WO2016008766A1 - Material für ein thermoelektrisches element und verfahren zur herstellung eines materials für ein thermoelektrisches element - Google Patents
Material für ein thermoelektrisches element und verfahren zur herstellung eines materials für ein thermoelektrisches element Download PDFInfo
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- WO2016008766A1 WO2016008766A1 PCT/EP2015/065470 EP2015065470W WO2016008766A1 WO 2016008766 A1 WO2016008766 A1 WO 2016008766A1 EP 2015065470 W EP2015065470 W EP 2015065470W WO 2016008766 A1 WO2016008766 A1 WO 2016008766A1
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- atoms
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- C04B2235/76—Crystal structural characteristics, e.g. symmetry
- C04B2235/768—Perovskite structure ABO3
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- C04B2235/00—Aspects relating to ceramic starting mixtures or sintered ceramic products
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- C04B2235/70—Aspects relating to sintered or melt-casted ceramic products
- C04B2235/74—Physical characteristics
- C04B2235/78—Grain sizes and shapes, product microstructures, e.g. acicular grains, equiaxed grains, platelet-structures
- C04B2235/786—Micrometer sized grains, i.e. from 1 to 100 micron
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- C04B2235/00—Aspects relating to ceramic starting mixtures or sintered ceramic products
- C04B2235/70—Aspects relating to sintered or melt-casted ceramic products
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- C04B2235/00—Aspects relating to ceramic starting mixtures or sintered ceramic products
- C04B2235/70—Aspects relating to sintered or melt-casted ceramic products
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Definitions
- thermoelectric element Material for a thermoelectric element and method for producing a material for a thermoelectric
- thermoelectric element It is a material for a thermoelectric element and a method for producing a material for a thermoelectric element and a method for producing a material for a thermoelectric element
- thermoelectric element specified is an electron conductor based on a
- complex metal oxide in particular a ceramic.
- thermoelectric conversion is an attractive way to increase the overall efficiency of energy supply and can contribute to the reduction of C02 _ production.
- thermoelectric efficiency of a thermoelectric material To describe the thermoelectric efficiency of a thermoelectric material
- the dimensionless quality factor ZT can be used. This results from
- thermoelectric conversion material which can be used as a thermoelectric conversion material. It is an object, an improved material for a thermoelectric element and an improved method for producing a material for a thermoelectric
- a material for a thermoelectric element comprises calcium-manganese oxide, preferably of the general formula CaMnO 3.
- the calcium-manganese oxide has partially doped with Fe atoms on sites of Mn atoms.
- the material is in a perovskite crystal structure, which is defined by the general
- A represents the A-sites and B represents the B-sites of the perovskite lattice.
- the A-sites are predominantly occupied by Ca2 + atoms and the B sites predominantly by Mn ⁇ + atoms.
- Fe atoms are doped, parts of the B sites are occupied by Fe ⁇ + atoms. This corresponds to an "isovalent" doping without donor effect.
- the doping with Fe atoms is present in a proportion z with z ⁇ 20%. This means that up to 20% of the Mn sites in the lattice, especially the B sites in the perovskite lattice, are occupied by Fe ⁇ + atoms.
- the proportion can be in the range of 0.01% to 20%.
- the material is preferably of the "n-type." In the case of an "n-type” material, electrons are present as charge carriers. In a “p-type” material holes are present as charge carriers.
- partially Ca atoms in the material are replaced by other atoms in order to further improve the material properties.
- the material has a partially doped with an element which Ca ⁇ "is replaced in the crystal lattice and providing electrons for the electrical conductivity.
- the member of a group is selected, from the rare earth metals, Sb3 + and Bi + 3.
- the group consists of Y 3+, Sc 3+, La 3+, Nd 3+, Gd 3+, Dy 3+, Yb 3+, Ce 4+, Sb 3+ and Bi 3+ .
- the doping with the element Ca ⁇ is replaced in the crystal lattice and providing electrons for the electrical conductivity in a proportion y with 0% ⁇ y -S 50% before.
- y 0% ⁇ y -S 50% before.
- the material has a partial doping with a divalent element at the sites of Ca 2+ atoms.
- the divalent element is selected from a group consisting of Mg 2+ , Sr 2+ , Ba 2+ , Zn 2+ , Pb 2+ , Cd 2+ and Hg 2+ .
- Sr 2+ is used.
- the doping is with the bivalent
- the calcium-manganese oxide is described by the general formula CaMnO n , where n is the
- n ⁇ 2 holds.
- n ⁇ 3 or n 3.
