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CN115231834A - A design method of radiation cooling glass with two-way regulation of inner and outer radiation characteristics - Google Patents

A design method of radiation cooling glass with two-way regulation of inner and outer radiation characteristics Download PDF

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CN115231834A
CN115231834A CN202210783189.0A CN202210783189A CN115231834A CN 115231834 A CN115231834 A CN 115231834A CN 202210783189 A CN202210783189 A CN 202210783189A CN 115231834 A CN115231834 A CN 115231834A
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CN115231834B (en
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陈梅洁
闫红杰
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    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C17/00Surface treatment of glass, not in the form of fibres or filaments, by coating
    • C03C17/34Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions
    • C03C17/36Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions at least one coating being a metal
    • C03C17/3602Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions at least one coating being a metal the metal being present as a layer
    • C03C17/3644Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions at least one coating being a metal the metal being present as a layer the metal being silver
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C17/00Surface treatment of glass, not in the form of fibres or filaments, by coating
    • C03C17/34Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions
    • C03C17/36Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions at least one coating being a metal
    • C03C17/3602Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions at least one coating being a metal the metal being present as a layer
    • C03C17/3657Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions at least one coating being a metal the metal being present as a layer the multilayer coating having optical properties
    • C03C17/366Low-emissivity or solar control coatings
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C17/00Surface treatment of glass, not in the form of fibres or filaments, by coating
    • C03C17/34Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions
    • C03C17/36Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions at least one coating being a metal
    • C03C17/38Surface treatment of glass, not in the form of fibres or filaments, by coating with at least two coatings having different compositions at least one coating being a metal at least one coating being a coating of an organic material
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C2218/00Methods for coating glass
    • C03C2218/10Deposition methods
    • C03C2218/15Deposition methods from the vapour phase

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Abstract

本发明公开了一种内外侧辐射特性双向调控的辐射制冷玻璃设计方法,以TiO2/Ag/TiO2作为反射层,记为NIR;PDMS作为发射层;对于室内无或关闭制冷系统的建筑,辐射制冷玻璃的结构从外到内依次为PDMS/NIR/Glass;对于室内开启制冷系统的建筑,辐射制冷玻璃的结构从外到内依次为PDMS/Glass/NIR。本发明根据室内外环境的相对变化,设计不同结构的辐射制冷玻璃,通过内外侧辐射特性双向调控以最大化的实现建筑节能降耗的目的。

Figure 202210783189

The invention discloses a design method for radiation refrigeration glass with two-way regulation of inner and outer radiation characteristics. TiO 2 /Ag/TiO 2 is used as a reflective layer, which is recorded as NIR; PDMS is used as an emission layer; for buildings without or closed indoor refrigeration systems, The structure of radiation cooling glass is PDMS/NIR/Glass from outside to inside; for buildings with indoor cooling systems, the structure of radiation cooling glass is PDMS/Glass/NIR from outside to inside. According to the relative changes of the indoor and outdoor environments, the invention designs radiation cooling glass with different structures, and realizes the purpose of building energy saving and consumption reduction to the maximum extent through the bidirectional regulation of the radiation characteristics of the inner and outer sides.

Figure 202210783189

Description

一种内外侧辐射特性双向调控的辐射制冷玻璃设计方法A design method for radiative cooling glass with two-way control of inner and outer radiation characteristics

技术领域technical field

本发明属于辐射制冷技术领域,具体涉及一种内外侧辐射特性双向调控的辐射制冷玻璃设计方法。The invention belongs to the technical field of radiation cooling, and in particular relates to a radiation cooling glass design method with bidirectional control of inner and outer radiation characteristics.

背景技术Background technique

制冷是生产生活中必不可少的需求,大多数建筑使用的传统冷却系统在消耗电力的同时产生大量的温室气体,辐射制冷技术不消耗外界能量,广泛应用于建筑节能、服饰降温、水冷风冷、电池降温等领域。窗户玻璃是建筑或车窗等封闭空间中能效最低的部分,对于这些特殊的应用场合,需要兼顾透明度和制冷双重需求,但是投射进入内部的太阳光会带入热量,影响辐射制冷性能。因此要求辐射制冷涂层满足:(1)在可见光范围(0.4~0.8μm)具有高透过率,最大限度满足室内的采光需求;(2)在太阳光波段(0.3~2.5μm)具有高反射率,以尽可能减少太阳辐射热量的积聚;(3)在大气窗口(8~13μm)具有高发射率,将热量有效地辐射到外太空。Refrigeration is an essential requirement in production and life. The traditional cooling system used in most buildings consumes electricity and produces a large amount of greenhouse gases. Radiant cooling technology does not consume external energy and is widely used in building energy saving, clothing cooling, water cooling and air cooling , battery cooling and other fields. Window glass is the part with the lowest energy efficiency in closed spaces such as buildings or car windows. For these special applications, both transparency and cooling needs to be taken into account, but the sunlight projected into the interior will bring heat and affect the radiative cooling performance. Therefore, the radiative cooling coating is required to meet: (1) high transmittance in the visible light range (0.4-0.8 μm) to meet the indoor lighting requirements to the greatest extent; (2) high reflection in the sunlight band (0.3-2.5 μm) Efficiency to reduce the accumulation of solar radiation heat as much as possible; (3) High emissivity in the atmospheric window (8-13μm), effectively radiating heat to outer space.

