CN113563769A - Infrared radiation refrigeration optical coating and optical film - Google Patents

Infrared radiation refrigeration optical coating and optical film Download PDF

Info

Publication number
CN113563769A
CN113563769A CN202111132388.7A CN202111132388A CN113563769A CN 113563769 A CN113563769 A CN 113563769A CN 202111132388 A CN202111132388 A CN 202111132388A CN 113563769 A CN113563769 A CN 113563769A
Authority
CN
China
Prior art keywords
infrared radiation
rare earth
source
radiation refrigeration
optical coating
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
CN202111132388.7A
Other languages
Chinese (zh)
Inventor
尹晓峰
赵佰金
刘艳国
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Jiangsu Bolin Plastics Co ltd
Original Assignee
Jiangsu Bolin Plastics Co ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Jiangsu Bolin Plastics Co ltd filed Critical Jiangsu Bolin Plastics Co ltd
Priority to CN202111132388.7A priority Critical patent/CN113563769A/en
Publication of CN113563769A publication Critical patent/CN113563769A/en
Withdrawn legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C09DYES; PAINTS; POLISHES; NATURAL RESINS; ADHESIVES; COMPOSITIONS NOT OTHERWISE PROVIDED FOR; APPLICATIONS OF MATERIALS NOT OTHERWISE PROVIDED FOR
    • C09DCOATING COMPOSITIONS, e.g. PAINTS, VARNISHES OR LACQUERS; FILLING PASTES; CHEMICAL PAINT OR INK REMOVERS; INKS; CORRECTING FLUIDS; WOODSTAINS; PASTES OR SOLIDS FOR COLOURING OR PRINTING; USE OF MATERIALS THEREFOR
    • C09D127/00Coating compositions based on homopolymers or copolymers of compounds having one or more unsaturated aliphatic radicals, each having only one carbon-to-carbon double bond, and at least one being terminated by a halogen; Coating compositions based on derivatives of such polymers
    • C09D127/02Coating compositions based on homopolymers or copolymers of compounds having one or more unsaturated aliphatic radicals, each having only one carbon-to-carbon double bond, and at least one being terminated by a halogen; Coating compositions based on derivatives of such polymers not modified by chemical after-treatment
    • C09D127/12Coating compositions based on homopolymers or copolymers of compounds having one or more unsaturated aliphatic radicals, each having only one carbon-to-carbon double bond, and at least one being terminated by a halogen; Coating compositions based on derivatives of such polymers not modified by chemical after-treatment containing fluorine atoms
    • C09D127/16Homopolymers or copolymers of vinylidene fluoride
    • CCHEMISTRY; METALLURGY
    • C09DYES; PAINTS; POLISHES; NATURAL RESINS; ADHESIVES; COMPOSITIONS NOT OTHERWISE PROVIDED FOR; APPLICATIONS OF MATERIALS NOT OTHERWISE PROVIDED FOR
    • C09DCOATING COMPOSITIONS, e.g. PAINTS, VARNISHES OR LACQUERS; FILLING PASTES; CHEMICAL PAINT OR INK REMOVERS; INKS; CORRECTING FLUIDS; WOODSTAINS; PASTES OR SOLIDS FOR COLOURING OR PRINTING; USE OF MATERIALS THEREFOR
    • C09D5/00Coating compositions, e.g. paints, varnishes or lacquers, characterised by their physical nature or the effects produced; Filling pastes
    • C09D5/32Radiation-absorbing paints
    • CCHEMISTRY; METALLURGY
    • C09DYES; PAINTS; POLISHES; NATURAL RESINS; ADHESIVES; COMPOSITIONS NOT OTHERWISE PROVIDED FOR; APPLICATIONS OF MATERIALS NOT OTHERWISE PROVIDED FOR
    • C09DCOATING COMPOSITIONS, e.g. PAINTS, VARNISHES OR LACQUERS; FILLING PASTES; CHEMICAL PAINT OR INK REMOVERS; INKS; CORRECTING FLUIDS; WOODSTAINS; PASTES OR SOLIDS FOR COLOURING OR PRINTING; USE OF MATERIALS THEREFOR
    • C09D7/00Features of coating compositions, not provided for in group C09D5/00; Processes for incorporating ingredients in coating compositions
    • C09D7/40Additives
    • C09D7/60Additives non-macromolecular
    • C09D7/61Additives non-macromolecular inorganic
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B1/00Optical elements characterised by the material of which they are made; Optical coatings for optical elements
    • G02B1/10Optical coatings produced by application to, or surface treatment of, optical elements

