• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    A method for determining a state of charge of a latent heat accumulator (1) is proposed, wherein in the latent heat accumulator (1) a phase change material (2) is arranged substantially stationary, wherein at least two positions (3) of the latent heat accumulator (1) a temperature by means of temperature sensors (4) is measured, with the measured temperatures of a computing unit, a temperature field (5) in the phase change material (2) is calculated, and then on the basis of the temperature field (5) a charge state (6) of the latent heat storage (1) is determined.
    公开号:AT518791A4
    申请号:T51140/2016
    申请日:2016-12-14
    公开日:2018-01-15
    发明作者:Ing Tilman Barz Dr
    申请人:Ait Austrian Institute Tech Gmbh；
    IPC主号:
    专利说明:

    The invention relates to a method for determining a state of charge of a latent heat accumulator according to claim 1.
    Latent heat storage are storage for thermal energy, in which the heat is stored in the form of latent energy during a phase change. The determination of the state of charge of a latent heat storage, in particular the question of the still absorbable heat energy, has proven to be difficult.
    A determination of the state of charge can be effected in that the phase change material is in thermal equilibrium with a heat transfer fluid, and is closed by the temperature of the heat transfer fluid to the temperature of the phase change material. The disadvantage of this is that this method is only sufficiently accurate if the amount of heat transfer fluid significantly exceeds the amount of phase change material. In more compact versions of a latent heat storage, this method is therefore insufficient.
    Another way of determining the state of charge can be done by determining parameters such as the pressure, which indicates depending on the state of the phase change material valid for the entire latent heat storage value. A disadvantage of this method, however, is the comparatively increased effort for calibration and the less accurate measurement method.
    The object of the invention is therefore to provide a method of the type mentioned, with which the mentioned disadvantages can be avoided, with which it is possible to determine the state of charge of a latent heat storage simply and with high accuracy.
    This is achieved by the features of claim 1 according to the invention.
    This has the advantage that the state of charge of a latent heat storage can be determined easily and with high accuracy. In this case, due to the measurement of the temperature in a few places, a temperature field can be calculated within the phase change material, and then be closed reliably due to the calculated temperature field on the state of charge. As a result, the state of charge of compact and / or complex latent heat storage in which large differences in the temperature within the phase change material can occur can also be reliably determined. The use of temperature sensors makes the procedure easy to carry out by the measuring technology. Furthermore, the latent heat storage can be quickly loaded and unloaded with heat energy, since the adjustment of an equilibrium does not have to wait to determine the state of charge. Since the state of charge can be determined quickly and reliably, a latent heat storage device monitored by this method can also be used in more complex control systems, in particular in the regulation of the provision of thermal energy in a building, preferably low energy house or passive house, or by industrial process heat, in particular steam networks, thermal oil plants and / or the provision of hot water. As a result, a latent heat storage device monitored by this method can help prevent the generation of heat energy and associated emission of greenhouse gases.
    Furthermore, the invention relates to a latent heat storage according to claim 9.
    The object of the invention is therefore further to provide a latent heat storage of the type mentioned, with which the mentioned disadvantages can be avoided, with which it is possible to determine the state of charge easily and with high accuracy.
    This is achieved by the features of claim 9 according to the invention.
    The advantages of the latent heat storage according to the advantages of the method for determining the state of charge of the latent heat storage.
    The subclaims relate to further advantageous embodiments of the invention.
    It is hereby expressly referred to the wording of the claims, whereby the claims at this point are incorporated by reference into the description and are considered to be reproduced verbatim.
    The invention will be described in more detail with reference to the accompanying drawings, in which only preferred embodiments are shown by way of example. Showing:
    1 shows a first preferred embodiment of a latent heat storage in an axonometric representation.
    FIG. 2 shows an energy balance equation of a heat transfer fluid of the first preferred embodiment of the latent heat accumulator; FIG.
    FIG. 3 is an energy balance equation of an inner wall of the first preferred embodiment of the latent heat accumulator; FIG.
    4 is an energy balance equation of a phase change material of the first preferred embodiment of the latent heat accumulator;
    FIG. 5 shows starting polynomials for the energy balance equations in FIGS. 2 to 4; FIG.
    Fig. 6 is a calculated temperature field for the first preferred embodiment;
    FIG. 7 shows a distribution of a local charge state determined from the temperature field in FIG. 6; FIG.