已经有学者针对透明辐射制冷涂层展开研究,并将其用于制备辐射制冷玻璃,进而用于建筑节能,但是其均只考虑了室外环境(如地理位置、天气条件等)变化的影响,并未涉及室内环境变化的影响,从而导致制得的辐射制冷玻璃不能最大化的实现节能降耗的目的。Some scholars have conducted research on transparent radiative cooling coatings, and used them to prepare radiative cooling glass for building energy saving, but they only considered the impact of changes in the outdoor environment (such as geographical location, weather conditions, etc.) The impact of indoor environment changes is not involved, so that the obtained radiant cooling glass cannot maximize energy saving and consumption reduction.

发明内容Contents of the invention

为了解决现有辐射制冷玻璃存在的缺陷,本发明的目的在于提供一种内外侧辐射特性双向调控的辐射制冷玻璃设计方法,根据室内外环境的相对变化,设计不同结构的辐射制冷玻璃,通过内外侧辐射特性双向调控以最大化的实现建筑节能降耗的目的。In order to solve the defects existing in the existing radiation cooling glass, the purpose of the present invention is to provide a radiation cooling glass design method with two-way control of the radiation characteristics of the inside and outside, according to the relative changes in the indoor and outdoor environments, design radiation cooling glass with different structures, through the inner and outer The two-way regulation of the outer radiation characteristics maximizes the energy saving and consumption reduction of the building.

为了实现上述技术目的,本发明采用如下技术方案:In order to realize above-mentioned technical purpose, the present invention adopts following technical scheme:

一种内外侧辐射特性双向调控的辐射制冷玻璃设计方法,以TiO2/Ag/TiO2作为反射层,记为NIR;PDMS作为发射层;A radiation cooling glass design method with two-way control of the radiation characteristics inside and outside, using TiO 2 /Ag/TiO 2 as the reflective layer, denoted as NIR; PDMS as the emitting layer;

对于室内无或关闭制冷系统的建筑,辐射制冷玻璃的结构从外到内依次为PDMS/NIR/Glass;For buildings without or with closed cooling systems indoors, the structure of radiative cooling glass is PDMS/NIR/Glass from outside to inside;

对于室内开启制冷系统的建筑,辐射制冷玻璃的结构从外到内依次为PDMS/Glass/NIR。For buildings with indoor refrigeration systems, the structure of radiant cooling glass is PDMS/Glass/NIR from outside to inside.

发明人发现,建筑的制冷能耗不仅受地理位置和天气条件的影响,同时室内空调系统的开闭对制冷能耗也会产生影响。在夏季炎热天气中,对于开启空调系统的建筑,其外部结构(包括屋顶、墙壁和窗户等)温度较高,而室内温度较低,内层具有低发射率,高反射率的节能窗可以最大程度上减少外界对建筑室内的传热,维持内部较低温度,从而降低制冷能耗;而对于无或关闭空调系统的建筑,由于其太阳光透过玻璃对室内的加热,使得室内温度较高,内层具有高发射率,即高吸收率的节能窗可以提高建筑室内向外部散热,以达到降低室内温度,节约制冷能耗的效果。因此,本发明根据室内外环境的相对变化,设计不同结构的辐射制冷玻璃,通过内外侧辐射特性双向调控以最大化的实现建筑节能降耗的目的。The inventors found that the cooling energy consumption of a building is not only affected by geographical location and weather conditions, but also the opening and closing of the indoor air-conditioning system will also have an impact on the cooling energy consumption. In hot summer weather, for buildings with air-conditioning systems turned on, the temperature of the external structure (including the roof, walls, and windows, etc.) is high, while the indoor temperature is low, and the inner layer has low emissivity. Reduce the heat transfer from the outside to the interior of the building to a certain extent, maintain a lower internal temperature, thereby reducing cooling energy consumption; and for buildings without or with air-conditioning systems turned off, the indoor temperature is higher due to the heating of the interior by sunlight through the glass , The inner layer has a high emissivity, that is, energy-saving windows with a high absorption rate can improve the heat dissipation from the interior of the building to the outside, so as to reduce the indoor temperature and save cooling energy consumption. Therefore, according to the relative changes of the indoor and outdoor environments, the present invention designs radiation cooling glass with different structures, and achieves the purpose of building energy saving and consumption reduction to the greatest extent through bidirectional regulation of the radiation characteristics of the inside and outside.

