ENERGY-SAVING HEAT INSULATION OF BUILDINGS

Abstract: It is a new method of thermal insulation of buildings. Its practical implementation is realized with two manners, that is:1. With a diffused reflection of the thermal radiation and with a diffused reflection of the thermal transition of the air, from the internal and the external surfaces (1a, 5a) of the sublayers of the external masonry, of the external roofs, the internal masonry and the internal ceilings of the buildings. 2. With a low emission of thermal radiation, with a diffused reflection of thermal radiation and a diffused reflection of thermal transition of the air, from the internal surfaces of a parallel plane division with an enclosed layer of air (4f), which is constructed at the internal side of the sublayers (1f, 2f) of the external masonry and the external roofs of the buildings. These surfaces are covered with a liquid, white colored insulating material (3f, 6f), which is manufactured in three types, A, B and C, and can be colored with the addition of coloring pigments, when it dries it is not dissolved with water and forms the final surface of the above sublayers.

Description: DESCRIPTION - ENERGY-SAVING HEAT INSULATION OF BUILDINGS This invention refers to a new method of thermal insulation of buildings, with a diffused reflection of the thermal radiation and a diffused reflection of the thermal transition of the air. The practical implementation is made with two manners. 1. With a diffused reflection of the thermal radiation and a diffused reflection of the thermal transition of the air, from the internal and the external surfaces of the sub-layers of the external masonry, of the external roofs, the internal masonry and the internal ceilings of the buildings. 2. With a low emission of thermal radiation, with a diffused reflection of thermal radiation and a diffused reflection of thermal transition of the air, from the internal surfaces of a parallel plane division with an enclosed layer of air, which is constructed at the internal side of the sub-layers of the external masonry and the external roofs of the buildings. The diffused reflection of the thermal radiation and the diffused reflection of the thermal transition of the air, as well as the low emission of thermal radiation, are attained with a liquid insulating material (heat insulating, reflecting and sealing), white colored, used to cover the surfaces of the above sub-layers and which constitute the final surface of these sub-layers. The white colored liquid insulating material, is manufactured in three types A, B and C, and can be colored with the addition of coloring pigments, and following its practical application, in a solid form (after it dries), it does not dilute in water. The loss of heating energy and cooling energy of internal spaces of buildings, through the sub-layers of the external masonry and the external roofs of the buildings, as well as, through the sub-layers of their internal masonry and their internal ceilings, which are close to non-heated and non-cooled closed spaces, are due to: The absorption of an important quantity of energy, by the falling thermal radiation and the falling thermal transition of the air, from the internal and the external surfaces of these sub-layers. The absorbed energy is transformed into heat and is transmitted with thermal convection inside these sub-layers. The absorption of an important quantity of energy, by the internal and external surfaces of these sub-layers, is due to the following reasons: 1. The internal and external surfaces of the above sub-layers are non- reflective, non-heat-insulating and moderately electrically conductive. Being moderately electrically conductive, these surfaces do not preserve constant (in the same areas) the developing electric charges within their mass, resulting in not preserving constant (at the same areas) the developing attractive and repelling forces, between the atoms of their molecules in their mass, and consequently, disturbing at a considerable degree, the energetic equilibrium wiithin the mass of these surfaces. 2. The internal and external surfaces of the above sub-layers are mainly consisting of a set of millions of microscopic concave surfaces, of an irregular and different shape, for each single concave microscopic surface. The concave microscopic surfaces increase the surface on which falls the thermal radiation and the thermal transition of the air and absorb an important quantity of energy, because: a) They absorb (focus, concentrate) the thermal radiation which falls over them, due to the successive reflections of electromagnetic waves, over every concave, microscopic surface, Fig. 1. b) They absorb (focus, concentrate) the thermal transition of the air that falls over them, due to the successive reflections of the atoms of the mass molecules of the air at a higher temperature, on every concave, microscopic surface, Fig. 2. The concave, microscopic surfaces absorb an important quantity of energy from the sound waves (from the oscillations of the air pressure) which fall on them, because: They absorb (focus, concentrate) the sound waves (the oscillations of the air pressure) which fall on them, due to the successive reflections of the sound waves, on every concave, microscopic surface, Fig. 3. Until this day, the conventional heat insulation of the internal spaces of buildings, is being used with the addition of heat insulating material inside the sub-layers of the external masonry and the external roofs of the buildings, as well as their sub-layers of their internal masonry and their internal ceilings, which are in contact to non-heated and non-cooled closed spaces. The heat insulating material that is being added, does not form the final surface of these sub-layers. With the addition of a heat insulating material inside the above sublayers, the resistance to heat-leak 1/Λ is increased and the coefficient of heat transfer K (coefficient of heat permeability) is decreased, having as a result the decrease of heating energy and cooling energy losses of internal spaces of sub-layers of buildings, through these sub-layers. The heat transfer coefficient K, is the same for losses of heating and cooling energy, through each of the above sub-layers of the building materials and structural element. The conventional heat insulation of the internal spaces of buildings presents the following disadvantages: 1. A large consumption of energy is required, having as a result, the pollution of the environment. The increased consumption of energy is due to the following reasons: a) The manufacture of large quantities of heat-insulating materials and their transport. b) The manufacture of large quantities of sealing materials, for the protection of the heat-insulating capacity of the heat-insulating materials. 1.1. A large consumption of energy and a high heating and cooling costs of the internal spaces of buildings, are required for the following reasons: a. To the losses of heating energy, at the starting of the heating operation of internal spaces of buildings. b. To the losses of heating and cooling energy, from the protrusions of the concrete (thermal-bridges) of the roofs and facades of the buildings. c. To the increased losses of heating energy and cooling energy, of the internal spaces of the buildings, because the further decrease of these losses is uneconomical. 2. The effective surface of the internal spaces of buildings is decreased due to the increase of the thickness of the external masonry. 3. The great cost for the insulation of new and existing non-insulated buildings, due to the long duration of the insulation works. 4. Great erection cost for new buildings, due to the large insulating costs and the decrease of the effective surface of the internal spaces of these buildings. The energy-saving heat insulation of the buildings, with a diffused reflection of the thermal radiation and diffused reflection of the thermal transition of the air, is a new method for the heat insulation of buildings. Its practical application is realized with two manners, that is: 1. With a diffused reflection of thermal radiation and with a diffused reflection of thermal transition of the air, from the internal and external surfaces of the sub-layers of external masonry, the external roofs, the internal masonry and the internal ceilings of the buildings. 2. With a low emission of thermal radiation, with a diffused reflection of thermal radiation and a diffused reflection of thermal transition of the air, from the internal surfaces of a parallel plane division with an enclosed layer of air, which is constructed at the internal side of the sub-layers of the external masonry and the external roofs of the buildings. The know-how for its construction, transforms the non-insulating and non- reflective internal and external surfaces of the sub-layers of the external and the internal masonry, the external roofs and the internal ceilings of the buildings, as well as the internal surfaces of the parallel level division with an enclosed air layer, into heat-insulating and reflective to the thermal radiation and to the thermal transition of the air, as follows : These surfaces are covered with a white colored liquid insulating material (heat insulating, reflective and sealing), which forms the final surface of these sub-layers. The white colored liquid insulating material, is manufactured in three types A, B and C and can be colored with the addition of coloring pigments and after its practical application in a solid form (when it dries), it is does not dilute in water. These surfaces are heat insulating, reflective, electrically insulating, they have a low emission of thermal radiation and they reflect (re-reflection) in a diffused manner, the larger part of the energy from the falling thermal radiation and the falling thermal transition of the air, because : 1. Being electrically insulating, these surfaces retain constant (in the same areas) the electrical loads developing inside their mass, and consequently, they keep constant (in the same areas) also the developing attractive and repelling forces between the atoms of their mass molecules, and as a result, the energetic equilibrium in the mass of these surfaces, is affected at a small degree. 