WO2012063838A1 - 太陽熱蓄熱方法およびシステム - Google Patents
太陽熱蓄熱方法およびシステム Download PDFInfo
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- WO2012063838A1 WO2012063838A1 PCT/JP2011/075761 JP2011075761W WO2012063838A1 WO 2012063838 A1 WO2012063838 A1 WO 2012063838A1 JP 2011075761 W JP2011075761 W JP 2011075761W WO 2012063838 A1 WO2012063838 A1 WO 2012063838A1
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- C—CHEMISTRY; METALLURGY
- C04—CEMENTS; CONCRETE; ARTIFICIAL STONE; CERAMICS; REFRACTORIES
- C04B—LIME, MAGNESIA; SLAG; CEMENTS; COMPOSITIONS THEREOF, e.g. MORTARS, CONCRETE OR LIKE BUILDING MATERIALS; ARTIFICIAL STONE; CERAMICS; REFRACTORIES; TREATMENT OF NATURAL STONE
- C04B35/00—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products
- C04B35/01—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics
- C04B35/26—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics based on ferrites
- C04B35/2666—Other ferrites containing nickel, copper or cobalt
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24S—SOLAR HEAT COLLECTORS; SOLAR HEAT SYSTEMS
- F24S20/00—Solar heat collectors specially adapted for particular uses or environments
- F24S20/20—Solar heat collectors for receiving concentrated solar energy, e.g. receivers for solar power plants
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24S—SOLAR HEAT COLLECTORS; SOLAR HEAT SYSTEMS
- F24S60/00—Arrangements for storing heat collected by solar heat collectors
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24S—SOLAR HEAT COLLECTORS; SOLAR HEAT SYSTEMS
- F24S60/00—Arrangements for storing heat collected by solar heat collectors
- F24S60/20—Arrangements for storing heat collected by solar heat collectors using chemical reactions, e.g. thermochemical reactions or isomerisation reactions
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24S—SOLAR HEAT COLLECTORS; SOLAR HEAT SYSTEMS
- F24S70/00—Details of absorbing elements
- F24S70/10—Details of absorbing elements characterised by the absorbing material
- F24S70/16—Details of absorbing elements characterised by the absorbing material made of ceramic; made of concrete; made of natural stone
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28D—HEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
- F28D20/00—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00
- F28D20/003—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00 using thermochemical reactions
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- C—CHEMISTRY; METALLURGY
- C04—CEMENTS; CONCRETE; ARTIFICIAL STONE; CERAMICS; REFRACTORIES
- C04B—LIME, MAGNESIA; SLAG; CEMENTS; COMPOSITIONS THEREOF, e.g. MORTARS, CONCRETE OR LIKE BUILDING MATERIALS; ARTIFICIAL STONE; CERAMICS; REFRACTORIES; TREATMENT OF NATURAL STONE
- C04B2235/00—Aspects relating to ceramic starting mixtures or sintered ceramic products
- C04B2235/02—Composition of constituents of the starting material or of secondary phases of the final product
- C04B2235/30—Constituents and secondary phases not being of a fibrous nature
- C04B2235/32—Metal oxides, mixed metal oxides, or oxide-forming salts thereof, e.g. carbonates, nitrates, (oxy)hydroxides, chlorides
- C04B2235/327—Iron group oxides, their mixed metal oxides, or oxide-forming salts thereof
- C04B2235/3279—Nickel oxides, nickalates, or oxide-forming salts thereof
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- C—CHEMISTRY; METALLURGY
- C04—CEMENTS; CONCRETE; ARTIFICIAL STONE; CERAMICS; REFRACTORIES
- C04B—LIME, MAGNESIA; SLAG; CEMENTS; COMPOSITIONS THEREOF, e.g. MORTARS, CONCRETE OR LIKE BUILDING MATERIALS; ARTIFICIAL STONE; CERAMICS; REFRACTORIES; TREATMENT OF NATURAL STONE
- C04B2235/00—Aspects relating to ceramic starting mixtures or sintered ceramic products
- C04B2235/70—Aspects relating to sintered or melt-casted ceramic products
- C04B2235/96—Properties of ceramic products, e.g. mechanical properties such as strength, toughness, wear resistance
- C04B2235/9607—Thermal properties, e.g. thermal expansion coefficient
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- C—CHEMISTRY; METALLURGY
- C04—CEMENTS; CONCRETE; ARTIFICIAL STONE; CERAMICS; REFRACTORIES
- C04B—LIME, MAGNESIA; SLAG; CEMENTS; COMPOSITIONS THEREOF, e.g. MORTARS, CONCRETE OR LIKE BUILDING MATERIALS; ARTIFICIAL STONE; CERAMICS; REFRACTORIES; TREATMENT OF NATURAL STONE
- C04B2235/00—Aspects relating to ceramic starting mixtures or sintered ceramic products
- C04B2235/70—Aspects relating to sintered or melt-casted ceramic products
- C04B2235/96—Properties of ceramic products, e.g. mechanical properties such as strength, toughness, wear resistance
- C04B2235/9646—Optical properties
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24S—SOLAR HEAT COLLECTORS; SOLAR HEAT SYSTEMS
- F24S20/00—Solar heat collectors specially adapted for particular uses or environments
- F24S20/20—Solar heat collectors for receiving concentrated solar energy, e.g. receivers for solar power plants
- F24S2020/23—Solar heat collectors for receiving concentrated solar energy, e.g. receivers for solar power plants movable or adjustable
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F24—HEATING; RANGES; VENTILATING
- F24S—SOLAR HEAT COLLECTORS; SOLAR HEAT SYSTEMS
- F24S60/00—Arrangements for storing heat collected by solar heat collectors
- F24S60/10—Arrangements for storing heat collected by solar heat collectors using latent heat
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28D—HEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
- F28D20/00—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00
- F28D20/0056—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00 using solid heat storage material
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F28—HEAT EXCHANGE IN GENERAL
- F28D—HEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
- F28D20/00—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00
- F28D20/0034—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00 using liquid heat storage material
- F28D2020/0047—Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00 using liquid heat storage material using molten salts or liquid metals
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/40—Solar thermal energy, e.g. solar towers
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
- Y02E60/14—Thermal energy storage
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E70/00—Other energy conversion or management systems reducing GHG emissions
- Y02E70/30—Systems combining energy storage with energy generation of non-fossil origin
Definitions
- the present invention relates to a solar heat storage method and system for storing heat using solar energy.
