and constituted,, can be assembled and be produced even luminous intensity (peak intensity) and oval-shaped smooth type to the light that led chip sent of surface light emitting.

This LED assembly is to emit beam by a led chip (LED die), one Fresnel optical mirror slip forms the ellipse-shaped light type with collected light and with even luminous intensity, and adhesive layer (seal gel layer) is constituted to clog between Fresnel optical mirror slip and led chip, wherein, the Fresnel optical mirror slip can be the formed eyeglass of optical material of a plano-concave (plano-concave) tool tapering or zero draft, its concave surface is to the light source-side optical face of light source and can be sphere or aspheric surface, its plane for to as side as the side optical surface and have Fresnel formula optical surface, the optically focused curved surface of this Fresnel optical surface can be aspheric surface or sphere again, its anchor ring be perpendicular rings tooth (draft with vertical shape) and the ring degree of depth (equal zone height) such as can be or etc. ring spacing (equalzone pitch), and can meet the following conditions:

$0.7\≤\frac{f_s}{r_n}\≤2.2---\left(1\right)$

$0.1\≤(N_{d2}-1)\frac{d_2}{f_s}\≤1.25---\left(2\right)$

$\sqrt{{\left(\frac{{\mathrm{\φ}}_x-{\mathrm{\ω}}_x}{\mathrm{\π}}\right)}^2+{\left(\frac{{\mathrm{\φ}}_y-{\mathrm{\ω}}_y}{\mathrm{\π}}\right)}^2}\·f_g\≤0.6---\left(3\right)$

Wherein:

$f_g=|(\frac{1}{R_1}-\frac{1}{R_F})\·f_s|---\left(4\right)$

${\mathrm{\&omega;}}_x={\tan }^{-1}\left(\frac{D}{\mathrm{<figure-callout\; id="0"\; label="d"\; filenames="Y20082013316700412.png,Y20082013316700421.png"\; state="\{\{state\}\}">d</figure-callout>}0+\mathrm{<figure-callout\; id="1"\; label="d"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">d</figure-callout>}1+\mathrm{<figure-callout\; id="2"\; label="d"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">d</figure-callout>}2+\mathrm{Lx}}\right)---\left(5\right)$

${\mathrm{\&omega;}}_y={\tan }^{-1}\left(\frac{D}{\mathrm{<figure-callout\; id="0"\; label="d"\; filenames="Y20082013316700412.png,Y20082013316700421.png"\; state="\{\{state\}\}">d</figure-callout>}0+\mathrm{<figure-callout\; id="1"\; label="d"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">d</figure-callout>}1+\mathrm{<figure-callout\; id="2"\; label="d"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">d</figure-callout>}2+\mathrm{Ly}}\right)---\left(6\right)$

Wherein, f _sBe the length of the effective focal length (effective focal length) of this optical mirror slip, r _nBe the most last ring (Last Zone) radius of Fresnel optical surface R2, d ₂Be central shaft optical mirror slip thickness, N _D2Be the refractive index of optical mirror slip, 2 φ _xFor penetrating light via optical mirror slip at the half (I of highlight strength (intensity) of directions X _1/2) locate angle (degree, deg.), 2 φ _yFor penetrating light via optical mirror slip at the half (I of highlight strength of Y direction _1/2) locate angle (degree, deg.), 2Lx is the length of led chip at directions X, 2Ly is the length of led chip in the Y direction, f _gBe the length of the suitable focal length (relative focal length) of this optical mirror slip, R ₁Be the radius of curvature of light source-side optical face, R _FBe the radius of curvature (radius of fresnel convex surface) of the optically focused curved surface of picture side Fresnel optical surface, d ₀Be led chip thickness, d ₁Be the adhesive layer thickness of central shaft, D is the radius of optical mirror slip at picture side optical surface.

Further, in response to type angle and the optically focused characteristic of not sharing the same light, the radius of curvature R of the optically focused curved surface of this Fresnel optical surface _FCan be made as sphere or aspheric surface.

Make for simplifying, the Fresnel optical mirror slip is replaceable to be the made eyeglass of optical material on a plane (plano-plano), its to as side be Fresnel formula optical surface as side side optical surface, and can satisfy formula (1)～formula (3) condition.

Be to increase the efficient of LED assembly, the Fresnel optical mirror slip is replaceable to be the made eyeglass of optical material of a tool tapering υ, its to as side be Fresnel formula optical surface as the side optical surface, and can satisfy formula (1)～formula (3) condition.

Another purpose of the utility model is selected conveniently for using, and optical mirror slip can be optical glass or the optics plastic cement is made.