2. Being heat insulating, these surfaces are formed by a totality of millions of heat-insulating convex microscopic surfaces, with the same geometric shape for every heat-insulating convex microscopic surface, which contain enclosed air. The microscopic convex surfaces, decrease the surface on which fall the thermal radiation and the thermal transition of the air and they absorb a smaller quantity of energy, because: a) At the fall of the thermal radiation, the successive reflections of electromagnetic waves are avoided on every convex microscopic surface, Fig. 4. b) At the fall of the thermal transition of the air, the successive reflections of atoms, from the mass molecules of the air with a higher temperature, are avoided, on every convex microscopic surface, Fig. 5. The convex, microscopic surfaces, absorb a smaller quantity of energy, from the sound waves (from the oscillations of the air's pressure) which fall over them, because: At the fall of the sound waves, their successive reflection on every convex microscopic surface is prevented Fig.6. The reflected energy, from the fall of thermal transition of the air, is the same with the reflected energy, from the fall of sound waves, because every oscillation due to the pressure of the air exerts a thrust on the neighboring air molecules, Given that the internal and external surfaces of the sub-layers of the external masonry and the external roofs of the buildings are strained at a different extent, by the climatic conditions and the environmental influences, and the degree of requirements on the visual quality of coloring is different: The liquid insulating material (heat insulating, reflecting and sealing) is made in three types A, B and C. The composition of the liquid insulating material, which guarantees an efficacious operation of the new method for the heat insulation of buildings. Is the following: 1. Expanded perlite, with a microscopic granulometry 0 up to 130 μm, convex and of the same geometric shape for every convex microscopic granule, or 1a. Expanded ceramic material, with a microscopic granulometry 0 up to 130 μm, convex and of the same geometric shape for every convex microscopic granule. 2. Binding material, 100% pure acrylic. 3. Elastomeric co-polymerized acrylic. 4. Synthetic(plastic) materials. 5. White coloring pigments of titanium oxides. 6. Mineral chloric sodium. 7. Aluminum water glass. 8. Silica oxide. 9. Liquid silicone. 10. Fungicide material. 11. Antifreezing material. 12. Water. The proportion per volume, of the above materials (components), differs for every type of liquid insulating material, that is: Type A, provides an increased visual quality of the coloring on the covered surfaces and has a lower resistance against stresses from climatic conditions and environmental influences, in comparison to types B and C. Type A is used for the coating of the internal surfaces of sub-layers of the external masonry and roofs of buildings, as well as the surfaces of their internal masonry. Type B provides a decreased visual coloring quality of the covered surfaces and has an increased resistance to stresses, due to climatic conditions and environmental influences, in comparison to type A. Type B is used to cover the external surfaces of sub-layers of the external masonry of buildings and the external surfaces of projections of those sublayers. Type C provides a decreased visual coloring quality of the covered surfaces and has an increased resistance to stresses due to climatic conditions and environmental influences, in comparison to type B. Type C is used to cover the external surfaces of sub-layers of external roofs of buildings, the external surfaces of projections of those sub-layers and the internal surfaces of the sub-layers of the parallel level division, with enclosed air layer. During the coating of the three types A, B and C of liquid insulating material, the expanded convex microscopic granules are distributed in equal parts and cover uniformly the surface of every sub-layer, due to their content of liquid silicone. After the evaporation of its humidity, the expanded convex microscopic granules, in cooperation with the other components, form a unified and compact heat-insulating layer of a small thickness and increased insulating (heat-insulating, reflecting and sealing) capacity. The properties of the three types A, B and C of the liquid insulating material in solid form (when it dries), are the following: 1. Its primary color is white. It can be colored with the addition of coloring pigments and after its practical application in solid form (when it dries) it is not water-soluble. 2. It has high coefficient of thermal radiation and thermal transition of the air, due to the convex microscopic surfaces which are formed by the expanded convex microscopic granules and due to its content in: a) Mineral chloric sodium, for the reflection of the infrared radiation. b) Aluminum water glass, for the reflection of the visible (luminous) radiation. c) Silica oxides, for the reflection of the ultraviolet radiation. d) Immobilized enclosed air, inside the convex microscopic granules, for the increase of its heat-insulating quality and the reflection thermal transition of the air and the sound waves (the oscillations of the air pressure). 2.1. The type A has the following coefficients: p = 80%, A = ε = 0,2 and pi = p2 = 86%. 2.2. The type B has the following coefficients: p = 82%, A = ε = 0, 18 and pi = p2 = 88%. 2.3. The type C has the following coefficients: p = 84%, A = ε = 0,16 and pi = p2 = 90%. Where: p is the reflection coefficient of the thermal radiation. A is the degree of absorption of the thermal radiation, ε is the emission coefficient of the thermal radiation, pi is the reflection coefficient of the thermal transition of the air. p2 is the reflection coefficient of the sound waves. p< pi for increased energy saving. ε = A the same temperature of the liquid insulating material, in solid form. Changing the percentage in volume of the above ingredients, we reach different coefficients. 3. It has a strong adhesion, due to its content in synthetic (plastic) materials. 4. It is elastic. Due to its elasticity, it follows the movements of the sub-layers of the construction materials and the structural elements, during their expansion and contraction and thus, the creation of thermal bridges (fissures and cracks) is avoided, on their covered surfaces. Types B and C have a higher elasticity, in comparison to type A. It retains its elasticity from -30°C to +120°C. 5. It is water permeable (it breaths). It presents a low resistance to the diffusion of water vapors and allows their easy escape, from the sub-layers of the construction materials and the structural elements. 6. It is non-permeable by carbon dioxide CO2. It presents increased resistance to the diffusion of carbon dioxide CO2 and prevents the carbonization of the sub-layers of reinforced concrete. 7. It is sealing. It becomes waterproof when water settles on its surface and prevents the escape of water vapors through the sub-layers. When the water evaporates, it allows again the escape of the enclosed water vapors through the sub-layers. 8. It is solid and resists mechanical pressure and air pressure, leading to the result: The creation of thermal bridges and sound bridges (fissures and cracks), on the covered internal and external surfaces of sub-layers of the construction materials and the structural elements, is avoided, due to the high velocity of the air and due to hailstone fall, storms and small objects carried by the wind on the coated external surfaces of these sub-layers. Types B and C have a greater resistance, in comparison to type A. Type C resists to the stress of normal practicability. 9. It is non combustible, due to its content in titanium oxides and in expanded inert matter. 10. It is resistant to environmental influences. Types B and C present an increased content in synthetic (plastic) materials, compared to type A, which offers them a greater resistance to several chemical matters, like hoarfrost salts, atmospheric dirt, oils, benzene etc. 11. It presents a high resistance to aging. Thanks to its composition, it is protected from aging influence, since it is not affected by the ultraviolet radiation and it is not eroded by the climate conditions and the environmental influences. 12. It retains for a long time, the quality of its coloring, because with the property of reflection, it repels dust, smoke and dirt in general. The foreign particles laying on the covered surfaces of sub-layers of the construction materials and structural elements, lose photochemically their adhesion, thanks to the property of reflection, leading to the result that the internal covered surfaces can be cleaned easily and the covered external surfaces of these sub-layers, to be washed out with the next rain. The first means of application for the new method of heat insulation of buildings, presents the following advantages: 1. A large amount of energy is saved and the pollution of the environment is decreased, since with the thermal insulation of the internal spaces of buildings, we succeed simultaneously: The sound insulation of the buildings' internal spaces, against airborne sounds, the protection of the building materials and structural elements, from the stresses of climatic conditions and environmental influences and the coloring of internal and external surfaces of the sub-layers of the internal and external masonry, the external roofs and the internal ceilings of the buildings. 