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JP6510197B2 - Heat shield / insulation material and its manufacturing method - Google Patents
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JP6510197B2 - Heat shield / insulation material and its manufacturing method - Google Patents

Heat shield / insulation material and its manufacturing method Download PDF

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JP6510197B2
JP6510197B2 JP2014165594A JP2014165594A JP6510197B2 JP 6510197 B2 JP6510197 B2 JP 6510197B2 JP 2014165594 A JP2014165594 A JP 2014165594A JP 2014165594 A JP2014165594 A JP 2014165594A JP 6510197 B2 JP6510197 B2 JP 6510197B2
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良典 平野
良典 平野
敏文 加藤
敏文 加藤
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Nippon Filcon Co Ltd
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本発明は、太陽光及びその他の熱源からの熱エネルギを遮熱及び断熱する遮熱・断熱材及びその製法に関連する。   The present invention relates to a heat shield and heat insulating material for shielding and insulating heat energy from sunlight and other heat sources and a method of manufacturing the same.

原子力発電所の稼働停止に伴う電力供給力不足や大規模停電は、産業界だけでなく我が国社会全体に大きな影響を与えている。原子力の代替エネルギの目処が立たない現段階では、節電により電力需要を低減する以外、電力不足に対応する手段はなく、特にビル、家屋等の建物の空調設備が整備された今日では、夏場及び冬場の電力供給ピーク時の節電、電力需要の削減が急務となる。   The power supply shortage and large-scale blackouts caused by the shutdown of nuclear power plants have a great impact not only on industry but also on the whole of Japanese society. At the current stage where there is no prospect of alternative energy for nuclear power, there is no means to cope with the power shortage other than reducing the power demand by saving electricity, especially in the summer and in the air conditioning facilities of buildings such as buildings and houses. It is urgently needed to save electricity at the peak of power supply in winter and to reduce the demand for electricity.

空調使用電力の低減を目的として、屋根、建物壁、窓、ブラインド等に断熱及び遮熱処理を施し、夏は太陽光による熱エネルギの建物内への熱移動を遮断し、冬は外部への熱放出を防ぐ。「断熱」は、過密状態で接触した物質間の熱伝達の遮断を意味し、「遮熱」は、真空を含む空間を移動する熱エネルギ放射(輻射)の遮蔽を意味する。しかし、通常の熱移動では、両者が併存するため断熱と遮熱を厳密に区分けすることはできない。   In order to reduce power consumption for air conditioning, the roof, building walls, windows, blinds, etc. are thermally insulated and heat-insulated. In summer, heat transfer from sunlight to the building is blocked, and in winter, heat is transferred to the outside Prevent the release. "Adiabatic" refers to the interruption of heat transfer between densely contacted materials, and "thermal insulation" refers to the shielding of thermal energy radiation (radiation) moving through the space containing the vacuum. However, in normal heat transfer, heat insulation and heat shield can not be strictly divided because the two coexist.

近年、真空粒子を用いた断熱技術が注目されている。真空粒子は、セラミック外殻の内部にほぼ真空状態又は減圧状態の内部空洞を有する粒子であり、高断熱、低蓄熱の特徴を持つ。以下、真空粒子を断熱材又は遮熱材に適用した従来技術を示す。   In recent years, heat insulation technology using vacuum particles has attracted attention. The vacuum particle is a particle having an internal cavity in a substantially vacuum state or a reduced pressure state inside the ceramic shell, and has features of high heat insulation and low heat storage. Hereinafter, the prior art which applied vacuum particle | grains to the heat insulating material or the heat insulating material is shown.

特許文献1は、支持体の片面又は両面に熱絶縁性の粒子を複数層接合する柔軟性熱絶縁体を示し、柔軟性熱絶縁体をブラインド又はロールスクリーンに適用する。熱絶縁性粒子として、真空セラミック粒子、酸化チタニウム粒子を使用し、柔軟性熱絶縁体は、小隙間で過密に配置される大小複数の熱絶縁性粒子を含有する。   U.S. Pat. No. 5,959,099 shows a flexible thermal insulator in which multiple layers of thermally insulating particles are bonded to one or both sides of a support, wherein the flexible thermal insulator is applied to a blind or roll screen. Vacuum ceramic particles and titanium oxide particles are used as the heat insulating particles, and the flexible heat insulator contains a plurality of large and small heat insulating particles which are densely arranged in small gaps.

しかしながら、真空セラミック粒子は、非常に高価であるため、特許文献1の真空セラミック粒子の過密使用では、柔軟性熱絶縁体並びにブラインド及びロールスクリーンも当然高価となり、真空セラミック粒子のコストが柔軟性熱絶縁体の原料原価の7割以上を占める。また、特許文献1の柔軟性熱絶縁体では、多量の真空セラミック粒子同士が小さい隙間を介して互いに密に配置されるため、真空の内部空洞では熱伝導は生じないが、真空セラミック粒子の外殻に沿って熱伝導し易くなる。このため、真空セラミック粒子使用量に比例する所望の断熱効果は得られない。また、過密に配置される真空セラミック粒子を含む場合、柔軟性を有るものの真空セラミック粒子の動きが制限され、特に、外力が加えられるときの引張応力により、柔軟性熱絶縁体が破損するおそれがある。更に、塗布する原料(懸濁液)に多量の真空セラミック粒子を含む場合、多量粒子のため、10〜20Mpa(約100〜200気圧)の高圧塗布(噴霧)が要求される。   However, since the vacuum ceramic particles are very expensive, the flexible thermal insulator and the blind and roll screen are naturally also expensive in the overcrowded use of the vacuum ceramic particles of Patent Document 1, and the cost of the vacuum ceramic particles is the flexibility heat. It accounts for over 70% of the cost of raw materials for insulators. Further, in the flexible thermal insulator of Patent Document 1, since a large amount of vacuum ceramic particles are closely arranged to one another through a small gap, heat conduction does not occur in the internal cavity of the vacuum, but the outside of the vacuum ceramic particles It becomes easy to conduct heat along the shell. For this reason, the desired heat insulation effect proportional to the amount of vacuum ceramic particles used can not be obtained. In addition, when the vacuum ceramic particles are arranged excessively, although there is flexibility, the movement of the vacuum ceramic particles is limited, and in particular, the flexible thermal insulator may be damaged by the tensile stress when an external force is applied. is there. Furthermore, when the raw material (suspension) to be applied contains a large amount of vacuum ceramic particles, high pressure application (spraying) of 10 to 20 MPa (about 100 to 200 atm) is required because of the large amount of particles.

これに対し、真空セラミック微粒子を過密状態で配置しない遮熱布製品は、引用文献2に開示される。引用文献2の遮熱布製品では、被服、帽子、日傘等の布表面に、中空(真空)セラミック微粒子を含有する合成樹脂からなる遮熱層を形成する。遮熱層の合成樹脂と中空セラミック微粒子との配合割合は、合成樹脂100重量%に対して、中空セラミック微粒子20〜200重量%程度とする。   On the other hand, a heat shielding cloth product which does not arrange vacuum ceramic fine particles in an overcrowded state is disclosed in Patent Document 2. In the thermal barrier cloth product of Patent Document 2, a thermal barrier layer made of a synthetic resin containing hollow (vacuum) ceramic fine particles is formed on the surface of a cloth such as a coat, a hat or a parasol. The blend ratio of the synthetic resin of the heat shielding layer and the hollow ceramic fine particles is about 20 to 200% by weight of the hollow ceramic fine particles with respect to 100% by weight of the synthetic resin.

また、特許文献3は、中空球状又は鱗片状の低熱伝導体(中空粒子又は真空粒子)と、構造助剤と、シランカップリング剤とを含有する遮熱塗料組成物を示し、建築構造物の屋上、屋根、外壁の塗装に適用される。粒子径10〜200μmの低熱伝導体を0.5〜9.9重量%含有する。   Further, Patent Document 3 shows a thermal barrier coating composition containing a hollow spherical or scaly low thermal conductivity material (hollow particles or vacuum particles), a structural aid, and a silane coupling agent, and it is an architectural structure Applies to the painting of the roof, roof and outer wall. It contains 0.5 to 9.9% by weight of a low thermal conductor having a particle size of 10 to 200 μm.

前記特許文献2及び3の遮熱材は、高価な真空粒子を大量使用しないため、比較的安価に製造できる。しかしながら、少量の真空粒子(重量配合比:1/5〜2/3及び1/20〜1/10)に対し、樹脂(バインダ)の充填量が大きいため、樹脂に沿う熱伝導を防止できず、真空粒子を含まない遮熱材と比較しても顕著な断熱効果の差が出ない。また、特許文献2及び3では、複数の真空粒子の構成について言及がなく、特許文献2ではコンマ数μm〜数百μm程度の真空粒子が、特許文献3では10〜200μmの真空粒子が無秩序に構成される。無秩序な真空粒子の構成は、十分な断熱及び遮熱特性が効率的に得られない。   The heat shields of Patent Documents 2 and 3 can be manufactured relatively inexpensively because large amounts of expensive vacuum particles are not used. However, since the filling amount of the resin (binder) is large for a small amount of vacuum particles (weight blending ratio: 1/5 to 2/3 and 1/20 to 1/10), heat conduction along the resin can not be prevented. Also, there is no significant difference in the thermal insulation effect compared to a heat shield that does not contain vacuum particles. In Patent Documents 2 and 3, there is no mention of the configuration of a plurality of vacuum particles, and in Patent Document 2, vacuum particles of about a few μm to several hundred μm are random, and in Patent Document 3, vacuum particles of 10-200 μm are disordered. Configured The disordered vacuum particle configuration does not efficiently obtain sufficient thermal insulation and thermal insulation properties.

