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1.
A Standard Reference Material (SRM) for the Seebeck coefficient is critical for inter-laboratory data comparison and for instrument calibration. To develop this SRM, we have conducted an international round-robin measurement survey of two candidate materials—undoped Bi2Te3 and constantan (55% Cu and 45% Ni alloy). Measurements were performed in two rounds by twelve laboratories involved in active thermoelectric research using a number of commercial and custom-built measurement systems and techniques. We report the results of these measurements and the statistical analysis performed. Based on this extensive study, we have selected Bi2Te3 as the prototype standard material.  相似文献   

2.
We investigated the influence of negative pressure on the electrical conductivity, the Seebeck coefficient, and the power factor of Sb2Te3. We performed first-principles calculations with the linearized-augmented plane-wave method considering negative hydrostatic pressure in the range from zero to −2 GPa and doping for electrons and holes up to 1020 cm−3. Our results predict a significant increase of the Seebeck coefficient and the power factor under negative pressure for certain doping concentrations.  相似文献   

3.
Doubly substituted polycrystalline compound bulk samples of BaxAgyCa2.8Co4O9 were prepared via citrate acid sol-gel method followed by spark plasma sintering. The phase composition, orientation, texture and high temperature electrical properties were systematically investigated. The results showed that the orientation and the texture could be modified by altering ratio of Ba to Ag. The resistivity and the Seebeck coefficient of substituted samples were decreased by decreasing Ba/Ag ratio except for that of Ba0.1Ag0.1Ca2.8Co4O9 sample with lowest electrical resistivity (7.2 mΩ cm at 973 K), moderately high Seebeck coefficient (172 μV/K at 973 K) and improved power factor (0.42 mW/mK2 at 973 K).  相似文献   

4.
We have developed a high-throughput thermoelectric screening tool for the study of combinatorial thin films. This tool consists of a probe to measure resistance and Seebeck coefficient on an automated translation stage. A thin film library of the (Ca1−xySrxLay)3Co4O9 ternary system has been fabricated on a Si (1 0 0) substrate, using combinatorial pulsed laser deposition by the natural-composition-spread method. We have demonstrated successful mapping of the resistance and Seebeck coefficient of this film library. The mapping indicates that the substitution of La for Ca results in an increase of both resistance and Seebeck coefficient, and that of Sr results in a decrease of resistance. The screening tool allows us to measure 1080 data points in 6 h.  相似文献   

5.
Electrical resistivity and thermoelectric power (TEP) have been measured in polycrystalline sample of CeNi0.75Co0.25Al4. The magnetization measurements have been performed in oriented powder with a-axis of the crystallites parallel to the external magnetic field. All the data have been compared with its parent compound CeNiAl4. In the range 120-300 K, the Seebeck coefficient is significantly higher for alloy than for the parent material and exhibits a peak at ∼150 K. R(T)/R(300) follows a logarithmic temperature dependence for all samples above 100 K, and rapidly decreases as the temperature is lowered. The decrement is much faster in the cobalt doped samples than in the parent compound, suggesting stronger electronic correlations in the former. Inverse magnetic susceptibility in oriented powder follows a Curie-Weiss law above 100 K and shows peff=2.7 slightly higher than that of the free Ce3+ ion value of 2.5.  相似文献   

6.
Discrete phase libraries of thermoelectric compounds, MgxSiyGe1−y, were fabricated by a combinatorial pulsed laser deposition followed by annealing as a thin film form on an integrated ceramic substrate. In the substrate are embedded four probe electrical contacts to each sample, lead wires and pads to be accessed by needle probes. Resistivity and Seebeck coefficient were evaluated electrically, while temperature difference was locally given to each sample by a local heater also embedded in the substrate. The sample temperature (300-673 K) was controlled by a heating stage and temperature difference at the two contact points for each sample was evaluated by an infrared camera. The dependences of polarity and absolute values of Seebeck coefficient on the composition agree well with the data in literature.  相似文献   

7.
A new compound UPd2Sb was prepared and studied by means of X-ray diffraction, magnetization, electrical resistivity, magnetoresistivity, thermoelectric power and specific heat measurements. The phase crystallizes with a cubic structure of the MnCu2Al-type (s.g. ). It orders antiferromagnetically at TN=55 K and exhibits a modified Curie-Weiss behaviour with reduced effective magnetic moment at higher temperatures. The electrical resistivity behaves in a manner characteristic of systems with strong electronic correlations, showing Kondo effect in the paramagnetic region and Kondo-like response to the applied magnetic field. The Seebeck coefficient exhibits a behaviour expected for scattering of conduction electrons on a narrow quasiparticle band near the Fermi energy. The low-temperature electronic specific heat in UPd2Sb is moderately enhanced being about 81 mJ/mol K2.  相似文献   