Landscapes

  • Chemical & Material Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • Wood Science & Technology (AREA)
  • Organic Chemistry (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Inorganic Chemistry (AREA)
  • Paints Or Removers (AREA)

Abstract

The invention discloses an infrared radiation refrigeration optical coating and an optical film. Wherein the optical coating comprises a resin and an infrared radiation refrigeration composition dispersed in the resin; the infrared radiation refrigeration composition comprises rare earth silicate particles formed by reacting components including a rare earth source, an Ra ion metal source and an Si source. Compared with the prior art, the invention can realize higher radiation refrigeration performance and can be industrialized more easily.

Description

Infrared radiation refrigeration optical coating and optical film
Technical Field
The invention relates to the technical field of radiation refrigeration, in particular to an infrared radiation refrigeration optical coating and an optical film.
Background
In recent years, a novel cooling method has attracted interest and the technology is expected to be applied to the electroless cooling of buildings. The principle of the refrigeration mode is as follows: according to the Planck black body radiation law, any object with the temperature higher than absolute zero radiates heat energy to the outside in the form of electromagnetic waves, and the temperature of the object is reduced due to the radiation of the energy outwards, namely radiation cooling. Stefan-boltzmann states that the full radiated power of a black body is proportional to its absolute temperature to the power of 4, and it is calculated that a 1 square meter absolute black body radiates 460W of radiant energy in the full band at 300K. A black body will reduce its temperature at a significant rate if it only radiates without absorbing energy from the environment. In theory, radiation cooling can be used to develop refrigeration technology that does not require electrical energy nor rely on external energy sources, which is radiation refrigeration technology. The material used to achieve the radiation refrigeration effect is the radiation refrigeration material.
According to the research on the atmospheric transmittance, the absorption of various gas molecules in the wave band of 8-13 μm is relatively weak, and the infrared rays in the wave band can directly reach the outer space with lower temperature without being absorbed by the atmosphere, and the region is called as an atmospheric window.
In recent years, researchers are constantly researching and developing infrared radiation refrigeration materials, and most of the infrared radiation refrigeration materials adopt silicon dioxide
Figure 666109DEST_PATH_IMAGE001
On the basis of this, as in 2014, the research group of professor Shanhui Fan, university of Stanford, by depositing seven layers alternately
Figure 386940DEST_PATH_IMAGE001
And hafnium oxide form a layered structure. The layered structure can release energy to the outside by radiating infrared rays with the wavelength of 8-13 mu m, and can reflect up to 97% of sunlight, thereby avoiding the temperature rise caused by the sunlight as much as possible. Experiments have shown that such a layered structure is still able to keep the temperature of the object covered under it at 5 degrees celsius below the temperature of the surrounding atmosphere, even during the day and in direct sunlight. The Xiaoobo Yin of Colorado university is incorporated into polymethylpentene (TPX)
Figure 552342DEST_PATH_IMAGE001
The microbead is used to draw the finished product into a sheet with thickness of about 50 μm, then the back surface is coated with silver, 96% of sunlight can be reflected back by the composite material, and at the same time, the material radiates heat energy to space by infrared, especially 8-13 μm atmosphere infrared window.
However, the performance of the infrared radiation refrigeration cannot meet the current requirements in the two modes. Therefore, a material with higher radiation refrigeration performance is urgently needed at present.
Disclosure of Invention
The invention provides an infrared radiation refrigeration optical coating and an optical film, which have higher radiation refrigeration performance compared with the prior art.
The invention provides the following scheme:
in one aspect, an infrared radiation refrigerating optical coating is disclosed, the optical coating comprising a resin and an infrared radiation refrigerating composition dispersed in the resin; the infrared radiation refrigeration composition comprises rare earth silicate particles formed by reacting components including a rare earth source, an Ra ion metal source and an Si source.
In a particular embodiment, the anion of the rare earth source is selected from at least one of rare earth nitrate, rare earth chloride; the source of Ra ion metal is selected from
Figure 649611DEST_PATH_IMAGE002
Figure 466126DEST_PATH_IMAGE003
Figure 92280DEST_PATH_IMAGE004
Figure 744978DEST_PATH_IMAGE005
At least one of (a); the Si source is selected from the group consisting of nano
Figure 380358DEST_PATH_IMAGE006
Wherein x is more than 0 and less than or equal to 2.
In a particular embodiment, the cation of the rare earth source is selected from at least one of La, Sm, Eu, Gd, Tb, Dy, Er, Tm, Yb, Y, Sc.
In a specific embodiment, the rare earth silicate particles comprise, by mass fraction, 50-77% of the rare earth source, 20-45% of the Ra ion metal source, and 0.3-10% of the Si source.
In a specific embodiment, the Si source comprises
Figure 536533DEST_PATH_IMAGE007
Particles.
In a particular embodiment, the rare earth silicate particles have a particle size in the range of 50-200nm or 1-10 μm.