特開2010−169259公報JP, 2010-169259, A 特開2002−166505公報Japanese Patent Application Laid-Open No. 2002-166505 特開2006−45447公報Japanese Patent Application Publication No. 2006-45447

そこで本発明は、遮熱及び断熱特性に優れ内部及び表面温度を低下できる遮熱・断熱材及びその製法を提供することを目的とする。また、本発明は、安価で優れた物理的特性を発揮する遮熱・断熱材及びその製法を提供することを目的とする。更に、本発明は、粒子を規則的に配置して、遮熱及び断熱を効率的に行う遮熱・断熱材及びその製法を提供することを目的とする。更に、本発明は、低圧かつ飛散の少ない塗布を実現できる遮熱・断熱材及びその製法を提供することを目的とする。   Then, an object of this invention is to provide the heat insulation * heat insulation material which can be excellent in a heat insulation and heat insulation characteristic and can reduce internal and surface temperature, and its manufacturing method. Another object of the present invention is to provide a heat insulating and heat insulating material which exhibits low cost and excellent physical characteristics, and a method of manufacturing the same. Another object of the present invention is to provide a heat shield and heat insulating material that arranges particles regularly to efficiently perform heat shield and heat insulation, and a method of manufacturing the same. Another object of the present invention is to provide a thermal barrier / insulation material which can realize low pressure and low scattering application, and a method of manufacturing the same.

本発明による遮熱・断熱材は、複数の第1の粒子(1)と、第1の粒子(1)を包囲する複数の第2の粒子(2)と、第2の粒子(2)の周囲を包囲する複数の第3の粒子(3)と、第1、第2及び第3の粒子(1,2,3)の同種及び異種粒子間を結合しかつ基体(50)の表面に第1、第2及び第3の粒子(1,2,3)を接着するバインダ(6)とを備える。第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)は、何れも内部空洞(1b,2b,3b)を有し、第2の粒子は、第1の粒子(1)より粒径が小さく、第3の粒子(3)は、第2の粒子(2)より粒径が小さい。第1の粒子(1)の粒径は50〜100μm、第2の粒子(2)の粒径は10〜50μm、第3の粒子(3)の粒径は0.5〜10μmである。複数の第2の粒子(2)は、各第1の粒子(1)を覆う第2の粒子層(12)を形成し、複数の第3の粒子(3)は、第2の粒子層(12)を覆う第3の粒子層(13)を形成する。   The thermal barrier / insulation material according to the present invention comprises a plurality of first particles (1), a plurality of second particles (2) surrounding the first particles (1), and a second particle (2). A plurality of third particles (3) surrounding the periphery, and homogeneous and dissimilar particles of the first, second and third particles (1, 2, 3) are bonded to each other and are bonded to the surface of the substrate (50) 1. A binder (6) for bonding the second and third particles (1, 2, 3). Each of the first particle (1), the second particle (2) and the third particle (3) has an internal cavity (1b, 2b, 3b), and the second particle is a first particle The particle size is smaller than (1), and the third particle (3) is smaller than the second particle (2). The particle diameter of the first particles (1) is 50 to 100 μm, the particle diameter of the second particles (2) is 10 to 50 μm, and the particle diameter of the third particles (3) is 0.5 to 10 μm. The plurality of second particles (2) form a second particle layer (12) covering each first particle (1), and the plurality of third particles (3) 12) form a third particle layer (13) covering the same.

第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)は、互いに接近して配置されても、バインダ(6)の薄膜でそれぞれ被覆されかつ互いに結合されるため、第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)が互いに直接接触しない。このため、粒子間の直接接触による熱伝導を生じない。第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)は、内部空洞(1b,2b,3b)を形成する外殻(1a,2a,3a)に熱を一時的に吸収(D1,D2,D3)するが、内部空洞(1b,2b,3b)は蓄熱も熱伝達も行わず、第1〜第3の粒子(1,2,3)の外殻(1a,2a,3a)は、外部から伝達される熱を外殻(1a,2a,3a)で外側に反射(B1,B2,B3)し又は放射(E1,E2,E3)し、外殻(1a,2a,3a)は、僅かな熱を一時的に吸収する。このため、最も小粒径の第3の粒子(3)の外殻(3a)は、表面で外部に熱を反射(B3)又は放射(E3)し、外殻(3a)に一時的に吸収される熱量は、僅かである。   The first particles (1), the second particles (2) and the third particles (3) are each coated with a thin film of the binder (6) and bonded to one another, even when placed close to one another , The first particle (1), the second particle (2) and the third particle (3) are not in direct contact with each other. For this reason, heat conduction due to direct contact between particles does not occur. The first particle (1), the second particle (2) and the third particle (3) temporarily heat the outer shell (1a, 2a, 3a) forming the internal cavity (1b, 2b, 3b) (D1, D2, D3), but the internal cavities (1b, 2b, 3b) do not store heat or transfer heat, and the outer shell (1a of the first to third particles (1, 2, 3) , 2a, 3a) reflect (B1, B2, B3) or radiate (E1, E2, E3) the heat transmitted from the outside by the outer shell (1a, 2a, 3a), and the outer shell (1a) , 2a, 3a) temporarily absorb a small amount of heat. For this reason, the outer shell (3a) of the third particle (3) having the smallest particle diameter reflects (B3) or radiates (E3) heat to the outside on the surface, and is temporarily absorbed in the outer shell (3a) The amount of heat generated is small.

第3の粒子(3)の外殻(3a)から反射(B3)又は放射(E3)される熱は、第2の粒子(2)の外殻(2a)の表面で反射(B2)され、外殻(2a)は、僅かな熱を一時的に吸収(D2)する。熱の反射及び放射は、第3の粒子層(13)の複数の第3の粒子(3)間及び第2の粒子層(12)の複数の第2の粒子(2)間でも反復される。更に、第2の粒子(2)の外殻(2a)の表面から反射(B2)又は放射(E2)される熱は、第1の粒子(1)の外殻(1a)の表面で反射(B1)され、外殻(1a)は、熱を一時的に吸収(D1)する。 The heat reflected (B3) or emitted (E3) from the outer shell (3a) of the third particle (3) is reflected (B2) on the surface of the outer shell (2a) of the second particle (2), The outer shell (2a) temporarily absorbs a small amount of heat (D2). Heat reflection and radiation are also repeated between the plurality of third particles (3) of the third particle layer (13) and between the plurality of second particles (2) of the second particle layer (12) . Furthermore, the heat reflected (B2) or emitted (E2) from the surface of the outer shell (2a) of the second particle (2) is reflected (at the surface of the outer shell (1a) of the first particle (1) B1) The shell (1a) temporarily absorbs heat (D1).

遮熱・断熱材は、外部から熱を受けても、第3の粒子(3)から外部に熱を反射し又は放散するので、第1〜第3の粒子(1,2,3)の外殻(1a,2a,3a)に一時的に吸収される熱は、基体(50)には伝達されず、最終的に外殻(1a,2a,3a)及びバインダ(6)を通じて外部に放出される。このように、遮熱・断熱材の片側に発生する熱の殆どを反射(B1,B2,B3)し、時間の経過に伴い遮熱・断熱材自体も放熱するので、一時的に吸収(D1,D2,D3)する熱も徐々に外部に放散されて、遮熱・断熱材の基体(50)側に伝達しない。本発明では、各第1の粒子(1)の周囲に複数の第2の粒子(2)をバインダ(6)で接合した第2の粒子層(12)が形成され、第2の粒子層(12)の周囲に第3の粒子(3)がバインダ(6)で接合された第3の粒子層(13)が形成されるので、第1の粒子(1)に蓄積される熱は、第2の粒子層(12)及び第3の粒子層(13)を介して最終的に外部に放出される。 Since the heat shield / heat insulator reflects or dissipates heat from the third particles (3) to the outside even when receiving heat from the outside, the outside of the first to third particles (1, 2, 3) The heat temporarily absorbed by the shells (1a, 2a, 3a) is not transmitted to the substrate (50) and is finally released to the outside through the outer shells (1a, 2a, 3a) and the binder (6). Ru. As described above, most of the heat generated on one side of the heat shield / heat insulator is reflected (B1, B2, B3), and the heat shield / heat insulator itself is also dissipated with the passage of time, so it is temporarily absorbed (D1 , D2, D3) are also dissipated gradually to the outside, and they are not transmitted to the side of the substrate (50) of the heat and heat insulating material. In the present invention, a second particle layer (12) is formed around each first particle (1) by bonding a plurality of second particles (2) with a binder (6), Since the third particle layer (13) in which the third particles (3) are joined with the binder (6) is formed around 12), the heat accumulated in the first particles (1) It is finally released to the outside through the second particle layer (12) and the third particle layer (13).

