CN111649271B - Rayleigh scattering sunlight lamp - Google Patents

Rayleigh scattering sunlight lamp Download PDF

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Publication number
CN111649271B
CN111649271B CN202010652043.3A CN202010652043A CN111649271B CN 111649271 B CN111649271 B CN 111649271B CN 202010652043 A CN202010652043 A CN 202010652043A CN 111649271 B CN111649271 B CN 111649271B
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collimating lens
light
lens array
array
rayleigh scattering
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CN202010652043.3A
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CN111649271A (en
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罗平平
罗敏敏
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Xiyangyang Nanjing Technology Development Co ltd
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Xiyangyang Nanjing Technology Development Co ltd
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Priority to PCT/CN2020/107790 priority patent/WO2022007095A1/en
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21SNON-PORTABLE LIGHTING DEVICES; SYSTEMS THEREOF; VEHICLE LIGHTING DEVICES SPECIALLY ADAPTED FOR VEHICLE EXTERIORS
    • F21S8/00Lighting devices intended for fixed installation
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V5/00Refractors for light sources
    • F21V5/002Refractors for light sources using microoptical elements for redirecting or diffusing light
    • F21V5/005Refractors for light sources using microoptical elements for redirecting or diffusing light using microprisms
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V5/00Refractors for light sources
    • F21V5/04Refractors for light sources of lens shape
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V5/00Refractors for light sources
    • F21V5/08Refractors for light sources producing an asymmetric light distribution
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21YINDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO THE FORM OR THE KIND OF THE LIGHT SOURCES OR OF THE COLOUR OF THE LIGHT EMITTED
    • F21Y2115/00Light-generating elements of semiconductor light sources
    • F21Y2115/10Light-emitting diodes [LED]

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  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Optical Elements Other Than Lenses (AREA)
  • Planar Illumination Modules (AREA)
  • Non-Portable Lighting Devices Or Systems Thereof (AREA)

Abstract

The invention relates to a Rayleigh scattering sunlight lamp, which consists of an LED light source array, a collimating lens array, a honeycomb core material, a diffusion plate and a blue light scattering plate from top to bottom in sequence, wherein light emitted by the LED light source array is collimated into parallel light after passing through the collimating lens array, the collimating lens array comprises a first collimating lens array, a second collimating lens array and a mirror body array arranged between the first collimating lens array and the second collimating lens array, the LED light source array consists of a plurality of LED lamp beads, each LED lamp bead is placed on the focus of each first collimating lens array, the second collimating lens array is arranged in one-to-one correspondence with the honeycomb core material, and the diffusion plate is used for converting uneven light sources into area light sources with even distribution and fuzzy lattice points; the blue light diffusion plate is used to diffuse the transmitted white light or cold white light into blue light. The invention effectively solves the problem of providing the Rayleigh scattering sunlight lamp for diffusing blue light under the condition of lacking natural light.

