EP2389556A1 - Accumulateur de chaleur latente à haute température - Google Patents

Accumulateur de chaleur latente à haute température

Info

Publication number
EP2389556A1
EP2389556A1 EP10704337A EP10704337A EP2389556A1 EP 2389556 A1 EP2389556 A1 EP 2389556A1 EP 10704337 A EP10704337 A EP 10704337A EP 10704337 A EP10704337 A EP 10704337A EP 2389556 A1 EP2389556 A1 EP 2389556A1
Authority
EP
European Patent Office
Prior art keywords
storage medium
storage
latent heat
wall
temperature
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP10704337A
Other languages
German (de)
English (en)
Inventor
André THESS
Jürgen BÜHL
Dietmar Schulze
Andreas Nilius
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Technische Universitaet Ilmenau
Original Assignee
Technische Universitaet Ilmenau
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Technische Universitaet Ilmenau filed Critical Technische Universitaet Ilmenau
Publication of EP2389556A1 publication Critical patent/EP2389556A1/fr
Withdrawn legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28HEAT EXCHANGE IN GENERAL
    • F28DHEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
    • F28D20/00Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00
    • CCHEMISTRY; METALLURGY
    • C09DYES; PAINTS; POLISHES; NATURAL RESINS; ADHESIVES; COMPOSITIONS NOT OTHERWISE PROVIDED FOR; APPLICATIONS OF MATERIALS NOT OTHERWISE PROVIDED FOR
    • C09KMATERIALS FOR MISCELLANEOUS APPLICATIONS, NOT PROVIDED FOR ELSEWHERE
    • C09K5/00Heat-transfer, heat-exchange or heat-storage materials, e.g. refrigerants; Materials for the production of heat or cold by chemical reactions other than by combustion
    • C09K5/02Materials undergoing a change of physical state when used
    • C09K5/06Materials undergoing a change of physical state when used the change of state being from liquid to solid or vice versa
    • C09K5/063Materials absorbing or liberating heat during crystallisation; Heat storage materials
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F24HEATING; RANGES; VENTILATING
    • F24SSOLAR HEAT COLLECTORS; SOLAR HEAT SYSTEMS
    • F24S60/00Arrangements for storing heat collected by solar heat collectors
    • F24S60/10Arrangements for storing heat collected by solar heat collectors using latent heat
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F24HEATING; RANGES; VENTILATING
    • F24SSOLAR HEAT COLLECTORS; SOLAR HEAT SYSTEMS
    • F24S60/00Arrangements for storing heat collected by solar heat collectors
    • F24S60/30Arrangements for storing heat collected by solar heat collectors storing heat in liquids
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28HEAT EXCHANGE IN GENERAL
    • F28DHEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
    • F28D20/00Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00
    • F28D20/02Heat storage plants or apparatus in general; Regenerative heat-exchange apparatus not covered by groups F28D17/00 or F28D19/00 using latent heat
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28HEAT EXCHANGE IN GENERAL
    • F28FDETAILS OF HEAT-EXCHANGE AND HEAT-TRANSFER APPARATUS, OF GENERAL APPLICATION
    • F28F19/00Preventing the formation of deposits or corrosion, e.g. by using filters or scrapers
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28HEAT EXCHANGE IN GENERAL
    • F28FDETAILS OF HEAT-EXCHANGE AND HEAT-TRANSFER APPARATUS, OF GENERAL APPLICATION
    • F28F2270/00Thermal insulation; Thermal decoupling
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/40Solar thermal energy, e.g. solar towers
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E60/00Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
    • Y02E60/14Thermal energy storage