上述设计方法中,PDMS厚度的设计方法具体为:Among the above design methods, the design method of PDMS thickness is as follows:

大气窗口平均发射率

Figure BDA0003730534200000021
Atmospheric window average emissivity
Figure BDA0003730534200000021

其中,IBB(T,λ)表示温度为T的黑体光谱发射强度,ε(λ)表示涂层的发射率;Among them, I BB (T, λ) represents the emission intensity of the blackbody spectrum at temperature T, and ε(λ) represents the emissivity of the coating;

如图1所示,在中红外部分,单层Ag膜和TiO2/Ag/TiO2三层膜的反射率基本一致,将TiO2/Ag/TiO2简化为单层的Ag膜,选定Ag膜的厚度,并设定PDMS厚度HPDMS与Ag膜的厚度在同一数量级范围内变化,计算得到大气窗口平均发射率

Figure BDA0003730534200000022
进而选定PDMS厚度。As shown in Figure 1, in the mid-infrared part, the reflectivity of the single-layer Ag film and the TiO 2 /Ag/TiO 2 three-layer film are basically the same. The TiO 2 /Ag/TiO 2 is simplified as a single-layer Ag film, and the selected The thickness of the Ag film, and the PDMS thickness is set. The thickness of the PDMS and the Ag film varies within the same order of magnitude, and the average emissivity of the atmospheric window is calculated.
Figure BDA0003730534200000022
The PDMS thickness is then selected.

进一步优选的,选定Ag膜的厚度为10μm,PDMS厚度HPDMS在10μm~100μm范围内变化,计算大气窗口平均发射率

Figure BDA0003730534200000023
如图2所示,当PDMS厚度HPDMS为50μm时,
Figure BDA0003730534200000024
当PDMS厚度HPDMS继续增长时,大气窗口平均发射率
Figure BDA0003730534200000025
增长趋于平坦,故选定PDMS厚度范围为50μm~100μm;最优选的PDMS厚度HPDMS=50μm。Further preferably, the thickness of the selected Ag film is 10 μm, and the PDMS thickness H PDMS varies in the range of 10 μm to 100 μm, and the average emissivity of the atmospheric window is calculated
Figure BDA0003730534200000023
As shown in Figure 2, when the PDMS thickness H PDMS is 50 μm,
Figure BDA0003730534200000024
Atmospheric window average emissivity when PDMS thickness H PDMS continues to grow
Figure BDA0003730534200000025
The growth tends to be flat, so the selected PDMS thickness ranges from 50 μm to 100 μm; the most preferred PDMS thickness H PDMS =50 μm.

上述设计方法中,TiO2/Ag/TiO2厚度的设计方法具体为:Among the above design methods, the design method of the thickness of TiO 2 /Ag/TiO 2 is as follows:

平均可见光透过率

Figure BDA0003730534200000026
Average Visible Light Transmittance
Figure BDA0003730534200000026

平均太阳光反射率

Figure BDA0003730534200000027
Average solar reflectance
Figure BDA0003730534200000027

其中,IAM1.5(λ)表示AM1.5标准太阳强度,T(λ)、R(λ)分别表示涂层的光谱透过率、反射率;Wherein, I AM1.5 (λ) represents AM1.5 standard solar intensity, and T (λ), R (λ) represent spectral transmittance, reflectivity of coating respectively;

太阳光波段,在同一数量级范围内,选定Ag膜的厚度HAg和上下两层TiO2的厚度H1、H2,计算不同厚度组合下的平均太阳光反射率

Figure BDA0003730534200000031
和平均可见光透过率
Figure BDA0003730534200000032
In the sunlight band, within the same order of magnitude, the thickness of the Ag film H Ag and the thicknesses H 1 and H 2 of the upper and lower layers of TiO 2 are selected to calculate the average solar reflectance under different thickness combinations
Figure BDA0003730534200000031
and average visible light transmittance
Figure BDA0003730534200000032

为了满足最低要求的日常采光需求,取平均可见光透过率

Figure BDA0003730534200000033
不低于0.7,基于此,取最大
Figure BDA0003730534200000034
出现的HAg、H1、H2,分别设定为Ag膜的厚度、上层TiO2的厚度、下层TiO2的厚度。In order to meet the minimum daily lighting requirements, take the average visible light transmittance
Figure BDA0003730534200000033
Not less than 0.7, based on this, take the maximum
Figure BDA0003730534200000034
H Ag , H 1 , and H 2 appearing are respectively set as the thickness of the Ag film, the thickness of the upper layer TiO 2 , and the thickness of the lower layer TiO 2 .