In a particular embodiment, the resin is selected from at least one of polyvinyl fluoride PVF, polyvinylidene fluoride PVDF, polychlorotrifluoroethylene PCTFE, polytetrafluoroethylene PTFEDE, polytetrafluoroethylene PTFE, polyvinylidene fluoride hexafluoropropylene (P (VDF-HFP)).
In a specific embodiment, the rare earth silicate particles comprise 5-20% by volume of the optical coating.
The application also discloses an infrared radiation refrigeration optical film, which comprises an infrared radiation refrigeration functional layer formed by the infrared radiation refrigeration optical coating.
In a particular embodiment, the optical film further comprises a metallic reflective layer.
In a particular embodiment, the thickness of the metallic reflective layer is in the range of 0.15-1 μm or 1-150 nm.
In a specific embodiment, the thickness of the infrared radiation refrigeration functional layer is 0.1-5 μm.
According to the specific embodiment provided by the invention, the invention discloses the following technical effects:
the infrared radiation refrigeration optical coating provided by the invention contains rare earth silicate particles formed by reacting rare earth source, Ra ion metal source and Si source. The rare earth cations are compounded by utilizing the network structure of silicate glass, have octahedral coordination and have strong accumulation capacity on free oxygen. The silicate anion group has various polymerization forms, rare earth cations are doped in the silicate anion group, the structure of the anion group and the cation field where the anion group is located are adjusted, the silica network structure of the silicate is adjusted to have higher symmetry, the rare earth cations have better absorption performance at a near infrared wave band, and the combination of the rare earth cations and the near infrared wave band can realize higher infrared radiation refrigeration performance. Further, in the metal source of Ra ion
Figure 599167DEST_PATH_IMAGE008
The ions have a high valueThe ion activity and the capability of competing for oxygen are stronger, and the silicon-oxygen network structure is damaged strongly. The rare earth ions can more easily occupy the lattice position with higher symmetry in the silicate, and the infrared radiation refrigeration performance of the rare earth silicate particles is further improved.
Detailed Description
The technical solutions in the embodiments of the present invention will be clearly and completely described below, and it is obvious that the described embodiments are only a part of the embodiments of the present invention, and not all embodiments. All other embodiments that can be derived by one of ordinary skill in the art from the embodiments given herein are intended to be within the scope of the present invention.
The following describes a specific implementation scheme provided by the embodiment of the present invention in detail.
The invention provides an infrared radiation refrigeration optical coating, which comprises a resin and an infrared radiation refrigeration composition dispersed in the resin; the infrared radiation refrigeration composition comprises rare earth silicate particles formed by reacting components including a rare earth source, an Ra ion metal source and an Si source.
The rare earth ions have better absorption performance at the near infrared position, the rare earth ions are compounded by utilizing the glass silica network structure of the silicate, the rare earth ions have octahedral coordination and have strong accumulation capacity on free oxygen, silicate anion groups have various polymerization forms, the rare earth ions are doped in the silicate anion groups, the anion group structure and the cation field where the anion groups are located are adjusted, the silica network structure of the rare earth silicate is adjusted to have higher symmetry, and better infrared radiation performance can be realized.
And in the Ra ion metal source
Figure 473582DEST_PATH_IMAGE008
The ions have higher ion activity and stronger oxygen competition capability, and have strong destructive effect on the silicon-oxygen network structure. Adding Ra ion metal source during preparing RE silicate particle,
Figure 912654DEST_PATH_IMAGE008
ion pair silica netThe strong destruction and regulation of the complex structure makes the rare earth cation occupy the lattice position with higher symmetry in the silicate more easily, so as to improve the infrared radiation refrigerating capacity of the rare earth silicate particles.
In a particular embodiment of the present application, the anion of the rare earth source is selected from one or both of rare earth nitrate, rare earth chloride. The rare earth source is easy to decompose under the high-temperature reaction condition, and the rare earth compound formed after decomposition has higher activation energy and high reaction activity, thereby being beneficial to the diffusion of rare earth ions and promoting the reaction, and leading the damage of the silica network structure to be more thorough.
The cation of the rare earth source may be at least one selected from La, Sm, Eu, Gd, Tb, Dy, Er, Tm, Yb, Y and Sc.
The Ra ion metal source can be selected from
Figure 939647DEST_PATH_IMAGE009
Figure 438761DEST_PATH_IMAGE010
Figure 800473DEST_PATH_IMAGE011
Figure 777656DEST_PATH_IMAGE012
At least one of (1).
In a preferred embodiment of the present application, the Si source is selected from the group consisting of nano-sized Si
Figure 908423DEST_PATH_IMAGE013
Wherein x is more than 0 and less than or equal to 2. Preferably of nanometer
Figure 312859DEST_PATH_IMAGE014
Has smaller grain diameter, better size distribution, larger specific surface area and specific surface energy and relatively higher reaction activity.