- the material is described by the following general formula:
- DON element that can replace Ca ⁇ " in the crystal lattice and electrons for electrical conductivity
- x, y, z and n may be selected as described above.
- x, y, z and n are in the
- Proportion of ISO 0 ⁇ x ⁇ 0.5, in particular 0.05 ⁇ x ⁇ 0.20 proportion of DON: 0 ⁇ y ⁇ 0.5, in particular 0.01 ⁇ y ⁇ 0.10 proportion of Fe: 0, 0001 ⁇ z ⁇ 0.2
- the material preferably contains no or only small amounts of expensive or toxic elements.
- the material is free of selenium and telur.
- thermoelectric element comprising the material described above.
- the thermoelectric element is used, for example, as a generator.
- two conductors made of different materials are electrically
- a leader can be any leader that can be connected with each other.
- a leader can be any leader that can be used to connect to each other.
- N-type material and the other conductor have a p-type material.
- the n-type material used herein is the doped calcium-manganese oxide described herein.
- the materials are designed as rod-shaped or disc-shaped components.
- the thermoelectric element additionally comprises a p-type material.
- a sodium cobaltate is suitable for this purpose.
- the material is based on a composition described by the formula (Ca 3 - x Na x ) ⁇ o 4 ⁇ 9 - ⁇ , with 0.1 ⁇ x ⁇ 2.9 and 0 ⁇ ⁇ ⁇ 2, in particular 0.3 ⁇ x ⁇ 2 , 7 and 0 ⁇ ⁇ 1. It has been found that such a material has a high
- thermoelectric Thermo-power and high conductivity.
- multiple thermoelectric In one embodiment, multiple thermoelectric
- Interconnecting elements to a module. At least one
- thermoelectric element has the above-described
- the material is in a simple manner with
- thermoelectric element specified the material described above can be produced by the process become. All properties disclosed in relation to the material are also disclosed accordingly in relation to the method and vice versa, even if the respective property is not explicitly mentioned in the context of the respective aspect.
- the method can also be used for producing another material for a thermoelectric element.
- it may be a material based on calcium manganese oxide, which has no doping with Fe atoms.
- the method comprises a firing process, wherein the maximum temperature in the firing process is just below the melting point of the material. For example, the maximum applies
- T max Tg - 75 ° C, where Tg denotes the melting temperature of the material.
- Tg denotes the melting temperature of the material. The maximum temperature should be chosen so that no melting of the
- the maximum temperature is at least 10 ° C below the melting temperature. Due to the high firing temperature can be a good growth of
- Polycrystals are achieved.
- the number of grain boundaries per can be determined by the high firing temperature
- the temperature is maintained for several hours, for example for at least 10 hours, in the range indicated above.
- Oxygen sintered for example, sintered in air or with an additional enrichment with oxygen. Furthermore, the method has a slow cooling rate. In particular, a cooling rate of less than or equal to 2 ° C / min, preferably less than or equal to l ° C / min is used.
- an additional holding time of at least 30 minutes, preferably of at least one hour, is preferably maintained during cooling, in particular in the range from 1000 ° C. to 600 ° C.
- the temperature during the hold time is in a range of 700 ° C to 800 ° C, for example, 750 ° C.
- This additional hold time allows the most complete re-oxidation of Mn ⁇ + to Mn ⁇ + and improves the thermoelectric properties, such.
- Figure 1 is a diffractogram of a material for a
- thermoelectric element Figure 2 is a diagram of the electrical conductivity in
- FIG. 3 shows a microstructure of a material
- FIG. 4 shows a diagram of the electrical conductivity in FIG.
- FIG. 5 is a diagram of the Seebeck coefficient in FIG.
- FIG. 6 shows a diagram of the thermal conductivity as a function of the temperature for the material from FIG. 4, FIG.
- FIG. 7 shows a graph of the quality factor as a function of the temperature for the material from FIG. 4,
- FIG. 8 shows a diagram of the thermal conductivity as a function of the temperature for two further materials
- FIG. 9 shows a diffractogram of two materials
- FIG. 10 shows a diagram of the sintering density as a function of
- FIG. 11 is a diagram of the Seebeck coefficient in FIG. 11
- FIG. 12 shows a diagram of the sintering density as a function of
- FIG. 13 is a diagram of the Seebeck coefficient in FIG. 13
- Figure 14 shows an embodiment of a thermoelectric generator having a plurality of thermoelectric elements.
- thermoelectric element First, a method for producing a material for a thermoelectric element will be described.
- the method is a material of
- thermoelectric elements Material limited, but is also suitable for the production of other materials for thermoelectric elements.