进一步优选的,太阳光波段,考虑蒸镀纳米尺度膜的误差,在5~30nm范围内,以5nm为间隔选取Ag膜的厚度HAg,在0~60nm的厚度范围内,以10nm为间隔选取上下两层TiO2的厚度H1、H2,计算不同厚度组合下的平均太阳光反射率

Figure BDA0003730534200000035
和平均可见光透过率
Figure BDA0003730534200000036
Further preferably, in the solar light band, considering the error of vapor-depositing nanoscale films, the thickness H Ag of the Ag film is selected at intervals of 5 nm within the range of 5 to 30 nm, and at intervals of 10 nm within the range of thickness of 0 to 60 nm. The thickness H 1 and H 2 of the upper and lower layers of TiO 2 is used to calculate the average solar reflectance under different thickness combinations
Figure BDA0003730534200000035
and average visible light transmittance
Figure BDA0003730534200000036

取平均可见光透过率

Figure BDA0003730534200000037
不低于0.7,基于此,如图3所示,最大
Figure BDA0003730534200000038
出现在HAg=25nm,H1=H2=40nm处,此时该辐射制冷玻璃在满足采光需求下,具有最优的辐射制冷性能。Take the average visible light transmittance
Figure BDA0003730534200000037
not less than 0.7, based on this, as shown in Figure 3, the maximum
Figure BDA0003730534200000038
Appearing at H Ag =25nm, H 1 =H 2 =40nm, at this time, the radiation cooling glass has the best radiation cooling performance under the condition of meeting the lighting requirements.

本发明的优势在于:The advantages of the present invention are:

本发明根据室内外环境的相对变化,设计了PDMS/NIR/Glass和PDMS/Glass/NIR两种不同结构的辐射制冷玻璃,二者均使用PDMS作为发射涂层,TiO2/Ag/TiO2作为反射涂层,外层结构的光谱特性曲线保持一致,均具有高太阳光反射率,高可见光透过率和高大气窗口发射率。PDMS/Glass/NIR将反射涂层置于玻璃最内层,其内层平均发射率

Figure BDA0003730534200000039
外层大气窗口平均发射率
Figure BDA00037305342000000310
PDMS/NIR/Glass则将玻璃作为最内层,其内层平均发射率
Figure BDA00037305342000000311
外层大气窗口平均发射率
Figure BDA00037305342000000312
本发明证实了辐射制冷玻璃内层发射率对开启和关闭空调系统建筑内部温度的影响,对于室内无或关闭空调系统的建筑应选用具有高内层发射率的辐射制冷玻璃,对于开启空调系统的建筑应选用具有低内层发射率的辐射制冷玻璃,通过内外侧辐射特性双向调控,从而实现建筑内部降温和节约制冷能耗的目的。According to the relative changes of indoor and outdoor environments, the present invention designs radiation cooling glasses with two different structures, PDMS/NIR/Glass and PDMS/Glass/NIR, both of which use PDMS as the emission coating, and TiO 2 /Ag/TiO 2 as the The reflective coating and the spectral characteristic curve of the outer structure are consistent, and all have high solar reflectance, high visible light transmittance and high atmospheric window emissivity. PDMS/Glass/NIR places the reflective coating on the innermost layer of the glass, and the average emissivity of the inner layer
Figure BDA0003730534200000039
Average emissivity of the outer atmosphere window
Figure BDA00037305342000000310
PDMS/NIR/Glass uses glass as the innermost layer, and the average emissivity of the inner layer
Figure BDA00037305342000000311
Average emissivity of the outer atmosphere window
Figure BDA00037305342000000312
The present invention proves the influence of the emissivity of the inner layer of the radiation cooling glass on the internal temperature of the building with the air-conditioning system turned on and off. For buildings without or with the air-conditioning system closed indoors, radiation cooling glass with a high inner layer emissivity should be selected. For buildings with the air-conditioning system turned on Buildings should use radiation-cooled glass with low inner layer emissivity, and through two-way regulation of the inner and outer radiation characteristics, so as to achieve the purpose of cooling the building and saving cooling energy consumption.

附图说明Description of drawings

图1为中红外部分单层Ag膜和TiO2/Ag/TiO2三层膜的反射率图;Figure 1 is a reflectance diagram of a single-layer Ag film and a TiO 2 /Ag/TiO 2 three-layer film in the mid-infrared part;

图2为PDMS厚度HPDMS与大气窗口平均发射率

Figure BDA0003730534200000041
的关系变化图;Figure 2 shows the PDMS thickness H PDMS and the average emissivity of the atmospheric window
Figure BDA0003730534200000041
The relationship change diagram;

图3为TiO2/Ag/TiO2中的Ag厚度HAg与平均可见光透过率

Figure BDA0003730534200000042
和平均太阳光反射率
Figure BDA0003730534200000043
的关系变化图。Figure 3 shows the Ag thickness H Ag and the average visible light transmittance in TiO 2 /Ag/TiO 2
Figure BDA0003730534200000042
and mean solar reflectance
Figure BDA0003730534200000043
relationship change graph.