本発明による遮熱・断熱材の製法は、内部空洞(1b)を有する複数の第1の粒子(1)5〜30重量部と、第1の粒子(1)より粒径が小さくかつ内部空洞(2b)を有する複数の第2の粒子(2)1〜20重量部と、第2の粒子(2)より粒径が小さくかつ内部空洞(3b)を有する複数の第3の粒子(3)0.1〜10重量部と、バインダ(6)15〜40重量部と、揮発性溶媒5〜30重量部とを含む懸濁液(31)を準備する工程と、0.2〜0.4MPaに加圧した気流と共に懸濁液(31)を二流体混合方式によりノズル(33)から空気中に速度10〜500mm/secで噴射して、ノズル(33)からの噴射距離が0.1m〜2mである基体(50)の表面に懸濁液(31)を均一に散布する工程と、バインダ(6)の薄膜で被覆される第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)を含む懸濁液(31)を基体(50)の表面に均一に散布する運動中に、粒径50〜100μmの複数の第1の粒子(1)を互いに個別に分離しかつ各第1の粒子(1)の周囲を粒径10〜50μmの第2の粒子(2)を主成分とする第2の粒子層(12)により包囲し、かつ粒径0.5〜10μmの第3の粒子(3)を主成分とする第3の粒子層(13)により包囲して、第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)を基体(50)の表面に付着させる工程と、基体(50)に付着する懸濁液(31)を乾燥させて、第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)をバインダ(6)により接着する工程とを含む。   The method for producing a heat shield / insulation material according to the present invention comprises 5 to 30 parts by weight of a plurality of first particles (1) having an internal cavity (1b) and a smaller particle size than the first particles (1) and an internal cavity A plurality of second particles (2) having (2b) (1 to 20 parts by weight), and a plurality of third particles (3) having a smaller particle size than the second particles (2) and having an internal cavity (3b) Preparing a suspension (31) comprising 0.1 to 10 parts by weight, 15 to 40 parts by weight of the binder (6), and 5 to 30 parts by weight of a volatile solvent, and 0.2 to 0.4 MPa The suspension (31) is injected into the air from the nozzle (33) at a velocity of 10 to 500 mm / sec by the two-fluid mixing method together with the pressurized air flow, and the injection distance from the nozzle (33) is 0.1 m to Uniformly spraying the suspension (31) on the surface of the substrate (50) which is 2 m, and first particles (1), second particles (2) and second particles coated with a thin film of the binder (6) The suspension (31) containing the third particles (3) is uniformly applied to the surface of the substrate (50) During the exercise, the plurality of first particles (1) of 50 to 100 μm in size are separated from each other separately, and the second particles of 10 to 50 μm in diameter are dispersed around each first particle (1) 2) is surrounded by a second particle layer (12) whose main component is the main component, and is surrounded by a third particle layer (13) whose main component is the third particles (3) having a particle diameter of 0.5 to 10 μm Attaching the first particles (1), the second particles (2) and the third particles (3) to the surface of the substrate (50), and 31) drying to bond the first particles (1), the second particles (2) and the third particles (3) with a binder (6).

第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)は、懸濁液(31)中でバインダ(6)の薄膜により被覆される。基体(50)の表面に懸濁液(31)を均一に散布するとき、ノズル(33)からの噴射時の衝撃力が噴射される懸濁液(31)に加えられるため、最大の質量を持つ複数の第1の粒子(1)は、互いに分離されて、通常単独で空気中を移動する。このとき、比較的質量の小さい複数の第2の粒子(2)と複数の第3の粒子(3)は、バインダ(6)の表面張力又は粘性で第1の粒子(1)に付着し、空気中を移動する。このため、複数の第1の粒子(1)の各々は、互いに分離しかつ各第1の粒子(1)の周囲に第2の粒子(2)及び第3の粒子(3)を伴送させて、基体(50)の表面に付着させる。   The first particles (1), the second particles (2) and the third particles (3) are covered in a suspension (31) by a thin film of binder (6). When uniformly spraying the suspension (31) on the surface of the substrate (50), the impact force at the time of spraying from the nozzle (33) is added to the sprayed suspension (31), so the maximum mass can be obtained. The plurality of first particles (1) that are carried are separated from one another and usually move alone in the air. At this time, the relatively small mass second particles (2) and the plurality of third particles (3) adhere to the first particles (1) by the surface tension or viscosity of the binder (6), Move in the air. Thus, each of the plurality of first particles (1) separates from each other and causes the second particles (2) and the third particles (3) to be entrained around each first particle (1). And adhere to the surface of the substrate (50).

本発明では、ほぼ同径の粒子を各々含む第2の粒子層と第3の粒子層とが第1の粒子を包囲するため、熱の吸収及び反射を効率良く繰り返し、優れた遮熱及び断熱効果を発揮する。本発明の遮熱・断熱材は、真空セラミック粒子の使用量を最小限に抑えるため、低コストで製造でき、耐衝撃性、可撓性及び耐久性に優れる。   In the present invention, since the second particle layer and the third particle layer, each of which has approximately the same diameter, surround the first particle, heat absorption and reflection are efficiently repeated, resulting in excellent heat and heat insulation. Exert an effect. The heat shield / insulation material of the present invention can be manufactured at low cost in order to minimize the amount of vacuum ceramic particles used, and is excellent in impact resistance, flexibility and durability.

本発明による遮熱・断熱材の第1の実施の形態を示す概略断面図Schematic sectional drawing which shows 1st Embodiment of the heat insulation * thermal insulation by this invention 本発明による遮熱・断熱材の第2の実施の形態を示す概略断面図Schematic sectional drawing which shows 2nd Embodiment of the heat insulation * heat insulating material by this invention 本発明による遮熱・断熱材の粒子集合体を示す概略断面図Schematic cross section showing the particle assembly of the heat shield / insulation material according to the present invention 本発明による遮熱・断熱材の熱エネルギ減衰メカニズムを示す概略断面図Schematic sectional drawing which shows the thermal energy damping mechanism of the heat insulation * thermal insulation material by this invention 本発明による遮熱・断熱材の製法を示す概略図Schematic diagram showing the method of manufacturing the heat shield / insulator according to the present invention 本発明による遮熱・断熱材の製法を示す概略断面図Schematic cross-sectional view showing the method of manufacturing the heat shield / insulator according to the present invention 遮熱及び断熱作用を説明する概略図Schematic to explain heat insulation and heat insulation 熱照射試験による温度と日射量の関係を示すグラフGraph showing the relationship between temperature and amount of solar radiation by heat irradiation test

本発明による遮熱・断熱材及びその製法の実施の形態を図1〜図8について以下説明する。
図1〜図3に示す粒子集合体(10)は、第1の粒子(1)と、第1の粒子(1)の周囲に配置される複数の第2の粒子(2)と、各第2の粒子(2)の周囲に配置される複数の第3の粒子(3)と、第1、第2及び第3の粒子(1,2,3)の同種及び異種粒子間を結合するバインダ(6)とを備え、本発明による遮熱・断熱材を構成する。第1、第2及び第3の粒子(1,2,3)は、何れも内部空洞(1b,2b,3b)を有し、各内部空洞(1b,2b,3b)は、減圧状態又はほぼ真空状態である。第1、第2及び第3の粒子(1,2,3)として、外殻(1a,2a,3a)がセラミックにより形成される真空セラミック粒子の使用が好ましい。内部空洞(1b,2b,3b)をほぼ真空状態にすることにより、遮熱・断熱材の断熱特性を向上し、特に、第1の粒子(1)は、内部空洞(1b)が大きく熱伝導を完全に抑制できる。
Embodiments of the heat shield and heat insulator according to the present invention and the method of manufacturing the same will be described below with reference to FIGS. 1 to 8.
The particle assembly (10) shown in FIGS. 1 to 3 includes a first particle (1), a plurality of second particles (2) arranged around the first particle (1), and A plurality of third particles (3) arranged around the two particles (2), and a binder for binding between homogeneous and dissimilar particles of the first, second and third particles (1, 2, 3) And (6) to constitute the heat shield / heat insulator according to the present invention. Each of the first, second and third particles (1, 2, 3) has an internal cavity (1b, 2b, 3b), and each internal cavity (1b, 2b, 3b) is under reduced pressure or substantially It is in a vacuum state. The use of vacuum ceramic particles in which the outer shell (1a, 2a, 3a) is formed of a ceramic as the first, second and third particles (1, 2, 3) is preferred. By placing the internal cavity (1b, 2b, 3b) in a substantially vacuum state, the heat insulation and thermal insulation properties are improved, and in particular, the first particle (1) has a large internal cavity (1b) and is thermally conductive. Can be completely suppressed.