Definitions

  • the invention relates to a latent heat storage, which allows the recording, storage and delivery of thermal energy at a temperature level, which equals or exceeds the temperatures of technical combustion processes.
  • Storage medium is, the greater efficiencies are achievable in the conversion of the heat contained in the memory into mechanical or electrical energy. It is therefore desirable to develop latent heat storage with the highest possible operating temperatures.
  • latent heat accumulators with salt melts belong to the state of the art as storage media.
  • Semiconductor material silicon are characterized by high enthalpies of fusion and thus by a high thermal storage capacity. Furthermore, the materials mentioned have a high thermal conductivity compared to molten salts, which facilitates the thermal loading and unloading.
  • the liquid metals mentioned in the cited work are aggressive and cause strong erosion phenomena on the walls and on thermal loading and unloading equipment. As will be described in the publication CN 1504716A, this erosion can be limited by limiting the operating temperature to below 620 0 C, but not completely prevented.
  • WO 79/01004 A1 describes a solar energy system with a collector for collecting and concentrating the solar radiation and a collector coupled to the receiver, which is to convert the radiation into thermal energy.
  • a thermal energy accumulator is provided, which contains a mixture of meltable salts. The latent heat amount of the salts can be used to increase the time over which the accumulator usable heat can be withdrawn.
  • the fusible salts are enclosed with a refractory seal, which
  • Metal plates and straps is supported.
  • the molten salt serving as the storage medium is in direct contact with the refractory seal in the state of maximum thermal loading, so that the known problems of excessive erosion occur there.
  • the present invention has for its object to provide a latent heat storage, the storage medium both a high heat storage capacity and a high
  • a sub-task consists of quickly and thermally loading and unloading the heat accumulator in a contact-free manner, as well as minimizing memory losses.
  • FIG. 1 shows a phase diagram for a binary system iron-aluminum
  • FIG. 2 shows a phase diagram for a eutectic solution of iron and silicon
  • FIG. 3 shows a first embodiment of a high-temperature latent heat accumulator with indirect electrical charging and convective discharge
  • FIG. 4 shows a second embodiment of the high-temperature latent heat accumulator with convective charging and convective discharge
  • FIG. 5 shows a third embodiment of the high-temperature latent heat accumulator with direct electrical charging and convective discharge
  • FIG. 6 shows a fourth embodiment of the high-temperature latent heat accumulator with arc charging and convective discharge
  • FIG. 7 shows a fifth embodiment of the high-temperature latent heat accumulator with arc charging and convective discharge
  • Figure 8 - a sixth embodiment of the high-temperature latent heat storage as a double tube storage with indirect electrical loading and convective
  • FIG. 9 shows a seventh embodiment of the high-temperature latent heat accumulator with inductive electrical charging and convective discharge
  • FIG. 10 an eighth embodiment of the high-temperature latent heat storage with loading by radiant heating and discharge by thermal radiation.
  • the phenomenon of erosion in high-temperature processes is due to the fact that the wall material and the melt are generally not in a stable thermodynamic equilibrium.
  • the thermodynamic cause of the erosion can be explained using the example of the phase diagram shown in FIG. 1 of the binary system iron-aluminum. Filling one liquid aluminum at a temperature of 900 0 C, its state is represented by point 11 in Figure 1, in an iron crucible, then the resulting system is initially away from the thermodynamic equilibrium. In order to reach thermodynamic equilibrium, part of the solid wall material dissolves in the liquid aluminum and thus leads to erosion of the wall.
  • the binary system iron-aluminum has reached the state of thermodynamic equilibrium at a temperature of 900 0 C, when the melt consists of about 90 percent by mass of aluminum and about 10 percent by mass of iron. This condition is characterized by the point 12 in FIG. If such a condition is reached, it is called a solubility equilibrium. After reaching the solubility equilibrium, no further migration erosion takes place.
  • the invention is based i.a. Recognizing that the problem of wander erosion in high-temperature latent heat storage can be solved by a coordinated selection of storage medium, wall material and storage temperature.
  • a part of the storage container inner wall is preferably "sacrificed" during the first thermal loading in order to be dissolved in the storage medium and form the thermodynamic equilibrium even before the first load, a corresponding amount of the material from which the storage tank inner wall consists is dissolved.
  • FIG. 22 A second example of preventing migration erosion by providing a solubility weight is shown in FIG. If a eutectic alloy of iron and silicon is heated starting from the solid state of matter identified as point 21 in FIG. 2 in the liquid state of aggregation designated as point 22
  • thermodynamic equilibrium a part of the solid wall material dissolves in the liquid melt and thus leads to the erosion of the wall.
  • the binary system iron-silicon which is also referred to as ferrosilicon, at a temperature of 1400 0 C has reached the marked in Figure 2 as point 23 state of thermodynamic equilibrium on the liquidus curve 24 when the melt to about 90 percent by mass of iron and to about 10 percent by mass silicon. After reaching this state, no further migration erosion takes place.