The utility model also provides a kind of light-emitting diode component, it is to comprise as plano-concave described in the utility model or a two flat Fresnel light emitting diode (LED) light eyeglass and a light-emitting diode chip for backlight unit, it is characterized in that this light-emitting diode component has the requirement greater than 85% (η=beta/alpha 〉=85%) of elliptical light type, its luminous flux ratio η, and meet the following conditions:

E _1/2≤0.7E _d (7)

Wherein,

${\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}=\frac{I_{1/2}}{(\mathrm{\&pi;}{r}_n*\sin {\mathrm{\&phi;}}_x)*(r_n*\sin {\mathrm{\&phi;}}_y)}*\mathrm{\&eta;}---\left(8\right)$

Wherein, r _nBe the most last ring (Last Zone) radius of Fresnel optical surface R2,2 φ _xFor penetrating light via optical mirror slip at the half (I of highlight strength (intensity) of directions X _1/2) angle (degree deg.) located, 2 φ _yFor penetrating light via optical mirror slip at the half (I of highlight strength of Y direction _1/2) angle (degree deg.) located, r _nBe the most last ring (Last Zone) radius of Fresnel optical surface R2, α is the luminous flux that led chip emits beam, and β is the relative unlimited distance of picture side (100 times of f _s) not considering the luminous flux of the light of AF, η is luminous flux ratio η=beta/alpha, E _dBe the illumination (Incidance) that led chip sends, E _1/2The illumination at half place of highlight strength that sends for the Fresnel optical mirror slip.

By this, plane of the present utility model Fresnel light emitting diode (LED) light eyeglass and the light-emitting diode component that is constituted thereof can have the ellipse-shaped light type, and meet luminous flux ratio greater than 85% requirement, and this optical mirror slip has the characteristic of thin thickness, can be used for single LEDs or array LED, provide the flash lamp that gives illumination or mobile phone, camera to use.

Description of drawings

Figure 1A, 1B have the use LED optical mirror slip of skill now in the schematic diagram of LED assembly;

Fig. 2 is that use zero draft Fresnel LED optical mirror slip of the present utility model is in the schematic perspective view of LED assembly;

Fig. 3 is that use of the present utility model has tapering Fresnel LED optical mirror slip in the schematic perspective view of LED assembly;

Fig. 4 is the Fresnel LED optical mirror slip and the optically focused curvature of curved surface radius relationship figure of the ring spacings such as perpendicular rings tooth of use of the present utility model;

Fig. 5 is the Fresnel LED optical mirror slip and the optically focused curvature of curved surface radius relationship figure of ring such as the perpendicular rings tooth of the use of the present utility model degree of depth;

Fig. 6 is the formation schematic diagram of LED optical mirror slip of the present utility model in the LED assembly;

Fig. 7 is the tapering presentation graphs that tapering Fresnel LED optical mirror slip is arranged;

Fig. 8 is that Fresnel LED optical mirror slip of the present utility model is in LED assembly light path schematic diagram;

Fig. 9 is Fresnel LED optical mirror slip A group's light of the present utility model and B group's line refraction schematic diagram;

Figure 10 is Fresnel LED optical mirror slip A group's light of the present utility model and B group's linear light road schematic diagram;

Figure 11 is the A group's light of Fig. 9 and Figure 10 and the schematic diagram that B group's line is combined into even luminous intensity;

Figure 12 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of first embodiment of the present utility model;

Figure 13 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of second embodiment of the present utility model;

Figure 14 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 3rd embodiment of the present utility model;

Figure 15 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 4th embodiment of the present utility model;

Figure 16 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 5th embodiment of the present utility model;

Figure 17 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 6th embodiment of the present utility model;

Figure 18 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 7th embodiment of the present utility model;

Figure 19 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 8th embodiment of the present utility model;

Figure 20 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 9th embodiment of the present utility model;

Figure 21 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the tenth embodiment of the present utility model;

Figure 22 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 11 embodiment of the present utility model;

Figure 23 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 12 embodiment of the present utility model; And

Figure 24 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of the 13 embodiment of the present utility model.

Description of reference numerals:

The 10-LED assembly; 11,21-LED chip; 12,22-adhesive layer; 13,23-optical mirror slip; R1-light source-side optical face (optical surface on source side); R ₁Radius of curvature (radiuson optical axis) for R1; R2-is as side optical surface (optical surface on forward side); R ₂Radius of curvature (radius on optical axis) for R2; R _F-as the optically focused curvature of curved surface radius (radius of fresnel convex surface) of side Fresnel optical surface; Led chip thickness on the d0-central shaft (LED die thickness on optical axis); The led chip surface is to the optical surface distance (thickness from die surface to R1 on optical axis) of optical mirror slip light source side on the d1-central shaft; D2-central shaft optical mirror slip thickness (lens thickness on optical axis); r ₁-the first ring radius (first zone radius); r _n-the most last ring radius (last zone radius); r _t-ring spacing (zone pitch); h _d-ring the degree of depth (zone height); N _d-refractive index (Refractive index); v _d-Abbe number (Abbe number); E _dThe illumination that-led chip sends (Incidance); E _1/2The illumination (Incidance) at half place of highlight strength that-Fresnel optical mirror slip sends; The luminous flux that α-led chip emits beam (Flux); β-as the luminous flux (Flux) of the relative unlimited distance light of side.