Preferably, the rare earth silicate particles comprise 50-77% of the rare earth source, 20-45% of the Ra ion metal source and 0.3-10% of the Si source in mass fraction. The ratio ofThe range of more rare earth ions entering into a silicon-oxygen network structure is beneficial to the mass generation of non-bridging oxygen bonds Si-O if
Figure 161867DEST_PATH_IMAGE008
When the ions are excessive, the rare earth ions are converted into network forming ions from the network exo-ions, so that the fractured silicon-oxygen network structure starts to polymerize again.
In one embodiment, the rare earth silicate particles have a particle size in the range of 50-200 nm. In this particle size range, the visible light transmittance can be improved.
In another embodiment, the rare earth silicate particles have a particle size in the range of 1-10 μm. The particle microspheres have different resonance forms excited by the interaction with incident wavelength, and when the rare earth silicate particles are in the particle size range, the rare earth silicate particles can be excited by 8-13 mu m magnetic waves to form high-order resonance forms, so that the rare earth silicate particles have high emissivity in the wavelength range of 8-13 mu m. The particles having a particle diameter within the above range have excellent forward scattering ability, so that the heat radiating property thereof can be improved.
In another embodiment of the present application, the Si source in the optical coating is nano
Figure 949867DEST_PATH_IMAGE015
Particles.
The resin in the coating can be at least one selected from polyvinyl fluoride PVF, polyvinylidene fluoride PVDF, polychlorotrifluoroethylene PCTFE, polytetrafluoroethylene PTFEDE, polytetrafluoroethylene PTFE and polyvinylidene fluoride-hexafluoropropylene (P (VDF-HFP)). The materials have good weather resistance and good anti-fouling effect.
The application also discloses an infrared radiation refrigeration optical film in another aspect, and the optical film comprises an infrared radiation refrigeration functional layer formed by the infrared radiation refrigeration optical coating mentioned in the embodiment.
In order to realize the reflection of light under sunlight and further improve the refrigeration performance, the optical film also comprises a metal reflecting layer. The metal in the metal reflective layer is selected from: aluminum, silver alloys.
In a specific embodiment, the thickness of the metal reflective layer is set to be in the range of 0.15 to 1 μm in order to improve the reflectivity. When the metal reflecting layer is too thin, the reflectivity of the visible light wave band is low because most visible light directly penetrates through the composite film. When the metal reflecting layer is larger than 1 μm, the reflectivity of the metal reflecting layer achieves the ideal effect, and when the thickness exceeds a certain value, the sunlight reflectivity is kept unchanged.
If there is a high demand for visible light transmittance of the entire film in some cases, the thickness of the metal reflective layer may be set to be in the range of 1 to 150 nm.
The thickness range of the infrared radiation refrigeration functional layer is selected from 0.1-5 mu m, and when the thickness range is within the range, multiple scattering and absorption can be generated when light waves pass through the infrared radiation refrigeration functional layer, so that the refrigeration effect is better.
The rare earth silicate particles in the infrared radiation refrigeration functional layer account for 5-20% of the volume fraction range of the infrared functional layer, the infrared emissivity is gradually increased along with the increase of the filling volume fraction, but the transmittance of a film material is influenced when the filling volume fraction is increased to a certain degree, and meanwhile, the infrared radiation refrigeration functional layer is not beneficial to industrial processing.
The present application also provides a method for preparing an infrared radiation refrigeration composition in an optical coating, comprising:
taking alcohol as a ball milling medium, and performing ball milling on a rare earth source, an Ra ion metal source and an Si source at a rotating speed of 100-200 r/min. And (5) after ball milling for a preset time, putting into an oven for drying. Finally placing the mixture in a high-temperature furnace for reaction to obtain the infrared radiation refrigeration composition.
In a preferred embodiment, the temperature of the high temperature furnace is set to 700-900 ℃ and the reaction time is 12-16 hours. Exceeding this temperature range leads to the onset of melting of the rare earth silicate and the tendency of the silicon tetrahedron to re-associate into aggregates. The appropriate time is favorable for further diffusion among reactants in the solid-phase reaction, so that the reaction is more thorough, and the rare earth ions enter a silicon-oxygen network structure, so that silicon-oxygen tetrahedrons in the product are regularly arranged and bond angles are close.
The following effects are illustrated by experimental data of examples and comparative examples:
comparative example 1
Blank test thermocouple was placed directly in the incubator and is designated as R11.
Comparative example 2
Weighing 80 g
Figure 200720DEST_PATH_IMAGE016
Is a rare earth source, 5 g
Figure 41637DEST_PATH_IMAGE017