    Fig. 8 shows an apparent specific heat capacity of a phase change material as a function of temperature;
    FIG. 9 shows a latent portion of the specific heat capacity of FIG. 8; FIG.
    Fig. 10 is an integral of the latent portion of the specific heat capacity of a phase change material of Fig. 9;
    FIG. 11 shows the function of FIG. 10 with a hysteresis effect; FIG.
    12 shows the first preferred embodiment of the latent heat accumulator in an exploded view;
    13 shows a first preferred arrangement of a temperature sensor as a schematic diagram; 14 shows a second preferred arrangement of a temperature sensor as
    Schematic diagram;
    15 shows a third preferred arrangement of a temperature sensor as a schematic diagram; and
    16 shows a fourth preferred arrangement of a temperature sensor as a schematic diagram.
    1 to 16 show preferred embodiments and illustrations of a method for determining a state of charge of a latent heat storage 1. A latent heat storage 1 is a storage for thermal energy, the heat energy is stored mainly in the form of latent heat of reversible thermodynamic state changes. In the method, a charge state of a latent heat accumulator 1 is determined. The state of charge of the latent heat accumulator 1 can be, in particular, a value from which the latent heat energy stored in the latent heat accumulator 1 can be deduced.
    It is provided that in the latent heat storage 1, a phase change material 2 is arranged substantially stationary. Such phase change materials 2 are often referred to as PCM or phase-changing material. Here, a plurality of phase change materials 2 having different phase transformation temperatures are known. Suitable phase change materials 2 may in particular be polymers or salts. Depending on the phase change material 2, the phase transition can take place at exactly one temperature or in one temperature range.
    These state changes can be in particular the phase transition of the phase change material 2 between solid and liquid. The phase transition temperature may in particular be a melting temperature or solidification temperature of the first phase change material 2.
    Alternatively it can be provided that the state change is the transition between two solid phase states of the phase change material 2, in particular a change in the crystal structure, preferably between amorphous and crystalline.
    The substantially stationary arrangement of the phase change material 2 in this context means that the phase change material 2 is sufficiently localized even in a liquid phase state, so that its arrangement for the calculation of a temperature field 5 can be assumed to be static. Here, a heat transfer takes place in the phase change material 2 essentially only by heat conduction, while a heat transfer via convection takes place only locally and is negligible. The substantially stationary arrangement can be achieved in particular by stationary chambers, in which chambers the phase change material 2 is arranged.
    It is further provided that at at least two positions 3 of the latent heat accumulator 1 a temperature is measured by means of temperature sensors 4, with the measured temperatures of a computing unit, a temperature field 5 is calculated in the phase change material 2, and then on the basis of the temperature field 5, a charge state 6 of the latent heat storage. 1 is determined. The at least two positions 3 of the latent heat accumulator 1 are thermally in contact with each other, that is not thermally insulated, so that due to the heat conduction, a heat flow between these at least two positions 3 can form. In particular, it can be provided that the at least two positions 3 are arranged in the same, contiguous phase change material 2. On the basis of the measured temperature at the at least two positions 3, the temperature field 5, that is to say the locally resolved temperature distribution, can then be calculated in the phase change material 2. Due to the temperature field 5, the state of charge 6 of the latent heat accumulator 1 can then be determined.
    This results in the advantage that the state of charge of a latent heat accumulator 1 can be determined easily and with high accuracy. In this case, due to the measurement of the temperature in a few places, a temperature field 5 can be calculated within the phase change material 2, and then closed due to the calculated temperature field 5 reliably to the state of charge 6. As a result, the state of charge 6 of compact and / or complex latent heat storage 1, in which there are large differences of the
    Temperature within the phase change material 2 can be reliably determined. By the use of temperature sensors 4, the method by the measurement technique is easy to carry out. Furthermore, the latent heat storage 1 can be quickly loaded and unloaded with heat energy, since the setting of an equilibrium does not have to wait to determine the state of charge 6. Since the charge state 6 can be determined quickly and reliably, a latent heat storage device 1 monitored by this method can also be used in more complex control systems, in particular in the regulation of the provision of thermal energy in a building, preferably a low energy house or passive house, or industrial process heat, in particular steam networks , Thermal oil systems and / or the provision of hot water. As a result, a latent heat storage device 1 monitored by this method can help prevent the generation of heat energy and associated emissions of greenhouse gases. In particular, the local arrangement of the phase change material 2 can be used for the calculation of the temperature field 5. A model of the shape and position of the phase change material 2 can be stored in particular in the arithmetic unit. For the calculation of the temperature field 5, in particular the caloric data of the phase change material 2 can be used. The caloric data of the phase change material 2 can be stored in particular in the arithmetic unit. The caloric data of the phase change material 2 relate in particular to its specific heat capacity. These caloric data can be taken from data sheets and / or determined experimentally.