The specific embodiment

For making the utility model clear and definite more full and accurate, enumerate preferred embodiment now and cooperate following graphicly, structure of the present utility model and technical characterictic are described in detail as the back:

With reference to shown in Figure 6, it is the structural representation of plane of the present utility model Fresnel light emitting diode (LED) light eyeglass and the light-emitting diode component 10 that constituted thereof, it is arranged by light source along central shaft Z: led chip 11, adhesive layer 12 and optical mirror slip 13, after light is sent by led chip 11, via adhesive layer 12, the light beam that light-ray condensing is also formed the ellipse-shaped light type that is symmetrical in central shaft Z by optical mirror slip 13 is to the irradiation of picture side; Optical mirror slip 13 is the made lens of an optical material, its concave surface is the light source-side optical face R1 to light source, and optical surface R1 can be aspheric surface or sphere, its opposite face for to as the Fresnel optical surface R2 of side for having the Fresnel optical surface of perpendicular rings tooth (draft with vertical shape); The optical surface R2 of optical mirror slip 13, optical mirror slip thickness d ₂Reach the condition that satisfies formula (1) and formula (2) between effective focal length length, angle 2 ψ (directions X 2 φ of the light type that optical mirror slip 13 formed luminous intensities form _xWith Y direction 2 φ _y) satisfy the condition of formula (3).

Wherein, adhesive layer 12 does not limit the material of use, optical resin (resin) commonly used or silica gel different materials such as (silicon gel) on the LED assembly; And optical mirror slip 13 can be made by optical glass or optics plastic material.

As shown in Figure 2, be to use flat (plano-plano) Fresnel LED optical mirror slip of a pair of in the schematic diagram of a LED assembly, it is arranged by light source along central shaft Z: a led chip 11, an adhesive layer 12 and the flat Fresnel optical mirror slip 13 of a pair of, wherein optical mirror slip 13 is at the optical surface R1 of light source side, and it is that the plane (is its radius of curvature R ₁=∞), its another plane (opposite face) is for being the Fresnel optical surface with perpendicular rings tooth to the Fresnel optical surface R2 as side.The optical surface R2 of this optical mirror slip 13, optical mirror slip thickness d ₂Reach the condition that satisfies formula (1) and formula (2) between effective focal length length, angle 2 ψ (directions X 2 φ of the light type that optical mirror slip 13 formed luminous intensities form _xWith Y direction 2 φ _y) satisfy the condition of formula (3).

Again as shown in Figure 3, it is another form of the present utility model, be to use a Fresnel optical mirror slip in the schematic diagram of a LED assembly 20, it is arranged by light source to as side being in regular turn along central shaft Z: a led chip 21, an adhesive layer 22 and the flat Fresnel optical mirror slip 23 of a pair of, wherein Fresnel optical mirror slip 23 be have a tapering v optical mirror slip as shown in Figure 7.After light is sent by led chip 21, behind adhesive layer 22, by optical mirror slip 23 with light-ray condensing and to form to be symmetrical in central shaft Z and to take the angle be that the light beam of ellipse-shaped light type shines the picture side; By having the Fresnel optical mirror slip 23 of tapering v, can reduce light by the side dissipation of optical mirror slip 23, raise the efficiency.The optical surface R2 of this optical mirror slip 23, optical mirror slip thickness d ₂Reach the condition that satisfies formula (1) and formula (2) between effective focal length length, angle 2 ψ (directions X 2 φ of the light type that optical mirror slip 23 formed luminous intensities form _xWith Y direction 2 φ _y) satisfy the condition of formula (3).

For optical mirror slip 13 or optical mirror slip 23, it is the Fresnel optical surface as side optical surface R2.The utility model use as side optical surface R2 for Fresnel optical surface with perpendicular rings tooth (draft with vertical shape) shown in Fig. 4,5, wherein, this Fresnel optical surface (R2) as side is by an optically focused curved surface (R _F) shift to form, and the Fresnel optical surface that can form first-class ring spacing (equal zone pitch) according to different branch modes respectively as shown in Figure 4 or the Fresnel optical surface of the first-class ring degree of depth (equal zone height) as shown in Figure 5; With reference to figure 4, be the Fresnel optical surface that waits ring spacing (equal zone pitch), just ring spacing (zone pitch) r as side optical surface R2 _tBe fixed value, it is at optically focused curvature of curved surface radius R _FOptically focused curved surface (RF) go up ring spacing (zone pitch) r to equate _tBut the drop that waits (central shaft Z point is a peak) not, the ring degree of depth that does not just wait (zone height) h _d, optically focused curved surface (RF) is translated into the ring-type Fresnel optical surface (as side optical surface R2) of equidistant ring, just by outside its ring degree of depth (zone height) h of central shaft Z _dGradually greatly as shown in Figure 4; Each ring (zone) of ring-type Fresnel optical surface (as side optical surface R2) is to be made of an inclined-plane (slope) and a vertical anchor ring (vertical draft) again, and its first ring radius is r ₁, the most last ring is r for radius _nWhen light is incident in Fresnel optical surface (R2), by the inclined-plane of each ring, incident ray is produced refraction, and the light effect of reaching similar parabolic curved surface (or optically focused curved surface) as shown in Figure 9.With reference to figure 5, be for waiting the Fresnel optical surface of the ring degree of depth (equal zone height), just encircling degree of depth h again as side optical surface R2 _dBe fixed value, it is at optically focused curvature of curved surface radius R _FOptically focused curved surface (RF) go up drop (central shaft Z point is a peak) to equate, just the ring degree of depth of Xiang Denging (zone height) h _d, but the ring spacing that does not wait (zone pitch) r _t, with ring-type Fresnel optical surface (as side optical surface R2) the ring-type Fresnel optical surface of the ring degree of depth (equal zone height) such as optically focused curved surface RF translates into, just by outside its ring spacing (zone pitch) r of central shaft Z _tGradually little as shown in Figure 5, its first the ring radius be r ₁In like manner,,, incident ray is produced refraction, and the light effect of reaching similar parabolic curved surface (or optically focused curved surface) as shown in Figure 9 by each interannular inclined-plane when light is incident in the Fresnel optical surface.