图4为PDMS(50μm)/TiO2(40nm)/Ag(25nm)/TiO2(40nm)/Glass辐射制冷玻璃的光谱特性曲线;Fig. 4 is the spectral characteristic curve of PDMS(50μm)/TiO 2 (40nm)/Ag(25nm)/TiO 2 (40nm)/Glass radiation cooling glass;

图5为不同内层发射率辐射制冷玻璃应用,其中:(a)开启空调系统模型;(b)无或关闭空调系统模型;(c)低内层发射率辐射制冷玻璃内外侧实验光谱特性;(d)高内层发射率辐射制冷玻璃内外侧实验光谱特性;(e)开启空调系统内部温度随内层发射率变化;(f)无或关闭空调系统内部温度随内层发射率变化。Figure 5 shows the application of radiation cooling glass with different inner layer emissivity, in which: (a) model with air conditioning system turned on; (b) model without or with air conditioning system turned off; (c) experimental spectral characteristics of the inside and outside of radiation cooling glass with low inner layer emissivity; (d) Experimental spectral characteristics of the inner and outer sides of radiation-cooled glass with high inner emissivity; (e) The internal temperature of the air-conditioning system changes with the emissivity of the inner layer; (f) The internal temperature of the air-conditioning system with no or closed changes with the emissivity of the inner layer.

具体实施方式Detailed ways

现结合实施例对本发明的技术方案进行进一步说明,但是本发明不仅限于下述的实施情形。The technical solutions of the present invention will now be further described in conjunction with examples, but the present invention is not limited to the following implementation situations.

本发明中选择75mm×75mm玻璃基片为基底,利用热蒸发镀膜制备反射涂层,得到NIR/Glass和Glass/NIR透明反射玻璃。使用涂膜器制备PDMS发射涂层,得到PDMS/NIR/Glass和PDMS/Glass/NIR透明辐射制冷玻璃。In the present invention, a 75mm×75mm glass substrate is selected as a substrate, and a reflective coating is prepared by thermal evaporation coating to obtain NIR/Glass and Glass/NIR transparent reflective glass. The PDMS emissive coating was prepared using a film applicator to obtain PDMS/NIR/Glass and PDMS/Glass/NIR transparent radiation cooling glass.

1、PDMS层的厚度设计方法为:1. The thickness design method of PDMS layer is:

大气窗口平均发射率

Figure BDA0003730534200000044
Atmospheric window average emissivity
Figure BDA0003730534200000044

其中,IBB(T,λ)表示温度为T的黑体光谱发射强度,ε(λ)表示涂层的发射率;Among them, I BB (T, λ) represents the emission intensity of the blackbody spectrum at temperature T, and ε(λ) represents the emissivity of the coating;

如图1所示,在中红外部分,单层Ag膜和TiO2/Ag/TiO2三层膜的反射率基本一致,将TiO2/Ag/TiO2简化为单层的Ag膜,选定Ag膜的厚度为10μm,涂覆10μm~100μm范围内不同厚度PDMS,计算大气窗口平均发射率

Figure BDA0003730534200000045
可以发现大气窗口平均发射率随着PDMS层厚度的增加而逐渐增大,当HPDMS=50μm时,
Figure BDA0003730534200000046
此后HPDMS
Figure BDA0003730534200000047
影响较小,增长趋于平坦,故选定PDMS层的最佳厚度为50μm。As shown in Figure 1, in the mid-infrared part, the reflectance of the single-layer Ag film and the TiO 2 /Ag/TiO 2 three-layer film are basically the same, and the TiO 2 /Ag/TiO 2 is simplified as a single-layer Ag film, and the selected The thickness of the Ag film is 10 μm, and PDMS with different thicknesses in the range of 10 μm to 100 μm is coated, and the average emissivity of the atmospheric window is calculated
Figure BDA0003730534200000045
It can be found that the average emissivity of the atmospheric window increases gradually with the increase of the thickness of the PDMS layer. When H PDMS =50 μm,
Figure BDA0003730534200000046
Thereafter H PDMS pair
Figure BDA0003730534200000047
The influence is small, and the growth tends to be flat, so the optimal thickness of the selected PDMS layer is 50 μm.