内部に中空部が形成される第1、第2及び第3の粒子(1,2,3)は、アルミナ、シリカ、酸化チタン、酸化マグネシウム、酸化亜鉛等から選択された1種又は2種以上を低圧状態又はほぼ真空状態で粒径数μm〜百μm程度に球状化したものである。空隙率は、50体積%〜90体積%程度である。基体(50)の表面に第1〜第3の粒子を強固に接着するバインダ(6)は、例えば、塩化ビニル樹脂、アクリル樹脂、シリコーン樹脂、ウレタン樹脂、アクリルシリコーン樹脂、アクリルウレタン樹脂、ウレタンフッ素樹脂、ポリエステル共重合樹脂、アルコキシシラン化合物を主成分とする無溶剤型の無機系のポリマー等の任意の合成樹脂を使用することができる。バインダ(6)は、水等の無機溶媒又は/及びアルコール、アセトン等の有機溶媒を混入してもよい。   The first, second and third particles (1, 2, 3) in which the hollow part is formed inside are one or more selected from alumina, silica, titanium oxide, magnesium oxide, zinc oxide etc. Is spheroidized to a particle diameter of several μm to about 100 μm in a low pressure state or a substantially vacuum state. The porosity is about 50% by volume to 90% by volume. The binder (6) for firmly bonding the first to third particles to the surface of the substrate (50) is, for example, vinyl chloride resin, acrylic resin, silicone resin, urethane resin, acrylic silicone resin, acrylic urethane resin, urethane fluorine Any synthetic resin such as a resin, a polyester copolymer resin, and a solventless inorganic polymer mainly composed of an alkoxysilane compound can be used. The binder (6) may be mixed with an inorganic solvent such as water or / and an alcohol, or an organic solvent such as acetone.

本発明の遮熱及び断熱の対象となる基体(50)は、織布、不織布等の布、樹脂材、セラミック材、木材、金属材により形成された屋根、建物外壁、ブラインド、屋上水槽、危険物貯蔵タンク、水道管、工場配管、自動車、衣服、カーテンである。基体(50)表面に本発明の遮熱・断熱材を形成すれば、夏は、太陽光からの熱エネルギが遮熱・断熱材の反対側、即ち、室内、タンク内部、管内部まで到達すること防ぐ。冬は、内部の熱を保温して外部に放出しない。このため、空調設備の電力使用量を低減し、省エネルギ及び消費電力の大幅な削減を図ることができる。また、管内部の液体の高温化又は凍結を防止できる。   The substrate (50) to be a target of heat and heat insulation according to the present invention is a cloth such as woven fabric, non-woven fabric, resin material, ceramic material, wood, roof made of metal, building outer wall, blind, roof water tank, danger Storage tanks, water pipes, factory piping, cars, clothes, curtains. If the heat shield and heat insulating material of the present invention is formed on the surface of the substrate (50), the heat energy from sunlight reaches the opposite side of the heat shield and heat insulator, ie, the room, the tank interior, and the tube interior in summer. Prevent that. In winter, the heat inside is kept warm and not released outside. For this reason, the amount of power consumption of the air conditioning equipment can be reduced, and energy saving and significant reduction in power consumption can be achieved. In addition, it is possible to prevent the temperature rise or freezing of the liquid inside the tube.

第2の粒子(2)は、第1の粒子(1)より粒径が小さく、第3の粒子(3)は、第2の粒子(2)より粒径が小さい。具体的には、第1の粒子(1)の粒径は50〜100μm、第2の粒子(2)の粒径は10〜50μm、第3の粒子(3)の粒径は0.5〜10μmである。   The second particles (2) have a smaller particle size than the first particles (1), and the third particles (3) have a smaller particle size than the second particles (2). Specifically, the particle diameter of the first particles (1) is 50 to 100 μm, the particle diameter of the second particles (2) is 10 to 50 μm, and the particle diameter of the third particles (3) is 0.5 to 0.5 It is 10 μm.

図3の通り、本発明の遮熱・断熱材では、複数の第2の粒子(2)は、第1の粒子(1)の周囲を覆う第2の粒子層(12)を形成し、第2の粒子(2)間がバインダ(6)で接合される。複数の第3の粒子(3)は、第2の粒子層(12)の周囲を覆う第3の粒子層(13)を形成し、第3の粒子(3)間がバインダ(6)で接合される。   As shown in FIG. 3, in the heat / insulation material of the present invention, the plurality of second particles (2) form a second particle layer (12) covering the periphery of the first particles (1), and The two particles (2) are bonded with a binder (6). The plurality of third particles (3) form a third particle layer (13) covering the periphery of the second particle layer (12), and the third particles (3) are bonded with the binder (6) Be done.

第1の粒子(1)間(粒子集合体(10)間)の距離は70〜500μm、第1の粒子(1)と第2の粒子(2)との間の距離は10〜50μm、第2の粒子(2)間の距離は5〜20μm、第3の粒子(3)間の距離は0.5〜10μmである。第3の粒子(3)からの第3の熱エネルギ(A3)は、日射の熱エネルギ(A)より波長が長く、第3の粒子(3)間距離を0.5〜10μmとして、エネルギの吸収効率を高め、優れた遮熱特性が得られる。第3の粒子(3)からの第3の熱エネルギ(A3)に比べ、第2の粒子(2)からの第2の熱エネルギ(A2)は、波長が長いため、第2の粒子(2)間距離を5〜20μmにすることにより、エネルギの吸収効率を向上する。また、第1の粒子(1)−第2の粒子(2)間距離を10〜50μmとすると、第2の粒子(2)からの第2の熱エネルギ(A2)を第1の粒子(1)により吸収し易く、第1の粒子(1)によるエネルギ減衰の効果が効率的に得られる。第2の粒子(2)からの第2の熱エネルギ(A2)に比べ、第1の粒子(1)からの熱エネルギ(A1)は、波長が長いため、第1の粒子(1)間の距離を70〜500μmとすると、第1の粒子(1)からの第1の熱エネルギ(A1)を他の第1の粒子(1)によって効率良く吸収できる。   The distance between the first particles (1) (between the particle assembly (10)) is 70 to 500 μm, the distance between the first particles (1) and the second particles (2) is 10 to 50 μm, The distance between the two particles (2) is 5 to 20 μm, and the distance between the third particles (3) is 0.5 to 10 μm. The third thermal energy (A3) from the third particle (3) has a wavelength longer than that of solar thermal energy (A), and the distance between the third particles (3) is 0.5 to 10 μm. The absorption efficiency is enhanced, and excellent heat shielding properties are obtained. The second thermal energy (A2) from the second particle (2) has a longer wavelength than the third thermal energy (A3) from the third particle (3), so the second particle (2) The energy absorption efficiency is improved by setting the distance between 5 and 20 μm. Also, assuming that the distance between the first particle (1) and the second particle (2) is 10 to 50 μm, the second thermal energy (A2) from the second particle (2) is converted to the first particle (1) ), And the effect of energy attenuation by the first particle (1) is efficiently obtained. The thermal energy (A1) from the first particle (1) has a longer wavelength than the second thermal energy (A2) from the second particle (2). When the distance is 70 to 500 μm, the first heat energy (A1) from the first particle (1) can be efficiently absorbed by the other first particles (1).

次に、粒子集合体(10)が照射された熱エネルギを減衰するメカニズムを図4について説明する。太陽光及びその他の熱エネルギによる入射熱(A)は、その一部が第3の粒子(3)の外殻(3a)表面で他の第1、第2及び第3の粒子(1,2,3)に向けて反射する(B3)。その他の入射熱(A)は、外殻(3a)表面を透過し(C3)、外殻(3a)内部を拡散し一部が吸収及び蓄積される(D3)。第3の粒子層(13)を構成する複数の第3の粒子(3)の外殻(3a)では、熱エネルギの拡散及び吸収が繰り返される。透過熱(C3)のうち吸収熱(D3)を除く部分は、外殻(3a)から放射(輻射)熱(E3)として、他の第1、第2及び第3の粒子(1,2,3)に向け反射熱(B3)と共に放射される。反射熱(B3)と放射(輻射)熱(E3)とを合わせた第3の熱エネルギ(A3)は、入射熱の熱エネルギ(A)と比べ、外殻(3a)で吸収された熱エネルギ分(D3)だけ小さい(A3=A-D3)。   Next, the mechanism by which the particle assembly (10) attenuates the irradiated thermal energy will be described with reference to FIG. The incident heat (A) due to sunlight and other thermal energy is partially generated by the first, second and third particles (1, 2) on the surface of the outer shell (3a) of the third particle (3). , 3) to reflect (B3). The other incident heat (A) passes through the surface of the outer shell (3a) (C3), diffuses inside the outer shell (3a), and is partially absorbed and accumulated (D3). In the outer shell (3a) of the plurality of third particles (3) constituting the third particle layer (13), the thermal energy diffusion and absorption are repeated. The portion of the transmitted heat (C3) excluding the heat of absorption (D3) is emitted from the outer shell (3a) as radiation (radiation) heat (E3), and the other first, second and third particles (1, 2, 3) It is emitted together with the reflected heat (B3) toward 3). The third thermal energy (A3), which is the combination of the reflected heat (B3) and the radiant (radiative) heat (E3), is the thermal energy absorbed by the outer shell (3a) compared to the thermal energy of the incident heat (A) It is small by a minute (D3) (A3 = A-D3).