With reference to figure 9, Figure 10 and shown in Figure 11, after A group's light (A1, A2 and A3) reflected via the Fresnel optical surface, because A1, its incident angle difference of A2 or A3, its shooting angle ψ angle position on object was different from Figure 10 again; For after the outgoing with the radial position of central shaft, A group's light will present the stronger light group of luminous intensity at center; In like manner, after B group's light (B1, B2 and B3) reflects via the Fresnel optical surface, also will present the stronger light group of luminous intensity at center; Via after the combination of A group and B group's light as shown in figure 11, produce the light type of luminous intensity homogeneous, use avoid or reduce that center intensity is strong excessively, marginal zone light a little less than, even a circle that produces between secretly exposing encloses phenomenon.

The optical surface R1 of optical mirror slip 13 or the optical surface R1 of optical mirror slip 23, if constituted with the aspherics face, its aspheric equation (Aspherical Surface Formula) is formula (9)

$Z=\frac{{\mathrm{<figure-callout\; id="2"\; label="ch"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">ch</figure-callout>}}^2}{1+\sqrt{(1-(1+K)c^2{h}^2)}}+A_4{h}^4+A_6{h}^6+A_8{h}^8+A_{10}{h}^{10}---\left(9\right)$

Wherein, c is a curvature, and h is the eyeglass height, and K is circular cone coefficient (Conic Constant), A ₄, A ₆, A ₈, A ₁₀The asphericity coefficient (Nth Order Aspherical Coefficient) on difference four, six, eight, ten rank.

The optically focused curvature of curved surface radius R of Fresnel optical surface _FAlso with formula (9) definition, for paraboloidal optically focused curvature of curved surface radius R _FCircular cone COEFFICIENT K=-1, for the optically focused curvature of curved surface radius R of sphere _FCircular cone COEFFICIENT K=0.

See also Fig. 8, be the light path schematic diagram of the utility model LED optical mirror slip in the LED assembly, among the figure, led chip 11 (21) emits beam, and is back with 2 ψ angles (directions X 2 φ via optical mirror slip 13 (23) gatherings and refraction _xWith Y direction 2 φ _y) form the requirement of needed elliptical light type and beta/alpha 〉=85%, wherein, α is the luminous flux that led chip emits beam, β is the relative unlimited distance of picture side (100 times of f _s) luminous flux of light, and ignore the refraction (refraction) and scattering effects such as (scattering) of air, and meet the condition of formula (7).Mat said structure, the utility model utilize a plano-concave or a two flat Fresnel light emitting diode (LED) light eyeglass and a led chip, can make LED assembly 10 can send the ellipse-shaped light type of predetermined even luminous intensity, can be single and use or form array with the type of not sharing the same light and use.

The following most preferred embodiment that is disclosed of the utility model, be at the main composition element of the utility model reality and explain, be explanation and the application scenarios that compares each embodiment, the chip of 1.85x0.77mm size is used in employing with led chip 11, its wavelength is that maximum intensity (lst peak wave-length) wavelength is that 450nm and time high strength (2nd peak wave-length) wavelength are the chip of the blue light of 550nm, at directions X angle of departure ω _x=39.8 °, Y direction angle of departure ω _y=35.2 °, the blue light of α=78.5 lumens (1m), illumination Ed=23.97 Lux (Lux); It is explanation that optical mirror slip 13 (or optical mirror slip 23) uses diameter 5mm (D=2.5mm); The Fresnel optical surface selects to have waiting ring spacing or waiting the Fresnel optical surface that encircles the degree of depth of perpendicular rings tooth; Adhesive layer 12 is to utilize refractive index N _D1Transparent optical silica gel by 1.491 is clogged.But with regard to the LED assembly that generally has optical mirror slip and constituted, except optical mirror slip and LED assembly thereof that the utility model disclosed, other structures are the technology of General Notifications, just form, ring spacing and the ring degree of depth etc. of the size of each composed component of this optical mirror slip and LED assembly thereof, use material, LED wavelength and emission angle, Fresnel optical surface are to carry out many changes, modification even equivalence change.

Below in first to the 7th embodiment be to use have zero draft and etc. the light-emitting diode component that constituted of the plane Fresnel optical mirror slip of the ring degree of depth, the the 8th to the 9th embodiment be to use tapering and etc. the light-emitting diode component that constituted of the plane Fresnel optical mirror slip of the ring degree of depth, the the tenth to the 11 embodiment be to use zero draft and etc. the light-emitting diode component that constituted of the plane Fresnel optical mirror slip of ring spacing, the the 12 to the 13 embodiment be to use zero draft and etc. the light-emitting diode component that constituted of the planoconcave Fresnel optical mirror slip of the ring degree of depth.