  • the melt solidifies, the composition of the solid phase being determined by the solidus curve 25 in FIG.
  • Silicon has a very high melting enthalpy and is therefore suitable as a storage medium for latent heat storage.
  • the example shown in FIG. 2 illustrates that an erosion of the wall can be prevented by a suitable combination of the storage medium ferrosilicon with the wall material iron.
  • thermodynamic equilibrium is not a solubility equilibrium but an equilibrium phase.
  • the inner wall of the storage container and the storage medium may consist of silicon (melting temperature about 1400 ° C.). If the heat to be stored is deliberately introduced through an entry surface (eg with a radiant heater), the material will melt only locally and, with the appropriate dimensioning, leave a solid outer wall as a container inner wall.
  • a high-temperature latent heat store can be produced if the liquid storage medium and the solid wall material are brought into a thermodynamic equilibrium, preferably a solubility equilibrium, in the case of maximum thermal loading, as a result of which further traveling erosion is prevented.
  • the solution of the Wanderosionsproblems in a high-temperature latent heat storage succeeds in the special case mentioned in the third example, in which the wall material consists of the same substance as the storage medium.
  • the desired thermodynamic equilibrium is not a solubility equilibrium, but a phase equilibrium must be achieved.
  • the high-temperature latent heat storage device comprises a storage container 32 in which the storage medium 31 is located, which in the case of maximum thermal loading is in contact with a storage container inner wall 33.
  • the surface of the storage medium 31 is limited by a protective gas 34.
  • the materials of storage medium 31 and storage container inner wall 33 and the operating temperature of the memory are so coordinated with each other, that at the initial thermal loading a part, namely a so-called sacrificial portion of the inner wall material in the liquid storage medium dissolves and forms a stable thermodynamic solubility equilibrium.
  • the thickness of the inner wall of the storage container is to be chosen such that the inner wall is closed and sealed for the storage medium (31) even after the replacement of the sacrificial portion, that is, it can continue to fulfill its wall function.
  • the storage inner wall can be supported by other components, for example, by adjacent wall panels made of other materials, by carriers or other supporting structures.
  • the material of the storage container inner wall is preferably soluble in the liquid storage medium, wherein the concentration of dissolved in the liquid storage medium material of the storage container inner wall is equal to the valid for the operating temperature of the high-temperature latent heat storage equilibrium concentration.
  • a thickness of the inner wall of the storage container which satisfies the mechanical stability requirements remains at the set solubility equilibrium between the liquid storage medium and the material of the storage container inner wall.
  • the storage medium and the storage container inner wall form a material unit after the first loading operation and are no longer clearly distinguishable from one another in the subsequent loading and unloading cycles.
  • the storage medium from the outset a material content of the material Storage inner wall added.
  • the thermodynamic equilibrium is thus established faster, so that the sacrificial portion to be detached from the inner wall of the storage tank is lower.
  • the memory shown in FIG. 3 furthermore contains an insulation layer 35, which is in contact with the storage container inner wall 33 through a connection layer 36.
  • the loading of the storage takes place by means of a tubular heater 37, which consists of a heating conductor 38, a cladding tube 39 and an outer layer 40 and is coupled via an electrical connection 41 to a power supply system.
  • the materials of storage medium and outer layer 40 of the tubular heater and the operating temperature of the memory are coordinated so that in the first loading also a sacrificial portion of the outer layer 40 dissolves in the liquid storage medium 31 and a stable thermodynamic solubility Golichtec develops, which prevents the erosion of the heating system.
  • the concentration of dissolved in the liquid storage medium 31 material of the outer layer 40 is equal to the valid equilibrium concentration at the operating temperature of the high-temperature latent heat storage.
  • the discharge of the storage takes place by means of a heat exchanger tube 42 through which a heat transfer fluid 45 circulates.
  • This type of thermal discharge is referred to below as convective discharge.
  • the heat exchanger tube 42 consists of an inner tube 44, which serves the structural stability, as well as an outer layer 43.
  • the materials of storage medium 31 and outer layer 43 of the heat exchanger tube 42 and the operating temperature of the memory are coordinated so that a part of the outer layer 43 in the liquid storage medium 31 can solve and forms a stable thermodynamic solubility balance, which prevents the erosion of the discharge system.
  • the concentration of the material of the outer layer (43) of the heat transfer tubes dissolved in the liquid storage medium (31) is equal to the equilibrium concentration valid there at the operating temperature of the high-temperature latent heat store.
  • a correspondingly modified embodiment of the high-temperature latent heat accumulator according to the invention is characterized in that at least one heat transfer tube 42 for thermal loading and one heat transfer tube constructed in the same way for the thermal discharge are installed in the interior of the storage tank 32 such that their outer layers 43 are in direct contact Contact with the liquid storage medium 31 stand.
