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1.
The electrical conductivity, crystal structure and phase stability of La0.99Ca0.01Nb1−xTaxO4−δ (x = 0, 0.1, 0.2, 0.3, 0.4 and 0.5, δ = 0.005), a potential candidate for proton conductor for solid oxide fuel cells (SOFCs), have been investigated using AC impedance technique and in situ X-ray powder diffraction. Partially substituting Nb with Ta elevates the phase transition temperature (from a monoclinic to a tetragonal structure) from ∼520 °C for x = 0 to above 800 °C for x = 0.4. AC conductivity of the La0.99Ca0.01Nb1−xTaxO4−δ both in dry and wet air decreased slightly with increasing Ta content above 750 °C, while below 500 °C, it decreased by nearly one order of magnitude for x = 0.4. It was also determined that the activation energy for the total conductivity increases with increasing Ta content from 0.50 eV (x = 0) to 0.58 eV (x = 0.3) for the tetragonal phase, while it decreases with increasing Ta content from 1.18 eV (x = 0) to 1.08 eV (x = 0.4) for the monoclinic phase. By removing the detrimental structural phase transition from the intermediate-temperature range, consequently avoiding the severe thermal expansion problem up to 800 °C, partial substitution of Nb with Ta brings this class of material closer to its application in electrode-supported thin-film intermediate-temperature SOFCs.  相似文献   

2.
Scheelite-type, LaxCa1−xMoO4+δ electrolyte powders, are prepared by the sol-gel process. The crystal structure of the samples is determined by employing the technique of X-ray diffraction (XRD). According to XRD analysis, the continuous series of LaxCa1−xMoO4+δ (0 ≤ x ≤ 0.3) solid solutions have the structure of tetragonal scheelite. Their lattice parameters are greater than that of the original sample, and increase with increasing values of x in the La-substituted system. Results of sinterability and electrochemical testing reveal that the performances of La-doped calcium molybdate are superior to that of pure CaMoO4. LaxCa1−xMoO4+δ ceramics demonstrate higher sinterability. The La0.2Ca0.8MoO4+δ sample that achieved 96.5% of the theoretical density was obtained after being sintered at 1250 °C for 4 h. The conductivity increases with increasing lanthanum content, and a total conductivity of 7.3 × 10−3 S cm−1 at 800 °C could be obtained in the La0.2Ca0.8MoO4+δ compound sintered at 1250 °C for 4 h.  相似文献   

3.
The lattice parameters, electrical conductivity, activation energy, mechanical properties, and microstructure of (La0.8Ca0.2)CrO3−δ-based specimens were investigated systematically in this paper. The tolerance factors for (La0.8Ca0.2)CrO3−δ-based specimens were all greater than 0.9, indicating the perovskite was not distorted with different cations (Al3+, Co3+, Cu2+, Fe3+) substitution for B site of (La0.8Ca0.2)CrO3−δ. (La0.8Ca0.2)Cr0.9Co0.1O3−δ specimen revealed the maximum electrical conductivity, σ850 °C = 59.59 S/cm with minimum activation energy, Ea = 11.2 kJ/mol among (La0.8Ca0.2)CrO3−δ-based specimens. The grain size seemed dependent on doping species and the grain sizes were distributed in the range of 2.4-5.6 μm for (La0.8Ca0.2)CrO3−δ-based specimens. The rate of grain growth was proportional to the boundary mobility Mb, which was related to the diffusion coefficient of doping cation. (La0.8Ca0.2)CrO3−δ-based specimens revealed variety in microhardness, in the range of 4.33-9.85 GPa and the fracture toughness were distributed in the range of 3.52-4.33 MPa m1/2. Based on the results in terms of grain size and mechanical properties, we concluded that the microhardness and fracture toughness were dependent on the dopant ions. The (La0.8Ca0.2)Cr0.9Co0.1O3−δ specimen shows high electrical conductivity and mechanical properties Consequently, it is a promising candidate as an interconnect material for intermediate temperature solid oxide fuel cell (IT-SOFC) applications.  相似文献   

4.
La2−xMxNiO4+δ (M = Ba, Sr; x = 0.1, 0.3), with a formula of A2BO4, has been prepared and investigated as cathode for solid oxide fuel cells to understand the influence of A-site dopants on the lattice structure, electrical conductivity and electrochemical properties of La2NiO4+δ. All the compositions belong to tetragonal I4/mmm space group. La2−xBaxNiO4+δ shows larger lattice parameters than La2−xSrxNiO4+δ due to the large ionic radius of Ba2+ compared with Sr2+. For both Ba and Sr, the parameters a and b decrease while the c increases with increasing doping level. Rietveld refinement demonstrates that the increase in c parameter is partially originated from the increase in rocksalt layer thickness (La–O2( × 1) bond), which makes the adsorbed oxygen on particle surface much easier to enter the lattice and form interstitials, and thereby promoting the electrode reaction. The electrical conductivity of La2−xMxNiO4+δ increases with doping level but decrease with increasing ionic radius of dopants. Both Ba and Sr doping decrease the electrode polarization and increase the power density of single-cell. La1.7Ba0.3NiO4+δ exhibits superior electrochemical properties than La1.7Sr0.3NiO4+δ. The La1.7Ba0.3NiO4+δ electrode exhibits the best performance with an ASR of 0.13 Ω cm2 and a maximum power density of 310 mW cm−2 at 800 °C under electrolyte (La0.8Sr0.2Ga0.83Mg0.17O3−δ, 300 μm) – supported configuration.  相似文献   