1.1. We achieve a large saving of energy, and also, a smaller heating and cooling cost for the internal spaces of the buildings, for the following reasons: a) Due to smaller losses of heating energy, at the starting of the heating of the internal spaces of the buildings. b) Due to smaller losses of heating and cooling energy, from the reinforced concrete protrusions (thermal bridges) of the roofs and the facades. c) Due to smaller losses of heating and cooling energy, of the internal spaces of the buildings, during their heating and cooling. 2. The effective surface of internal spaces of buildings is increased due to the reduction of the thickness of the external masonry. 3. A lower cost for the insulation of new and existing non-insulated buildings is achieved, thanks to the short duration of the insulation works. 4. A lower cost for the erection of new buildings is achieved, thanks to the lower cost for the insulation and the increase of the effective surface of the internal spaces of the buildings. 5. A thermal comfort is achieved, thanks to the uniform distribution of temperature, in the internal spaces of the buildings. 6. A noise comfort is achieved, thanks to the uniform distribution of sound waves, inside the internal spaces of the buildings and an adding action of the sound waves ensues, which increases the acoustic impression. The main advantages of the second method of application of the new method of thermal insulation of buildings are the following: 1. The possibility for the decoration of internal and external surfaces, of the sublayers of the external masonry and the external roofs of the buildings, is provided. 2. Large savings in energy is achieved, with the decrease of losses of heating and cooling energy, through the sublayers of the external masonry and the external roofs of the buildings and with the decrease of the heating energy losses at the starting of the heating of internal spaces of the buildings. 3. At the same time, the sound insulation of internal spaces of the buildings is achieved, against the airborne noises, with the attenuation of the absorbed sound waves inside the enclosed layer of air, with their consecutive reflections by the parallel heat-insulating and reflecting internal surfaces. 4. The time of resonance of the internal spaces of buildings with large volume is decreased. A practical application of the new heat insulating method for internal spaces of buildings, is given with reference to the attached drawings: In Fig.1 we see in section, the absorption of the thermal radiation that falls on a concave surface. In Fig.2 we see in section, the absorption of the thermal transition of the air, that falls on a concave surface. In Fig.3 we see in section, the absorption of the sound waves that fall on a concave surface. In Fig.4 we see in section, the absorption of the thermal radiation that falls on a convex surface. In Fig.5 we see in section, the absorption of the thermal transition of the air, that falls on a convex surface. In Fig.6 we see in section, the absorption of the sound waves that fall on a convex surface. In Fig.7 we see in section, a sublayer of a reinforced concrete low wall of the external masonry, thermally insulated against the cold and heat of the external environment. In Fig.8 we see in section, a sublayer of the external masonry, from perforated bricks, thermally insulated against the cold and heat of the external environment. In Fig.9 we see in section, a sublayer of the reinforced concrete slab of the terrace (roof), thermally insulated against the cold and heat of the external environment. In Fig.10 we see in section, a sublayer of the wooden roof with tiles (sloped roof), thermally insulated against the cold and heat of the external environment. In Fig.11 we see in section, a sublayer of the internal masonry, from perforated bricks which is adjacent to a non heated, closed space, thermally insulated against the cold. In Fig.12 we see in section, a sublayer of a reinforced concrete low wall of the external masonry, with a parallel plane division, with enclosed layer of air. In Fig.13 we see in section, a sublayer of the external masonry, from perforated bricks, with a parallel plane division, with enclosed layer of air. In Fig.14 we see in section, a sublayer of the reinforced concrete slab of the terrace (roof), with a parallel plane division, with enclosed layer of air. In Fig.15 we see in section, a sublayer of the wooden roof with tiles (sloped roof), with a parallel plane division, with enclosed layer of air. Referring to Fig. 7, the sublayer of the reinforced concrete low wall of the external masonry, is made up of the liquid insulating material, type A, in solid form at its internal surface -1-, of a layer of common or heat insulating plaster at its internal side -2-, of a low reinforced concrete wall -3-, of a layer of common or heat insulating plaster, at its internal side -4- and of the liquid insulating material type B in solid form, at its external surface -5-. Referring to Fig. 8, the perforated bricks sublayer of the external masonry, is made up of the liquid, insulating material, type A, in solid form at its internal surface -1a-, of a layer of common plaster with sand, at its internal side -2a-, of the perforated bricks -3a-, of horizontal layers of common building plaster -4a-, of a layer of common building plaster with sand, at its external side -5a- and of the liquid insulating material, type B in solid form, at its external surface -6a-. Referring to Fig. 9, the sublayer of the reinforced concrete slab of the terrace (roof), is made up of the liquid insulating material, type A, in solid form at its internal surface -1 b-, of a layer of common or heat insulating plaster, at its internal side -2b-, of the reinforced concrete slab -3b- and of the liquid insulating material, type C in solid form, at its external surface -4b-. Referring to Fig. 10, the sublayer of the wooden roof (sloping roof) with tiles, is made up of the liquid insulating material, type A, in solid form at its internal surface -1c-, of a layer of wooden revetment, at its internal side -2c-, of the supporting beams -3c-, of the chief-rafters -4c-, of the cross-girders -5c-, layer of MDF -6c-, of a layer of tiles at its external side -7c- and the liquid insulating material, type C in solid form, at its external surface -8c-. Referring to Fig. 11 , the sublayer of perforated bricks of the internal masonry, is made up of the liquid insulating material, type A, in solid form at its internal surface -1 d-, of a layer of common plaster, at its internal side -2d-, of the perforated bricks -3d-, of horizontal layers of common construction plaster -4d-, and a layer of common plaster with sand, at its external side -5d -. Referring to Fig. 12, the sublayer of the reinforced concrete parapet of the external masonry, is made up of a layer of common plaster with sand, at its internal side -1e-, of a layer of plaster board -2e-, of the liquid insulating material, type C, in solid form -3e- of the enclosed layer of air -4e-, of the supports of the plaster board -5e-, of the liquid insulating material type C in solid form -6e-, of the reinforced concrete parapet -7e- and of a layer of common plastering with sand, at its external side -8e-. Referring to fig. 13, the sublayer of the perforated bricks of the external masonry, is made up of a layer of common plastering with sand, at its internal side -1f-, of a layer of plaster board -2f-, of the liquid insulating material, type C, in solid form -3f-, of the enclosed layer of air -4f-, of the supports of the plaster board -5f-, of the liquid insulating material type C in solid form -6f-, of the horizontal layers of common plastering -7f-, of the perforated bricks -8f- and of a layer of common plastering with sand, at its external side -9f-. Referring to Fig. 14, the sublayer of the reinforced concrete slab of the terrace (roof), is made up of a layer of common plastering with sand, at its internal side -1g- , of a layer of plaster board -2g-, of the liquid insulating material, type C, in solid form -3g-, of the enclosed layer of air -4g- , of the supports of the plaster-board -5g-, of the liquid insulating material type C in solid form -6g- and of the reinforced concrete slab -7g -. Referring to Fig. 15, the sublayer of the wooden roof (sloping roof) with tiles, is made up of a layer of wooden revetment, at its internal side -1h- , of the supporting beams -2h-, of the chief-rafters -3h-, of the cross-girders -4h-, of a layer of MDF -5h-, of the liquid insulating material, type C in solid form -6h-, of the enclosed layer of air -7h-, of the supports of the plaster board -8h-, of the liquid insulating material, type C in solid form -9h-, of a layer of MDF -10h- and of a layer of tiles at its external side -11 h -. In the new method of thermal insulation of buildings: The coefficient of heat convey (the coefficient of thermal transmittance) K, of every sublayer of the construction materials and the structural elements, is decreased with the decrease of the quantity of absorbed energy, by the falling thermal radiation and by the falling thermal transition of the air, from the internal and the external surface of the sublayer. The quantity of absorbed energy, by the internal and external surface of the sublayer, is