- the material in particular a complex metal oxide, can be produced, for example, by the so-called “mixed-oxide” technique, although others can also be used
- Manufacturing process can be applied, for. As wet-chemical routes or mechanical alloying.
- complex metal oxide is carried out, for example, at 1100 ° C in air for several hours. It will
- FIG. 1 shows an X-ray diffractogram (XRD) for the
- Embodiment There are plotted against the angle between the radiation source, sample and detector (20-angle), the measured radiation intensities I ⁇ . From a
- components are molded by dry pressing.
- rod-shaped or cylindrical components are needed.
- thermal debinding it is advantageous to first decarburize the parts (thermal debinding). It has been found that the burning of the components for the shaping of the
- thermoelectric properties of the described material is of great importance.
- the sintering density measurements were carried out on a cylindrical component having a diameter of 11 mm and a height of 5.5 mm. The measurements for the electrical
- the optimized combustion process developed is ⁇ below for the materials Cap r, ⁇ ⁇ ⁇ f Q5MnÜ3 and Cap r r gsGdp Q5Mn03 exemplified.
- the process is not limited to these materials but has been successfully used in the preparation of all complex metal oxide formulations studied.
- a particularly high maximum combustion temperature is used.
- the maximum firing temperature should be below the melting point, otherwise it will melt and destroy the
- the firing temperature is just below the melting temperature of the material used.
- the maximum firing temperature T max at 100 ° C below the embarkschmelztemperatur Tg or above, ie Tmax ⁇ Tg - 100 ° C.
- Tmax ⁇ Tg - 75 ° C for example, Tmax ⁇ Tg - 50 ° C.
- the firing temperature is at least 10 ° C below the Aufschmelztemperatur, ie, Tmax ⁇ Tg - 10 ° C.
- the firing temperature is in a range of 10 ° C to 50 ° C below the melting temperature.
- the melt temperature is about 1400 ° C.
- the process has a very long hold time at the maximum temperature.
- the process has a very long hold time at the maximum temperature.
- Holding time at least 10 h.
- the holding time is at least 15 h.
- Oxygen sintered for example, sintered in air or with an additional enrichment with oxygen.
- the method has a slow cooling rate.
- a cooling rate of less than or equal to 1 ° C / min is used.
- an additional hold time of at least one hour is preferably used when cooling from 1000 ° C to 600 ° C.
- the slow cooling rate and additional hold time allow the most complete conversion of reduced Mn3 + in Mn ⁇ +, so that a possible stoichiometric compound is obtained with particularly good thermoelectric properties. This is the falling below a certain temperature necessary.
- the rate of diffusion of the oxygen required in the ceramic decreases.
- this temperature is in the range of 700 ° C to 800 ° C, z. At 750 ° C.
- the oxygen uptake is associated with phase transformations in which the brittle ceramic can easily crack.
- a slow cooling rate in the area of phase transformation and below makes it possible to produce a crack-free or low-crack ceramic.
- the material in air is up to high
- Figure 2 shows a graphical representation of the electrical conductivity o as a function of the maximum
- Firing temperature T max for both formulations.
- the electrical conductivity shows a nearly linear dependence on the maximum firing temperature.
- FIG. 3 shows the microstructure achieved during sintering
- Grain diameter can be attributed, since only a small scattering of the charge carriers at the grain boundaries
- thermoelectric conversion in particular the following properties are relevant.
- Thermo power -125 yV / K
- thermoelectric conversion in particular the dependence of the properties on the ambient temperature is of interest.
- the ends of a thermoelectric component are at different temperature levels.
- FIG. 4 shows the temperature dependence of the electrical conductivity ⁇ for the Ca Q f g7 La Q f Q 3 MnO 3 ceramic.
- the electrical conductivity ⁇ increases with increasing
- FIG. 5 shows the temperature dependence of the Seebeck coefficient for the two components. Here an increase of the absolute value with increasing temperature is to be observed.
- FIG. 6 shows the temperature dependence of
- Thermal conductivity was measured by a laser flash method. The thermal conductivity increases with increasing
- FIG. 7 shows the profile of the quality factor ZT, measured on the two components of the Ca Q f g 7 La Q f Q 3 MnO 3 ceramic.
- the quality factor reflects the efficiency of the thermoelectric conversion.
- Element cell of the perovskite structure should thereby increase the density of the material and the thermal conductivity can be reduced.
- Thermo power (Seebeck coefficient) -101 yV / K
- thermo-power the improved electrical conductivity is compensated by the reduced thermo-power, so that the power factor is about the same remains.