＜the first embodiment 〉

Please refer to Fig. 6 and shown in Figure 12, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of first embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation () by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R (mm) or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F(mm), tapering υ, each refractive index (N of spacing di (mm) (the on-axis surface spacing), optical mirror slip 13 _d) etc.Present embodiment be to use have zero draft and etc. the Fresnel optical mirror slip made of the flat glass material of the ring degree of depth, be the plane in the R1 of Fig. 6 optical surface.

Table (one)

^*Aspherical?Zone?Fesnel

In table (), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (two) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, the Fresnel ring degree of depth (zone height) h _dAnd Fresnel number of rings amount (No.of zone):

Table (two)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 68 ° of directions Xs, 30 ° in Y direction according to the angle, in β=69.201 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.8815

I _1/2＝33.5

φ _x＝32.5

φ _y＝15.2

$\frac{f_s}{r_n}=0.8130$

$(N_{d2}-1)\frac{d_2}{f_s}=0.5751$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.2394$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.4489$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 12 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; Wherein, light distribution (illumination) changes (X, the Y direction is with reference to shown in Figure 8) with directions X angle and Y orientation angle difference, and the longitudinal axis is marked with 0,10,20,30.40,50,60 represent illumination (luminous intensity) by 0 (little) to 60 (greatly).Curve " C " is represented illumination (luminous intensity) distribution and the polar coordinates graph of a relation that shines the angle of X-axis (with reference to figure 8), and the illumination (luminous intensity) that curve " D " is represented as Y-axis (with reference to figure 8) distributes and the polar coordinates graph of a relation that shines the angle.Reference axis and the implication of curve in figure of following Figure 13 in Figure 24 is identical with Figure 12, also be illumination (luminous intensity) distribution and the polar coordinates graph of a relation that shines the angle that curve " C " is represented X-axis (with reference to figure 8), the illumination (luminous intensity) that curve " D " is represented as Y-axis (with reference to figure 8) distributes and the polar coordinates graph of a relation that shines the angle.Be illustrated in the lump at this, and repeat no more below.By above-mentioned table (), table (two) and shown in Figure 12, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the second embodiment 〉

Please refer to Fig. 6 and shown in Figure 13, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (three) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have zero draft and etc. the Fresnel optical mirror slip made of the flat glass material of the ring degree of depth, be the plane in the R1 of Fig. 6 optical surface.

Table (three)

^*Aspherical?Zone?Fesnel

In table (three), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (four) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring degree of depth h _dAnd Fresnel number of rings amount:

Table (four)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 68 ° of directions Xs, 33 ° in Y direction according to the angle, in β=70.245 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.8948

I _1/2＝32.5

φ _x＝33.7

φ _y＝16.8

$\frac{f_s}{r_n}=1.0203$

$(N_{d2}-1)\frac{d_2}{f_s}=1.1410$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.1319$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.3915$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 13 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (three), table (four) and shown in Figure 13, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the three embodiment 〉

Please refer to Fig. 6 and shown in Figure 14, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (five) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have zero draft and etc. the Fresnel optical mirror slip made of the flat glass material of the ring degree of depth, be the plane in the R1 of Fig. 6 optical surface.

Table (five)

^*Aspherical?Zone?Fesnel

In table (five), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (six) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring degree of depth h _dAnd Fresnel number of rings amount:

Table (six)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 64 ° of directions Xs, 36 ° in Y direction according to the angle, in β=69.816 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.8893

I _1/2＝30.0

φ _x＝32.1

φ _y＝18.1

$\frac{f_s}{r_n}=1.0081$

$(N_{d2}-1)\frac{d_2}{f_s}=0.4601$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.2108$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.3406$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 14 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (five), table (six) and shown in Figure 14, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the four embodiment 〉

Please refer to Fig. 6 and shown in Figure 15, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (seven) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have zero draft and etc. the Fresnel optical mirror slip made of plane plastic cement PMMA (polymethyl methacrylate) material of the ring degree of depth, be the plane in the R1 of Fig. 6 optical surface.

Table (seven)

^*Aspherical?Zone?Fesnel

In table (seven), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (eight) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring degree of depth h _dAnd Fresnel number of rings amount:

Table (eight)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.491, Abbe number v _D2Be that 32 PMMA plastic cement material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 68 ° of directions Xs, 43 ° in Y direction according to the angle, in β=72.48 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.9233

I _1/2＝23.5

φ _x＝34.0

φ _y＝21.5

$\frac{f_s}{r_n}=1.0081$

$(N_{d2}-1)\frac{d_2}{f_s}=0.3881$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.1672$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.2231$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 15 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (seven), table (eight) and shown in Figure 15, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the five embodiment 〉

Please refer to Fig. 6 and shown in Figure 16, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (nine) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have zero draft and etc. the plane Fresnel optical mirror slip of ring spacing, the radius of curvature R of its Fresnel optical mirror slip _FBeing sphere, is the plane in the R1 of Fig. 6 optical surface.