  • the materials of storage medium 31, storage tank inner wall 33 and outer layer 43 of the heat transfer tube 42 and the operating temperature of the memory are in turn coordinated so that a part of the storage tank inner wall 33 and the outer layer 43 can dissolve in the liquid storage medium 31 during thermal loading and a stable forms thermodynamic solubility Gie, which prevents the further erosion of the storage tank inner wall and the heat exchanger tubes.
  • the embodiment of the high-temperature latent heat accumulator shown in FIG. 4 is particularly suitable for applications in parabolic trough solar power plants or in solar tower power plants in which the energy to be stored is obtained in the form of heat.
  • FIG. 5 shows a further embodiment of the high-temperature latent heat accumulator with direct electrical heating.
  • the storage medium 31 located in the storage container 32 is bounded by a suitable material of the storage container inner wall 33 and upwardly by an inert covering medium 34 and isolated by a layer 35 to the outside.
  • By means of two or more electrodes 46, which are coated with a suitable outer layer 47 electric current is fed into the storage medium and the storage medium is thereby heated. This type of heating is called direct electrical heating.
  • the thermal discharge takes place by means of a system of heat exchanger tubes 48, which are integrated in the insulating material of the storage container.
  • FIG. 6 shows a fourth embodiment of the high-temperature latent heat accumulator.
  • the storage container 32, storage medium 31, storage container inner wall 33, insulation layer 35 with integrated heat exchanger tubes 48, connecting Density layer 36, inert cover medium 34 and multiple electrodes 46 existing memory is further characterized by the fact that the thermal loading by ignition of arcs 49 between the electrodes and the surface of the storage medium 31 takes place. This form of loading allows a non-contact electrical coupling of heat.
  • the thermal discharge takes place by means of a system of heat exchanger tubes 48 which are embedded in the insulation layer 35 of the memory.
  • FIG. 7 shows a further advantageous development of the high-temperature latent heat accumulator according to the invention, in which the storage medium 31 and the storage container inner wall 33 are made of the same material.
  • the storage medium 31 is located inside a bearing 50 rotating
  • Storage container 51 which has the insulation layer 35 and the connection layer 36 to the storage medium 31. Due to the rotation of the storage container creates a radially outwardly directed centrifugal force that presses the liquid storage medium 31 at sufficiently fast rotation of the storage container inner wall 33 and generates a free surface 52 in the storage medium.
  • the thermal loading of the high-temperature latent heat storage takes place by two electrodes 46 are inserted into the memory in two on the axis of rotation in the rotating storage container 51 lent openings 53 and between them an arc 49 is ignited. After thermal loading, the electrodes can be removed and replaced with two closure elements (not shown). For thermal discharge of the memory, the closure elements are removed.
  • a gaseous heat transfer medium is introduced into the storage through one of the two openings 53.
  • the heat transfer medium receives by convective heat transport energy from the storage medium and is characterized by the other opening 53 removed from the memory.
  • the embodiment illustrated in FIG. 7 is particularly suitable for storage media such as silicon, which are distinguished by a relatively high melting temperature and a high melting enthalpy.
  • FIG. 1 Another embodiment of the high-temperature latent heat accumulator as a double tube storage is shown in FIG.
  • the storage medium 31 is located in a double tube storage container 55 formed by an outer tube 56, an inner tube 57 and two cover surfaces 58.
  • the materials of storage medium 31 and storage container inner wall 33 as well as the operating temperature of the storage are matched to one another such that a part of the storage container inner wall 33 in the liquid storage medium 31 can solve and forms a stable thermodynamic solubility equilibrium, which prevents the erosion of the storage tank inner wall.
  • the thermal loading device of the memory consists of an intermediate layer 59, which is supplied with electrical current by means of two or more electrical connections 41. The resulting Joule
  • Heat is transferred to the storage medium 31.
  • a gaseous or liquid heat transfer medium is introduced into the storage at a first end of the inner tube 57.
  • a discharge flow 60 absorbs energy from the storage medium by convective heat transport and is removed from the storage at a second end of the inner tube 57.
  • Inductor coil thus represents simultaneously loading and unloading. It is embedded by means of a temperature-resistant electrical insulation layer 62 in the memory.
  • FIG 10 an eighth design variant of the high-temperature latent heat storage is shown, from the storage container 32, a storage chamber 64 with the storage container inner wall 33 and the storage medium 31 contained therein, the insulating layer 35 embedded with
  • Heat exchanger tubes 48 and temperature radiators 65 and a lifting beam 66 is.
  • the storage chamber 64 can be moved by means of the lifting beam 66 in the vertical direction.
  • the storage chamber 64 is moved into the lower half of the storage container 31.
  • the input of thermal energy by means of a plurality of temperature radiators 65, which are embedded in the insulating layer 35 of the storage container.
  • the storage chamber 64 is moved to the upper position.
  • a heat transfer fluid 45 is pumped through the embedded in the insulating layer 35 system of heat exchanger tubes 48, which receives the radiant heat of the storage chamber. LIST OF REFERENCE NUMBERS