- FIG. 8 shows the temperature dependence of
- thermoelectric conversion The three examples show that structures with increased density and reduced thermal conductivity can improve the efficiency of the thermoelectric conversion. It would be expected that this effect by further or complete replacement of Ca2 + atoms by specific
- Efficiency can be achieved by the incorporation of suitable, specifically even heavier atoms than Sr ⁇ +.
- suitable, specifically even heavier atoms than Sr ⁇ + for example, Ba 2 " and Pb 2+ are suitable for this purpose.
- Example Ca 0f 85 Sr 0f IQXQ, 0 5M1 1 _ 7 Fe 7 Q ⁇ (X Dy, Bi)
- a material on the basis of CaMnC> 3 having a doping with Fe atoms, which take the place of Mn atoms a material is characterized in the following, by the formula Ca Q ⁇ 85Sr Q ⁇ ] _Q XQ ⁇ Q 5Mn ] __ z Fe z C> 3, where X is Dy or Bi.
- some of the Mn atoms in the B sites are exchanged by Fe atoms.
- the majority (> 80%) of the B-sites are occupied by Mn atoms. This leaves the for the
- thermoelectric conversion advantageous crystal structure and stability of manganate compound largely retained.
- FIG. 11 shows the dependence of the Seebeck coefficient on the Fe content z in this material. It was at
- Thermoregulator has a negative sign up to about 10% Fe (material is "n-type") and up to 5%
- thermoelectric conversion can be optimized. It has been found that a material having an Fe content in the range of 0.0001 to 0.2 has advantageous properties. With an Fe content of z> 0.2, the electronic conductivity is only very low.
- thermopower has a negative sign (material is "n-type").
- thermoelectric power increases in an advantageous manner.
- Figure 14 shows an embodiment of a
- thermoelectric element 1 thermoelectric element 1, in particular one
- thermoelectric generator thermoelectric generator
- the generator has a so-called ⁇ structure.
- the generator is designed as a module comprising a plurality of materials 2, 3 of different types.
- the materials 2, 3 form the legs of the generator.
- the first material 2 is of the n type and is based on calcium manganese oxide as described above.
- the second material 3 is p-type.
- the two materials 2, 3 have comparable Q factors. In this case, a particularly good energy conversion can be achieved overall.
- the legs having the materials 2, 3 are thermally connected in parallel and electrically in series.
- For electrical wiring contacts 6 are provided, which are formed for example from an Ag paste.
- the generator has two electrical connections 4, 5.
- thermal contact elements 7, 8 are present, which simultaneously form electrical insulation.
- AI2O3, A1N and / or S13N4 is used for this purpose.
- the materials 2, 3 are sintered together with the electrical contacts 6 and the thermal contact elements 7, 8.
- Connections 4, 5 a voltage, the so-called thermoelectric generated.
- thermoelectric element in particular a
- thermoelectric generator only two legs with different materials 2, 3 on. Reference sign list
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Abstract
Description
Claims
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US15/327,012 US20170158563A1 (en) | 2014-07-17 | 2015-07-07 | Material for a Thermoelectric Element and Method for Producing a Material for a Thermoelectric Element |
EP15741952.4A EP3169644A1 (de) | 2014-07-17 | 2015-07-07 | Material für ein thermoelektrisches element und verfahren zur herstellung eines materials für ein thermoelektrisches element |
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DE102017216990B4 (de) * | 2017-09-25 | 2019-05-02 | Michael Bittner | Thermoelektrische Oxidkeramik und Verfahren zu ihrer Herstellung |
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PARK ET AL: "Moessbauer Studies of Perovskite La0,67Ca0,33Mn1-xFe1O3", MATERIALS SCIENCE FORUM, TRANS TECH PUBLICATIONS LTD- SWITZERLAND, CH, vol. 373-376, 10 June 2000 (2000-06-10), pages 565 - 568, XP009186517, ISSN: 0255-5476 * |
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ZAJAC T ET AL: "Electron spin resonance in iron-substituted manganites La0.67Ca0.33Mn1-xFexO3", JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS, ELSEVIER SCIENCE PUBLISHERS, AMSTERDAM, NL, vol. 272-276, 1 May 2004 (2004-05-01), pages 120 - 121, XP004516028, ISSN: 0304-8853, DOI: 10.1016/J.JMMM.2003.11.057 * |
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US20170158563A1 (en) | 2017-06-08 |
JP6426824B2 (ja) | 2018-11-21 |
DE102014110065A1 (de) | 2016-01-21 |
JP2017528905A (ja) | 2017-09-28 |
EP3169644A1 (de) | 2017-05-24 |
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