    The phase change material 2 of the latent heat accumulator 1 may in particular be homogeneous, ie consist only of a material with the same caloric data.
    Alternatively it can be provided that the phase change material 2 of the latent heat accumulator 1 has a plurality of materials with different caloric data, for example different phase transition temperatures.
    The model of the shape and position of the phase change material 2 in the arithmetic unit can also include the division of the different materials.
    Furthermore, a latent heat accumulator 1 is provided, the substantially stationary phase change material 2 is provided, wherein the temperature sensors 4 are arranged at the at least two positions 3 of the latent heat accumulator 1, wherein the temperature sensors 4 are circuitry connected to the computing unit for determining a state of charge 6 of the latent heat accumulator 1 , wherein for determining the state of charge 6 of the computing unit based on the measured temperatures of the temperature sensors 4, the temperature field 5 is calculated in the phase change material 2, and based on the temperature field 5, the charge state 6 of the latent heat storage 1 is determined.
    The computing unit, which is not shown in the figures, may in particular be electronic, and preferably comprise a processor.
    The arithmetic unit may in particular be arranged separately from the remaining latent heat accumulator 1, and be connected via data cable or radio circuitry with the temperature sensors 4.
    In particular, the arithmetic unit can have a data output unit which transmits data relating to the state of charge 6 by cable and / or by radio. As a result, the data relating to the state of charge 6 can be integrated into a control system.
    In particular, the state of charge 6 of the latent heat accumulator 1 can be used for the regulation of a control system for the provision of heat energy. The control system may in particular be a predictive control system.
    The control system can be used in particular for the provision of heat energy in a building. By accurately determining the state of charge 6 of the latent heat storage device 1, the control system can predict, for example, whether the stored heat energy is sufficient to bridge a period of high energy costs, or whether additional heat energy is needed. As a result, in the sense of intelligent energy systems, the energy consumption can be shifted to times with usually low load, whereby costs and environmental pollution can be kept low.
    Such a control can be used both in the area of a building with private homes but also in industrial plants.
    Furthermore, it can be provided that the arithmetic unit is connected in circuit technology with a display unit.
    According to a preferred embodiment, which is particularly simple, it can be provided that the temperature field 5 between the positions 3 is calculated by linear interpolation. As a result, the computational effort can be kept low, with larger deviations between the calculated temperature field 5 and the reality can be present.
    Particularly preferably, it can be provided that, for the calculation of the temperature field 5, at least for the phase change material 2, an energy balance equation is created. By the energy balance equation of at least the phase change material 2 can be calculated based on the heat conduction and the specific heat capacity, a model for a, the reality modeled temperature field 5 in the phase change material 2, and adapted to the measured temperatures. As a result, a calculation of the temperature field 5 is much more accurate and realistic than with a linear interpolation, or achieved with less temperature sensors 4 an equally high accuracy.
    The latent heat accumulator 1 can in particular be traversed by its own heat transfer fluid 8. The heat transfer fluid 8 is used for supplying and / or dissipating heat energy into or out of the latent heat storage 1. The heat transfer fluid 8 may be in particular water.
    The latent heat storage 1 may further comprise fixed latent heat storage structure elements 11.
    Latent heat storage structure elements 11 are stationary structures within the latent heat accumulator 1, which are thermally conductive, and perform no phase change in the operating temperature range of the latent heat accumulator 1. The latent heat storage structure elements 11 may in particular comprise inner walls between the heat transfer fluid 8 and the phase change material 2 and / or support structures.
    The latent heat storage structure elements 11 may be formed in particular as tubes.
    Preferably, several tubes can be combined to form a tube bundle.
    Furthermore, it can be provided that an energy balance equation is created for the calculation of the temperature field 5 for the heat carrier fluid 8 and / or the latent heat storage structure elements 11. As a result, these boundary conditions can also be included in the calculation of the temperature field 5.