reduced as follows: a) By reflection (retransmission) of the larger quantity of energy of the falling thermal radiation and the falling thermal transition of the air, from the heat insulating internal and external surface of the sublayer. b) By reducing the thermal flow through the sublayer, which is transmitted by thermal radiation and thermal transition of the enclosed air within the sublayer, due to the low degree of exchange of thermal radiation, between the parallel heat insulating internal surfaces and due to the reflection of the thermal transition of the enclosed air, from every parallel heat insulating internal surface. The thermal flow of the heating energy QΘ in Kcal/m 2 h and the thermal flow QΨ in Kcal/m 2 h which corresponds to the losses of cooling energy, through every non-insulated sublayer, is calculated with the relations: QΘ = K • DTι and QΨ= K • DT2 Where: K is the coefficient of heat convey of every non-insulated sublayer in Kcal/ m 2 h°C. DT1 = T1-T2, is the difference of temperature in Centigrade, between the temperature T1 of the internal air and the temperature T2 of the external air. DT2 = T2-T1 , is the difference of temperature in Centigrade, between the temperature T2 of the external air and the temperature T1 of the internal air. The thermal flow of the heating energy Q1 in Kcal/m 2 h through every heat insulated sublayer, is calculated with the relation: Qι = Kι • DTι = QΘ - Qθμ Where: Q©μ is the reduced quantity of absorbed energy (the reflected energy) in Kcal/ m 2 h by the internal surface of the sublayer, and is calculated with the relation: Qθμ = QΘ • p∑i. Kι is the coefficient of the thermal convey in Kcal/m 2 h°C, of the thermal flow of heating energy through the heat insulating sublayer, p∑i is the overall coefficient of the reflection of the heat insulating internal surface of the sublayer, or the overall coefficient of the diminution of the thermal flow of the heating energy, through the sublayer, which is transmitted with thermal radiation and with thermal transition of the enclosed air, inside the sublayer. Since: Qi = Ki • DTi = QΘ - Qθμ = QΘ - QΘ • p∑i = QΘ • (1- p∑i). Ki is : K, = -^L = ^≤-. (1 - p ) => !<, = K (1 -p Σ1 ) , because -5 ® - = K of 1 D D ∑1 1 ∑1 D^ the non-insulated sublayer. The overall coefficient p∑i of the diminution of the thermal flow of the heating energy through the sublayer, is also the overall diminution coefficient p∑i of the coefficient of thermal convey K of the non-insulated sublayer and is equivalent to an increase of the thermal leak resistance 1/Λ of the sublayer, by: - - --- in m 2 h°C/Kcal. λ K, K The thermal flow Q2 in Kcal/m 2 h , from the external environment to the internal spaces of the buildings, through the thermally insulated sublayer, corresponds to the losses of cooling energy, through the sublayer and is calculated with the relation: Q2 = K2 ■ DT2 = Qψ - Q Ψμ . Where: Qψμ is the reduced quantity of absorbed energy (the reflected energy) in Kcal/m 2 h from the external surface of the sublayer, and is calculated by the relation: Qψμ = Qψ ■ p∑2. K2 is the coefficient of heat conveyance in Kcal/m 2 h°C of the thermal flow through the thermally insulated sublayer, from the external environment, to the internal spaces of the buildings. p∑2 is the overall reflection coefficient of the heat insulating external surface of the sublayer, or the overall coefficient of the reduction of the thermal flow which corresponds to the losses of cooling energy, through the sublayer, which is transmitted with thermal radiation and with thermal transition of the enclosed air, inside the sublayer. Because : Q2 = K2 - DT2 = Qψ - Qψμ = Qψ - Qψ ■ p∑2 = Qψ-(1 - p∑2) . K2 ls : K 2 = -^- = ^- . (i _ p ) => κ 2 = K (1- p Σ2 ) , because -5ϋ = K 2 DT 2 DT 2 Σ2 2 Σ2 DT 2 of the non-insulated sublayer. The overall reduction coefficient p∑2 of the losses of cooling energy through the sublayer, is the overall reduction coefficient of the coefficient K of the heat convey of the non-insulated sublayer, and is equivalent to the increase of the thermal leak resistance 1/Λ of the sublayer, by: — = in λ, K 2 . mVC/Kcal . Every sublayer of the construction materials and the structural elements which is thermally insulated against the cold and heat of the external environment, operates with a reduced coefficient of heat conveyance Kι, of the thermal flow of heating energy and with a reduced coefficient of heat conveyance K2 of the thermal flow which corresponds to the losses of cooling energy, through it. The overall coefficients of reduction p∑i and p∑2 are comparative magnitudes for the reduction of the thermal flow, through every sublayer of the construction materials and the structural elements. The first mode for the implementation of the new method of heat insulation of buildings, provides the following possibilities: 1. The heat insulation of the internal spaces of buildings against the cold of the external environment, which is realized as follows: The internal surfaces of sublayers of the external masonry and roofs of the buildings, as well as the internal surfaces of sublayers of the internal masonry, which are adjacent to no heated closed spaces, are coated with the white colored liquid insulating material, type A, with a minimum approximate coating thickness of approximately D = 0,3 millimeters. These sublayers, as well as the sublayers of the internal ceilings of the buildings, operate with a reduced coefficient of thermal conveyance K1 of the heating energy losses, through them. Simultaneously, a sound insulation of the internal spaces against the airborne noise, is obtained through these sublayers to the direction of every adjacent internal or external space. 2. The heat insulation of the internal spaces of buildings against the heat of the external environment, which is realized as follows: a) The external surfaces of sublayers of the external masonry of the buildings, as well as the external surfaces of the protrusions of these sublayers are coated with the white colored liquid insulating material, type B, with a minimum approximate coating thickness of approximately D = 0,3 millimeters. b) The external surfaces of sublayers of the internal masonry which are adjacent to non cooled closed spaces are coated with the white colored liquid insulating material, type A, with a minimum approximate coating thickness of approximately D=0,3 millimeters. c) The external surfaces of sublayers of the external roofs of the buildings, as well as the external surfaces of the protrusions of these sublayers are coated with the white colored liquid insulating material, type C, with a minimum approximate coating thickness of D = 0,4 millimeters. These sublayers operate with a reduced coefficient of thermal conveyance K2 of the thermal flow which corresponds to the cooling energy losses, through them. Simultaneously, a sound insulation of the internal spaces against the airborne noise, is obtained through these sublayers from the external environment and from every adjacent, non cooled internal space. 3. The heat insulation of the internal spaces of buildings against the cold and the heat of the external environment, which is realized as described above, in paragraphs 1 and 2. A practical application is show in Drawings Fig.7, Fig.8, Fig.9 and Fig.10. The sublayers of the external masonry, of the external roofs and the sublayers of the internal masonry, which are adjacent to non-heated and to non cooled closed spaces, operate with a reduced coefficient of heat conveyance K1 of the losses of heating energy and with a reduced coefficient of heat conveyance K2 of the losses of cooling energy, through them. Simultaneously, a sound insulation of the internal spaces of the buildings against the airborne noise, is obtained through these sublayers from every adjacent internal or external space and from the external environment. The white insulating material is mixed with a mixer adapted to a slow, electric bore machine, before being coated and every ten to fifteen minutes during all the length of the coating, in order to have an isomehc distribution of its ingredients on every coated surface. The liquid insulating material must dry normally, not to be absorbed abruptly and not to evaporate abruptly. It is coated with an environmental temperature of +5°C to +25°C. It is coated with a roll and every coat is applied crosswise, after the previous one has dried. The surfaces of the sublayers of the construction materials and structural elements, which will be coated with the liquid insulating material, must be clean (they are washed with water in order to remove the dust), dry and solid (hard). The solidification of the surfaces of the sublayers of the construction materials and structural elements, in order to reduce the cost, is made with their impregnation (priming) with an elastic acrylic synthetic emulsion (with a high content of plastic substances), which is coated with a paintbrush or a brush. Follows a smoothening out of the internal and external surfaces of the sublayers of the external masonry, of the surfaces of sublayers of internal masonry and of the internal surfaces of the sublayers of internal ceilings of the buildings with acrylic stucco. The smoothening out of the external surfaces of the sublayers of reinforced concrete of external roofs of buildings is made with a sealing cement plaster. The expansion joints of the sublayers of reinforced concrete of the external masonry and the external roofs of buildings, are filled with a material of high elasticity, which does not acquire permanent deformations and are covered with an elastic polyesteric gauze for the strengthening of the elastic revetments, which is glued with an elastic, acrylic