Is a source of Si. Taking ethanol as a ball milling medium, performing ball milling for 10 hours at the rotating speed of 90 r/min, putting the ball milled mixture into a 60 ℃ oven for drying, and finally reacting for 15 hours at the temperature of 600 ℃ in a high-temperature furnace to obtain the rare earth silicate. The particle size of the prepared rare earth silicate is 300 nm. Preparing the infrared radiation refrigeration coating by the prepared rare earth silicate and polyvinylidene fluoride, wherein the rare earth silicate accounts for 10% of the volume fraction of the infrared radiation refrigeration coating, and then coating the coating on a silver alloy reflecting layer far away from a base material layer prepared from the polyvinylidene fluoride. The thickness of the substrate layer is 50 μm, the thickness of the silver alloy reflective layer is 0.5 μm, and the thickness of the functional layer formed by the coating is 5 μm. The resulting film was designated R12.
Example 1
The difference from comparative example 2 is that 15 g is added
Figure 377940DEST_PATH_IMAGE018
Is a source of Ra ion metal to prepare the rare earth silicate. The prepared rare earth silicate and polyvinylidene fluoride are prepared into infrared radiation refrigeration coating, and the infrared radiation refrigeration coating is coated on the silver alloy reflecting layer far away from the base material layer. The resulting film was designated R21.
Example 2
The difference from the embodiment 1 is that,
Figure 696926DEST_PATH_IMAGE019
the mass of (a) is 45 g,
Figure 802285DEST_PATH_IMAGE020
the weight of the mixture is 50 g,
Figure 548524DEST_PATH_IMAGE021
is 5 g. The prepared rare earth silicate and polyvinylidene fluoride are prepared into infrared radiation refrigeration coating, and the infrared radiation refrigeration coating is coated on the silver alloy reflecting layer far away from the base material layer. The resulting film was designated R22.
Example 3
The difference from the embodiment 1 is that,
Figure 857277DEST_PATH_IMAGE022
the mass of (a) is 75 g,
Figure 979954DEST_PATH_IMAGE023
the mass of (a) is 20 g,
Figure 939820DEST_PATH_IMAGE024
the mass of the rare earth silicate is 5 g, and the rare earth silicate is prepared. The prepared rare earth silicate and polyvinylidene fluoride are prepared into infrared radiation refrigeration coating, and the infrared radiation refrigeration coating is coated on the silver alloy reflecting layer far away from the base material layer. The resulting film was designated R23.
Example 4
The difference from the embodiment 1 is that,
Figure 122539DEST_PATH_IMAGE025
the mass of (a) is 50 g,
Figure 433435DEST_PATH_IMAGE026
the mass of (a) is 45 g,
Figure 94223DEST_PATH_IMAGE027
the mass of the rare earth silicate is 5 g, and the rare earth silicate is prepared. The prepared rare earth silicate and polyvinylidene fluoride are prepared into infrared radiation refrigeration coating, and the infrared radiation refrigeration coating is coated on the silver alloy reflecting layer far away from the base material layer. The resulting film was designated R24.
Example 5
The difference from the embodiment 1 is that,
Figure 908596DEST_PATH_IMAGE028
the mass of (a) is 65 g,
Figure 511484DEST_PATH_IMAGE029
the mass of (a) is 30 g,
Figure 44097DEST_PATH_IMAGE030
the mass of (2) is 5 g, and the prepared rare earth silicate. The prepared rare earth silicate and polyvinylidene fluoride are prepared into infrared radiation refrigeration coating, and the infrared radiation refrigeration coating is coated on the silver alloy reflecting layer far away from the base material layer. The resulting film was designated R25.
Example 6
The difference from example 5 is that the reaction was carried out at 700 ℃ in a high temperature furnace. The resulting film was designated R26.
Example 7
The difference from example 5 is that the reaction was carried out at 900 ℃ in a high temperature furnace. The resulting film was designated R27.
Example 8
The difference from example 7 is that the reaction was carried out in a high temperature furnace for 13 hours. The resulting film was designated R28.
Example 9
The difference from example 8 is that the rotation speed is 100 r/min. The resulting film was designated R29.
Example 10
The difference from example 8 is that the rotation speed is 200 r/min. The resulting film was designated R210.
Example 11
The difference from example 10 is that the particle size of the obtained rare earth silicate is 4 μm. The resulting film was designated as R211.
Example 12
The difference from example 11 is that the particle size of the obtained rare earth silicate is 100 nm. The resulting film was designated R212.
And (3) respectively putting the prepared films into a heat preservation box, covering the heat preservation box with a transparent cover plate, arranging a thermocouple temperature measuring point at the lower part of the film material, and testing for 3 hours. The R11 blank test was performed by placing a thermocouple directly into the incubator for 3 hours. And recording the temperature value of the temperature measuring point of the thermocouple after 3 hours. The results are given in table 1 below:
table 1 optical film temperature testing
Figure 508576DEST_PATH_IMAGE031
As can be seen from the table above, the addition of the Ra ion metal source improves the infrared radiation refrigeration effect. And the Ra ion metal source has better effect at 20-45%. And when the particle size of the rare earth silicate is in the micron level, the infrared radiation refrigeration effect is better. Meanwhile, the temperature, the grinding speed and the reaction time of the high-temperature furnace have certain influence on the infrared radiation refrigeration effect.
The above description is only for the purpose of illustrating the preferred embodiments of the present invention and is not to be construed as limiting the invention, and any modifications, equivalents, improvements and the like that fall within the spirit and principle of the present invention are intended to be included therein.