Landscapes

  • Engineering & Computer Science (AREA)
  • Thermal Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Sustainable Energy (AREA)
  • Sustainable Development (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Materials Engineering (AREA)
  • Organic Chemistry (AREA)
  • Filling Or Discharging Of Gas Storage Vessels (AREA)

Abstract

L'invention concerne un accumulateur de chaleur latente à haute température comprenant un réservoir d'accumulateur (32) avec une paroi interne de réservoir d'accumulateur (33) ainsi qu'un fluide accumulateur (31) qui est disposé dans le réservoir d'accumulateur (32), qui est directement au contact de la paroi interne de réservoir d'accumulateur (33) et qui se présente sous un état physique liquide, au moins à une température de fonctionnement. Il est prévu en outre une couche isolante (35), un dispositif de chargement thermique et un dispositif de déchargement thermique. Selon l'invention, les matériaux du fluide accumulateur (31) et de la paroi interne de réservoir d'accumulateur (33), ainsi que la température de fonctionnement de l'accumulateur de chaleur latente, sont choisis pour que, lors du chargement thermique jusqu'à la température de fonctionnement, une partie sacrifiée du matériau de la paroi interne de réservoir d'accumulateur (33) se dissolve dans le fluide accumulateur (31) liquide jusqu'à ce qu'il s'établisse un équilibre thermodynamique stable. L'épaisseur de la paroi interne de réservoir d'accumulateur (33) est sélectionnée de manière qu'après dissolution de la partie sacrifiée à la charge thermique maximale, elle reste close et étanche pour le fluide accumulateur (31), afin de répondre aux exigences de stabilité mécanique.
EP10704337A 2009-01-26 2010-01-21 Accumulateur de chaleur latente à haute température Withdrawn EP2389556A1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DE102009006784A DE102009006784A1 (de) 2009-01-26 2009-01-26 Hochtemperatur-Latentwärmespeicher
PCT/EP2010/050698 WO2010084161A1 (fr) 2009-01-26 2010-01-21 Accumulateur de chaleur latente à haute température