8.
La1−xCaxMnO3+δ (0.0?x?1.0) samples were prepared and their resistivity and Seebeck coefficients were measured in the high-temperature range. Ca doping changes the ratio of Mn3+/Mn4+ and influences the electronic transport behavior markedly. With the increase of Ca concentration, the samples change from a p-type semiconductor to an n-type one and Seebeck coefficient becomes increasingly negative. Low doping (x=0.2) and high doping (x=0.8) induces the drop of the resistivity compared with undoped LaMnO3+δ and CaMnO3+δ samples due to the rise of carrier concentration. However, the resistivity of moderate-doped samples (x=0.4, 0.6) is larger than low- and high-doped samples because dopant scattering decreases carrier mobility.  相似文献   

9.
Bi85Sb15−xPrx (x=0,1,2,3) alloys with partial substitution of Pr for Sb were synthesized by mechanical alloying followed by high-pressure sintering. The crystal structure was characterized by X-ray diffraction. The electrical conductivity and Seebeck coefficient were measured in the temperature range of 80–300 K. The results show that the electrical conductivity and Seebeck coefficient of Pr-substituted samples are both larger than those of the reference sample, Bi85Sb15, in the whole measurement temperature range. The power factor of Bi85Sb13Pr2 reaches a maximum value of 3.83×10−3 W K−2 m−1 at 235 K, which is about four times larger than that of the reference sample, Bi85Sb15, at the same temperature.  相似文献   

10.
The electrical conductivity, Seebeck coefficient, and Hall coefficient of three-micron-thick films of amorphous Ge2Sb2Te5 have been measured as functions of temperature from room temperature down to as low as 200 K. The electrical conductivity manifests an Arrhenius behavior. The Seebeck coefficient is p-type with behavior indicative of multi-band transport. The Hall mobility is n-type and low (near 0.07 cm2/V s at room temperature).  相似文献   

11.
The thermoelectric power was measured in the temperature range 6-300 K for a few Ce-based compounds known as intermediate valent systems, i.e. Ce2Ni2In, Ce2Rh2In, Ce2Ni2Ga and CeNi5Sn, in order to scan these ternaries for possible low-temperature thermoelectric applications. The experimental data were analyzed in terms of phenomenological models and compared to those reported in the literature for similar materials. The results corroborated unstable character of the Ce valence in the ternaries studied. However, the magnitude of the Seebeck coefficient, though being considerably enhanced, is for all of them much lower than those known for the best performers in the field of strongly correlated thermoelectrics: CePd3 and YbAl3.  相似文献   

12.
Single crystals of YbRhIn5 and YbIrIn5 have been grown by flux method. The crystals were characterized by means of X-ray diffraction, magnetic and electrical transport measurements. Both compounds were found to be weak diamagnets with metallic character of the electrical conductivity and the Seebeck coefficient.  相似文献   

13.
Electrical resistivity and Seebeck coefficients of Y BaCo4−xZnxO7 (x=0.0,0.5,1.0,2.0) were investigated in the temperature range 350-1000 K. It was found that the electrical resistivity and activation energy increase with increasing Zn concentration, while Seebeck coefficients do not increase but decrease when electrical resistivity increases. We explained the increase of electrical resistivity and the drop of Seebeck coefficients for Zn-substituted samples by the decrease of carrier mobility, rather than of carrier concentration. The effect of oxygen absorption and desorption on the electrical resistivity and Seebeck coefficients was also investigated. An abrupt change of transport properties happens at about 650 K for x=0.0 and 0.5 samples measured in oxygen. For x=1.0 and 2.0 samples, however, such change disappears and the transport behavior in oxygen is almost same as that in nitrogen due to the significant suppression of oxygen diffusion caused by the higher Zn concentration in these samples.  相似文献   

14.
The Bi0.9Sb0.1 powders were prepared by mechanical alloying and then pressed under 6 GPa at different pressing temperatures. X-ray diffraction spectra showed that the single phase was formed. The nanostructure of grain was observed by bright-field imaging. Electrical conductivity, Seebeck coefficient, and thermal conductivity had been investigated in the temperature range of 80-300 K. The absolute Seebeck coefficient value of 120.3 μV/K was measured at 130 K. The figure-of-merit reached a maximum value of 0.90×10−3 K−1 at 140 K.  相似文献   