synthetic emulsion along all their length. The losses of heating energy and cooling energy of the internal spaces of the buildings, through the sublayers of the external masonry and the external roofs of the buildings, as well as through the sublayers of their internal masonry and their internal ceilings adjoining to non heated and non cooled closed spaces, are decreased as follows: At the fall of thermal radiation and thermal transition of the air, on the heat insulating internal and external surfaces of their sublayers, due to the small degree of derangement of the energy equilibrium i their mass, the larger part of the falling energy is reflected (retransmitted) and the quantity of energy penetrating these sublayers is reduced, having as result: 1. The temperature Twi, of the heat insulating internal surfaces of these sublayers is increased and the difference of temperature DTι=Tι-Twι between the temperature Ti of the internal air and the temperature Twi is decreased during the heating of the internal spaces of the buildings. Due to the decrease of the difference of temperature DTι=Tι-Twι, the coefficient of heat convey K of the losses of heating energy, of every upper sublayer of the construction materials and structural elements is decreased, because the difference of temperature DTι=Tι-Twι is the motive power for the losses of heating energy, through these sublayers. The percentage of decrease of the difference in temperature DTι=Tι-Twι is equal to the percentage of the overall reflection coefficient of every heat insulating internal surface of these sublayers, is equal to the percentage of decrease of the heat conveyance coefficient K and remains constant at the increase and decrease of the losses of heating energy, through every above mentioned sublayer. 2. The temperature Tw2 of the heat insulating external surfaces of these sublayers is increased and the difference of temperature DT2=T2-Tw2 between the temperature T2 of the external air and the temperature Tw2 during the cooling of the internal spaces of buildings is decreased. Due to the decrease of the difference of temperature DT2=T2-Tw2, the coefficient K of heat conveyance of the losses of cooling energy of every above mentioned sublayer of the building materials and structural elements is decreased, because the difference of temperature DT2=T2-Tw2, is the motive power for the thermal flow, through these sublayers, which corresponds to the losses of cooling energy, through these sublayers. The percentage of decrease of the difference in temperature DT2=T2-Tw2 is equal to the percentage of the overall reflection coefficient of every heat insulating external surface of these sublayers, is equal to the percentage of decrease of the coefficient of heat conveyance K and remains constant at the increase and decrease of the thermal flow, which corresponds to the losses of the cooling energy, through every above mentioned sublayer. The coefficient of reflection of the thermal radiation p and the coefficient of reflection of the thermal transition of the air pi, of every heat insulating internal and external surface of the above sublayers, decrease the coefficient K of the heat conveyance of every above sublayer, of the building materials and the structural elements, because they remain constant at the increase and decrease of the losses of heating energy and cooling energy, through every, above mentioned sublayer. During the heating of the internal spaces of buildings, the overall coefficient of decrease p∑i of the coefficient of heat conveyance K of the losses of heating energy of every above sub-layer, is equal to the overall coefficient of the reflection of the heat insulating internal surface of every above sub-layer and is calculated as follows: a) During the heating of the internal spaces of buildings, with radiators of thermal radiation, the transfer of heat for the heating of the internal air is made with thermal radiation. The reflection of the larger quantity of falling energy, by the heat insulating internal surface of every above sub-layer, is made with the reflection coefficients p and pi. When p < pi = p∑i = p and Ki = K - K ■ p∑i = K- (1 - p∑i) = K- (1 - p). When p > pi => p∑i = pi and Ki = K - K ■ p∑i = K- (1 - p∑i) = K- (1 - pi). b) During the heating of the internal spaces of buildings, with the adduction of heated air, the transfer of heat for the heating of the internal air is made with thermal transition towards the adjacent internal air. The reflection of the larger quantity of the falling energy, by the heat insulating internal surface of every above sublayer, is made with the coefficient of reflection of the thermal transition p∑i = pi and Ki = K - K ■ p∑i = K • (1 - p∑i) = K- (1 - pi). c) During the heating of the internal spaces of buildings, with contact - transfer radiators, the transfer of heat for the heating of the internal air, is made with thermal radiation and with thermal transition to the adjacent internal air. The reflection of larger quantity of the falling energy, by the heat insulating internal surface of every above sub-layer, is made with the coefficient of reflection p and pi. When p < pi => p∑i = p ■ n% + pi • m% . When p > pi ==> p∑i = pi • n% + pi ■ m% = pi ■ (n% + m%) = p∑i = pi . Ki is : Kι = K - K - p∑ι = K - (1 - p∑i) . Where : p and pi are the coefficients of reflection of every heat insulating internal surface of the above sublayers. n% is the percentage of heat transmission of the heat radiators with thermal reflection. m% is the percentage of heat transmission of the radiators with thermal transition to the internal air which is in contact. The overall decrease coefficient p∑i is equivalent to the increase of the thermal leak resistance 1/Λ of every above sublayer of building materials and structural elements, by: — = in m 2 h°C/Kcal . λ K j K The above sublayers, in order to operate with the smaller coefficient of thermal conveyance K2 of the losses of cooling energy, during the cooling of internal spaces of buildings, it should be p<pι because the overall coefficient of diminution p∑2 of the coefficient K of the heat conveyance, of the losses of cooling energy of every above sublayer, depends on the mode of transmission of the larger quantity of heat, to the heat insulating external surfaces of the above sublayers, during the cooling of the internal spaces of the buildings and is calculated as follows: a) For the heat insulating external surfaces of the sublayers of external masonry and external roofs of buildings, the transmission of the larger quantity of heat to the heat insulating external surfaces of these sublayers, during the operation of the cooling of the internal spaces of buildings is made with thermal radiation (with the direct and diffused solar radiation). As an overall decrease coefficient p∑2, we take the coefficient of reflection thermal radiation p of every heat insulating external surface of these sublayers, that is: p∑2 = ρ and K2 = K - K - p∑2 = K • (1 - p∑2) = K - (1- p). During the operation of cooling of the internal spaces of the buildings, in which the transmission of the larger part of heat, to the heat insulating external surfaces of these sub-layers is made with a thermal transition from the external air, these sublayers operate with a reduced coefficient of heat conveyance K2, of the losses of the cooling energy by: p∑2 = ρι and K2 = K - K - p ∑2 = K - (1- p∑ 2 ) = K • (1 - p i) . b) For the heat insulating external surfaces of the sublayers of internal masonry which are close to non cooled closed spaces, the transmission of the larger quantity of heat, to the heat insulating external surfaces of these sublayers, during the operation of the cooling of the internal spaces of the buildings is made with thermal transition from internal air. As an overall decrease coefficient p∑2, we take the coefficient of reflection of the thermal transition of the air pi of every heat insulating external surface of these sublayers, that is: p∑2 = pι and «2 = K - K - p∑2 = K - (1- p∑2) = K ■ (1- pi) . The overall decrease coefficient P∑2 is equivalent to the increase of the thermal leak resistance 1/Λ of every above sublayer of the building materials and the structural elements, by: — = in m 2 h°C/Kcal. λ K 2 K The low coefficient ε of thermal radiation emission, of the heat insulating internal and external surfaces of the sublayers of the external masonry and the external roofs of the buildings, is not taken into consideration at the decrease of the coefficient of heat conveyance K of these sublayers, because : During the heating of the internal spaces of the buildings, the transmission of the larger quantity of heat, from the heat insulating external surfaces of these sublayers, is made with a thermal transition towards the adjacent external air. During the cooling of the internal spaces of the buildings, the transmission of the larger quantity of heat, from the heat insulating internal surfaces of these sublayers, is made with a thermal transition towards the adjacent internal air. The sublayers of reinforced concrete have a low resistance of thermal leak D/λ. The revetment of the internal and external side of the sublayers of reinforced concrete of the external masonry with a heat insulating plastering, as well as the internal side of the sublayers of reinforced concrete of the external roofs of buildings, provides the possibility to these sublayers to operate with low coefficients of heat conveyance Ki and K2, without increasing their thickness. The addition of coloring substances to the liquid insulating material in order to change its white color, has the following results: 1. The coefficient of thermal conductivity λ of the heat insulating internal and external surface of the sublayers of the building materials and structural elements is increased and the resistance to heat leak D/λ is decreased, when during the coating of the liquid insulating material, the same covering is preserved in volume per square meters, with a result, the decrease of the coefficients of reflection p and pi. In order that the resistance of heat leak D/λ remains constant and the coefficients of reflection p and pi not to decrease, the covering in volume per square meters has to be preserved also with the increased volume of the liquid insulating material per volume of the coloring substances. 