Table (nine)

^*Spherical?Zone?Fesnel

In table (nine), optical surface (Surf.No.) has the Fresnel optical surface of mark * person for sphere.Following tabulation (ten) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring spacing r _tAnd Fresnel number of rings amount:

Table (ten)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 68 ° of directions Xs, 43 ° in Y direction according to the angle, in β=72.48 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.8980

I _1/2＝22.5

φ _x＝43.0

φ _y＝34.5

$\frac{f_s}{r_n}=2.0243$

$(N_{d2}-1)\frac{d_2}{f_s}=0.2300$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.4536$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.1111$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 16 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (nine), table (ten) and shown in Figure 16, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the six embodiment 〉

Please refer to Fig. 6 and shown in Figure 17, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (11) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have zero draft and etc. the Fresnel optical mirror slip made of the flat glass material of the ring degree of depth, the radius of curvature R of its Fresnel optical mirror slip _FBeing sphere, is the plane in the R1 of Fig. 6 optical surface.

Table (11)

^*Aspherical?Zone?Fesnel

In table (11), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (12) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring degree of depth h _dAnd Fresnel number of rings amount:

Table (12)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 68 ° of directions Xs, 43 ° in Y direction according to the angle, in β=72.48 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.8913

I _1/2＝32.5

φ _x＝31.0

φ _y＝17.0

$\frac{f_s}{r_n}=1.0213$

$(N_{d2}-1)\frac{d_2}{f_s}=1.1401$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.1030$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.4161$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 17 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (11), table (12) and shown in Figure 17, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the seven embodiment 〉

Please refer to Fig. 6 and shown in Figure 180, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (13) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have zero draft and etc. the Fresnel optical mirror slip made of the flat glass material of the ring degree of depth, the radius of curvature R of its Fresnel optical mirror slip _FBeing sphere, is the plane in the R1 of Fig. 6 optical surface.

Table (13)

^*Aspherical?Zone?Fesnel

In table (13), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (14) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring degree of depth h _dAnd Fresnel number of rings amount:

Table (14)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 65 ° of directions Xs, 40 ° in Y direction according to the angle, in β=69.33 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.8832

I _1/2＝27.5

φ _x＝33.7

φ _y＝19.5

$\frac{f_s}{r_n}=1.0146$

$(N_{d2}-1)\frac{d_2}{f_s}=1.1475$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.1252$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.2799$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 18 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (13), table (14) and shown in Figure 180, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the eight embodiment 〉

Please refer to Fig. 6 and shown in Figure 19, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (15) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have tapering and etc. the Fresnel optical mirror slip made of the flat glass material of the ring degree of depth, be the plane in the R1 of Fig. 6 optical surface.

Table (15)

^*Aspherical?Zone?Fesnel

In table (15), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (16) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring degree of depth h _dAnd Fresnel number of rings amount:

Table (16)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 65 ° of directions Xs, 60 ° in Y direction according to the angle, in β=69.588 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.8976

I _1/2＝22.0

φ _x＝37.5

φ _y＝27.0

$\frac{f_s}{r_n}=1.0598$

$(N_{d2}-1)\frac{d_2}{f_s}=0.4601$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.2176$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.3022$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 19 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (15), table (16) and shown in Figure 19, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the nine embodiment 〉

Please refer to Fig. 6 and shown in Figure 20, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (17) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have tapering and etc. the Fresnel optical mirror slip made of the flat glass material of the ring degree of depth, be the plane in the R1 of Fig. 6 optical surface.

Table (17)

^*Aspnerical?Zone?Fesnel

In table (17), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (18) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring degree of depth h _dAnd Fresnel number of rings amount:

Table (18)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 68 ° of directions Xs, 33 ° in Y direction according to the angle, in β=71.267 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.9078

I _1/2＝34.0

φ _x＝33.8

φ _y＝16.8

$\frac{f_s}{r_n}=1.2045$

$(N_{d2}-1)\frac{d_2}{f_s}=0.4601$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.2176$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.4998$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 20 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (17), table (18) and shown in Figure 20, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the ten embodiment 〉

Please refer to Fig. 6 and shown in Figure 21, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (19) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have tapering and etc. the Fresnel optical mirror slip made of the flat glass material of ring spacing, be the plane in the R1 of Fig. 6 optical surface.

Table (19)

^*Aspherical?Zone?Fesnel

In table (19), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (20) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring spacing r _tAnd Fresnel number of rings amount:

Table (20)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 68 ° of directions Xs, 70 ° in Y direction according to the angle, in β=72.056 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.9214

I _1/2＝26.0

φ _x＝40.5

φ _y＝35.0

$\frac{f_s}{r_n}=1.0121$

$(N_{d2}-1)\frac{d_2}{f_s}=0.4601$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.0081$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.1366$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 21 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (19), table (20) and shown in Figure 21, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the ten one embodiment 〉

Please refer to Fig. 6 and shown in Figure 22, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use of the present utility model plane Fresnel optical mirror slip is constituted;

Show respectively in the following tabulation (21) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have tapering and etc. the Fresnel optical mirror slip made of the flat glass material of ring spacing, be the plane in the R1 of Fig. 6 optical surface.