- Solar thermal energy storage is cost effective and reliable because it can directly store the thermal energy collected in a concentrated solar power (CSP) system without having to convert it to another energy This is the recommended method to meet the demand for solar thermal energy.
- CSP concentrated solar power
- the heat energy is stored in a container isolated from the outside world and can be recovered by a heat engine or the like that generates electricity (that is, it can be converted into electric energy).
- Patent Document 1 discloses a solar collector that collects solar thermal energy with high efficiency and high quality and stores the heat in a heat medium, and a solar light collecting reflector using the solar collector.
- a solar condensing system and a solar energy utilization system have been proposed.
- Patent Document 1 discloses a beam-down solar condensing system as a system for concentrating sunlight.
- a beam-down solar condensing system is also disclosed in Non-Patent Document 2.
- the beam-down-type sunlight condensing system includes a plurality of reflecting mirrors (heliostats) 61 arranged on the ground, and reflection of sunlight SB from the plurality of heliostats 61.
- the beam-down solar condensing system disclosed in Patent Document 1 and Non-Patent Document 1 collects sunlight in the daytime to approximately 1000 to 1300 Kelvin (K) (approximately 700 to 1000 ° C.).
- Heat can be supplied to external equipment and laying (hereinafter referred to as external equipment), but it is stored in the heat medium (molten salt) that circulates in the piping.
- external equipment external equipment and laying
- molten salt molten salt
- the present invention has been made in view of such circumstances, and an object of the present invention is to provide a solar heat storage method and system capable of supplying heat of about 1000 to 1300 K to external equipment for 24 hours with a simple configuration. .
- the present invention that has solved the above problems is a solar heat storage method for storing heat using solar energy, which releases oxygen when heated and changes from an oxidized form to a reduced form, and returns to an oxidized form when contacted with oxygen.
- Condensed beam irradiation step of moving the reactive ceramic layer formed using ceramics while irradiating the reactive ceramic layer with a condensed beam obtained by collecting sunlight and heating the reactive ceramic layer, and the condensed beam irradiation step
- a heat storage step of storing heat generated from the reactive ceramic layer in a heat storage means while contacting the reactive ceramic layer heated in step with a gas containing oxygen.
- the above-mentioned present invention preferably includes a heat extraction step for circulating the heat medium after the heat storage step and taking out the heat stored in the heat storage means to the outside of the heat storage means.
- the present invention also relates to a solar heat storage system for storing heat using solar energy, wherein a reactive ceramic layer is formed using a reactive ceramic that releases oxygen when heated and changes from an oxidized type to a reduced type.
- a rotating body formed on the surface, a driving means for rotating the rotating body in the circumferential direction, and an irradiation of the condensed beam, which is provided so as to cover the outer peripheral surface of the rotating body and collects sunlight, to the rotating body
- a heat insulating member having an opening that enables the heat storage means provided in the vicinity of the rotating body at a position spaced from the opening, and after the rotating rotating body passes through the opening, Gas supply means provided at an arbitrary position up to the heat storage means for supplying a gas containing oxygen toward the rotating body.
- the reactive ceramic layer is preferably formed of nickel ferrite.
- the heat storage unit includes a heat extraction unit that circulates a heat medium and extracts heat stored in the heat storage unit to the outside of the heat storage unit.
- the rotating body is a cylindrical body using alumina fibers.
- the heat storage means uses a heat storage material formed of at least one of a carbon material and a salt.
- the present invention it is possible to provide a solar heat storage method capable of supplying heat of about 1000 to 1300 K to external equipment for 24 hours. Further, according to the present invention, it is possible to provide a solar heat storage system capable of supplying heat of about 1000 to 1300 K to external equipment for 24 hours.
- a horizontal axis shows operation time (daytime) (time).
- the vertical first axis indicates the accumulated heat storage amount (MJ) (curve B) and the heat storage temperature (0.1 K) (curve D).