2. The coefficient pi of the reflection of thermal transition of the air, of every non white colored, heat insulating internal and external surface of the sublayers of building materials and structural elements remains constant, when the resistance of the heat leak D/λ remains constant. 3. The coefficient p of the reflection of thermal radiation of every, non white colored, heat insulating internal and external surface of the sublayers of building materials and structural elements is decreased, due to the absorption of the monochromatic radiation. For light colorings of white shades, the coefficient of reflection p of the thermal radiation is decreased by 2 to 5% approximately. The addition of water to the liquid insulating material has a result the creation of pores (thermal bridges), in every heat insulating internal and external surface of the sublayers, of the construction materials and the structural elements, given that the volume of pores created after the evaporation is equal to the volume of the added water. Example for the calculation of the reduced coefficients of heat conveyance Ki and K2, of the sublayer of a reinforced concrete parapet, of the external masonry, Fig. 7, with the following data: White colored liquid insulating material, type A in solid form -1 -. Layers of heat insulating plastering -2- and -4-. D2 = D = 2 centimeters and K2 = KΛ = 0,07 Kcal/mh°C. Reinforced concrete parapet -3-. D3 = 20 centimeters and λ3 = 1 ,75 Kcal/mh°C. White colored liquid insulating material , type B in solid form -5-. Coefficient of thermal transition of the internal air. ai = 7 Kcal /m 2 h°C, for a natural circulation of the air. Coefficient of thermal transition of the external air. a2=20 Kcal/m 2 h°C, for an air velocity of two meters per second (u= 2m/sec). The coefficients ai and a2 are given by the Regulations of Heat Insulation of Buildings. The resistance to heat leak 1/Λ of the non-insulated sublayer, is: 1 D 2 D, D 4 0,02 0,2 0,02 1 Λ j I 3 Λ 4 0,07 1,75 0,07 Λ The coefficient of heat transfer K of the non insulated sublayer is calculated with the equation: -^ = — + — + — = - +0,684+ — => — ,%lAm 2 h°CIKcal => K α, Λ a 2 7 20 K ' => K =1:0,874=1,144 Kcal lm 2 h°C or K = 1,33 W/nr K. 1. During the heating of internal spaces of buildings, with heat radiating radiators p∑i = p = 80%. The reduced coefficient of heat conveyance Ki is: Ki = K (1-p∑ι) = K (1-p) = 1 ,144 (1-80%) = => Ki =0,229Kcal/m 2 h°C or Kι=0,266 W/ m 2 K. The overall coefficient of reduction p∑i = p = 80% is equivalent to an increase of the resistance of the heat leak 1/Λ of the sublayer, by: D i l l I D 7 „ AΪT κ = ^ ]^ I= 3 - 492 m2h c κcat With the conventional heat insulation of the sublayer, with a heat insulating material having λ = 0,023 Kcal/mh°C, it is required to have a thickness of the heat insulating material : D = 3,492 ■ 0,023 ■ 100 = 8 centimeters. 2. During the heating of internal spaces of buildings, with the adduction The reduced coefficient of heat conveyance Ki is: Ki = K ■ (1-p∑ι) = K ■ (1-pι) = 1 ,144 ■ (1-86%) => Kι=0,16Kcal/m 2 h°C or Kι= 0,186 W/m 2 K. The overall coefficient of reduction p∑i = pi = 86% is equivalent to an increase of the resistance of the heat leak 1/Λ of the sublayer, by: _ = _L_± = J L_ ^ A. = 5; 37 6 mVC/Kcal. λ K , K 0,16 L144 λ With the conventional heat insulation of the sublayer, with a heat insulating material having λ = 0,023 Kcal/mh°C, it is required to have a thickness of the heat insulating material : D = 5,376 • 0,023 ■ 100 = 12,36 centimeters. 3. During the heating of internal spaces of buildings, with contact- conveyance radiators, for which n=40% and m=60% : p∑ι=p n%+pιm% = 80% ■ 40% + 86% ■ 60%= p∑ι =83,6%. Kι=K-(1-p∑ι)=1 ,144-(1-83,6%) = Kι=0,187Kcal/m 2 h°C or Kι=0,217W/m 2 K. The overall coefficient of reduction p∑ι=83,6% is equivalent to an increase of the resistance of the heat leak 1/Λ of the sublayer, by: __J_ \_ 1 D =4,473 mVC/Kcal. λ ~~ K ~ K ~ 0,187 ~ 1,144 => λ With the conventional heat insulation of the sublayer, with a heat insulating material having λ = 0,023 Kcal/mh°C , it is required to have a thickness of the heat insulating material : D = 4,473 ■ 0,023 • 100 = 10,28 centimeters. 4. During the cooling of internal spaces of buildings p∑2 = p = 82%. The reduced coefficient K_ of heat conveyance is : K2 = K-(1-p∑2) = K-(1-p) = 1 ,144-(1-82%) => K2=0,206Kcal/m 2 h°C or K2=0,24 W/m 2 K. The overall coefficient of reduction p∑2 = p = 82% is equivalent to an increase of the resistance of the heat leak 1/Λ of the sublayer, by: A D = J 1 1 L = _J 1 1 L_ => A D = 3 ι98 m 2 h °C/Kcal . λ K 2 K 0,206 1,144 λ With the conventional heat insulation of the sublayer, with a heat insulating material having λ = 0,023 Kcal/mh°C, it is required to have a thickness of the heat insulating material : D = 3,98 ■ 0,023 ■ 100 = 9, 15 centimeters. During the cooling of internal spaces of buildings, where the transmission of the larger quantity of heat, to the heat insulating external surface of the sublayer is made with thermal transition from the external air. The sublayer operates with a reduced coefficient of heat conveyance K2 by ρ∑2 = pi = 88%, that is : K2 = K ■ (1-p∑ 2 ) = K ■ (1-pι) = 1 ,144 ■ (1-88%) = K2 = 0,137Kcal/m 2 h°C or K2 = 0,159 W/m 2 K, and further reduction by 33,4% of the losses of the cooling energy is obtained through the sublayer. The sublayers of the external masonry and the external roofs of the buildings, which are not possible to be heat-insulated, due to the decoration of their internal or external surfaces, are thermally insulated with the second mode of implementation of the new method of heat insulation of buildings. A practical application of the second mode of application of the new method of heat insulation of buildings is shown in Drawings Fig.12, Fig.13, Fig 14 and Fig 15 The second mode of application of the new method of heat insulation of buildings offers the following possibilities 1. Heat insulation of internal spaces of buildings, against the cold and heat of the external environment, which is realized as follows With the construction of a parallel plane division with an enclosed layer of air, at the internal side of the sublayers of the external masonry and the external roofs of the buildings, by which is achieved the thermal flow, with thermal radiation and with thermal transition of the air through these sublayers and the reduction of the losses of heating energy, at the initiation of the heating operation of the internal spaces of the buildings At the same time is also achieved the sound insulation of the internal spaces of the buildings, against the airborne noise through these sublayers, towards any adjacent internal or external space and from the external environment 2. The possibility of a reliable construction of sublayers of the external masonry and the external roofs of buildings, with a parallel plane division with an enclosed layer of air at their internal side, due to the small thickness of the enclosed layer of air, up to D=10 millimeters The parallel internal surfaces and every surface which lies inside the enclosed layer of air, are covered with the white colored liquid insulating material type C, with a minimum thickness of coating D=0,3 millimeters approximately for the vertical surfaces and D=0,4 millimeters approximately for the horizontal and sloped surfaces In order to avoid the creation of thermal bridges Every junction line of the sublayers of reinforced concrete with building plaster, is internally and externally covered with an elastic polyesteric gauze for the strengthening of the elastic over-coatings, which is glued with an elastic acrylic synthetic emulsion along its entire length The peπmetπc surface of the supports sustaining the plaster-boards and the MDF is coated before its fixing with the type C white colored insulating liquid material, with a minimum coat thickness of approximately D=0,4 millimeters. The plaster-boards and MDF are joined together with a groove for a better fitting, and the surface of every groove is coated with the type B or type C white colored insulating liquid material. Every junction line of the plaster-boards and MDF is covered externally with an elastic polyesteric gauze for the strengthening of the elastic revetments, which is glued with an elastic acrylic synthetic emulsion along its entire length. The perimetric surface of the thickness of the MDF is coated the type C white colored insulating liquid material, with a minimum coat thickness of approximately D=0,4 millimeters, because the larger part of the heating is transmitted to their mass, along their fibers. 