Table (21)

^*Aspherical?Zone?Fesnel

In table (21), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (22) is Fresnel optical surface radius curve R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring spacing r _tAnd Fresnel number of rings amount:

Table (22)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 60 ° of directions Xs, 80 ° in Y direction according to the angle, in β=72.164 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.9192

I _1/2＝30.0

φ _x＝39.4

φ _y＝30

$\frac{f_s}{r_n}=1.0121$

$(N_{d2}-1)\frac{d_2}{f_s}=0.4601$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.1147$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.2184$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 22 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (21), table (22) and shown in Figure 22, the light-emitting diode component schematic diagram that provable by this plane of the present utility model Fresnel optical mirror slip is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the ten two embodiment 〉

Please refer to Fig. 6 and shown in Figure 23, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use planoconcave Fresnel optical mirror slip of the present utility model is constituted;

Show respectively in the following tabulation (23) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have zero draft and etc. the Fresnel optical mirror slip made of the planoconcave glass material of the ring degree of depth, its concave surface is to light source side.

Table (23)

^*Aspherical?Zone?Fesnel

In table (23), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (24) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring degree of depth h _dAnd Fresnel number of rings amount:

Table (24)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 60 ° of directions Xs, 40 ° in Y direction according to the angle, in β=69.506 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.8854

I _1/2＝30.0

φ _x＝33.1

φ _y＝19.0

$\frac{f_s}{r_n}=1.0008$

$(N_{d2}-1)\frac{d_2}{f_s}=0.4361$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.2053$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.2188$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 23 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (23), table (24) and shown in Figure 23, the light-emitting diode component schematic diagram that provable by this planoconcave Fresnel optical mirror slip of the present utility model is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

＜the ten three embodiment 〉

Please refer to Fig. 6 and shown in Figure 24, it is respectively light-emitting diode component schematic diagram and the light intensity distributions of present embodiment and the polar coordinates graph of a relation at photograph angle that use planoconcave Fresnel optical mirror slip of the present utility model is constituted;

Show respectively in the following tabulation (25) by led chip 11, adhesive layer 12, the light source-side optical face R1 of optical mirror slip 13 and radius of curvature R or the Fresnel central shaft optically focused curvature of curved surface radius R of picture side optical surface R2 of light source side to the picture side along central shaft Z _F, spacing di, optical mirror slip 13 tapering υ, each refractive index (N _d) etc.Present embodiment be to use have zero draft and etc. the Fresnel optical mirror slip made of the planoconcave glass material of the ring degree of depth, its concave surface is to light source side.

Table (25)

^*Aspherical?Zone?Fesnel

In table (25), optical surface (Surf.No.) has mark * person to be aspheric Fresnel optical surface.Following tabulation (26) is a Fresnel optical surface radius of curvature R _FAspheric surface in every coefficient of formula (9), the first Fresnel ring radius r of starting at along the center ₁, the most last Fresnel ring radius r _n, Fresnel ring degree of depth h _dAnd Fresnel number of rings amount:

Table (26)

In the present embodiment, optical mirror slip 13 is to utilize refractive index N _D2Be 1.582, Abbe number v _D2Be that 61.7 glass material is made.By the refraction coefficient and the Abbe number of collocation adhesive layer 12 and optical mirror slip 13, form the light refraction angle.After optical mirror slip thus 13 is assembled, with the ellipse of 60 ° of directions Xs, 40 ° in Y direction according to the angle, in β=69.506 lumens of unlimited distance (being) (ignoring effects such as the refraction of air and scattering) in 100 times of fs; Formula (1), (2), (3), (7) and formula (8) are respectively:

η＝0.8828

I _1/2＝29.0

φ _x＝31.0

φ _y＝20.2

$\frac{f_s}{r_n}=1.0081$

$(N_{d2}-1)\frac{d_2}{f_s}=0.3786$

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g=0.2227$

$\frac{{\mathrm{<figure-callout\; id="1"\; label="E"\; filenames="Y20082013316700383.png"\; state="\{\{state\}\}">E</figure-callout>}}_{1/2}}{E_d}=0.2103$

The formula that can satisfy condition (1), (2), (3) and formula (7).Figure 24 is the LED assembly light intensity distributions and the polar coordinates graph of a relation that shines the angle of present embodiment; By above-mentioned table (25), table (26) and shown in Figure 24, the light-emitting diode component schematic diagram that provable by this planoconcave Fresnel optical mirror slip of the present utility model is constituted has high efficiency and predetermined elliptical light type is arranged, the luminous intensity homogeneous of its each angle can promote application of the present utility model.

More than shown in only be preferred embodiment of the present utility model, only be illustrative for the utility model, and nonrestrictive.This professional skill field tool common knowledge personnel understand, and can carry out many changes, modification even equivalence change to it in the spirit and scope that the utility model claim is limited, but all will fall in the claim scope of the present utility model.