    A preferred procedure for calculating the temperature field 5 will be explained in more detail below with reference to the simple geometry of the first preferred embodiment in FIG. 1. The explanation is made on the basis of the first preferred embodiment, since this is easy to describe due to the simple geometry. By setting up energy balance equations, however, even very complex geometries can be solved numerically, which is why the calculation shown is not limited to simple geometries.
    1 shows the first preferred embodiment of a latent heat accumulator 1 with a hollow cylindrical latent heat storage structural element 11, which serves as a tube for the heat transfer fluid 8, and also forms the inner wall between the heat transfer fluid 8 and the phase change material 2. The latent heat storage structure element 11 has an inner radius η and an outer radius r0. To the latent heat storage structure element 11 is coaxially arranged also the hollow cylindrical phase change material 2, which has the inner radius rG and the outer radius re and the length L. For this simple geometry, the energy balance equations can be given in a cylindrical coordinate system.
    The energy balance equation of the first preferred embodiment for the heat transfer fluid 8 is shown in FIG. 2, wherein the indices H of the thermodynamic quantities relate to the heat transfer fluid 8.
    The energy balance equation of the first preferred embodiment for the
    Latent heat storage structure element 11 is shown in FIG. 3, wherein the indices W of the thermodynamic quantities relate to the latent heat storage structure element 11.
    The energy balance equation of the first preferred embodiment for the phase change material 2 is shown in FIG. 4, wherein the indices P of the thermodynamic quantities relate to the phase change material 2. The apparent specific heat capacity cp can be, in particular, a combination of a sensitive component and a latent component, wherein the latent component can be modeled in particular as a scaled distribution function, for example a Gauss or Weibull distribution.
    For model reduction, preference is given to using a local discretization. As an efficient and therefore preferred variant, a combination of the discretization with finite differences for the heat transfer fluid 8, and the discretization with the method of orthogonal collocation for the latent heat storage structure element 11 and the phase change material 2 has been shown. For the orthogonal collocation, in particular the approach polynomials shown in FIG. 5 can be used.
    FIG. 6 shows an exemplary temperature field 5 for the first preferred embodiment of the latent heat accumulator 1. The latent heat store 1 in this case has twelve temperature sensors 4, the positions 3 being arranged at four different locations along the length and in each case on the inside, middle and outside of the phase change material 2. Numerically, a suitable temperature field 5 for these twelve measured temperatures can then be calculated on the basis of the energy balance equations.
    Alternatively, the temperature field 5 could be determined with temperature sensors 4, which are arranged only along the length. As a result, the number of temperature sensors 4 could be reduced from twelve to four.
    It is preferably provided that for a quasi-continuous determination of the state of charge 6, the temperature field 5 is tracked to the measured temperatures of the temperature sensors 4. Preferably, this can be a dynamic
    State estimators are used, such as a Kalman filter. As a state estimator, a so-called Extended Kalman Filter or an Unscented Kalman Filter can be used with preference. Furthermore, a moving horizon estimator could be used as a state estimator
    Furthermore, a linearization of the energy balance equations for the use of linear estimators can be performed.
    Based on the temperature field 5, the state of charge 6 is then determined.
    It can preferably be provided that the charge state 6 is a ratio of the phase change material 2 in a first phase state to the sum of the phase change material 2 in the first phase state and a second phase state. If the phase change between a solid phase state and a liquid phase state, the state of charge 6 may be in particular the ratio of a liquid phase change material 2 to the sum of solid and liquid phase change material 2. It has been found that such a definition of the state of charge is particularly meaningful and increases linearly with the stored latent heat energy.
    It can preferably be provided that a distribution of a local state of charge 6 is determined on the basis of the temperature field 5. The distribution of a local state of charge 6 can be referred to in particular as a state of charge field. The state of charge 6 can therefore preferably be determined as a state of charge field of the phase change material 2, the local state of charge 6 preferably being determined with the same local resolution as the temperature field 5. The distribution of the local state of charge 6 can be output in particular via the data output unit. In order to determine a global charge state 6 of the entire phase change material 2, the local charge state 6 can be integrated via the volume of the phase change material 2. The distribution of the local state of charge 6 in a temperature field according to FIG. 6 is shown in FIG. 7.