第3の熱エネルギ(A3)は、第2の粒子層(12)を通過する際、前記第3の粒子(3)と同様に、第2の粒子(2)の外殻(2a)表面から一部が内部に透過し拡散及び吸収(D2)を繰り返して放射(E2)を生じる。第3の熱エネルギ(A3)の他の部分は、図4に示す通り、第2の粒子(2)の外殻(2a)表面から反射する(B2)。このような、入射(A3)、反射(B2)、透過(C2)、吸収(D2)及び放射(E2)を第2の粒子層(12)の複数の第2の粒子(2)により繰り返し、熱エネルギが減衰する。第2の粒子(2)からの反射熱(B2)と放射(輻射)熱(E2)とを合わせた第2の熱エネルギ(A2)は、第3の熱エネルギ(A3)と比べ、外殻(2a)で吸収された熱エネルギ分(D2)だけ小さい(A2=A3-D2)。   As the third thermal energy (A3) passes through the second particle layer (12), it is from the surface of the outer shell (2a) of the second particle (2) as in the case of the third particle (3). A portion is transmitted internally and repeats diffusion and absorption (D2) to produce radiation (E2). The other part of the third thermal energy (A3) is reflected (B2) from the surface of the outer shell (2a) of the second particle (2) as shown in FIG. Such incidence (A3), reflection (B2), transmission (C2), absorption (D2) and radiation (E2) are repeated by the plurality of second particles (2) of the second particle layer (12), Thermal energy is attenuated. The second heat energy (A2) which is the combination of the heat of reflection (B2) from the second particle (2) and the heat of radiation (radiation) (E2) is the outer shell compared with the third heat energy (A3) (2a) is smaller by the heat energy absorbed (D2) (A2 = A3-D2).

同様に、第2の熱エネルギ(A2)は、第1の粒子(1)の外殻(1a)表面から一部が透過し拡散及び吸収(D1)を繰り返して放射(E1)を生じる。第2の熱エネルギ(A2)の他の部分は、第1の粒子(1)の外殻(1a)表面から反射する(B1)。このような、入射(A2)、反射(B1)、透過(C1)、吸収(D1)及び放射(E1)を複数の第1の粒子(1)により繰り返し、熱エネルギが減衰する。第1の粒子(1)からの熱エネルギ(A1)は、第2の熱エネルギ(A2)と比べ、外殻(1a)で吸収された熱エネルギ分(D1)だけ小さい(A1=A2-D1)。   Similarly, the second thermal energy (A2) is partially transmitted from the surface of the outer shell (1a) of the first particle (1) and repeats diffusion and absorption (D1) to generate radiation (E1). The other part of the second thermal energy (A2) reflects (B1) from the surface of the outer shell (1a) of the first particle (1). Such incident (A2), reflection (B1), transmission (C1), absorption (D1) and radiation (E1) are repeated by the plurality of first particles (1), and thermal energy is attenuated. The thermal energy (A1) from the first particle (1) is smaller than the second thermal energy (A2) by the thermal energy absorbed by the outer shell (1a) (D1) (A1 = A2-D1) ).

本発明では、第1の粒子(1)、第2の粒子層(12)及び第3の粒子層(13)を含む図3の粒子集合体(10)を複数重ねて、図1に示す厚さ(T)0.1〜1.0mmの積層体(20)を形成する。粒子集合体(10)を複数重ね合わせることにより、積層体(20)に進入した熱エネルギを図4の減衰メカニズムに従い減衰でき、熱エネルギの遮熱・断熱材(積層体(20))厚さ(T)方向の通過を大部分抑止できる。また、積層体(20)の内部で熱エネルギを減衰できるので、遮熱・断熱材表面の温度が高温化することを防ぐ。また、積層体(20)は、粒子集合体(10)間に空隙(25)を備えるため、バインダ(6)を介する伝熱を最小限に抑え断熱効果を高めると共に、高価な真空粒子(1,2,3)の使用量を減量できる。   In the present invention, a plurality of particle aggregates (10) of FIG. 3 including the first particle (1), the second particle layer (12) and the third particle layer (13) are stacked to form the thickness shown in FIG. A laminate (20) having a length (T) of 0.1 to 1.0 mm is formed. By superimposing a plurality of particle aggregates (10), the thermal energy entering the laminate (20) can be attenuated according to the damping mechanism of FIG. 4, and the thermal energy insulating / insulating material (laminate (20)) thickness The passage of (T) direction can be mostly suppressed. In addition, since the thermal energy can be attenuated inside the laminate (20), the temperature of the surface of the heat shield and heat insulator is prevented from rising. In addition, since the laminate (20) includes the air gap (25) between the particle assembly (10), the heat transfer through the binder (6) is minimized and the heat insulation effect is enhanced, and the expensive vacuum particles (1) , 2, 3) can be reduced.

図2に示す他の積層体(20’)は、第3の粒子(3)より小さい粒径の第4の粒子(4)により形成される表面層(21)を備え、表面層(21)は、第3の粒子層(13)より過密に形成して平滑面構造とする。このため、積層体(20’)に入射する熱エネルギを反射して、遮熱・断熱材内部への進入を最小限に抑える。第4の粒子(4)は、0.1〜1.0μmの真空セラミック粒子が使用される。   Another laminate (20 ') shown in FIG. 2 comprises a surface layer (21) formed by the fourth particles (4) having a smaller particle size than the third particles (3), and the surface layer (21) Is formed more densely than the third particle layer (13) to form a smooth surface structure. For this reason, the thermal energy which injects into a laminated body (20 ') is reflected, and the approach to the inside of a thermal insulation / thermal insulation is minimized. As the fourth particles (4), vacuum ceramic particles of 0.1 to 1.0 μm are used.

次に、図5及び図6について本発明による遮熱・断熱材の製法を説明する。本実施の形態では、最初に、内部空洞(1b)を有する複数の第1の粒子(1)、第1の粒子(1)より粒径が小さくかつ内部空洞(2b)を有する複数の第2の粒子(2)及び第2の粒子(2)より粒径が小さくかつ内部空洞(3b)を有する複数の第3の粒子(3)を懸濁したバインダ(6)を含む懸濁液(31)を準備する。第1、第2及び第3の粒子(1,2,3)はそれぞれ、減圧状態又はほぼ真空状態の各内部空洞(1b,2b,3b)を有する真空セラミック粒子である。第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)は、懸濁液(31)中でバインダ(6)の薄膜により被覆される。懸濁液(31)は、バインダとして好ましくは無機及び有機の複合樹脂(6)15〜40重量部に対し、第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)をそれぞれ、5〜30重量部、1〜20重量部及び0.1〜10重量部と共に、水等の揮発性溶媒5〜30重量部を含有する。   Next, the manufacturing method of the thermal insulation / heat insulating material by this invention is demonstrated about FIG. 5 and FIG. In the present embodiment, first, a plurality of first particles (1) having an internal cavity (1b), and a plurality of second particles having a smaller particle size than the first particle (1) and having an internal cavity (2b) A suspension (31) comprising a binder (6) in which a plurality of third particles (3) having a smaller particle size than the second particles (2) and the inner cavity (3b) are suspended Prepare). The first, second and third particles (1, 2, 3) are vacuum ceramic particles having respective internal cavities (1b, 2b, 3b) in a reduced pressure or substantially vacuum state. The first particles (1), the second particles (2) and the third particles (3) are covered in a suspension (31) by a thin film of binder (6). The suspension (31) is preferably used as a binder for the first particles (1), the second particles (2) and the third particles (15 to 40 parts by weight of the composite resin (6)). 3) contains 5 to 30 parts by weight of a volatile solvent such as water together with 5 to 30 parts by weight, 1 to 20 parts by weight and 0.1 to 10 parts by weight, respectively.