Claims (10)

1. An infrared radiation refrigerating optical coating, characterized in that the optical coating comprises a resin and an infrared radiation refrigerating composition dispersed in the resin; the infrared radiation refrigeration composition comprises rare earth silicate particles formed by reacting components including a rare earth source, an Ra ion metal source and an Si source.
2. An infrared radiation refrigeration optical coating as recited in claim 1, wherein the anion of said rare earth source is selected from at least one of rare earth nitrate, rare earth chloride;
and/or the presence of a gas in the gas,
the source of Ra ion metal is selected from
Figure 564723DEST_PATH_IMAGE001
Figure 560360DEST_PATH_IMAGE002
Figure 963660DEST_PATH_IMAGE003
Figure 488182DEST_PATH_IMAGE004
At least one of (a);
and/or the presence of a gas in the gas,
the Si source is selected from the group consisting of nano
Figure 39249DEST_PATH_IMAGE005
Wherein x is more than 0 and less than or equal to 2;
and/or the presence of a gas in the gas,
the resin is at least one selected from polyvinyl fluoride, polyvinylidene fluoride, polychlorotrifluoroethylene, polytetrafluoroethylene and polyvinylidene fluoride-hexafluoropropylene.
3. An infrared radiation refrigerating optical coating as recited in claim 1, wherein the cation of said rare earth source is selected from at least one of La, Sm, Eu, Gd, Tb, Dy, Er, Tm, Yb, Y, Sc.
4. An infrared radiation refrigeration optical coating as recited in claim 1, wherein said rare earth silicate particles comprise, in mass fraction, 50-77% of said rare earth source, 20-45% of said Ra ion metal source, and 0.3-10% of said Si source.
5. The infrared radiation refrigeration optical coating of claim 1 wherein the Si source is
Figure 510682DEST_PATH_IMAGE006
Particles; the particle size range of the rare earth silicate particles is 50-200nm or 1-10 mu m.
6. An infrared radiation refrigerating optical coating as claimed in claim 5 wherein said rare earth silicate particles occupy 5-20% by volume of said optical coating.
7. An infrared radiation refrigerating optical film, characterized in that the optical film comprises an infrared radiation refrigerating functional layer formed by the infrared radiation refrigerating optical coating material according to any one of claims 1 to 6.
8. The infrared radiation refrigerating optical film of claim 7 wherein the optical film further comprises a metal reflective layer.
9. An infrared radiation refrigerating optical film as recited in claim 8, wherein the thickness of the metal reflective layer is 0.15-1 μm or 1-150 nm.
10. The infrared radiation refrigeration optical film of claim 8 wherein the infrared radiation refrigeration functional layer has a thickness of 0.1 to 5 μm.
CN202111132388.7A 2021-09-27 2021-09-27 Infrared radiation refrigeration optical coating and optical film Withdrawn CN113563769A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202111132388.7A CN113563769A (en) 2021-09-27 2021-09-27 Infrared radiation refrigeration optical coating and optical film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202111132388.7A CN113563769A (en) 2021-09-27 2021-09-27 Infrared radiation refrigeration optical coating and optical film