Claims (11)

1, a kind of plane Fresnel light emitting diode (LED) light eyeglass, for being used in the light-emitting diode component, this light-emitting diode component in regular turn comprises light-emitting diode chip for backlight unit, adhesive layer and optical mirror slip by light source side to arranging as side along central shaft; This optical mirror slip is characterised in that:

This optical mirror slip has a picture side optical surface and a light source-side optical face, should be the Fresnel optical surface on a plane wherein as the side optical surface, and the anchor ring of this Fresnel optical surface is to be shifted by an optically focused curved surface to form, and its anchor ring has the perpendicular rings tooth, and this optical mirror slip meets the following conditions:

$0.7\&le;\frac{f_s}{r_n}\&le;2.2$

$0.1\&le;(N_{d2}-1)\frac{d_2}{f_s}\&le;1.25$

Wherein, f _sEffective focal length, r for this optical mirror slip _nThe most last ring radius, d for the Fresnel optical surface ₂Be central shaft optical mirror slip thickness, N _D2Refractive index for optical mirror slip.

2, plane according to claim 1 Fresnel light emitting diode (LED) light eyeglass is characterized in that this optical mirror slip further meets the following conditions:

$\sqrt{{\left(\frac{{\mathrm{\&phi;}}_x-{\mathrm{\&omega;}}_x}{\mathrm{\&pi;}}\right)}^2+{\left(\frac{{\mathrm{\&phi;}}_y-{\mathrm{\&omega;}}_y}{\mathrm{\&pi;}}\right)}^2}\&CenterDot;f_g\&le;0.6$

Wherein:

$f_g=\left|(-\frac{1}{R_F}\&CenterDot;f_s)\right|$

${\mathrm{\&omega;}}_x={\tan }^{-1}\left(\frac{D}{d0+d1+d2+\mathrm{Lx}}\right)$

${\mathrm{\&omega;}}_y={\tan }^{-1}\left(\frac{D}{d0+d1+d2+\mathrm{Ly}}\right)$

Wherein, f _sBe the effective focal length of this optical mirror slip, r _nBe the most last ring radius of Fresnel optical surface, d ₂Be central shaft optical mirror slip thickness, N _D2Be the refractive index of optical mirror slip, 2 φ _xFor penetrate the angle (degree) of light at half place of highlight strength of directions X, 2 φ via optical mirror slip _yFor penetrate the angle (degree) of light at half place of highlight strength of Y direction via optical mirror slip, 2Lx is the length of led chip at directions X, and 2Ly is the length of led chip in the Y direction, and fg is the suitable focal length of this optical mirror slip, R ₁Be the radius of curvature of light source-side optical face, R _FBe the optically focused curvature of curved surface radius of picture side Fresnel optical surface, d ₀Be led chip thickness, d ₁Be the adhesive layer thickness of central shaft, D is the radius of optical mirror slip at picture side optical surface.

3, plane according to claim 1 Fresnel light emitting diode (LED) light eyeglass is characterized in that the light source-side optical face of this optical mirror slip is a plane.

4, plane according to claim 1 Fresnel light emitting diode (LED) light eyeglass is characterized in that the light source-side optical face of this optical mirror slip is a concave surface.

5, plane according to claim 1 Fresnel light emitting diode (LED) light eyeglass is characterized in that, should be sphere in order to shift the optically focused curved surface that forms the Fresnel optical surface.

6, plane according to claim 1 Fresnel light emitting diode (LED) light eyeglass is characterized in that, should be aspheric surface in order to shift the optically focused curved surface that forms the Fresnel optical surface.

7, plane according to claim 1 Fresnel light emitting diode (LED) light eyeglass is characterized in that, the anchor ring of this Fresnel optical surface is for waiting ring degree of depth.

8, plane according to claim 1 Fresnel light emitting diode (LED) light eyeglass is characterized in that, the anchor ring of this Fresnel optical surface is for waiting ring spacing.

9, plane according to claim 1 Fresnel light emitting diode (LED) light eyeglass is characterized in that the outer edge surface of this optical mirror slip has tapering.

10, plane according to claim 1 Fresnel light emitting diode (LED) light eyeglass is characterized in that this optical mirror slip is a kind of made by being selected from plastic optical material and the glass optical material.

11, a kind of light-emitting diode component, it is comprised light-emitting diode chip for backlight unit, adhesive layer in regular turn to arranging as side, is reached each the described Fresnel light emitting diode (LED) light eyeglass just like claim 1 to 10 by light source side along central shaft; It is characterized in that:

This light-emitting diode component has oval according to angle light type, penetrates angle, the most last ring radius of Fresnel optical surface and the luminous flux that led chip emit beam of light at half place of highlight strength of Y direction by optical mirror slip and meets the following conditions:

E _1/2≤0.7E _d；

Wherein, $E_{1/2}=\frac{I_{1/2}}{(\mathrm{\&pi;}{r}_n*\sin {\mathrm{\&phi;}}_x)*(r_n*\sin {\mathrm{\&phi;}}_y)}*\mathrm{\&eta;};$

Wherein, r _nThe most last ring radius, 2 φ for the Fresnel optical surface _xFor penetrating light via optical mirror slip at half I of highlight strength of directions X _1/2Angle (degree), 2 φ at place _yFor penetrating light via optical mirror slip at half I of highlight strength of Y direction _1/2Angle (degree), the r at place _nFor the most last ring radius, the α of Fresnel optical surface is that luminous flux, the β that led chip emits beam is the relative unlimited distance of picture side, 100 times of f _s, luminous flux, the η that does not consider the light of AF is luminous flux ratio η=beta/alpha, E _dThe illumination of the light that sends for led chip.

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