15.
The resultant local Seebeck coefficient α R (=α Sα T) at the interface of a thermoelement has not yet been measured, although it is an important factor governing the thermoelectric efficiency, where α S is the local Seebeck coefficient and α T is the one caused by the Thomson effect. It is shown in this paper that α S, α T, and α R of the p- and n-type Cu/Bi–Te/Cu composites are obtained analytically and experimentally on the assumption that the local temperature of the composite on which the temperature difference ΔT is imposed varies linearly with changes in position along the composite. They were indeed estimated as a function of position from the local experimental data of RIT, and V generated by applying an additional current of ±I to the composite, where R is the electrical resistance and ΔI is a current generated by the composite. As a result, it was found that the absolute values of α S at the hot interface of the p- and n-type composites are approximately 1.5 and 1.4 times higher than their lowest values in the middle region of the composite, respectively, while those of α T are less than 8% of α S all over the composite and are so small that the relation α Rα S can be held. We thus succeeded in measuring α R at the interfaces of the composite.  相似文献   

16.
Electrical conductivity and Seebeck coefficient for the Bi2−xYxRu2O7 pyrochlores with x=0.0,0.5,1.0,1.5,2.0 were measured in the temperature range of 473-1073 K in air. With increasing Bi content, the temperature dependence of the electrical conductivity changed from semiconducting to metallic. The signs of the Seebeck coefficient were positive in the measured temperature range for all the samples, indicating that the major carriers were holes. The temperature dependence of the Seebeck coefficient for the Y2Ru2O7 indicated the thermal activation-type behavior of the holes, while that for the Bi2−xYxRu2O7 with x=0.0-1.5 indicated the itinerant behavior of the holes. The change in the conduction behavior from semiconductor to metal with increasing Bi content is consistent with the increase in the overlap between the Ru4d t2g and O2p orbitals, but the mixing of Bi6s, 6p states at EF may not be ruled out. The thermoelectric power factors for the Bi2−xYxRu2O7 with x=1.5 and 2.0 were lower than 10−5 W m−1 K−2 and those with x=0.0,0.5,1.0 were around 1-3×10−5 W m−1 K−2.  相似文献   

17.
Pb- or Sn-doped Bi88Sb12 alloys were prepared by direct melting, quenching, and annealing. The Bi-Sb alloy phase was predominant in all samples. Pb or Sn atoms were distributed almost uniformly in Bi88Sb12, while some segregation was confirmed at the grain boundaries when Pb or Sn was involved heavily. The thermoelectric properties of these doped materials were investigated by measuring the Hall coefficient, electrical resistivity, and Seebeck coefficient between 20 K and 300 K. The Hall and Seebeck coefficients of Pb- or Sn-doped samples were positive at low temperatures, indicating that the doping element acted as an acceptor. Temperatures resulting in positive Hall and Seebeck coefficients further increased with increasing doping amount and with respect to the annealing process. As a result, a large power factor of 1.2 W/mK2 could be obtained in the 3-at% Sn-doped sample at 220 K, with a large positive Seebeck coefficient.  相似文献   

18.
Effect of high electric field on the dc conductivity of TeO2-V2O5-MoO3 amorphous bulk samples with different molar ratio of each component was investigated with gap-type electrode arrangement. At low electric fields, the current-voltage (I–V) characteristics has a linear shape, while at high electric fields (>103 V/cm), bulk samples show nonlinear behavior (nonohmic conduction) and current-voltage characteristics shows increasing deviation from Ohm’s law with increasing current density. High-field effect of Pool-Frenkel type was observed at electrical fields about 103−104 V/cm. In addition, positive deviation from Pool-Frenkel effect was observed when a field higher than about 104 V/cm was applied.  相似文献   

19.
The nanocrystalline materials with the general formula Bi85Sb15−xNbx (x=0, 0.5, 1, 2, 3) were prepared by mechanical alloying and subsequent high-pressure sintering. Their transport properties involving electrical conductivity, Seebeck coefficient and thermal conductivity have been investigated in the temperature range of 80-300 K. The absolute value of Seebeck coefficient of Bi85Sb13Nb2 reaches a maximum of 161 μV/K at 105 K, which is 69% larger than that of Bi85Sb15 at the same temperature. The power factor and figure-of-merit are 4.45×10−3 WK−2m−1 at 220 K and 1.79×10−3 K−1 at 196 K, respectively. These results suggest that thermoelectric properties of Bi85Sb15 based material can be improved by Nb doping.  相似文献   

20.
The effect of Na doping and annealing time on the structure, electrical properties, magnetoresistance and thermopower properties has been investigated in perovskite La1−xNaxMnOy (x=0.025, 0.075 and 0.1) systems. La1−xNaxMnOy crystallizes in a single-phase rhombohedral structure. It is observed a simultaneous occurrence of the ferromagnetic to paramagnetic state and metallic to insulating state. In the meanwhile, a large negative magnetoresistance with low applied magnetic field is observed. In addition, ρ(T) curves for Na-doped samples exhibit another broad transition Tms2 below Tms. Such double peak behavior in the ρ(T) curve interpreted by the electronic inhomogeneity in the samples. The sign of S changes from positive to negative depending on composition. The values of Seebeck coefficient are small (in the microvolt range).  相似文献   

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