Description

Rayleigh scattering sunlight lamp
Technical Field
The invention relates to the technical field of photoelectricity, in particular to a Rayleigh scattering sunlight lamp.
Background
At present, research shows that people perform better and feel more comfortable in indoor environments with sunlight. The sunlight irradiation reduces the working pressure and negative influence of people, enhances the comfort emotion and working efficiency, and improves the physical and mental health of people living indoors in the long term.
However, some places in the room cannot be allowed to be irradiated with sunlight due to a certain factor, at this time, a virtual sun and a diffuse blue sky are created, and the lamp can be installed in offices, conference rooms, underground shops and other places without natural environment light, and in addition, when the outside has no obvious view, many closed offices and rooms are seen to be quite claustrophobic and easy to feel depression, so that the Rayleigh scattering sunlight lamp can solve the problems.
Disclosure of Invention
The invention aims to provide a Rayleigh scattering sunlight lamp which can effectively solve the problem that the Rayleigh scattering sunlight lamp can provide diffuse blue light under the condition of lacking natural light.
In order to achieve the above purpose, the technical scheme of the invention is as follows:
the Rayleigh scattering sunlight lamp comprises a sunlight lamp shell, wherein the sunlight lamp shell sequentially comprises an LED light source array, a collimating lens array, a honeycomb core material, a diffusion plate and a blue light diffusion plate from top to bottom, the collimating lens array comprises a first collimating lens array, a second collimating lens array and a mirror body array arranged between the first collimating lens array and the second collimating lens array, the LED light source array comprises a plurality of LED lamp beads, each LED lamp bead is placed on a lens focus of each first collimating lens array, the second collimating lens array is arranged in one-to-one correspondence with the honeycomb core material, and the diffusion plate is attached to the bottom surface of the honeycomb core material and used for converting uneven light sources into surface light sources with uniform distribution and fuzzy lattice points; the blue light scattering plate is fixedly arranged at the bottom of the sunlight lamp shell and used for diffusing white light transmitted by the diffusion plate into blue light.
Further, the first collimating lens array is composed of a plurality of first collimating lenses, one surface of each first collimating lens, which is close to the LED light source, is a light incident surface, one surface, which is far away from the LED light source, is a light emergent surface, wherein the light incident surface is a concave surface, and the light emergent surface is a spherical convex surface; the second collimating lens array is composed of a plurality of second collimating lenses, one surface of each second collimating lens, which is close to the LED light source, is a light incident surface, one surface of each second collimating lens, which is far away from the LED light source, is a light emergent surface, wherein the light incident surface is a plane, and the light emergent surface is a spherical convex surface.
Further, the first collimating lens and the second collimating lens are transparent solid materials.
Further, the mirror body array is a plurality of regular hexagonal prisms made of black solid materials and is arranged in a honeycomb seamless splicing mode.
Further, the honeycomb core material is made of one of aluminum alloy, glass fiber fabric impregnated with resin, aromatic fiber paper, kraft paper, graphite fiber or kevlar fiber.
Further, the diffusion plate is made of PC, PMMA or transparent glass attached with a diffusion film, wherein the diffusion film is attached to one surface of the transparent glass connected with the honeycomb core material or the diffusion film is attached to both surfaces of the transparent glass.
Further, the blue light scattering plate is composed of a transparent substrate and transparent titanium dioxide nanoparticles which have different refractive indexes relative to the transparent substrate and have average sizes which are obviously smaller than the wavelength of visible light, and the titanium dioxide nanoparticles can be embedded in the transparent substrate or made into a nano film to be adhered on the transparent substrate.
Further, the color temperature of each LED lamp bead is required to be above 5000K, and the dominant wavelength is 400-500 nm.
Compared with the prior art, the invention has the beneficial effects that: the diffusion blue sky and the virtual sun are led into the indoor space, so that an illumination system, a medical system and an air purification system can be realized, and the system can be applied to indoor illumination, such as home illumination, underground malls, parking lots, meeting rooms, office buildings and other places needing illumination, and can also be used for assisting in treating depression, such as hospitals, rehabilitation centers, medical research institutions and other places.
Drawings
In order to more clearly illustrate the technical solutions of the embodiments of the present invention, the drawings that are needed in the description of the embodiments will be briefly introduced below, and it is obvious that the drawings in the description below are only some embodiments of the present invention. Wherein:
FIG. 1 is a schematic diagram of a Rayleigh scattering sunlight lamp according to an embodiment of the present invention;
FIG. 2 is a schematic diagram of a Rayleigh scattering sunlight lamp according to an embodiment of the invention;
FIG. 3 is a partial layout of LED light beads according to an embodiment of the present invention;
FIG. 4 is a schematic view showing a partial structure of a collimating lens array according to an embodiment of the present invention;
FIG. 5 is a first collimating lens array layout diagram in accordance with an embodiment of the present invention;
FIG. 6 is a second collimating lens array layout of an embodiment of the present invention;
FIG. 7 is a schematic view of a first collimating lens according to an embodiment of the present invention;
FIG. 8 is a schematic diagram of a second collimating lens according to an embodiment of the present invention;
FIG. 9 is a schematic view of the structure of a honeycomb core according to an embodiment of the invention;
fig. 10 is a schematic structural view of a blue light diffusion plate according to an embodiment of the present invention;
FIG. 11 is a schematic view showing another structure of a blue light diffusion plate according to an embodiment of the present invention;
in the figure: 1. the LED light source comprises an LED light source array, 101, LED lamp beads, 2, a collimating lens array, 201, a first collimating lens array, 2011, a first collimating lens, 202, a lens array, 203, a second collimating lens array, 2031, a second collimating lens, 3, a honeycomb core material, 4, a diffusion plate, 5, a blue light diffusion plate, 501, a transparent substrate, 502, titanium dioxide nano particles, 503, a titanium dioxide nano film and 6, and the sun.
Detailed Description
The following description of the embodiments of the present invention will be made clearly and fully with reference to the accompanying drawings, in which it is evident that the embodiments described are some, but not all embodiments of the invention. All other embodiments, which can be made by those skilled in the art based on the embodiments of the present invention without making any inventive effort, shall fall within the scope of the present invention.
Fig. 1 shows a rayleigh scattering sunlight lamp according to an embodiment of the present invention, which is composed of an LED light source array 1, a collimator lens array 2, a honeycomb core 3, a diffusion plate 4 and a blue light scattering plate 5 in this order from top to bottom.