Publications (1)

Publication Number Publication Date
EP2389556A1 true EP2389556A1 (fr) 2011-11-30

Family

ID=42153770

Family Applications (1)

Application Number Title Priority Date Filing Date
EP10704337A Withdrawn EP2389556A1 (fr) 2009-01-26 2010-01-21 Accumulateur de chaleur latente à haute température

Country Status (3)

Country Link
EP (1) EP2389556A1 (fr)
DE (1) DE102009006784A1 (fr)
WO (1) WO2010084161A1 (fr)

Families Citing this family (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102011050200A1 (de) * 2011-05-06 2012-11-08 Dbk David + Baader Gmbh Wärmespeicher
DE102012101862A1 (de) 2011-05-28 2012-11-29 Ed. Züblin Ag Mehrteiliger Hochtemperaturwärmespeicher aus Speichermaterialien unterschiedlicher Temperaturbeständigkeit
DE102011056279A1 (de) * 2011-12-12 2013-06-13 Escad Ag Verfahren zum Umwandeln und Speichern von Energie
DE102012210957A1 (de) * 2012-06-27 2014-01-02 Enolcon Gmbh Hochtemperatur-Wärmespeicher mit Induktionsheizung und Metallschmelze und Wärmespeicher-Verbundsystem
DE102012019791A1 (de) 2012-10-04 2014-04-10 Technische Universität Ilmenau Kugelumlauf-Wärmespeicher
DE102014107804B4 (de) * 2014-06-03 2020-02-27 Deutsches Zentrum für Luft- und Raumfahrt e.V. Wärmespeichervorrichtung, Solarkraftwerk und Verfahren zum Speichern und Bereitstellen von Wärme
DE102015111235A1 (de) 2015-03-23 2016-09-29 Deutsches Zentrum für Luft- und Raumfahrt e.V. Wärmespeichervorrichtung und Verfahren zum Betreiben einer Wärmespeichervorrichtung
DE102019118105A1 (de) * 2019-07-04 2021-01-07 Deutsches Zentrum für Luft- und Raumfahrt e.V. Behältervorrichtung für Metallschmelzen und Fahrzeug
DE102020107464A1 (de) 2020-03-18 2021-09-23 Deutsches Zentrum für Luft- und Raumfahrt e.V. Wärmespeichervorrichtung
DE102020107465A1 (de) 2020-03-18 2021-09-23 Deutsches Zentrum für Luft- und Raumfahrt e.V. Be- und entladevorrichtung für einen wärmespeicher, wärmespeicher sowie betriebsverfahren für einen wärmespeicher
KR20240045208A (ko) 2021-08-06 2024-04-05 쉘 인터내셔날 리써취 마트샤피지 비.브이. 에너지 저장 장치 및 열전달 유체 가열 방법
CN114719654B (zh) * 2022-05-17 2024-02-13 苏州惟新传热科技有限公司 一种利用自然对流强化相变过程的相变蓄能装置