Publications (1)

Publication Number Publication Date
CN113563769A true CN113563769A (en) 2021-10-29

Family

ID=78174699

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202111132388.7A Withdrawn CN113563769A (en) 2021-09-27 2021-09-27 Infrared radiation refrigeration optical coating and optical film

Country Status (1)

Country Link
CN (1) CN113563769A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115353779A (en) * 2022-08-18 2022-11-18 江苏博云塑业股份有限公司 Radiation refrigeration coating, preparation method thereof and radiation refrigeration film
CN115537056A (en) * 2022-08-18 2022-12-30 江苏博云塑业股份有限公司 Rare earth silicate, radiation refrigeration composition, radiation refrigeration coating and preparation method
CN117567894A (en) * 2024-01-11 2024-02-20 中稀易涂科技发展有限公司 High-emission rare earth-based radiation refrigeration coating

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006233136A (en) * 2005-02-28 2006-09-07 Hitachi Chem Co Ltd Method for producing phosphor composition and phosphor composition obtained by the method
CN108641155A (en) * 2018-04-27 2018-10-12 武汉理工大学 A kind of passive radiation cooling film and preparation method thereof
CN110305539A (en) * 2019-07-30 2019-10-08 南京工业大学 A kind of day and night Dual-efficiency radiation cooling device and preparation method thereof