次に、0.1〜0.6MPa(約1〜6気圧)、好ましくは0.2〜0.4MPa(約2〜4気圧)に加圧した気流をノズル(33)から常温常圧下の空気中に噴出するとき、ノズル(33)のベンチュリ構造を構成する縮管部(34)に接続した容器内の懸濁液(31)を図5に示すように、二流体混合方式により噴射して基体(50)の表面に懸濁液(31)を均一に散布する。従来は、懸濁液(31)自体に直接高い圧力(10〜20MPa)を加え噴霧していたが、前記二流体混合方式により、本実施の形態では、70〜80体積%の多量の粒子(1,2,3)を含む懸濁液(31)でも、低圧で飛散の少ない噴射が可能となる。基体(50)の表面に懸濁液(31)を均一に散布するとき、ノズル(33)からの噴射時の衝撃力が噴射される懸濁液(31)に加えられるため、最大の質量を持つ複数の第1の粒子(1)は、互いに分離されて、通常単独で空気中を移動する。このとき、比較的質量の小さい複数の第2の粒子(2)と複数の第3の粒子(3)は、バインダ(6)の表面張力又は粘性で第1の粒子(1)に付着し、空気中を移動する。このため、複数の第1の粒子(1)の各々は、互いに分離しかつ各第1の粒子(1)の周囲に第2の粒子(2)及び第3の粒子(3)を伴送させて、基体(50)の表面に付着させる。これにより、第2の粒子(2)と第3の粒子(3)が分離し、第1の粒子(1)の周囲に第2の粒子(2)を主成分として含む第2の粒子層(12)を形成し、第2の粒子層(12)の周囲に第3の粒子(3)を主成分として含む第3の粒子層(13)を形成する。   Next, an air stream pressurized at 0.1 to 0.6 MPa (about 1 to 6 atmospheres), preferably 0.2 to 0.4 MPa (about 2 to 4 atmospheres) from the nozzle (33) at normal temperature and normal pressure As shown in FIG. 5, the suspension (31) in the container connected to the constricted pipe portion (34) constituting the venturi structure of the nozzle (33) is jetted by the two-fluid mixing method when it is jetted into the inside. The suspension (31) is spread uniformly on the surface of the substrate (50). Conventionally, high pressure (10 to 20 MPa) was directly applied to the suspension (31) itself for spraying, but in the present embodiment, a large amount of particles of 70 to 80 volume% Even with the suspension (31) containing 1, 2, 3), it is possible to inject at low pressure and with little scattering. When uniformly spraying the suspension (31) on the surface of the substrate (50), the impact force at the time of spraying from the nozzle (33) is added to the sprayed suspension (31), so the maximum mass can be obtained. The plurality of first particles (1) that are carried are separated from one another and usually move alone in the air. At this time, the relatively small mass second particles (2) and the plurality of third particles (3) adhere to the first particles (1) by the surface tension or viscosity of the binder (6), Move in the air. Thus, each of the plurality of first particles (1) separates from each other and causes the second particles (2) and the third particles (3) to be entrained around each first particle (1). And adhere to the surface of the substrate (50). Thereby, the second particle (2) and the third particle (3) are separated, and the second particle layer containing the second particle (2) as a main component around the first particle (1) 12) to form a third particle layer (13) containing the third particles (3) as the main component around the second particle layer (12).

第2の粒子層(12)及び第3の粒子層(13)の形成原理は、前記質量や表面張力によるものと共に、バインダ(6)中の水分(7)移動による作用と考えられる。即ち、図5の通り加圧散布された懸濁液(31)は、第2の粒子(2)、第3の粒子(3)及びバインダ(6)が第1の粒子(1)の周囲に混在した状態で、粒径が大きい第1の粒子(1)同士が徐々に分離する。分離した第1の粒子(1)周囲のバインダ(6)中では、図6に示す水分(水泡)(7)が外方向に移動して蒸発し、水分(7)の動きと共に、粒径が小さく軽い第3の粒子(3)が水分(7)に担持されてバインダ(6)中を外方向に押されて移動する。これにより、第2の粒子(2)と第3の粒子(3)が分離し、第2の粒子層(12)及び第3の粒子層(13)を形成する。   The formation principle of the second particle layer (12) and the third particle layer (13) is considered to be the action by the movement of the water (7) in the binder (6) as well as the one by the mass and surface tension. That is, the suspension (31) pressurized and sprayed as shown in FIG. 5 has the second particles (2), the third particles (3) and the binder (6) around the first particles (1). In the mixed state, the first particles (1) having large particle sizes are gradually separated from each other. In the binder (6) around the separated first particles (1), the water (water bubbles) (7) shown in FIG. 6 moves outward and evaporates, and along with the movement of the water (7), the particle size is The small and light third particles (3) are carried by the water (7) and pushed outward in the binder (6) to move. Thereby, the second particles (2) and the third particles (3) are separated to form the second particle layer (12) and the third particle layer (13).

第1、第2及び第3の粒子(1,2,3)を含む粒子集合体(10)が基体(50)に到達する速度は、天候、気温、湿度、気圧等により異なるが、10〜500mm/secに調整され、10〜100mm/secが好ましい。ノズル(33)先端より噴出された第1、第2及び第3の粒子(1,2,3)は、空気の乱流により粒子(1,2,3)同士が衝突しながら、バインダ(6)内の固形化が進行し、粒子集合体(10)に成長して基体(50)に達する。この成長過程では、粒子集合体(10)の中心部から表面に向けて揮発成分の蒸散移動及び毛細管現象により、小径の第3の粒子(3)は粒子群外側の表面に集まる。また、揮発成分(水、有機揮発成分)の蒸散により、静電的に粒子(1,2,3)は同極性に帯電し、互いにクーロン力により反発し合い接触が抑制された状態で粒子集合体(10)を形成する。   The speed at which the particle assembly (10) containing the first, second and third particles (1, 2, 3) reaches the substrate (50) varies depending on the weather, air temperature, humidity, air pressure, etc. It is adjusted to 500 mm / sec, preferably 10 to 100 mm / sec. The first, second and third particles (1, 2, 3) ejected from the tip of the nozzle (33) are caused to collide with each other while the particles (1, 2, 3) collide with each other due to the turbulent air flow. Solidification proceeds to grow into particle aggregates (10) to reach the substrate (50). In this growth process, the small-diameter third particles (3) gather on the outer surface of the particle group due to transpirational movement of volatile components and capillary action from the center of the particle assembly (10) to the surface. In addition, the particles (1, 2, 3) are electrostatically charged to the same polarity by evaporation of volatile components (water, organic volatile components), and particle aggregation occurs in a state where mutual repulsion due to coulomb force suppresses contact. Form the body (10).

このように、バインダ(6)の薄膜で被覆される第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)を含む懸濁液(31)を基体(50)の表面に均一に散布する運動中に、複数の第1の粒子(1)を互いに個別に分離しかつ各第1の粒子(1)の周囲に第2の粒子(2)及び第3の粒子(3)を伴送させて、基体(50)の表面に付着させることができる。その後、基体(50)に付着する懸濁液(31)を乾燥させて、第1の粒子(1)、第2の粒子(2)及び第3の粒子(3)をバインダ(6)により強固に接着させる。   Thus, the substrate (50) is a suspension (31) comprising the first particles (1), the second particles (2) and the third particles (3) coated with the thin film of the binder (6) Separates the plurality of first particles (1) separately from one another during the motion of uniformly spreading the surface of the second particles (2) and the third particles around each first particle (1) (3) can be entrained to adhere to the surface of the substrate (50). Thereafter, the suspension (31) attached to the substrate (50) is dried to strengthen the first particles (1), the second particles (2) and the third particles (3) with the binder (6). Adhere to

第1の粒子(1)の周囲に規則正しく第2の粒子層(12)及び第3の粒子層(13)を備える図3の粒子集合体(10)は、基体(50)、例えば、屋根、壁面、ブラインド等の表面に連続的に複数重畳されて積層体(20,20’)を形成する。ノズル(33)から基体(50)表面までの噴射距離は0.1m〜2m、好ましくは0.1〜0.5mである。   The particle assembly (10) of FIG. 3 comprising a second particle layer (12) and a third particle layer (13) regularly around the first particles (1) is a substrate (50), for example a roof, A plurality of layers (20, 20 ') are formed by being successively and continuously superimposed on the surface of a wall surface, a blind or the like. The jet distance from the nozzle (33) to the surface of the substrate (50) is 0.1 m to 2 m, preferably 0.1 to 0.5 m.

規則正しく第2の粒子(2)及び第3の粒子(3)をそれぞれ配置した第2の粒子層(12)及び第3の粒子層(13)を形成することにより、高遮熱かつ高断熱の本発明による遮熱・断熱材が得られる理由を図7について説明する。日射熱による赤外線等の電磁波は、非可干渉性の平面波として図1及び図2の積層体(20,20’)内に進入し、粒子(1,2,3)の表面で拡散して図7に示す包絡曲面の球面波(16)を形成する。図7は、球面波(16)の特定波長の一波長の距離(L)だけ離間した一対の第3の粒子(真空セラミック粒子)(3’,3”)を示す。説明の便宜のため、第3の粒子(3’,3”)のみ例示するが、これに限定されず、第1及び第2の粒子(真空セラミック粒子)(1,2)でも同様の下記作用効果が得られる。   By forming the second particle layer (12) and the third particle layer (13) in which the second particles (2) and the third particles (3) are regularly arranged, high thermal and thermal insulation The reason why the heat shielding and heat insulating material according to the present invention is obtained will be described with reference to FIG. An electromagnetic wave such as infrared rays due to solar radiation enters the laminate (20, 20 ') of FIGS. 1 and 2 as a noncoherent plane wave and diffuses on the surface of the particles (1, 2, 3). Form a spherical wave (16) of the envelope surface shown in FIG. Fig. 7 shows a pair of third particles (vacuum ceramic particles) (3 ', 3 ") separated by a distance (L) of one wavelength of a specific wavelength of the spherical wave (16). Although only the third particles (3 ′, 3 ′ ′) are illustrated, the present invention is not limited thereto, and the same effects as described below can be obtained with the first and second particles (vacuum ceramic particles) (1, 2).