    The provision of the distribution of the local charge state 6 has the advantage over the global charge state 6 that not only the stored heat energy can be determined based on this, but also predictions can be made as to how a loading or unloading process of the latent heat storage device 1 will take place. For example, when the phase change material 2 is melted mainly on a side of the phase change material 2 facing the heat transfer fluid 8, more heat energy can be dissipated in a short global period of time, such as a uniform distribution of the local state of charge 6 and therefore also of the latent heat energy in the entire phase change material 2. This allows the control system to detect how the current charge state 6 a loading or unloading process will take place, and in particular whether the required heat energy for a process from the latent heat storage 1 can be completely removed, or if an additional generation of heat energy necessary is.
    Particularly preferably, it can be provided that the temperature field 5 is recalculated at predeterminable time intervals. Such a regular recalculation of the temperature field 5 can also be called quasi-continuous.
    The predefinable time interval may be in particular between 1 hour and 1 second, in particular between 10 minutes and 10 seconds, wherein the predeterminable time interval may depend in particular on the size of the latent heat accumulator 1.
    Preferably, it can further be provided that a temporal change of the calculated temperatures is created by a comparison of the temperature field 5 with the preceding temperature field 5.
    Particularly preferably, it can be provided that a temporal change of the measured temperatures of the arithmetic unit for calculating the temperature field 5 in the phase change material 2 is used. Thus, two physical measured variables are available per temperature sensor 4, which can be used for comparison with the calculated temperature field 5, namely the temperature per se but also the temporal change, ie dissipation, of the temperature. This doubles for a constant number
    Temperature sensor 4, the measured values, which are available for the calculation of the temperature field 5, whereby the calculated temperature field 5 can be calculated with an even lower error, or a similar accuracy with less temperature sensors 4 can be achieved.
    When determining the state of charge 6, the temperature-dependent behavior of the phase change material 2 can be taken into account, which is preferably present as caloric data.
    FIG. 8 shows by way of example the apparent specific heat capacity cp of a phase change material 2 as a function of the temperature at which the phase transition takes place within a temperature range.
    In Fig. 9, the latent portion Φ of the heat capacity is shown, which corresponds to the hatched area in Fig. 8.
    FIG. 10 shows an integral representation of the latent component Φ of the heat capacity, which is normalized to 1 and which corresponds to the state of charge 6. The ordinate axis is labeled soc for "state of charge". The function shown in FIG. 10 represents an ideal state, which is bijective and therefore can be directly deduced from a temperature to a state of charge.
    In reality, this direct relationship is often not immediately given, but the phase change from the first phase state to the second phase state often follows a different curve than the reverse phase change, as exemplified in Fig. 11, or delayed in time. Such hysteresis-like effects are often caused by overheating or undercooling of the phase change material 2. Furthermore, a phase transformation does not occur abruptly in reality, but only after a certain time, for example because crystal growth takes a certain amount of time.
    In particular, it can be provided that for the determination of the state of charge 6 on the basis of the temperature field 5, a previous state of charge 6 of the phase change material 2 is included. The preceding charge state 6 is in this case a charge state 6 already determined in a previous measurement. In a quasi-continuous operation, the preceding charge state 6 may preferably be the immediately preceding charge state 6, that is to say last. As a result, in the determination of the charge state 6, the time profile of the change in the charge state 6, and thus also a time-dependent or direction-dependent behavior of the phase change material 2 can be taken into account. The temporal or direction-dependent behavior of the phase change material 2 can be present as part of the caloric data of the phase change material 2, in particular be stored. As a result, the determination of the state of charge 6 can also be improved in a simple manner and without additional sensors.
    Particularly preferably, both the previous charge state 6 and the temporal change of the temperature field 5 can be included for the determination of the charge state 6. This allows a particularly accurate determination of the state of charge 6.
    Preferably, it can further be provided that a heat input into the latent heat accumulator 1 and a heat dissipation from the latent heat accumulator 1 are measured and used by the arithmetic unit for calculating the temperature field 5 in the phase change material 2. The heat supply and the heat dissipation can be carried out in particular by means of the heat transfer fluid 8.
    By measuring the heat input into the latent heat storage 1 and a heat dissipation from the latent heat storage 1, the accuracy of the calculation can be easily improved.
    In the latent heat storage 1 can be provided that the latent heat storage 1 has an inlet 10 and an outlet for a heat transfer fluid 8, and that a sensor for determining the supplied heat energy and the heat energy removed is arranged at the inlet 10 and the outflow. The sensors for determining the heat energy supplied and the heat energy removed can in particular have a flow sensor and a further temperature sensor for measuring the temperature of the heat transfer fluid 8.