- the vertical second axis represents the amount of heat released per unit time (kJ / h) (curve C).
- the solar heat storage method according to an embodiment of the present invention includes a focused beam irradiation step S ⁇ b> 1 and a heat storage step S ⁇ b> 2.
- Condensed beam irradiation step S1 oxygen is released when heated to change from an oxidized type to a reduced type, and when contacted with oxygen, the reactive ceramic layer formed using reactive ceramics that returns to the oxidized type is moved, This is a step of heating the reactive ceramic layer by irradiating a condensed beam obtained by collecting sunlight.
- a means for obtaining a condensed beam there are a plurality of heliostats and a beam-down solar condensing system in which reflected light from the heliostat is reflected downward by a collecting mirror provided at a high place.
- a collecting mirror provided at a high place.
- the means for obtaining the condensed beam is not limited to these.
- a condensing lens can also be mentioned.
- the focused beam obtained by the above-described means has a high flux (high flux) of about 1300 to 2000 kW / m 2 . If such a high flux focused beam is used, the reactive ceramic layer 21 can be heated to about 1800 K as described later, and the heat can be stored in the heat storage means as described later.
- reactive ceramics include iron oxide ceramics.
- ferrite can be mentioned, and more specifically, spinel ferrite (AFe 2 O 4 (where A is at least one selected from Mn, Co, Ni, Cu, Zn). )).
- AFe 2 O 4 (where A is at least one selected from Mn, Co, Ni, Cu, Zn).
- NiFe 2 O 4 Ni ferrite, nickel ferrite
- Mn 2 O 3 manganese oxide
- Co 3 O 4 cobalt oxide
- the movement of the reactive ceramic layer can be performed by any means.
- a reactive ceramic layer using reactive ceramics is formed on the outer peripheral surface of a cylindrical rotating body and the rotating body is rotated by driving means such as a motor, the reactive ceramic layer is formed as described above. Can be moved.
- the heat storage step S2 to be performed next is a step of storing heat generated from the reactive ceramic layer in the heat storage means while bringing the reactive ceramic layer heated in the focused beam irradiation step S1 into contact with the gas containing oxygen. is there. In this heat storage step S2, the reactive ceramic layer continues to move.
- any gas containing oxygen can be used.
- air can be used.
- oxygen gas having a high oxygen concentration supplied from an oxygen cylinder or the like can be used alone or mixed with air at an arbitrary ratio.
- the heat storage means is preferably formed using, for example, a heat storage material formed from at least one of a carbon material and a salt.
- a heat storage material formed from at least one of a carbon material and a salt.
- the carbon material include graphite (graphite) and carbon composite.
- the salt include NaCl and rock salt.
- the heat storage means is provided at a slight distance from the reactive ceramic layer.
- heat transfer from the reactive ceramic layer to the heat storage means is performed by heat radiation from the reactive ceramic layer and convection of air generated between the reactive ceramic layer and the heat storage means.
- the process After transferring heat to the heat storage means in the heat storage step S2, the process returns to the condensed beam irradiation step S1 again and the same operation is repeated.
- solar heat can be continuously and efficiently stored in the heat storage means.
- the capacity of the heat storage means is appropriate, heat can be stored with an amount of heat sufficient to supply heat to external equipment at night (about 12 hours) when sunlight cannot be obtained.
- the solar heat storage method according to the embodiment described above further includes a heat extraction step.
- the heat extraction step (not shown in FIG. 1) is a step of extracting the heat stored in the heat storage means by circulating the heat medium to the outside of the heat storage means, that is, to external equipment. This step can be realized by heat exchange between the heat storage means and the external equipment, and heat of about 1000 to 1300 K can be supplied to the external equipment.
- the specific heat is absorbed to the specific heat absorption limit (1800K) by the focused beam of 1000 to 2000 kW / m 2 .
- the energy of the focused beam is absorbed by the non-equilibrium Frenkel defect generation phenomenon.
- Such a phenomenon is a chemical reaction that proceeds as an endothermic reaction accompanied by a high enthalpy change, that is, a coordinate change in a solid lattice structure, that is, a chemical reaction in units of a non-equilibrium state of a Frenkel defect structure. Therefore, in this step, the energy of the focused beam can be absorbed by the high enthalpy change of the reaction material.
- this step is anion (or cation) movement in the lattice structure, it is presumed that the chemical reaction in this step proceeds according to absorption of energy of the focused beam.
- the non-equilibrium state of the Frenkel defect structure during this chemical reaction is formed after absorption of high flux energy.
- the reactive ceramic that has been reduced in the previous step is oxidized with heat generation by the O 2 gas supplied in the heat storage step S2 (exothermic reaction).
- This oxidation reaction occurs at about 1400 to 1600K, which is about 200 to 400K lower than the focused beam irradiation step S1.
- enthalpy changes by exothermic reaction exothermic reaction enthalpy change (refer FIG. 2).
- heat storage step S2 heat corresponding to a temperature drop from 1800K to 1300K, that is, heat for 500K, is transferred to the heat storage means by radiation and convection from the reactive ceramic layer among the specific heat absorption of the reactive ceramic.