第3の粒子(3’,3”)が日射熱を受けると、特定の波長の電磁波(赤外線)の一部を吸収し90%以上を反射する。反射により、電磁波の偏光が回転偏光から直線偏光に変化し非可干渉性(インコヒーレント)から可干渉性(コヒーレント)となる(スペックル干渉)。電磁波は、第3の粒子(3’,3”)表層のあらゆる点から反射及び再放射され、球面波(16)として拡散伝播し、距離の二乗に反比例して熱エネルギ密度が減衰する。図7に示す通り一対の第3の粒子(3’,3”)が一波長離間する場合、符号18及び18’の位置で波動的に打ち消し合い熱エネルギ強度がゼロとなり、符号17及び17’の位置で波動的に強め合い熱エネルギ強度が2倍となる。強め合う位置(17,17’)に第3の粒子(3”’)が存在する場合、他の位置に比べ高効率で第3の粒子(3”’)が熱エネルギを吸収し保持するので、放射熱の伝播速度を遅らせて、遮熱及び断熱効果を高めることができる。即ち、本発明では、第1、第2及び第3の粒子(1,2,3)をそれぞれ規則正しく、特に、電磁波の強め合う位置(17,17’)付近に規則的に配置することにより、優れた遮熱及び断熱特性を有する遮熱・断熱材を形成することができる。一方、電磁波の弱め合う位置(18,18’)付近に粒子(1,2,3)を充填しても、効率的な熱の吸収は得られないため、高価な真空セラミック粒子の使用量を低減できることが理解できる。   When the third particle (3 ′, 3 ′ ′) receives solar heat, it absorbs a part of electromagnetic waves (infrared rays) of a specific wavelength and reflects 90% or more. By reflection, the polarization of electromagnetic waves is linear from rotational polarization Change in polarization and become incoherent to incoherent (speckle interference) Electromagnetic waves are reflected and re-emitted from every point on the surface of the third particle (3 ', 3 ") And diffuse and propagate as a spherical wave (16), and the heat energy density is attenuated in inverse proportion to the square of the distance. When the pair of third particles (3 ′, 3 ′ ′) are separated by one wavelength as shown in FIG. 7, the thermal energy intensity becomes zero at wave positions 18 and 18 ′, and the codes 17 and 17 ′ When the third particle (3 ′ ′ ′) is present at the position of reinforcement (17, 17 ′), the efficiency is higher than that at the other positions. Since the three particles (3 ′ ′ ′) absorb and retain the thermal energy, the propagation speed of radiant heat can be delayed to enhance the heat shielding and insulation effects. That is, in the present invention, the first, second and second By arranging the third particles (1, 2, 3) regularly, in particular, in the vicinity of the constructive positions (17, 17 ′) of the electromagnetic waves, a heat shield having excellent heat shield and heat insulation properties While heat insulation can be formed, efficient heat absorption is obtained even if particles (1, 2, 3) are filled in the vicinity of destructive positions (18, 18 ') of electromagnetic waves. Since it is not, it can be understood that it is possible to reduce the amount of expensive vacuum ceramic particles.

入射熱で吸収した電磁波は、第3の粒子(3’,3”)の外殻(3a)を通じて伝達され、入射側(19)の反対側(図示せず)にも放射熱として放出される。反対側では、入射側(19)と同様に、強め合う位置に第3の粒子が存在することにより熱エネルギを効率的に吸収できる。入射熱から吸収される熱エネルギは、入射熱の全エネルギの約10%足らずのため、図1及び図2に示す積層体(20,20’)では、内部に進むに従いエネルギは約1/10ずつ減衰してゼロに近づく。また、一対の粒子間を通過する電磁波の回折による可干渉でも、強め合う位置に粒子を配置して熱エネルギを効率的に吸収できる。また、入射熱のうち、第3の粒子(3’,3”)の周りを通過した電磁波は、入射側(19)の反対側(図示せず)で、第3の粒子(3’,3”)の回析による干渉により、前記同様に、強め合う位置に第3の粒子が存在することにより熱エネルギを効率的に吸収できる。 The electromagnetic wave absorbed by the incident heat is transmitted through the outer shell (3a) of the third particle (3 ′, 3 ′ ′) and is also emitted as radiation heat to the opposite side (not shown) of the incident side (19) On the opposite side, as with the incident side (19), the heat energy can be efficiently absorbed by the presence of the third particles at the intensifying positions.The heat energy absorbed from the incident heat is the total of the incident heat. In the stacks (20, 20 ') shown in FIG. 1 and FIG. 2, the energy decays by about 1/10 and approaches zero as it goes to the inside because the energy is less than about 10% of the energy. Even if the interference due to the diffraction of the electromagnetic wave passing through the particle is placed at a position where the particles are intensified, the heat energy can be absorbed efficiently, and around the third particle (3 ′, 3 ′ ′) of the incident heat, The electromagnetic waves having passed through are interfered by diffraction of the third particles (3 ′, 3 ′ ′) on the opposite side (not shown) of the incident side (19). As can be efficiently absorbs heat energy by the third particles are present in a position constructive.

本発明による遮熱・断熱材の遮熱及び断熱効果を測定する熱照射試験の実施例を以下説明する。   Examples of heat irradiation tests for measuring the heat shielding and heat insulating effects of the heat shielding and heat insulating material according to the present invention will be described below.

粒子集合体及び積層体の製造
3種類の真空セラミック粒子(1,2,3)と無機及び有機の複合樹脂(6)とを混合攪拌して得られた懸濁液(31)を気流(35)と共に二流体混合方式により加圧噴射装置のノズル(33)から約0.3MPa(約3気圧)で噴射した。懸濁液(31)は、空気中で粒子集合体(10)を形成し、厚さ30mmの断熱箱の上面を構成するガルバニュウム鋼板表面に、本発明による遮熱・断熱材の積層体(20)を0.29mm厚で形成した(本実施例)。他方、原料自体に直接約10MPa(約100気圧)の圧力を加え原料を高圧噴射し、粒子集合体を形成しない遮熱・断熱材を厚さ30mm断熱箱上面のガルバニュウム鋼板表面に2.0mm厚で形成した(比較例)。
Production of Particle Aggregates and Laminates The suspension (31) obtained by mixing and stirring three types of vacuum ceramic particles (1, 2, 3) and the inorganic and organic composite resin (6) is air-flowed (35) And at a pressure of about 0.3 MPa (about 3 atmospheres) from the nozzle (33) of the pressurized injection device in a two-fluid mixing system. The suspension (31) forms a particle assembly (10) in the air, and the laminate of the heat and heat insulating material according to the present invention is formed on the surface of the galvanium steel plate constituting the upper surface of the heat insulation box of 30 mm thickness. ) Was formed to a thickness of 0.29 mm (this example). On the other hand, a pressure of about 10MPa (about 100 atmospheres) is directly applied to the raw material itself to inject the raw material under high pressure, and heat and heat insulating materials that do not form particle aggregates are 30mm thick. (Comparative example).

熱照射試験及び試験結果
前記本実施例と比較例の各箱を密閉状態で屋外に並置し太陽光を照射した熱照射試験を8日間実施した。図8に試験結果を示す。図中、高さ方向中央の折れ線は、比較例から本実施例を引いた温度差[℃]を示し、図中下方の間欠的な折れ線は日射量[W/m2]を示す。間欠折れ線の開始点から次の間欠折れ線の開始点までが約24時間を示す。
Thermal Irradiation Test and Test Results A thermal irradiation test was conducted for 8 days, in which each box of the present example and the comparative example was placed outside in a closed state and juxtaposed outdoors and irradiated with sunlight. The test results are shown in FIG. In the figure, the broken line at the center in the height direction indicates the temperature difference [° C.] obtained by subtracting the present embodiment from the comparative example, and the intermittent broken line in the lower view indicates the amount of solar radiation [W / m 2 ]. The time from the start point of the intermittent broken line to the start point of the next intermittent broken line indicates approximately 24 hours.