    It can preferably be provided that the latent heat store 1 is less than 40, in particular less than 20, particularly preferably less than 10,
    Temperature sensors 4 has. In this case, the temperature would be measured at less than 40, in particular less than 20, more preferably less than 10, positions 3. As a result, the number of required temperature sensors 4 can be kept at an economically reasonable low number.
    Furthermore, it can be provided that the latent heat accumulator 1 has more than 3, preferably more than 5, temperature sensors 4.
    In particular, it can be provided that at least 2 of the temperature sensors 4 have a substantially immediate contact with the phase change material 2. The substantially direct contact means in this context that between the temperature sensor 4, or its sensor, and the phase change material 2, only a good heat-conducting separating layer can be arranged. As a result, the most immediate possible measurement of the temperature of the phase change material 2 can take place.
    Furthermore, it can be provided that the temperature sensors 4 are arranged in an outer shell of the latent heat accumulator 1. As a result, a subsequent retrofitting existing latent heat storage 1 is possible.
    The temperature sensors 4 may be arranged in the phase change material 2 according to the specification of the optimal support points of the selected approach polynomials. In particular, the determination of the positions 3 can take place after evaluation of the orthogonality conditions of the batch polynomials. This determination has to be made during the construction of the latent heat accumulator 1.
    FIGS. 13 to 16 show some preferred embodiments of the arrangement of temperature sensors in the case of some common geometry components of latent heat store 1.
    FIG. 13 shows a plate heat exchanger arrangement with phase change material 2 overflowed on both sides. The arrangement of the temperature sensors 4 can in this case be effected in particular in the middle of the phase change material 2.
    FIG. 14 shows a plate heat exchanger arrangement with a phase change material 2 flowed over on one side, wherein an insulating material 12 is located on a side facing away from the heat carrier fluid 8. Here, the temperature sensors 4 may be arranged in particular at the transition from the phase change material 2 to the insulating material 12, since heat removal via the insulating material 12 is usually negligible.
    FIG. 15 shows a tube heat exchanger arrangement with a jacket made of a phase change material 2. In this case, the temperature sensors 4 can be arranged centrally in the phase change material 2.
    In Fig. 16, a shell and tube heat exchanger assembly having a plurality of tube heat exchanger assemblies as shown in Fig. 15 is shown. Here, the temperature sensors 4 may be arranged at the contact points of the individual tubes with each other.
    In particular, it can be provided that the phase change material 2 for the calculation of the temperature field 5 along a flow direction 7 of a heat transfer fluid 8 is divided into several sectors 9, and that only one measured temperature per sector 9 is used for the calculation of the temperature field 5. In the case of the latent heat accumulator, it may be provided that the temperature sensors 4 are arranged along a flow direction 7 of the heat transfer fluid 8. Preferably, a balance segmentation of the latent heat accumulator 1 along the flow direction 7 of the heat transfer fluid 8 takes place. Thus, the number of temperature sensors 4 and the associated metrological effort can be kept low. An exemplary approach for segmenting the latent heat accumulator 1 along the flow direction 7 with the arrangement of the temperature sensors 4 is shown in FIG. 12.
    Furthermore, it can be provided that one of the temperature sensors 4 has a plurality of measuring sensors, wherein the measured temperature of the temperature sensor 4 is an average of measured values of the measuring sensors. The probes can be arranged at different locations where the same temperature can be expected. The measured value of the sensors is then averaged to determine the measured temperature. By such an arrangement, any measurement errors of the individual probes can be reduced.
    权利要求:
    Claims (12)
    [1]
    1. A method for determining a state of charge of a latent heat accumulator (1), wherein in the latent heat accumulator (1) a phase change material (2) is arranged substantially stationary, wherein at least two positions (3) of the latent heat accumulator (1) a temperature by means of temperature sensors (4 ) is measured, with the measured temperatures of a computing unit, a temperature field (5) in the phase change material (2) is calculated, and then on the basis of the temperature field (5) a charge state (6) of the latent heat storage (1) is determined.
    [2]
    2. The method according to claim 1, characterized in that for calculating the temperature field (5) at least for the phase change material (2) an energy balance equation is created.