- the heat of the exothermic reaction enthalpy change contained in the reactive ceramic layer is transferred to the heat storage means by radiation or convection (see FIG. 2).
- about 1000 to 1300 K of heat is stored in the heat storage means.
- the process After passing through the heat storage step S2, the process returns to the focused beam irradiation step S1, so that the same chemical reaction (reduction reaction with endotherm and oxidation reaction with heat generation) is continued in the reactive ceramic layer heated by the focused beam. Done.
- the reactive ceramic layer irradiated with the focused beam in the focused beam irradiation step S1 is heated to about 1300 to 1800K.
- enthalpy change in the Frenkel defect structure of magnetite Fe 3 O 4
- enthalpy change in the Frenkel defect structure of magnetite is considered to be almost the same as that of Ni ferrite because there is cation movement in the interstitial position. 754 kJ / mol.
- the thermal equilibrium is reached, and 1400 kW / m 2 of the heat flux is transferred in the heat storage step S2.
- the length of the thermal gradient region is estimated to be 0.8 m.
- the reaction in the focused beam irradiation step S1 proceeds rapidly, but the reaction in the heat storage step S2 proceeds slowly. Therefore, the area ratio of the reactive ceramic layers for carrying out these steps is such that if the area for carrying out the heat storage step S2 is larger than that of the focused beam irradiation step S1, the heating in the focused beam irradiation step S1 and the heat transfer in the heat storage step S2 The heat balance is improved.
- the area ratio of the area where the focused beam irradiation step S1 is performed and the area where the heat storage step S2 is performed is 1: 5
- graphite heat capacity 20 J / K / mol
- the focal region where the condensed beam irradiation step S1 is performed is 71 m 2 in the case of an average flux intensity of 1400 kW / m 2 .
- the size of the heat storage means capable of storing 12 hours is 10.6 m in diameter and 16 m in height.
- a solar heat storage system 1 includes a rotating body 2, a driving unit (not shown) that rotates the rotating body 2 in the circumferential direction, a heat insulating member 3, and a heat storage unit 4. Gas supply means 5.
- the rotating body 2 preferably has a cylindrical shape as already described in the condensed beam irradiation step S1.
- a reactive ceramic layer 21 using the above-described reactive ceramics is formed on the outer peripheral surface of the rotating body 2.
- the thickness of the reactive ceramic layer 21 is not particularly limited, but may be 2 mm, for example.
- the rotating body 2 is more preferably formed using alumina fibers.
- Alumina fiber has less heat shrinkage, is excellent in strength, and has heat insulation properties. Therefore, even if the reactive ceramic layer 21 is heated by irradiation with a high-flux condensed beam CB, it is difficult to release the heat (that is, It is difficult to lose) and is suitable.
- the reactive ceramic layer 21 heated by the focused beam CB is about 1800K.
- the rotating body 2 can have a length of about 1 to 5 m and a diameter ⁇ of about 1 m, for example.
- the drive means for example, an electric motor, a steam turbine, or the like can be used.
- the drive means is not limited to this, and any drive force that can rotate the rotating body 2 in the circumferential direction can be used. Anything can be used.
- the heat insulating member 3 prevents the temperature of the reactive ceramic layer 21 that has been heated by being irradiated with the focused beam CB from being reduced until the heat is transferred to the heat storage means 4 described later. It is provided so as not to lower the temperature of the heat-transmitted reactive ceramic layer 21. For this reason, the heat insulation member 3 is provided so that the outer peripheral surface of the rotary body 2 may be covered.
- the heat insulating member 3 is provided with an opening 31 that allows the rotating body 2 to be irradiated with the condensed beam CB. That is, the upper end portion of the rotating body 2 irradiated with the condensed beam CB is exposed from the heat insulating member 3.
- Examples of the heat insulating member 3 include aluminum wool, glass wool, rock wool, and ceramic cloth.
- the heat storage means 4 is preferably formed using, for example, a heat storage material formed of at least one of a carbon material and a salt.
- a heat storage material formed of at least one of a carbon material and a salt.
- the carbon material include graphite (graphite) and carbon composite as described above.
- the salt include NaCl and rock salt.
- the uppermost portion 41 that is provided in the vicinity of the rotating body 2 and receives heat from the rotating body 2 is made of a material that has particularly good thermal conductivity and excellent oxidation resistance. Is preferred. Examples of such materials include aluminum nitride, silicon nitride, silicon carbide, and carbon ceramics.
- the gas supply means 5 supplies a gas containing oxygen toward the rotating body 2.
- This gas supply means 5 can be provided at any position from the rotating rotator 2 passing through the opening 31 to the heat storage means 4.
- the gas supply means 5 can be composed of, for example, an air pump (not shown) and a nozzle (not shown) connected to the air pump and provided with a blowing port toward the reactive ceramic layer 21. Since the gas containing oxygen supplied by the gas supply means 5 has already been described, the description thereof is omitted.
- the heat storage means 4 described above preferably includes a heat extraction means 6 for circulating the heat medium HC and taking out the heat stored in the heat storage means 4 to the outside of the heat storage means 4.
- a heat extraction means 6 for circulating the heat medium HC and taking out the heat stored in the heat storage means 4 to the outside of the heat storage means 4.