2、TiO2/Ag/TiO2层的厚度设计方法为:2. The thickness design method of TiO 2 /Ag/TiO 2 layer is:

平均可见光透过率

Figure BDA0003730534200000051
Average Visible Light Transmittance
Figure BDA0003730534200000051

平均太阳光反射率

Figure BDA0003730534200000052
Average solar reflectance
Figure BDA0003730534200000052

其中,IAM1.5(λ)表示AM1.5标准太阳强度,T(λ)、R(λ)分别表示涂层的光谱透过率、反射率;Wherein, I AM1.5 (λ) represents AM1.5 standard solar intensity, and T (λ), R (λ) represent spectral transmittance, reflectivity of coating respectively;

太阳光波段,考虑蒸镀膜层厚度误差,在5~30nm范围内,以5nm为间隔选取Ag膜的厚度HAg,在0~60nm的厚度范围内,以10nm为间隔选取上下两层TiO2的厚度H1、H2,计算不同厚度组合下的平均太阳光反射率

Figure BDA0003730534200000053
和平均可见光透过率
Figure BDA0003730534200000054
In the solar light band, considering the thickness error of the evaporated film, within the range of 5-30nm, select the thickness H Ag of the Ag film at an interval of 5nm, and within the thickness range of 0-60nm, select the upper and lower layers of TiO2 Thickness H 1 , H 2 , calculate the average solar reflectance under different thickness combinations
Figure BDA0003730534200000053
and average visible light transmittance
Figure BDA0003730534200000054

对于建筑节能设计来讲,为了满足最低要求的日常采光需求,通常需要满足平均可见光透过率

Figure BDA0003730534200000055
不低于0.7。当要求
Figure BDA0003730534200000056
不低于0.7时,最大
Figure BDA0003730534200000057
出现在HAg=25nm处,优化得到的对应结构的PDMS(50μm)/TiO2(40nm)/Ag(25nm)/TiO2(40nm)/Glass辐射制冷玻璃的光谱特性曲线见图4。For building energy-saving design, in order to meet the minimum daily lighting requirements, it is usually necessary to meet the average visible light transmittance
Figure BDA0003730534200000055
Not less than 0.7. when requested
Figure BDA0003730534200000056
Not less than 0.7 when the maximum
Figure BDA0003730534200000057
Appearing at H Ag = 25nm, the optimized spectral characteristic curve of PDMS(50μm)/TiO 2 (40nm)/Ag(25nm)/TiO 2 (40nm)/Glass radiation cooling glass with corresponding structure is shown in Fig. 4 .

3、不同内层发射率辐射制冷玻璃应用3. Application of radiation cooling glass with different inner layer emissivity

建筑的制冷能耗不仅受地理位置和天气条件的影响,同时室内空调系统的开闭对制冷能耗也会产生影响。在夏季炎热天气中,对于开启空调系统的建筑,其外部结构(包括屋顶、墙壁和窗户等)温度较高,而室内温度较低,内层具有低发射率,高反射率的辐射制冷玻璃可以最大程度上减少对建筑室内的传热,维持内部较低温度,从而降低制冷能耗,如图5a所示;对于无或关闭空调系统的建筑,其外部结构的温度较低,而室内空气的温度较高,内层具有高发射率,即高吸收率的辐射制冷玻璃可以提高建筑室内向外部散热,以达到降低室内温度,节约制冷能耗的效果,如图5b所示。针对不同的建筑选取不同结构的辐射制冷玻璃是降低制冷能耗的有效策略。The cooling energy consumption of a building is not only affected by the geographical location and weather conditions, but also the opening and closing of the indoor air conditioning system will also have an impact on the cooling energy consumption. In hot summer weather, for buildings with air-conditioning systems turned on, the temperature of the external structure (including the roof, walls and windows, etc.) is high, while the indoor temperature is low, the inner layer has low emissivity, and the radiant cooling glass with high reflectivity can Minimize the heat transfer to the interior of the building to maintain a low internal temperature, thereby reducing cooling energy consumption, as shown in Figure 5a; for buildings without or with air-conditioning systems turned off, the temperature of the external structure is low, while the indoor air The temperature is high, and the inner layer has a high emissivity, that is, the radiation cooling glass with a high absorption rate can improve the heat dissipation from the interior of the building to the outside, so as to reduce the indoor temperature and save cooling energy consumption, as shown in Figure 5b. Choosing radiant cooling glass with different structures for different buildings is an effective strategy to reduce cooling energy consumption.

本发明设计了PDMS/NIR/Glass和PDMS/Glass/NIR两种不同结构的辐射制冷玻璃,二者均使用PDMS作为发射涂层,TiO2/Ag/TiO2作为反射涂层,外层结构的光谱特性曲线保持一致,均具有高太阳光反射率,高可见光透过率和高大气窗口发射率,它们的光谱特性曲线如图5c和5d所示。PDMS/Glass/NIR将反射涂层置于辐射制冷玻璃最内层,其内层平均发射率