Wherein the collimator lens array 2 comprises a first collimator lens array 201, a second collimator lens array 203 and a mirror array 202 mounted between the first collimator lens array 201 and the second collimator lens array 203. The LED light source array 1 consists of a plurality of LED lamp beads 101, each LED lamp bead 101 is placed on a lens focus of each first collimating lens array 201 in one-to-one correspondence, the second collimating lens arrays 203 are arranged in one-to-one correspondence with the honeycomb core materials 3, and a diffusion plate 4 is attached to the bottom surface of the honeycomb core materials 3 and used for converting uneven light sources into surface light sources with evenly distributed and fuzzy lattice points; a certain diffusion space is formed between the blue light diffusion plate 5 and the diffusion plate 4, and the blue light diffusion plate 5 is fixedly installed at the bottom of the sunlight lamp housing for diffusing the white light transmitted by the diffusion plate into blue light.
As shown in fig. 3, in this embodiment, in order to ensure uniform light intensity distribution, each LED lamp bead 101 is placed at the focal point of the collimator lens array 2 and arranged in a quincuncial array. The color temperature of the light source of the LED lamp beads 101 is generally 6000K-8000K, or 5000K-10000K, or more than 10000K. The main wavelength of the light source of the LED lamp beads 101 is 430-470 nm, or 400-500 nm.
Referring to fig. 4 to 8, the first collimating lens array 201 is composed of a plurality of first collimating lenses 2011, wherein a surface of each first collimating lens 2011, which is close to the LED light source, is a light incident surface, a surface of each first collimating lens, which is far away from the LED light source, is a light emitting surface, wherein the light incident surface is a concave surface, and the light emitting surface is a spherical convex surface. Similarly, the second collimating lens array 203 is composed of a plurality of second collimating lenses 2031, wherein a surface of each second collimating lens 2031 close to the LED light source is a light incident surface, a surface of each second collimating lens far away from the LED light source is a light emitting surface, the light incident surface is a plane, and the light emitting surface is a spherical convex surface.
The first collimating lens 2011 and the second collimating lens 2031 are made of any transparent solid material, including but not limited to acrylic, glass, etc., and the transmittance of the lens is generally 90-93%, or in a larger range, such as more than 93% or less than 80%.
The lens array 202 is a plurality of black regular hexagonal prisms, is arranged in a honeycomb seamless splicing manner, and is arranged in one-to-one correspondence with the first collimating lens array 201 and the second collimating lens array 203.
As shown in fig. 9, the honeycomb core 3 is made of a black solid core material made of one of aluminum alloy, glass fiber fabric impregnated with resin, aromatic fiber paper, kraft paper, graphite fiber or kevlar fiber, and has light guiding and heat dissipating effects.
The diffusion plate 4 is made of PC, PMMA, or transparent glass and transparent toughened glass bonded with diffusion films, wherein the diffusion films are bonded on one surface of the transparent glass connected with the honeycomb core material, or the diffusion films are bonded on two surfaces of the transparent glass. The diffusion plate 4 has the main functions of converting an uneven light source into a surface light source with evenly distributed and fuzzy lattice points and simultaneously shielding honeycomb core materials or other optical defects; secondly, improve the visual angle, increase the light source softness, thirdly, support backlight framework to the optical material of above is impaired.
Specifically, the light transmittance of the diffusion plate 4 is generally required to be 85% to 90%, or 80% to 92%, or 75% to 95%. The haze of the diffusion plate 4 is generally required to be 65% to 75%, or 60% to 80%, or 55% to 85%.
The blue light scattering plate 5 is composed of a transparent substrate 501 and transparent titanium dioxide nanoparticles having different refractive indexes relative to the transparent substrate 501 and an average size significantly smaller than the wavelength of visible light, and the titanium dioxide nanoparticles have the functions of absorbing and suppressing ultraviolet rays, self-cleaning, purifying air, and the like.
As an embodiment of the present invention, as shown in fig. 10, titanium dioxide nanoparticles 502 are uniformly embedded in a transparent substrate 501, and the transmitted white light is absorbed and suppressed by the titanium dioxide particles 502 in the transparent substrate 501, and long wave components in the sunlight are filtered, so that blue light and violet light penetrate a blue light scattering plate 5.
As an embodiment of the present invention, as shown in fig. 11, the titanium dioxide nano particles 502 are made into the titanium dioxide nano film 503, and the titanium dioxide nano film 503 is attached to the transparent substrate 501, and the transmitted white light is absorbed and suppressed by the titanium dioxide nano film 503 on the surface of the transparent substrate 501, so as to filter out the long wave component in the sunlight, and the blue light and the purple light penetrate the blue light scattering plate 5.
Blue light scattering can be explained by Rayleigh scattering, and since the intensity of Rayleigh scattering is inversely proportional to the fourth power of wavelength, the red light has longer wavelength, the scattered red light has weaker intensity, and the blue and purple light has shorter wavelength and stronger scattering intensity. Therefore, the atmospheric molecules are better than a filter screen, the components of long waves in sunlight are filtered out, and the rest blue and purple lights are sprayed to the ground. The human eye is very insensitive to violet light and therefore the sky presented is blue.
In order to meet the Rayleigh scattering requirement, the diameter d of the nanoparticle must be much smaller than the wavelength λ of the incident light, typically the upper bound is about 1/10 of the wavelength of blue light, e.g. 48nm, where the diameter d of the nanoparticle may be 40nm, 30nm, 20nm, 10nm or 5nm.
As shown in fig. 2, the light emitted from the LED light source array is collimated into parallel light after passing through the collimator lens array 2. The parallel light is guided to the diffusion plate 4 through the honeycomb core 3, so that the light is more uniform and softer. Directly above the observer, the sun 6 (warm light) formed by the parallel light passing through the partial honeycomb core 3 in the visual field is seen, while the light in other areas is blocked by the honeycomb core, and the blue sky (cool light) formed by the blue light scattering plate 5 is seen.
The invention introduces the diffusion blue sky and the virtual sun into the indoor space, can realize an illumination system, a medical system and an air purification system, can be applied to indoor illumination, such as home illumination, underground malls, parking lots, meeting rooms, office buildings and other places needing illumination, and can also be applied to auxiliary treatment of depression, such as hospitals, rehabilitation centers, medical research institutions and other places.
While the invention has been described with reference to certain preferred embodiments, it will be understood by those skilled in the art that various changes and substitutions of equivalents may be made and equivalents will be apparent to those skilled in the art without departing from the scope of the invention. Therefore, the protection scope of the invention is subject to the protection scope of the claims.