- the outside of the heat storage means 4 include external equipment such as equipment for reforming natural gas and methane gas, and gas turbine power generation equipment.
- Examples of the heat extraction means 6 include a heat exchanger. Specifically, when the heat medium HC is circulated through a hollow tube passing through the heat storage means 4, the heat stored in the heat storage means 4 can be suitably taken out to external equipment.
- the number of hollow tubes can be set arbitrarily. Further, it is also preferable that the hollow tube is folded back multiple times as necessary so that the heat medium HC can pass through the heat storage means 4 a plurality of times. If it does in this way, the heat of the thermal storage means 4 can be taken out out of the thermal storage means 4 efficiently.
- air, molten salt, or the like can be used as the heat medium HC.
- carbonates sodium, potassium, calcium, magnesium
- the heat extraction means 6 is preferably divided into, for example, an upper part and a lower part of the heat storage means 4, and the upper part is mainly used for daytime operation and the lower part is mainly used for nighttime operation.
- the laying distance of the hollow tube provided in the upper part is preferably shorter than the laying distance of the hollow tube provided in the lower part.
- the flow rate of the heat medium HC in the upper hollow tube and the flow rate of the heat medium HC in the lower hollow tube can be arbitrarily set.
- the thermal equilibrium between the reactive ceramic layer 21 and the heat storage means 4 can be controlled by controlling the flow rate of the heat medium HC. For example, if the flow rate of the heat medium HC is decreased, the temperature of the heat storage means 4 can be increased, and if the flow rate of the heat medium HC is increased, the temperature of the heat storage means 4 can be decreased.
- the amount of heat transferred from the rotating body 2 is extremely large and the temperature is high. Therefore, sufficient heat can be supplied to the external equipment even in the upper heat extraction means 6u where the installation distance of the hollow tube is short.
- the amount of heat transferred from the rotating body 2 is extremely large and the temperature is high. Therefore, the heat cannot be supplied to the external equipment by the upper heat extraction means 6u, and the surplus is transferred to the lower part of the heat storage means 4. It is. Therefore, about 1300 K of heat is also stored in the lower part of the heat storage means 4. That is, according to the upper heat extraction means 6u, heat utilization and heat storage can be performed simultaneously. Therefore, at night, the lower heat extraction means 6b can be operated to supply heat stored in the lower part of the heat storage means 4 to the external equipment.
- the heat extraction means 6 is not divided into two parts, the upper part and the lower part, and may be divided into three or more. This can be set arbitrarily.
- ⁇ density
- C p specific heat
- T temperature
- t time
- k thermal conductivity
- Q out the amount of heat transferred.
- Q in is the heat of oxidation in the reactive ceramic solar heat release chamber (between the rotator 2 and the uppermost portion 41 of the heat storage means 4; the same applies hereinafter)
- h conv is the absorption efficiency of the same surface
- ⁇ is the Stefan-Boltzmann factor
- T amb is the average temperature of the reactive ceramics of the rotating body 2 in the solar heat discharge chamber.
- Table 2 shows the physical constants.
- a curve A indicates the absorbed solar heat amount (cumulative) (MJ) (heat amount in the solar heat discharge chamber).
- Curve B shows the accumulated heat storage amount (MJ) of the heat storage means 4 using graphite.
- Curve C shows the amount of heat released (kJ / h) by the heat medium HC operating at 400 to 800 ° C. (673 to 1073 K).
- Curve D shows the temperature (K) of the uppermost part 41 of the heat storage means 4 using graphite.
- the amount of heat extracted by the heat medium HC is 1800 to 2000 MJ / h (3 to 5 hours) and 2500 MJ / h (6 to 8 hours). Further, as can be seen from the curves B and C, the amount of heat stored in 1 to 2 hours is very close to saturation, and the amount of heat that can be extracted in 3 hours of operation reaches 1700 MJ / h. In the case of steady operation at 1700-2500 MJ / h (0.47-0.69 MW) for 1-2 hours at start-up, it is preferable to back up with natural gas or the like. After 8 hours of daytime operation, 10320 MJ is stored. The temperature of the uppermost portion 41 of the heat storage means 4 using graphite is 1500 to 1550 ° C. (curve D).
- FIG. 5 shows the temperature distribution (K) in the heat storage means 4 with respect to the height of the heat storage means 4 using graphite and the heat storage amount distribution (MJ / m) in each operation time in the daytime operation mode. is there.
- the height width used for heat storage in the heat storage means 4 is 6 to 8 m, and the overall height of the heat storage means 4 is 10 m.
- the temperature rises by 100 ° C. at a height of 9 to 10 m.
- the temperature distribution and the heat storage amount distribution in the heat storage means 4 become substantially constant, and the heat storage amount in the daytime operation mode reaches almost saturation.
- the average heat storage amount is 8464 MJ, and the temperature is 1000 ° C. (about 1300 K).
- the temperature gradient in the heat storage means 4 is gradually relaxed, and the temperature of the uppermost portion 41 of the heat storage means 4 is also about 1000 ° C. This suggests that the outlet temperature of the heat medium HC can be maintained around 800 ° C. (about 1073 K) even during nighttime operation.