3. Increased energy saving, by reducing the thermal flow through these sublayers, which is transmitted with thermal radiation and with thermal transition of the enclosed air inside these sublayers, due to the low degree of exchange of thermal radiation, between the parallel heat insulating internal surfaces and due to the reflection of the thermal transition of the enclosed air, from every parallel heat insulating internal surface. The reduction of the thermal flow through these sublayers due to the small degree of disturbance of the energy equilibrium, in the mass of the parallel heat insulating internal surfaces during the exchange of thermal radiation between them and during the fall of the thermal transition of the enclosed air in them, has the following results : 1. The temperature Twi of the internal surfaces of these sublayers is increased, and the difference of temperature DTι=Tι-Twι between the temperature Ti of the internal air and the temperature Twi during the heating of the internal spaces of the buildings is decreased. Due to the reduction of the difference of temperature DTι=Tι-Twι, the coefficient of thermal convey K of the losses of heating energy of every above sublayer of the building materials and structural elements is decreased, because the difference of temperature DTι=Tι-Twι is the driving force for the losses of the heating energy through every one of the above sublayers. The percentage of reduction of the difference in temperature DTι=Tι-T ι, is equal to the percentage of reduction of the thermal flow through every sublayer of the building materials and the structural elements, is equal to the percentage of reduction of the coefficient of heat convey K, and remains constant during the increase and decrease of the losses of heating energy, through every above sublayer. 2. The temperature Tw2 of the external surfaces of these sublayers is increased and the difference of temperature DT2=T2-Tw2 between the temperature T2 of the external air and the temperature Tw2 during the cooling of the internal spaces of the buildings is decreased. Due to the reduction of the difference of temperature DT2=T2-Tw2 the coefficient K of the losses of cooling energy, of thermal convey of every above sublayer of the building materials and structural elements is decreased, because the difference of temperature DT2=T2-Tw2 is the driving force for the heat flow through these sub-layers, which corresponds to the losses of the cooling energy through these sublayers. The percentage of reduction of the difference in temperature DT2=T2-Tw2 is equal to the percentage of reduction of the thermal flow through every sublayer of the building materials and the structural elements, is equal to the percentage of reduction of the coefficient of heat convey K and remains constant during the increase and decrease of the thermal flow (losses of cooling energy), through every above sublayer. The coefficient of emission of the thermal radiation ε, the coefficient of reflection of the thermal radiation p, and the coefficient of reflection of the thermal transition of the air pi of every parallel heat insulating internal surface, reduce the coefficient of thermal convey K of every above sublayer, of the building materials and structural elements, because they remain constant during the increase and decrease of the losses of heating and cooling energy, through every above sublayer. The overall coefficient p∑i of reduction of the coefficient of thermal convey K of the losses of heating energy and the overall coefficient p∑2 of reduction of the coefficient of thermal convey K of cooling energy of every above sublayer, of the building materials and structural elements are calculated as follows: p∑i = ni2% ■ Cμi2% + m 12% ■ pi (2). p∑2 = n2i% ■ Cμ2i% + m 21% ■ pi (1). Where: ni2% and n2i% is the percentage of the thermal flow by thermal radiation, through every above sublayer. Cμi2% and Cμ2i% is the percentage of the decrease of the degree of exchange of thermal radiation C12 and C21, between the internal parallel heat insulating surfaces. C 12 = in W/m 2 K 4 . 8 ] ε ε 8 ] Gs = 5,67 W/m 2 K 4 is the constant of the dark color. m 12% and m 21% is the percentage of the thermal flow by thermal transition of the enclosed air, through every above sublayer. pi(2) and pi(i) are the coefficients of reflection of the thermal transition of the air, of every parallel heat insulating internal surface. The reduced thermal convey coefficient Ki of the losses of heating energy and the reduced thermal convey coefficient K2 of the losses of cooling energy, of every above sublayer of the building materials and structural elements, is : Ki = K - K • p∑i = K ■ (1 - p∑i) and K2 = K - K • p∑2 = K ■ (1 - p∑ 2 ). At the sublayers of the external masonry and the horizontal external roofs of buildings, the coefficient of thermal transition of the enclosed air aa is the same for the losses heating energy and cooling energy, through these sublayers, resulting in p∑i = p∑2 and Ki = K2. At the sublayers of the sloped external roofs of buildings, the coefficient of thermal transition of the enclosed air aa is larger for the losses heating energy through these sublayers, resulting in p∑i < p∑2 and Ki > K2. The overall reduction coefficients p∑i and p∑2 are equivalent to an increase of the resistance of thermal leak 1/Λ of every above sublayer of the building materials and structural elements, by " = A - ~ for the losses of A K ) K. D 1 1 the heating energy, and by A = — - 7 for the losses of the cooling A K. 2 K energy, through every above sublayer. Example for the calculation of the reduced coefficients of thermal convey Ki and K2, of a sublayer of perforated bricks, of the external masonry, Fig. 13, with the following data: Layers of common plaster with sand -1t- and -9f-. Dif = D9f =2 centimeters and λif = λε* = 0,75 Kcal/mh°C. Layer of plaster-board -2f - . Da = 10 millimeters and has =0,5 Kcal/mh°C. Liquid, white color insulating material, type C in solid form -3f- and -6 εi = ε2 = 0,16, p(i) = p(2) = 84% and pi(i) = pi(2) = 90%. Enclosed layer of air -4 D f =10 millimeters and λ f = 0,022 Kcal/mh°C. Horizontal layers of common, building plaster -7f- . D7f = 20centimeters, λ7f = 0,75Kcal/mh°C and covering proportion Eι=0,1 square meter per square meter of external masonry. Horizontal layers of perforated bricks -8f- . Dβf = 20centimeters, λβf =0,45Kcal/mh°C and covering proportion E2=0,9 square meter per square meter of external masonry. Coefficient of thermal transition of the internal air, ai =7 Kcal/m 2 h°C for a natural circulation of the air. Thermal transition coefficient of the external air, a2=20Kcal/m 2 h°C for an air velocity of two meters per second (u=2m/sec). Transmission coefficient of thermal radiation ε, of every parallel, non heat insulating internal surface ει= ε2=0,93. Thermal convey coefficient K of the non-insulated sublayer, without the enclosed layer of the air, K = 1 ,507Kcal/m 2 h°C. The degree of thermal radiation exchange, between the parallel, non-heat insulating internal surfaces of the non-insulated sublayer, is the same for the losses of heating energy and the cooling energy, through the sublayer, because : C i2 = C 21 = 4,93 W/m 2 K 4 or C12 = C2i = 4,239 Kcal/m 2 h°C. The thermal transition coefficient of the enclosed air, ad is calculated as follows : For a thickness of the enclosed layer of air D4f = 10 millimeters the Nusselt number is: Nu = i = 2l 2Kcal/m 2 h°C and is the same for the thermal flow of heating energy and the thermal flow which corresponds to losses of cooling energy through the sublayer, The thermal flow Q through the non insulated sublayer with a enclosed layer of air, is : Q = Ci2+αo = 4,239+2,2 = 6,439 Kcal/m 2 h°C => ni2 = n 2 ι = 65,8% and m 12 = m 21 = 34,2%. The thermal flow Q= λ' = 0,0644Kcal/mh°C . The equivalent thermal leak resistance of the enclosed layer of air, is : ^ = -°^ = 0,155 mVC/Kcal. λ' 0,0644 The thermal leak resistance of the layer of the plaster board is: 5* = l = o,02 m 2 h°C/Kcal. λ 2f 0,5 The overall thermal resistance 1/K of the non insulated sublayer with an enclosed layer of air is increased by, ^L + = 0,02 + 0,155 = 0,175 mVc/Kcal and becomes: λ 2f λ' — = - + 0,175 = -J— + 0,175 = 0,838 m 2 h°C/Kcal. K d K 1,507 The heat convey coefficient Kd of the non insulated sublayer with an enclosed layer of air is : K H = = 1,193 Kcal/m 2 h°C d 0,838 The degree of thermal radiation exchange, between the parallel heat insulating internal surfaces of the sublayer, is the same for the losses of the heating energy and the cooling energy through the sublayer, because Gs 5,67 , . C 12 = C 21 = - = — — => C 12 = C 2] =0,493 W/m 2 K 4 + — -1 £ 2 0,16 0. or Ci2 = C2i = 0,424 Kcal/m 2 h°C. (4,93-0,493)-! 00 C μ12 % = C μ21 % = ' ' => C μl2 = C μ21 =90% 4,93 p∑ι=p∑2= ni2 % ■ Cμi2 + m 12 % ■ Pi (2) = 65,8% ■ 90% + 34,2% • 90% = The reduced coefficients of heat convey Ki and K2 are: Ki = K2 = Kd - Kd - p∑ι= Kd - (1 - p∑i) = 1 ,193 ■ (1 - 90%) => => Ki = K2 = 0,12 Kcal/m 2 h°C or Ki = K2 = 0,14 W/m 2 K. The overall reduction coefficients p∑i and p∑2 are equal (p∑i = p∑2) and are equivalent to an increase of the resistance of the thermal leak 1/Λ of the non insulated sublayer with an enclosed layer of air, by: » = ±-± = -± = -L- L- => 2 = 7,495 mVC/Kcal. λ K, K d K 2 K d 0,12 1,193 λ In the conventional heat insulation of the sublayer, with a heat insulating material having an λ = 0,023 Kcal/mh°C it is required to have a thickness of heat insulating material: D=7, 495-0,023-100=17,23 centimeters. The heat conveyance coefficient K, of the non insulated sublayer, without the enclosed layer of air, from the value of K = 1 ,507 Kcal/m h°C has been reduced to Ki = K2 = 0,12 Kcal/m 2 h°C, which means that it has been reduced by p∑ = 92,1 %. The overall coefficient of reduction p∑ = 92,1 % is equivalent to an increase of the thermal leak resistance 1/Λ of the non insulated sublayer, without the enclosed layer of air, by : D 1 1 1 1 1 I D , n ln conventional heat insulation of the sublayer, with a heat insulating material having λ=0,023Kcal/mh°C, it is required to have a thickness of heat insulating material : D = 7,67 ■ 0,023 • 100 = 17,64 centimeters.