Figure BDA0003730534200000061
外层大气窗口平均发射率
Figure BDA0003730534200000062
PDMS/NIR/Glass将玻璃基底作为辐射制冷玻璃的最内层,其内层平均发射率
Figure BDA0003730534200000063
外层大气窗口平均发射率
Figure BDA0003730534200000064
The present invention designs radiation cooling glasses with two different structures, PDMS/NIR/Glass and PDMS/Glass/NIR, both of which use PDMS as the emission coating, TiO 2 /Ag/TiO 2 as the reflection coating, and the outer layer structure The spectral characteristic curves are consistent, and they all have high solar reflectance, high visible light transmittance and high atmospheric window emissivity, and their spectral characteristic curves are shown in Figure 5c and 5d. PDMS/Glass/NIR puts the reflective coating on the innermost layer of radiation cooling glass, and the average emissivity of the inner layer
Figure BDA0003730534200000061
Average emissivity of the outer atmosphere window
Figure BDA0003730534200000062
PDMS/NIR/Glass uses the glass substrate as the innermost layer of radiation cooling glass, and the average emissivity of the inner layer
Figure BDA0003730534200000063
Average emissivity of the outer atmosphere window
Figure BDA0003730534200000064

为了比较不同内层发射率辐射制冷玻璃的制冷性能,基于能量守恒方程,计算了不同内层发射率玻璃下室内温度。建筑开启空调系统时的计算结果如图5e所示,随着辐射制冷玻璃内层发射率的降低,高温辐射制冷玻璃与低温建筑内壁的辐射换热减弱,减小了系统内部冷量的丧失,内部平均温度降低,最高温度逐渐升高,因为系统最高温度为辐射制冷玻璃温度。建筑关闭空调系统时的计算结果如图5f所示,可知随着辐射制冷玻璃内层发射率的增加,低温辐射制冷玻璃与高温建筑内壁的辐射换热增强,系统向外界环境散热增强,系统平衡时内部最高温度和平均温度逐渐降低。计算结果证实了辐射制冷玻璃内层发射率对开启和关闭空调系统建筑内部温度的影响,对于无或者关闭空调系统的建筑应选用具有高内层发射率的辐射制冷玻璃,对于开启空调系统的建筑应选用具有低内层发射率的辐射制冷玻璃,从而实现建筑内部降温和节约制冷能耗的目的。In order to compare the cooling performance of radiation cooling glasses with different inner emissivity, the indoor temperature under the glass with different inner emissivity was calculated based on the energy conservation equation. The calculation results when the building’s air-conditioning system is turned on are shown in Figure 5e. As the emissivity of the inner layer of the radiative cooling glass decreases, the radiation heat exchange between the high-temperature radiative cooling glass and the inner wall of the low-temperature building weakens, reducing the loss of internal cooling capacity of the system. The average internal temperature decreases and the maximum temperature gradually increases as the maximum system temperature is the radiatively cooled glass temperature. The calculation results when the building’s air-conditioning system is turned off are shown in Figure 5f. It can be seen that with the increase of the emissivity of the inner layer of the radiative cooling glass, the radiation heat exchange between the low-temperature radiative cooling glass and the inner wall of the high-temperature building is enhanced, and the heat dissipation of the system to the external environment is enhanced, and the system is balanced. The maximum internal temperature and the average temperature gradually decrease. The calculation results confirm the influence of the emissivity of the inner layer of radiative cooling glass on the internal temperature of the building with the air-conditioning system turned on and off. For buildings without or with the air-conditioning system turned off, radiation-cooled glass with high inner layer emissivity should be selected. For buildings with the air-conditioning system turned on Radiation cooling glass with low inner layer emissivity should be selected to achieve cooling inside the building and save cooling energy consumption.

Claims (5)