- the inlet temperature of the heat medium HC is set to 400 ° C. (about 673 K).
- the amount of heat corresponding to 8464 MJ can be recovered.
- the heat flow rate per unit time is 1700 MJ / h (0.47 MW), and operation is possible for 4 hours.
- a 24-hour operation at a high temperature is possible.
- the simulation results described above can be evaluated as follows. In order to realize 1 MW as a solar heat storage system that stores heat for 4 hours, based on the simulation results evaluated for the practically operable temperature and the size of the heat storage means 4, the size of the heat storage means 4 is A calculation result of 6 m 3 (diameter ⁇ 1 m, height 8 m) was obtained.
- the condensing heat amount is 100 MW (heat storage amount 60 MW), and the heat storage time is Trial calculation was performed for 12 hours.
- the diameter was estimated to be 13.5 m, the height was 8 m, and the volume was 1100 m 3 . This size is presumed to be appropriate as the scale of the actual heat storage tank.
- the diameter of the ground condensing beam CB is 10 to 15 m. This size takes the height of the heat storage tank (heat storage means 4) into consideration, and if the focal position from the ground is increased accordingly, the diameter is further reduced.
- the rotating body 2 on which the reactive ceramic layer 21 is formed is directly irradiated with the condensing beam CB to store heat in the heat storage means 4.
- the diameter of the heat storage means 4 using graphite is 13.5 m is a fairly reasonable size.
- the thermal conductivity of graphite was 2000 W / m / K. This may be applied to 1000 to 100 W / m / K, but some carbon composites and nanotubes can be applied with numerical values like this time. In fact, recently, 500 W / m / K composites are commercially available. Further, even if the material having such high conductivity is not used as it is, the heat input on the heat storage means 4 is forcibly moved to the middle part of the heat storage means 4 by changing the structure and mechanism of the heat exchange system. It is possible. In combination with these, the best thermal conductivity material may be selected. Moreover, it is considered that the capacity itself of the heat storage means 4 can be further reduced by variously examining such application development. As a result, the heat storage capacity increases, leading to cost reduction.
- the beam-down solar condensing system has an excellent feature that a heavy heat storage facility can be directly heated on the ground because the condensed beam CB can be reproduced near the ground.
- the solar heat storage method and the solar heat storage apparatus 1 according to the present invention have a unique configuration in which a beam-down solar condensing system and a rotating body 2 having a reactive ceramic layer 21 are combined. It is possible to provide a solar heat utilization technology that can be operated for 24 hours at high temperature and high efficiency.