Claims (7)

1. The Rayleigh scattering sunlight lamp comprises a sunlight lamp shell, and is characterized in that the sunlight lamp shell is composed of an LED light source array, a collimating lens array, a honeycomb core material, a diffusion plate and a blue light scattering plate from top to bottom in sequence, wherein the collimating lens array comprises a first collimating lens array, a second collimating lens array and a mirror body array arranged between the first collimating lens array and the second collimating lens array, the mirror body array is a plurality of regular hexagonal prisms made of black solid materials and is in honeycomb seamless splicing arrangement, the LED light source array is composed of a plurality of LED light beads, each LED light bead is placed on a lens focus of each first collimating lens array, the second collimating lens array is arranged in one-to-one correspondence with the honeycomb core material, and the diffusion plate is attached to the bottom surface of the honeycomb core material and is used for converting uneven light sources into area light sources with uniform distribution and fuzzy lattice points; the blue light scattering plate is fixedly arranged at the bottom of the sunlight lamp shell and used for diffusing white light transmitted by the diffusion plate into blue light.
2. The rayleigh scattering sunlight lamp according to claim 1, wherein the first collimating lens array is composed of a plurality of first collimating lenses, wherein a face of each first collimating lens close to the LED light source is a light incident face, a face away from the LED light source is a light emergent face, wherein the light incident face of the first collimating lens is a concave face, and the light emergent face is a spherical convex face; the second collimating lens array is composed of a plurality of second collimating lenses, one surface of each second collimating lens, which is close to the LED light source, is a light incident surface, one surface of each second collimating lens, which is far away from the LED light source, is a light emergent surface, wherein the light incident surface of each second collimating lens is a plane, and the light emergent surface is a spherical convex surface.
3. The rayleigh scattering sunlight lamp of claim 1 or 2, wherein the first and second collimating lenses are transparent solid material.
4. The rayleigh scattering sunlight lamp according to claim 1, wherein the honeycomb core material is one of aluminum alloy, glass fiber fabric impregnated with resin, aromatic fiber paper, kraft paper, graphite fiber or kevlar fiber.
5. The rayleigh scattering sunlight lamp according to claim 1, wherein the diffusion plate is made of PC, PMMA, or transparent glass bonded with a diffusion film, wherein the diffusion film is bonded to one surface of the transparent glass connected with the honeycomb core material, or the diffusion film is bonded to both surfaces of the transparent glass.
6. The rayleigh scattering sunlight lamp according to claim 1, wherein the blue light scattering plate is composed of a transparent substrate and transparent titanium dioxide nanoparticles having different refractive indexes with respect to the transparent substrate and an average size significantly smaller than the wavelength of visible light, and the titanium dioxide nanoparticles may be embedded in the transparent substrate or made into a nano film to be adhered on the transparent substrate.
7. The rayleigh scattering sunlight lamp of claim 1, wherein the color temperature of each LED lamp bead is required to be above 5000K, and the dominant wavelength is 400 nm-500 nm.
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PCT/CN2020/107790 WO2022007095A1 (en) 2020-07-08 2020-08-07 Rayleigh scattering sunlight lamp

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