1.一种内外侧辐射特性双向调控的辐射制冷玻璃设计方法,其特征在于,以TiO2/Ag/TiO2作为反射层,记为NIR;PDMS作为发射层;1. A radiation cooling glass design method with two-way regulation of the radiation characteristics inside and outside, characterized in that TiO 2 /Ag/TiO 2 is used as the reflection layer, denoted as NIR; PDMS is used as the emission layer; 对于室内无或关闭制冷系统的建筑,辐射制冷玻璃的结构从外到内依次为PDMS/NIR/Glass;For buildings with no or closed indoor cooling system, the structure of radiation cooling glass is PDMS/NIR/Glass from outside to inside; 对于室内开启制冷系统的建筑,辐射制冷玻璃的结构从外到内依次为PDMS/Glass/NIR。For buildings with indoor refrigeration systems, the structure of radiant cooling glass is PDMS/Glass/NIR from outside to inside. 2.根据权利要求1所述的设计方法,其特征在于,PDMS厚度的设计方法具体为:2. the design method according to claim 1, is characterized in that, the design method of PDMS thickness is specifically: 大气窗口平均发射率
Figure FDA0003730534190000011
Atmospheric window average emissivity
Figure FDA0003730534190000011
其中,IBB(T,λ)表示温度为T的黑体光谱发射强度,ε(λ)表示涂层的发射率;Among them, I BB (T,λ) represents the black body spectral emission intensity at temperature T, and ε(λ) represents the emissivity of the coating; 将TiO2/Ag/TiO2简化为单层的Ag膜,选定Ag膜的厚度,并设定PDMS厚度HPDMS与Ag膜的厚度在同一数量级范围内变化,计算得到大气窗口平均发射率
Figure FDA0003730534190000012
进而选定PDMS厚度。
Simplify TiO 2 /Ag/TiO 2 into a single-layer Ag film, select the thickness of the Ag film, and set the PDMS thickness H. The thickness of PDMS and the Ag film change within the same order of magnitude, and calculate the average emissivity of the atmospheric window
Figure FDA0003730534190000012
Then select the thickness of PDMS.
3.根据权利要求2所述的设计方法,其特征在于,选定Ag膜的厚度为10μm,PDMS厚度HPDMS在10μm~100μm范围内变化,计算大气窗口平均发射率
Figure FDA0003730534190000013
当PDMS厚度HPDMS不低于50μm时,大气窗口平均发射率
Figure FDA0003730534190000014
增长趋于平坦,进而选定PDMS厚度范围为50μm~100μm。
3. design method according to claim 2, it is characterized in that, the thickness of selected Ag film is 10 μ m, PDMS thickness H PDMS changes in the scope of 10 μ m~100 μ m, calculates atmospheric window average emissivity
Figure FDA0003730534190000013
Atmospheric window average emissivity when PDMS thickness H PDMS is not less than 50 μm
Figure FDA0003730534190000014
The growth tends to be flat, and the PDMS thickness range is selected to be 50 μm to 100 μm.
4.根据权利要求1所述的设计方法,其特征在于,TiO2/Ag/TiO2厚度的设计方法具体为:4. The design method according to claim 1, characterized in that the design method for the thickness of TiO 2 /Ag/TiO 2 is specifically: 平均可见光透过率
Figure FDA0003730534190000015
Average Visible Light Transmittance
Figure FDA0003730534190000015
平均太阳光反射率
Figure FDA0003730534190000016
Average solar reflectance
Figure FDA0003730534190000016
其中,IAM1.5(λ)表示AM1.5标准太阳强度,T(λ)、R(λ)分别表示涂层的光谱透过率、反射率;Among them, I AM1.5 (λ) represents the AM1.5 standard solar intensity, and T(λ) and R(λ) represent the spectral transmittance and reflectance of the coating, respectively; 太阳光波段,在同一数量级范围内,选定Ag膜的厚度HAg和上下两层TiO2的厚度H1、H2,计算不同厚度组合下的平均太阳光反射率
Figure FDA0003730534190000017
和平均可见光透过率
Figure FDA0003730534190000021
In the sunlight band, within the same order of magnitude, the thickness of the Ag film H Ag and the thicknesses H 1 and H 2 of the upper and lower layers of TiO 2 are selected to calculate the average solar reflectance under different thickness combinations
Figure FDA0003730534190000017
and average visible light transmittance
Figure FDA0003730534190000021
取平均可见光透过率
Figure FDA0003730534190000022
不低于0.7,基于此,取最大
Figure FDA0003730534190000023
出现的HAg、H1、H2,分别设定为Ag膜的厚度、上层TiO2的厚度、下层TiO2的厚度。
Take the average visible light transmittance
Figure FDA0003730534190000022
Not less than 0.7, based on this, take the maximum
Figure FDA0003730534190000023
H Ag , H 1 , and H 2 appearing are respectively set as the thickness of the Ag film, the thickness of the upper layer TiO 2 , and the thickness of the lower layer TiO 2 .
5.根据权利要求4所述的设计方法,其特征在于,太阳光波段,在5~30nm范围内,以5nm为间隔选取Ag膜的厚度HAg,在0~60nm的厚度范围内,以10nm为间隔选取上下两层TiO2的厚度H1、H2,计算不同厚度组合下的平均太阳光反射率
Figure FDA0003730534190000024
和平均可见光透过率
Figure FDA0003730534190000025
5. The design method according to claim 4, characterized in that, in the solar light band, within the range of 5-30nm, the thickness H Ag of the Ag film is selected at an interval of 5nm, and within the thickness range of 0-60nm, the thickness H Ag of the Ag film is selected at an interval of 10nm Select the thickness H 1 and H 2 of the upper and lower layers of TiO 2 as the interval, and calculate the average solar reflectance under different thickness combinations
Figure FDA0003730534190000024
and average visible light transmittance
Figure FDA0003730534190000025
取平均可见光透过率
Figure FDA0003730534190000026
不低于0.7,基于此,最大
Figure FDA0003730534190000027
出现在HAg=25nm,H1=H2=40nm处。
Take the average visible light transmittance
Figure FDA0003730534190000026
not less than 0.7, based on which the maximum
Figure FDA0003730534190000027
Appears at H Ag = 25 nm, H 1 = H 2 = 40 nm.
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