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Abstract
Description
また、前記した本発明においては、前記蓄熱手段が、熱媒体を流通させて当該蓄熱手段に蓄熱された熱を前記蓄熱手段外に取り出す熱取り出し手段を備えているのが好ましい。
さらに、前記した本発明においては、前記回転体が、アルミナ繊維を用いた円筒体であるのが好ましい。
前記した本発明においては、前記蓄熱手段が、炭素材料および塩のうちの少なくとも一方で形成された蓄熱材を用いているのが好ましい。
また、本発明によれば、約1000~1300Kの熱を外部設備に24時間供給可能な太陽熱蓄熱システムを提供することができる。
はじめに、図1を参照して本発明に係る太陽熱蓄熱方法の一実施形態について説明する。図1に示すように、本発明の一実施形態に係る太陽熱蓄熱方法は、集光ビーム照射ステップS1と、蓄熱ステップS2と、を含んでなる。
集光ビーム照射ステップS1は、加熱されると酸素を放出して酸化型から還元型となり、酸素と接触すると酸化型に戻る反応性セラミックスを用いて形成された反応性セラミックス層を移動させつつ、この反応性セラミックス層に太陽光を集光した集光ビームを照射して加熱するステップである。
次に行う蓄熱ステップS2は、集光ビーム照射ステップS1で加熱された反応性セラミックス層と酸素を含むガスとを接触させつつ、この反応性セラミックス層から発せられる熱を蓄熱手段に蓄熱させるステップである。
なお、この蓄熱ステップS2でも反応性セラミックス層は移動し続けている。
熱取り出しステップ(図1において図示省略)は、熱媒体を流通させて蓄熱手段に蓄熱された熱を蓄熱手段外、つまり、外部設備に取り出すステップである。このステップは、蓄熱手段と外部設備の間の熱交換により具現でき、外部設備に約1000~1300Kの熱を供給することができる。
以上に説明した一実施形態に係る太陽熱蓄熱方法では、前記した各ステップにより、集光ビームと、反応性セラミックス層と、蓄熱手段との間で、図2に示すような反応や伝熱が行われる。
かかる現象は、高エンタルピー変化を伴った吸熱反応として進行する、固体格子構造中の配位変化、つまり、フレンケル欠陥構造の非平衡状態を単位とした化学反応である。従って、このステップでは、反応材料の高エンタルピー変化により集光ビームのエネルギーを吸収することができる。また、このステップは格子構造中における陰イオン(または陽イオン)移動であるから、当該ステップにおける化学反応は集光ビームのエネルギーの吸収に従って進行すると推察される。なお、この化学反応中のフレンケル欠陥構造の非平衡状態は、高フラックスエネルギーの吸収後に形成される。
すなわち、集光ビーム照射ステップS1では、集光ビームが反応性セラミックスによって吸収され、そしてセラミックス材料の還元型の化学エネルギーへ変換される。
以上に説明した各ステップを含んでなる太陽熱蓄熱方法を具現した太陽熱蓄熱システムの一実施形態について、図3を参照して以下に説明する。
回転体2については、集光ビーム照射ステップS1でも既に説明しているとおり、円筒状を呈するのが好ましい。この回転体2の外周面には、前記した反応性セラミックスを用いた反応性セラミックス層21が形成されている。反応性セラミックス層21の厚みは特に限定されるものではないが、例えば、2mmなどとすることができる。
駆動手段(図示省略)としては、例えば、電気モータ、蒸気タービンなどを用いることができるが、これに限定されるものではなく、回転体2を周方向に回転させる駆動力を発揮できるものであればどのようなものでも用いることができる。
断熱部材3は、集光ビームCBが照射されて加熱された反応性セラミックス層21が後記する蓄熱手段4に伝熱するまでその温度を低下させないようにするため、また、後記する蓄熱手段4に伝熱した反応性セラミックス層21の温度を低下させないようにするために設けられる。このため、断熱部材3は、回転体2の外周面を覆うようにして設けられている。
蓄熱手段4は、断熱部材3の開口部31から離間した位置で、回転体2に近接して設けられている。なお、集光ビームCBによって加熱された反応性セラミックス層21は約1800Kもの高温となっており、機械的強度が低下しているため、蓄熱手段4と接触させないようにするのが好ましい。回転体2からの伝熱により、蓄熱手段4には約1300Kの熱が蓄熱される。
ガス供給手段5は、酸素を含むガスを回転体2に向けて供給する。このガス供給手段5は、回転する回転体2が開口部31を通過した後、蓄熱手段4に至るまでの任意の位置に設けることができる。
ガス供給手段5は、例えば、エアポンプ(図示省略)と、これに接続され、吹き出し口が反応性セラミックス層21に向けて設けられたノズル(図示省略)とで構成することができる。ガス供給手段5によって供給される、酸素を含むガスについては既に説明しているので説明を省略する。
前記した蓄熱手段4は、熱媒体HCを流通させて当該蓄熱手段4に蓄熱された熱を蓄熱手段4外に取り出す熱取り出し手段6を備えているのが好ましい。なお、蓄熱手段4外として具体的には、天然ガスやメタンガスを改質する設備、ガスタービン発電設備などの外部設備を挙げることができる。
図4中において、曲線Aは、吸収太陽熱量(累積)(MJ)(太陽熱放出室における熱量)を示す。曲線Bは、黒鉛を用いた蓄熱手段4の累積蓄熱量(MJ)を示す。曲線Cは、400~800℃(673~1073K)で動作する熱媒体HCによる流出熱量(kJ/h)を示す。曲線Dは、黒鉛を用いた蓄熱手段4の最上部41の温度(K)を示す。
スタートアップ時の1~2時間を1700~2500MJ/h(0.47~0.69MW)で定常運転する場合、天然ガス等でバックアップするのが好適である。8時間日中運転後には10320MJが蓄熱されている。また、黒鉛を用いた蓄熱手段4の最上部41の温度は1500~1550℃(曲線D)となっている。
8時間運転後では、平均蓄熱量は8464MJとなり、温度も1000℃(約1300K)となる。日没後は、蓄熱手段4内の温度勾配が徐々に緩和され、蓄熱手段4最上部41の温度も1000℃付近となっている。これは、夜間運転においても、熱媒体HCの出口温度は800℃(約1073K)付近に維持できることを示唆している。今回の計算結果は、熱媒体HCの入口温度を400℃(約673K)としたが、この場合には、8464MJに相当する熱量を回収できる結果となった。この熱量の約70%に相当する6000MJが取り出せると仮定すると、単位時間当たりの熱流量は1700MJ/h(0.47MW)で、4時間運転が可能となる。この熱量を増大するには、下記のように蓄熱面積を増やすことによっても可能である。また、高温での24時間運転も可能である。
実用化可能で運転可能な温度と蓄熱手段4のサイズに対して評価を行ったシミュレーション結果から、4時間分の熱を蓄熱する太陽熱蓄熱システムとして1MWを実現するには、蓄熱手段4のサイズを6m3(直径φ1m、高さ8m)とする計算結果が得られた。