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006233136A (en) * 2005-02-28 2006-09-07 Hitachi Chem Co Ltd Method for producing phosphor composition and phosphor composition obtained by the method
CN108641155A (en) * 2018-04-27 2018-10-12 武汉理工大学 A kind of passive radiation cooling film and preparation method thereof
CN110305539A (en) * 2019-07-30 2019-10-08 南京工业大学 A kind of day and night Dual-efficiency radiation cooling device and preparation method thereof

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
中等专业学校物理学编写组编: "《中等专业学校试用教材 工业性质专业适用 物理(下册)》", 31 December 1960, 人民教育出版社 *

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115353779A (en) * 2022-08-18 2022-11-18 江苏博云塑业股份有限公司 Radiation refrigeration coating, preparation method thereof and radiation refrigeration film
CN115537056A (en) * 2022-08-18 2022-12-30 江苏博云塑业股份有限公司 Rare earth silicate, radiation refrigeration composition, radiation refrigeration coating and preparation method
CN117567894A (en) * 2024-01-11 2024-02-20 中稀易涂科技发展有限公司 High-emission rare earth-based radiation refrigeration coating
CN117567894B (en) * 2024-01-11 2024-04-05 中稀易涂科技发展有限公司 High-emission rare earth-based radiation refrigeration coating

Similar Documents

Publication Publication Date Title
CN113563769A (en) Infrared radiation refrigeration optical coating and optical film
Chen et al. Robust inorganic daytime radiative cooling coating based on a phosphate geopolymer
CN110305539B (en) Day and night dual-efficiency radiation cooler and preparation method thereof
CN107160773B (en) Composite membrane with infrared radiation heat dissipation function and preparation method and application thereof
US11136241B2 (en) Heat ray shielding fine particles, heat ray shielding fine particle dispersion liquid, coating liquid for heat ray shielding layer, and heat ray shielding layer, heat ray shielding resin film, heat ray shielding dispersion body using them
CN108912572B (en) Radiation-induced cooling film with self-cleaning function and preparation method thereof
CN109341137A (en) Passive refrigeration structure based on photonic crystal
CN112679223A (en) Large-scale preparation method of three-dimensional porous nano composite cooling film
CN110330818B (en) Infrared selective radiation cooling nano functional composition and preparation method thereof
Wang et al. A facial one-pot route synthesis and characterization of Y-stabilized Sb2O3 solar reflective thermal insulating coatings
CN115537056A (en) Rare earth silicate, radiation refrigeration composition, radiation refrigeration coating and preparation method
KR101602486B1 (en) Fabricating method of light shielding structure
CN111394069B (en) Silicon dioxide coated magnesium phosphite radiation refrigeration material and preparation method thereof
JP7395826B2 (en) Composite tungsten oxide film, method for producing the same, and film-forming substrate and article having the film
JP2006213576A (en) Boride microparticle for insolation shield, dispersion for forming insolation shield body using the boride microparticle and insolation shield body, and method of manufacturing boride microparticle for insolation shield and method of manufacturing dispersion for forming insolation shield body
KR102575326B1 (en) Near-infrared absorbing material particle dispersion, near-infrared absorber, near-infrared absorber laminate, and bonded structure for near-infrared absorption
CN111471359A (en) Preparation method and application of broad-spectrum high-emission particle material
CN114716148A (en) Visible light/laser/infrared/radar compatible stealth material and preparation method thereof
WO2022138568A1 (en) Heat ray-blocking resin sheet material
TWI700383B (en) Composite metal oxide target and composite metal oxide film formed from the composite metal oxide target
CN115449252B (en) Radiation refrigeration coating and preparation method thereof
CN113604089B (en) Broadband optical absorbent and coating preparation method
WO2022138591A1 (en) Laminated structure for solar radiation shielding
Lin et al. A Dual-Layer Coating Using Nanoparticle-Polymer Hybrid Materials for Daytime Passive Radiative Cooling
CN116604906A (en) Zero-energy-consumption infrared transparent heat pump film

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
WW01 Invention patent application withdrawn after publication

Application publication date: 20211029

WW01 Invention patent application withdrawn after publication