    [3]
    3. The method according to claim 1 or 2, characterized in that the state of charge (6) is a ratio of the phase change material (2) in a first phase state to the sum of the phase change material (2) in the first phase state and a second phase state.
    [4]
    4. The method according to any one of claims 1 to 3, characterized in that on the basis of the temperature field (5) a distribution of a local state of charge (6) is determined.
    [5]
    5. The method according to any one of claims 1 to 4, characterized in that a temporal change of the measured temperatures of the arithmetic unit for calculating the temperature field (5) in the phase change material (2) is used.
    [6]
    6. The method according to any one of claims 1 to 5, characterized in that for the determination of the state of charge (6) based on the temperature field (5) a previous state of charge (6) of the phase change material (2) is included.
    [7]
    7. The method according to any one of claims 1 to 6, characterized in that a heat input into the latent heat storage (1) and a heat dissipation from the latent heat storage (1) measured, and by the arithmetic unit for calculating the temperature field (5) in the phase change material (2 ) is used.
    [8]
    8. The method according to any one of claims 1 to 7, characterized in that the phase change material (2) for the calculation of the temperature field (5) along a flow direction (7) of a heat transfer fluid (8) into a plurality of sectors (9) is divided, and that only one measured temperature is used per sector (9) for the calculation of the temperature field (5).
    [9]
    9. latent heat accumulator (1) comprising a substantially stationary arranged phase change material (2), wherein at least two positions (3) of the latent heat accumulator (1) temperature sensors (4) are arranged, wherein the temperature sensors (4) circuitry with a computing unit for determining a charge state (6) of the latent heat accumulator (1) are connected, wherein for determining the state of charge (6) from the computing unit based on measured temperatures of the temperature sensors (4) a temperature field (5) in the phase change material (2) calculated, and based on the temperature field (5) a charge state (6) of the latent heat storage (1) is determined.
    [10]
    10. Latent heat store (1) according to claim 9, characterized in that the latent heat store (1) has an inflow (10) and an outflow for a heat transfer fluid (8), and that the inflow (10) and the outflow, a sensor for determining a supplied heat energy and a dissipated heat energy is arranged.
    [11]
    11. Latent heat store (1) according to claim 9 or 10, characterized in that the temperature sensors (4) along a flow direction (7) of a heat transfer fluid (8) are arranged.
    [12]
    12. Latent heat store (1) according to one of claims 9 to 11, characterized in that one of the temperature sensor (4) has a plurality of sensors, wherein the measured temperature of the temperature sensor (4) is an average of measured values of the sensor.
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    同族专利:
    公开号 | 公开日
    ES2834052T3|2021-06-16|
    EP3336473B1|2020-09-02|
    AT518791B1|2018-01-15|
    EP3336473A1|2018-06-20|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US20140124158A1|2011-07-12|2014-05-08|Sharp Kabushiki Kaisha|Cooling equipment, temperature control system, air conditioning system, and hot water supply system for the same|
    DE202012103718U1|2012-09-27|2013-01-03|Viessmann Kältetechnik AG|Device for determining the state of charge of a segmented thermal storage|
    US20140158340A1|2012-12-11|2014-06-12|Caterpillar Inc.|Active and passive cooling for an energy storage module|
    CH708711A1|2013-10-10|2015-04-15|Rep Ip Ag|Isolation time determining device for a heat-insulating container.|US10955151B2|2018-09-25|2021-03-23|Syracuse University|Cooling charge determination for a local thermal management system|
    CN111649613A|2020-04-27|2020-09-11|北京林业大学|Device for recovering and measuring waste gas and waste heat in wood or/and wood veneer thermal processing process|
    CN111504516B|2020-04-27|2021-10-22|北京林业大学|Method for measuring waste heat of recovered waste gas in thermal processing process of wood or/and wood veneer|
    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    ATA51140/2016A|AT518791B1|2016-12-14|2016-12-14|METHOD FOR DETERMINING A CHARGING STATE OF A LATENT HEAT STORAGE|ATA51140/2016A| AT518791B1|2016-12-14|2016-12-14|METHOD FOR DETERMINING A CHARGING STATE OF A LATENT HEAT STORAGE|
    ES17200136T| ES2834052T3|2016-12-14|2017-11-06|Procedure for determining a state of charge of a latent heat store|
    EP17200136.4A| EP3336473B1|2016-12-14|2017-11-06|Method for determining the charge level of a latent heat storage device|
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