以上に説明したように、本発明に係る太陽熱蓄熱方法および太陽熱蓄熱装置1は、ビームダウン方式の太陽光集光システムと反応性セラミックス層21を形成した回転体2とを組み合わせるという独自の構成によって、高温で高効率な24時間運転可能な太陽熱利用技術が提供可能である。
S2 蓄熱ステップ
1 太陽熱蓄熱システム
2 回転体
21 反応性セラミックス層
3 断熱部材
31 開口部
4 蓄熱手段
41 最上部
5 ガス供給手段
6 熱取り出し手段
6u 上部の熱取り出し手段
6b 下部の熱取り出し手段
CB 集光ビーム
Claims (9)
- 太陽光エネルギーを用いて熱を蓄熱する太陽熱蓄熱方法であって、
加熱されると酸素を放出して酸化型から還元型となり、酸素と接触すると酸化型に戻る反応性セラミックスを用いて形成された反応性セラミックス層を移動させつつ、当該反応性セラミックス層に太陽光を集光した集光ビームを照射して加熱する集光ビーム照射ステップと、
前記集光ビーム照射ステップで加熱された前記反応性セラミックス層と酸素を含むガスとを接触させつつ、前記反応性セラミックス層から発せられる熱を蓄熱手段に蓄熱させる蓄熱ステップと、
を含むことを特徴とする太陽熱蓄熱方法。 - 請求の範囲第1項に記載の太陽熱蓄熱方法であって、
前記蓄熱ステップ後、熱媒体を流通させて前記蓄熱手段に蓄熱された熱を前記蓄熱手段外に取り出す熱取り出しステップを含むことを特徴とする太陽熱蓄熱方法。 - 太陽光エネルギーを用いて熱を蓄熱する太陽熱蓄熱システムであって、
加熱されると酸素を放出して酸化型から還元型となり、酸素と接触すると酸化型に戻る反応性セラミックスを用いてなる反応性セラミックス層を表面に形成した回転体およびこれを周方向に回転させる駆動手段と、
前記回転体の外周面を覆うようにして設けられ、太陽光を集光させた集光ビームの前記回転体への照射を可能とする開口部を有する断熱部材と、
前記開口部から離間した位置で、前記回転体に近接して設けられた蓄熱手段と、
回転する前記回転体が前記開口部を通過した後、前記蓄熱手段に至るまでの任意の位置に設けられた、酸素を含むガスを前記回転体に向けて供給するガス供給手段と、
を備えることを特徴とする太陽熱蓄熱システム。 - 請求の範囲第3項に記載の太陽熱蓄熱システムであって、
前記反応性セラミックス層が、ニッケルフェライトで形成されていることを特徴とする太陽熱蓄熱システム。 - 請求の範囲第3項に記載の太陽熱蓄熱システムであって、
前記蓄熱手段が、熱媒体を流通させて当該蓄熱手段に蓄熱された熱を前記蓄熱手段外に取り出す熱取り出し手段を備えていることを特徴とする太陽熱蓄熱システム。 - 請求の範囲第4項に記載の太陽熱蓄熱システムであって、
前記蓄熱手段が、熱媒体を流通させて当該蓄熱手段に蓄熱された熱を前記蓄熱手段外に取り出す熱取り出し手段を備えていることを特徴とする太陽熱蓄熱システム。 - 請求の範囲第3項から請求の範囲第6項のいずれか1項に記載の太陽熱蓄熱システムであって、
前記回転体が、アルミナ繊維を用いた円筒体であることを特徴とする太陽熱蓄熱システム。 - 請求の範囲第3項から請求の範囲第6項のいずれか1項に記載の太陽熱蓄熱システムであって、
前記蓄熱手段が、炭素材料および塩のうちの少なくとも一方で形成した蓄熱材を用いていることを特徴とする太陽熱蓄熱システム。 - 請求の範囲第7項に記載の太陽熱蓄熱システムであって、
前記蓄熱手段が、炭素材料および塩のうちの少なくとも一方で形成した蓄熱材を用いていることを特徴とする太陽熱蓄熱システム。
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ES11839351.1T ES2630170T3 (es) | 2010-11-08 | 2011-11-08 | Método y sistema para almacenar calor solar |
EP11839351.1A EP2639527B1 (en) | 2010-11-08 | 2011-11-08 | Method and system for storing solar heat |
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WO2020158740A1 (ja) * | 2019-01-29 | 2020-08-06 | 国立大学法人東海国立大学機構 | 蓄熱装置 |
JP7482518B2 (ja) | 2019-01-29 | 2024-05-14 | 国立大学法人東海国立大学機構 | 蓄熱装置 |
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See also references of EP2639527A4 |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
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JP2020514116A (ja) * | 2016-12-29 | 2020-05-21 | ザ・ボーイング・カンパニーThe Boeing Company | 太陽エネルギーを使用して炭素繊維を再生するためのシステム及び方法 |
JP7241686B2 (ja) | 2016-12-29 | 2023-03-17 | ザ・ボーイング・カンパニー | 太陽エネルギーを使用して炭素繊維を再生するためのシステム及び方法 |
WO2020158740A1 (ja) * | 2019-01-29 | 2020-08-06 | 国立大学法人東海国立大学機構 | 蓄熱装置 |
JP7482518B2 (ja) | 2019-01-29 | 2024-05-14 | 国立大学法人東海国立大学機構 | 蓄熱装置 |
Also Published As
Publication number | Publication date |
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CN103168202A (zh) | 2013-06-19 |
JPWO2012063838A1 (ja) | 2014-05-12 |
EP2639527B1 (en) | 2017-06-21 |
US9372013B2 (en) | 2016-06-21 |
US20130269681A1 (en) | 2013-10-17 |
CN103168202B (zh) | 2015-10-21 |
ES2630170T3 (es) | 2017-08-18 |
EP2639527A1 (en) | 2013-09-18 |
EP2639527A4 (en) | 2014-11-12 |
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