図8より、日射が始まり日射量が最大値になる時間まで、温度差がプラスに大きくなる。これは、比較例の箱内の温度が急上昇する一方、本実施例では、強い日射を受けても実施例に比べ遮熱効果が高いことが分かる。次に、日射量最大時から日没までは、温度差がマイナスに大きくなる。比較例に対し本実施例の保温効果が高いと判断できる。本実施例の遮熱・断熱材の厚さは比較例に対し、約1/7にも関わらず、遮熱効果及び保温効果を格段に優れていることが分かる。   From FIG. 8, the temperature difference is positively increased until the time when the solar radiation starts and the solar radiation amount reaches the maximum value. It can be seen that while the temperature in the box of the comparative example rises rapidly, in the present embodiment, the heat shielding effect is higher than in the embodiment even when receiving strong solar radiation. Next, the temperature difference becomes negative from the maximum amount of solar radiation to the sunset. It can be judged that the heat retention effect of the present embodiment is higher than that of the comparative example. Although the thickness of the heat shield and heat insulating material of the present embodiment is about 1/7 of that of the comparative example, it can be seen that the heat shield effect and the heat retention effect are remarkably excellent.

本発明の遮熱・断熱材及びその製法は、屋根、建物外壁、ブラインド、屋上水槽、危険物貯蔵タンク、水道管、工場配管、自動車等の表面に塗布又は噴霧し、積層体を形成して内側への熱放射及び熱伝達を防止するだけでなく、表面温度を低下させることもできる。このため、道路、オートバイ、遊具、照明器具、家電製品、精密機器等の発熱及び保熱が好ましくない技術分野にも適用できる。また、衣料品、カーテン等の布製品表面に噴射又は塗布することも、繊維形成時に混練することも可能である。   The heat shield / insulation material of the present invention and the method for producing the same are applied or sprayed to the surface of a roof, building outer wall, blind, roof top water tank, hazardous material storage tank, water pipe, factory piping, automobile etc. In addition to preventing heat radiation and heat transfer inwards, the surface temperature can also be reduced. For this reason, it is applicable also to the technical field where heat generation and heat retention are not preferable, such as a road, a motorcycle, a playground equipment, a lighting fixture, a household appliance, a precision instrument etc. Also, it is possible to spray or apply on the surface of a cloth product such as clothing or curtain, or to knead at the time of fiber formation.

(1)・・第1の粒子(1)、 (2)・・第2の粒子、 (3)・・第3の粒子、 (6)・・バインダ、 (1a,2a,3a)・・外殻、 (1b,2b,3b)・・内部空洞、 (12)・・第2の粒子層、 (13)・・第3の粒子層、 (10)・・粒子集合体、 (20,20’)・・積層体、 (50)・・基体、   (1) · · First particle (1), (2) · · Second particle, (3) · · Third particle, (6) · Binder, (1a, 2a, 3a) · · External Shell, (1b, 2b, 3b) ··· Internal cavity, (12) · · Second particle layer, (13) · · Third particle layer, (10) · Particle assembly, (20, 20 ' ) · · Laminate, (50) · · Substrate,

Claims (6)

複数の第1の粒子と、第1の粒子の周囲を包囲する複数の第2の粒子と、第2の粒子の周囲を包囲する複数の第3の粒子と、第1、第2及び第3の粒子の同種及び異種粒子間を結合しかつ基体の表面に第1、第2及び第3の粒子を接着するバインダとを備え、
第1の粒子、第2の粒子及び第3の粒子は、何れも内部空洞を有し、
第2の粒子は、第1の粒子より粒径が小さく、第3の粒子は、第2の粒子より粒径が小さく、
第1の粒子の粒径は50〜100μm、第2の粒子の粒径は10〜50μm、第3の粒子の粒径は0.5〜10μmであり、
第2の粒子は、第1の粒子を覆う第2の粒子層を形成し、第3の粒子は、第2の粒子層を覆う第3の粒子層を形成することを特徴とする遮熱・断熱材。
A plurality of first particles, a plurality of second particles surrounding the periphery of the first particles, a plurality of third particles surrounding the periphery of the second particles, a first, a second and a third A binder which bonds the homogeneous and heterogeneous particles of the particles and adheres the first, second and third particles to the surface of the substrate,
The first particle, the second particle and the third particle all have an internal cavity,
The second particles are smaller in size than the first particles, and the third particles are smaller in size than the second particles,
The particle size of the first particle is 50 to 100 μm, the particle size of the second particle is 10 to 50 μm, and the particle size of the third particle is 0.5 to 10 μm,
The second particle forms a second particle layer covering the first particle, and the third particle forms a third particle layer covering the second particle layer. Insulation.
第3の粒子は、入射する熱エネルギを吸収し、入射する熱エネルギより小さい第3の熱エネルギを反射及び放射し、
第3の熱エネルギは、第2の粒子層を通過する際、第2の粒子に吸収されると共に、第2の粒子は、第3の熱エネルギより小さい第2の熱エネルギを反射及び放射し、
第2の熱エネルギは、第1の粒子に吸収されると共に、第1の粒子は、第2の熱エネルギより小さい第1の熱エネルギを反射及び放射する請求項1に記載の遮熱・断熱材。
The third particles absorb incident thermal energy, reflect and emit third thermal energy smaller than incident thermal energy,
The third thermal energy is absorbed by the second particle as it passes through the second particle layer, and the second particle reflects and emits the second thermal energy smaller than the third thermal energy. ,
The heat and heat insulation according to claim 1, wherein the second thermal energy is absorbed by the first particles, and the first particles reflect and emit the first thermal energy smaller than the second thermal energy. Material.
第1の粒子、第2の粒子及び第3の粒子の各内部空洞は、減圧状態又はほぼ真空状態である請求項1又は2に記載の遮熱・断熱材。   The heat shield / insulation material according to claim 1 or 2, wherein each internal cavity of the first particle, the second particle and the third particle is in a reduced pressure state or a substantially vacuum state. 第1の粒子、第2の粒子層及び第3の粒子層を含む粒子集合体を複数重ねて積層体を形成する請求項1〜3の何れか1項に記載の遮熱・断熱材。   The heat insulating and heat insulating material according to any one of claims 1 to 3, wherein a plurality of particle aggregates including the first particle, the second particle layer, and the third particle layer are stacked to form a laminate. 積層体は、第3の粒子より小さい粒径の第4の粒子により形成される表面層を備え、表面層は、第3の粒子層より過密に形成される請求項4に記載の遮熱・断熱材。   The heat shield according to claim 4, wherein the laminate comprises a surface layer formed of fourth particles smaller than the third particles, and the surface layer is formed more densely than the third particle layer. Insulation. 内部空洞を有する複数の第1の粒子5〜30重量部と、第1の粒子より粒径が小さくかつ内部空洞を有する複数の第2の粒子1〜20重量部と、第2の粒子より粒径が小さくかつ内部空洞を有する複数の第3の粒子0.1〜10重量部と、バインダ15〜40重量部と、揮発性溶媒5〜30重量部とを含む懸濁液を準備する工程と、
0.2〜0.4MPaに加圧した気流と共に懸濁液を二流体混合方式によりノズルから空気中に速度10〜500mm/secで噴射して、ノズルからの噴射距離が0.1m〜2mである基体の表面に懸濁液を均一に散布する工程と、
バインダの薄膜で被覆される第1の粒子、第2の粒子及び第3の粒子を含む懸濁液を基体の表面に均一に散布する運動中に、粒径50〜100μmの複数の第1の粒子を互いに個別に分離し、各第1の粒子の周囲を粒径10〜50μmの第2の粒子を主成分とする第2の粒子層により包囲し、かつ粒径0.5〜10μmの第3の粒子が揮発性溶媒の水分に担持されてバインダ中を外方向に移動することにより第2の粒子層の周囲を第3の粒子を主成分とする第3の粒子層により包囲して、第1の粒子、第2の粒子及び第3の粒子を基体の表面に付着させる工程と、
基体に付着する懸濁液を乾燥させて、第1の粒子、第2の粒子及び第3の粒子をバインダにより接着する工程とを含むことを特徴とする遮熱・断熱材の製法。
5 to 30 parts by weight of a plurality of first particles having an internal cavity, 1 to 20 parts by weight of a plurality of second particles having a smaller particle size than the first particle and having an internal cavity, and particles than a second particle Preparing a suspension comprising a plurality of third particles 0.1-10 parts by weight having a small diameter and an internal cavity, 15-40 parts by weight of a binder, and 5-30 parts by weight of a volatile solvent; ,
The suspension is jetted from the nozzle into the air at a velocity of 10 to 500 mm / sec by the two-fluid mixing method together with the air flow pressurized to 0.2 to 0.4 MPa, and the spray distance from the nozzle is 0.1 m to 2 m Uniformly spreading the suspension on the surface of a certain substrate;
A plurality of first particles with a particle size of 50 to 100 μm are in motion during the motion of uniformly spreading a suspension comprising the first particles, the second particles and the third particles coated with a thin film of the binder on the surface of the substrate. The particles are separated from each other, and each first particle is surrounded by a second particle layer mainly composed of second particles with a diameter of 10 to 50 μm, and a particle diameter of 0.5 to 10 μm The third particle layer is supported by the moisture of the volatile solvent and moves outward in the binder to surround the second particle layer by the third particle layer mainly composed of the third particles, Attaching the first particles, the second particles and the third particles to the surface of the substrate;
And drying the suspension adhering to the substrate to adhere the first particles, the second particles and the third particles with a binder.
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