Claims: C LAI MS 1. An energy saving heat insulation of buildings with a diffused reflection of the thermal radiation and with a diffused reflection of the thermal transition of the air, makes up a new method for the heat insulation of buildings which is characterized by the fact that its practical implementation is made with two modes, that is : With a diffused reflection of the thermal radiation and with a diffused reflection of the thermal transition of the air, from the internal and from the external surfaces of the sublayers of the external masonry, the external roofs, the internal masonry and the internal ceilings of the buildings. With a low emission of the thermal radiation, with a diffused reflection of the thermal radiation and with a diffused reflection of the thermal transition of the air, from the internal surfaces of a parallel plane division with an enclosed layer of air, which is constructed at the internal side of the sublayers of the external masonry and the external roofs of the buildings. The know how for its construction, transforms the non heat insulating and non reflective, internal and external surfaces of the sublayers of the internal and external masonry, the internal and external roofs of the buildings as well as the internal surfaces of the sublayers of the parallel plane division with an enclosed layer of air, into heat insulating and reflecting to the thermal radiation and the thermal transition of the air, as follows: These surfaces are covered with a white colored liquid insulating material, which is produced in three types A, B and C and forms the final surface of the above mentioned sublayers. The white colored liquid insulating material of the three types A, B and C can be colored with the addition of coloring pigments, and following its practical application, in a solid form (after it dries), it is not solvable in water. The composition of the white colored liquid insulating material which guarantees the effective operation of the new method of heat insulation of buildings, after its coating in a solid form, (after it dries) at a minimum thickness of the revetment, of 0,3 to 04 millimeters, is the following : Expanded perlite, with a microscopic granulometry 0 to 130 μm, convex and of the same geometric shape for every convex microscopic granule, or Expanded ceramic material, with a microscopic granulometry 0 to 130 μm, convex and of the same geometπc shape for every convex microscopic granule. Binding material, 100% pure acrylic. Elastomeric co-polymerized acrylic. Synthetic(plastic) materials. White coloring pigments of titanium oxides. Mineral chloric sodium. Aluminium water glass. Silica oxide. Liquid silicone. Fungicide material. Antifreezing material. Water. 2- An energy saving heat insulation of buildings, like in claim 1, which is characterized by the fact that the know how of the second mode of implementation of the new method of heat insulation of the buildings is based on the saving of energy with the creation of artificial conditions of low emission of thermal radiation, high reflection of thermal radiation and thermal transition of the air, inside the sublayers of the external masonry and the external roofs of the buildings, as follows : With the construction of a parallel level division with an enclosed layer of air, at the internal side of the sublayers of the external masonry and the external roofs of the buildings, by which the thermal flow by thermal radiation and by thermal transition of the air through these sublayers, and the decrease of the losses of heating energy at the initiation of the heating of the internal spaces of the buildings, is obtained. AMENDED CLAIMS [received by the International Bureau on 05 October 1999 (05.10.99); original claims 1 amended; remaining claim unchanged (2 pages)] 1. An energy saving heat insulation of buildings with a diffused reflection of the thermal radiation and with a diffused reflection of the thermal transition of the air, makes up a new method for the heat insulation of buildings which is characterized by the fact that its practical implementation is made with two modes, that is : With a diffused reflection of the thermal radiation and with a diffused reflection of the thermal transition of the air, from the internal and from the external surfaces of the sublayers of the external masonry, the external roofs, the internal masonry and the internal ceilings of the buildings. With a low emission of the thermal radiation, with a diffused reflection of the thermal radiation and with a diffused reflection of the thermal transition of the air, from the internal surfaces of a parallel plane division with an enclosed layer of air, which is constructed at the internal side of the sublayers of the external masonry and the external roofs of the buildings. The know how for its construction, transforms the non heat insulating and non reflective, internal and external surfaces of the sublayers of the internal and external masonry, the internal and external roofs of the buildings as well as the internal surfaces of the sublayers of the parallel plane division with an enclosed layer of air, into heat insulating and reflective to the thermal radiation and the thermal transition of the air, as follows: These surfaces are covered with a white colored liquid reflective insulating material, which is produced in three types A, B and C and forms the final surface of the above mentioned sublayers. The white colored liquid reflective insulating material of the three types A, B and C can be colored with the addition of coloring pigments, and following its practical application, in a solid form (after it dries), it is not solvable in water. The composition of the white colored liquid reflective insulating material which guarantees the effective operation of the new method of heat insulation of buildings, after its coating in a solid form, (after it dries) at a minimum thickness of the revetment, of 0,3 to 0,4 millimeters, is the following : Expanded perlite, with a microscopic granulometry 0 to 130 μm, convex and of the same geometric shape for every convex microscopic granule, or Expanded ceramic material, with a microscopic granulometry 0 to 130 μm, convex and of the same geometric shape for every convex microscopic granule. Binding material, 100% pure acrylic. Elastomeric co-polymerized acrylic. Synthetic(plastic) materials. White coloring pigments of titanium oxides. Mineral chloric sodium. Aluminium oxide. Silica oxide. Liquid silicone. Fungicide material. Antifreezing material. Water. 2- An energy saving heat insulation of buildings, like in claim 1, which is characterized by the fact that the know how of the second mode of implementation of the new method of heat insulation of the buildings is based on the saving of energy with the creation of artificial conditions of low emission of thermal radiation, high reflection of thermal radiation and thermal transition of the air, inside the sublayers of the external masonry and the external roofs of the buildings, as follows : With the construction of a parallel level division with an enclosed layer of air, at the internal side of the sublayers of the external masonry and the external roofs of the buildings, by which the thermal flow by thermal radiation and by thermal transition of the air through these sublayers, and the decrease of the losses of heating energy at the initiation of the heating of the internal spaces of the buildings, is obtained.

Inventors: KOTROTSIOS DIMITRIOS, KOTROTSIOS, DIMITRIOS
Applicants: KOTROTSIOS DIMITRIOS, KOTROTSIOS, DIMITRIOS
Application year: 1999
Main classification: E04B1
IPC codes: C04B26, E04B1, E04D13