Family Cites Families (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2407562A (en) * 1942-08-17 1946-09-10 Einar G Lofgren Induction heater
CA1060929A (fr) * 1975-04-16 1979-08-21 Robert S. Segsworth Four a arc prolonge et methode de fusion de charges particulaires
DE2645261A1 (de) * 1976-10-07 1978-04-13 Varta Batterie Wiederaufladbarer hochtemperaturakkumulator
WO1979001004A1 (fr) 1978-04-28 1979-11-29 Solar Dynamics Ltd Accumulateur d'energie thermique
US4249592A (en) 1978-12-21 1981-02-10 Kohler Co. High temperature, heat storage and retrieval system
US4512388A (en) 1981-06-19 1985-04-23 Institute Of Gas Technology High-temperature direct-contact thermal energy storage using phase-change media
US5685289A (en) 1994-10-04 1997-11-11 Yeda Research And Development Co., Ltd. Heat storage device
JPH10332288A (ja) 1997-05-29 1998-12-15 Eisuke Yoshinobu 蓄熱設備
CN1504716A (zh) 2002-12-02 2004-06-16 广东工业大学 金属与熔盐储能式供热装置
JP3848302B2 (ja) * 2003-06-04 2006-11-22 核燃料サイクル開発機構 ガラス溶融炉及びその運転方法

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See references of WO2010084161A1 *

Also Published As

Publication number Publication date
DE102009006784A1 (de) 2010-07-29
WO2010084161A1 (fr) 2010-07-29

Similar Documents

Publication Publication Date Title
WO2010084161A1 (fr) Accumulateur de chaleur latente à haute température
TWI855191B (zh) 儲熱方法及設備
EP2507563B1 (fr) Tuyau absorbeur
US20160201996A1 (en) PCSM-Based Energy Storage Devices and Methods
EP2314971B1 (fr) Accumulateur thermique doté d'une alimentation en énergie pour un rendement de puissance stable dans le temps et régulier ainsi que son procédé
DE10117027C2 (de) Flüssigkeitsgekühlte Röntgenröhre mit Phasenwechselmaterial(PCM) enthaltenden Mikrokapseln in der Kühlflüssigkeit
EP3969828B1 (fr) Système de stockage de chaleur à haute température dans des centrales électriques
White et al. Phase change salt thermal energy storage for dish stirling solar power systems
DE102012210957A1 (de) Hochtemperatur-Wärmespeicher mit Induktionsheizung und Metallschmelze und Wärmespeicher-Verbundsystem
DE1639004A1 (de) Kernreaktor
EP3260803B1 (fr) Accumulateur de vapeur
Kulkarni et al. Improving efficiency of solar water heater using phase change materials
DE2111689C3 (de) Röntgenröhren-Drehanode
DE102007049385A1 (de) Latentwärmespeicher
DE3401794A1 (de) Stromspeicherbatterie
AT518828B1 (de) Dampfspeicher
DE102011079878A1 (de) Röntgenröhre und Verfahren zu deren Herstellung
DE102019112229A1 (de) Durchlauferhitzer, Vorrichtung mit Durchlauferhitzer und Anlage mit Vorrichtung
Reed et al. New highly thermally conductive thermal storage media
AT518793A1 (de) Dampfspeicher
DE541333C (de) Verfahren und elektrischer Ofen zum Schmelzen von Metallen und Metallegierungen
CN219678703U (zh) 一种固液混合材料分离的加热系统
DE102020107465A1 (de) Be- und entladevorrichtung für einen wärmespeicher, wärmespeicher sowie betriebsverfahren für einen wärmespeicher
DE102014206415A1 (de) Wärmespeicheranordnung und Verfahren zum Betrieb einer solchen
DE102013109048A1 (de) Verfahren und Vorrichtung zur Kühlung von Strahlungsquellen auf Basis eines Plasmas

Legal Events

Date Code Title Description
PUAI Public reference made under article 153(3) epc to a published international application that has entered the european phase

Free format text: ORIGINAL CODE: 0009012

17P Request for examination filed

Effective date: 20110815

AK Designated contracting states

Kind code of ref document: A1

Designated state(s): AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO SE SI SK SM TR

DAX Request for extension of the european patent (deleted)
17Q First examination report despatched

Effective date: 20130923

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN

18D Application deemed to be withdrawn

Effective date: 20160802