5.
A-site-deficient (La0.3Sr0.7)1−xTiO3−δ materials were synthesized by conventional solid-state reaction. The A-site deficiency limit in (La0.3Sr0.7)1−xTiO3−δ was below 10 mol% in 5%H2/Ar at 1500 °C. A-site deficiency level promoted the sintering process of (La0.3Sr0.7)1−xTiO3−δ. The ionic conductivity increased but the electronic conductivity decreased with increasing A-site deficiency level. The ionic conductivity of (La0.3Sr0.7)0.93TiO3−δ sample was as high as 0.2–1.6 × 10−2 S/cm in 500–950 °C and 1.0 × 10−2 S/cm at 800 °C, over twice of La0.3Sr0.7TiO3−δ. Its electrical conductivity was in the range of 83–299 S/cm in 50–950 °C and 145 S/cm at 800 °C. A-site deficiency improved the thermal stability of (La0.3Sr0.7)1−xTiO3−δ and ensured the material with a stable electrical performance in different atmospheres.  相似文献   

6.
The aim of this study was to develop La1−xBaxGa1−yMgyO3−δ (x = 0.03–0.1, y = 0.2–0.25) (LBGM) electrolytes for intermediate-temperature solid-oxide fuel cells (SOFCs); these electrolytes were synthesized via a solid-state reaction. In the study, the La1−xBaxGa1−yMgyO3−δ samples crystallized in an orthorhombic (Imma) structure, and a BaLaGa3O7 phase was detected for x ≥ 0.08 at a fixed y = 0.2. The solubility limit of the Ba ions increased with an increase in the Mg content in the matrix. Two active Raman bands at ca. 677 and 739 cm−1 were observed, and they were attributed to the oxygen vacancies. The La0.95Ba0.05Ga0.75Mg0.25O3−δ sample had a higher conductivity ca. 0.1 S/cm at 800 °C, and an activation energy of ca. 0.83–1.27 eV at 500–800 °C. The thermal expansion coefficient (TEC) of the LBGM samples at 200–800 °C was in the range of 10 × 10−6 to 14 × 10−6/°C.  相似文献   

7.
In the current manufacturing process of novel LaNbO4-based proton conducting fuel cells a thin layer of the electrolyte is deposited by wet ceramic coating on NiO-LaNbO4 based anode and co-sintered at 1200-1300 °C. The chemical compatibility of NiO with acceptor doped LaNbO4 material is crucial to ensure viability of the cell, so potential effects of other phases resulting from off-stoichiometry in acceptor doped LaNbO4 should also be explored. Compatibility of NiO with Ca-doped LaNbO4 and its typical off-set compositions (La3NbO7 and LaNb3O9) are investigated in this work. It is shown that while NiO does not react with Ca-doped LaNbO4, fast reaction occurs with La3NbO7 or LaNb3O9. La3NbO7 and NiO form a mixed conducting perovskite phase LaNi2/3Nb1/3O3, while LaNb3O9 and NiO form either NiNb2O6 or Ni4Nb2O9 depending on the annealing temperature. This implies that manufacturing LaNbO4-based proton conducting fuel cells requires a strict control of the stoichiometry of the electrolyte.  相似文献   

8.
Cobalt-free perovskite oxides Ba1−xLaxFeO3−δ (x = 0.1–0.4) were synthesized by glycine-nitrate combustion method and investigated as a candidate cathode material for intermediate temperature solid oxide fuel cells (IT-SOFCs). Cubic perovskite structure was obtained when 10–20 mol% La was substituted at Ba-site in Ba1−xLaxFeO3−δ, and the crystal structure was transformed from cubic structure into orthorhombic one at x ≥ 0.2 with an addition of lanthanum doping. The thermal expansion coefficients of Ba1−xLaxFeO3−δ oxides decreased gradually with La content due to increasing electrostatic attraction forces. A gradual increase existed in electrical conductivity tendency with La content due to disproportionation of Fe3+ and the larger extent of electron clouds. The electrode redox performance was investigated by electrochemical impedance spectroscopy. Among Ba1−xLaxFeO3−δ series oxides, Ba0.9La0.1FeO3−δ exhibited the best electrochemical performance. The area specific resistance (ASR) of Ba0.9La0.1FeO3−δ was 0.079 Ω cm2, 0.37 Ω cm2, and 2.15 Ω cm2 at 800, 700 and 600 °C under open circuit potential. To investigate electrochemical performances after cathodic polarization, bias potentials were employed on Ba1−xLaxFeO3−δ cathode at 650–800 °C. The results demonstrated the potential applications for Ba0.9La0.1FeO3−δ as cathode materials for IT-SOFCs as a tradeoff between electrochemical and thermal expansion performance.  相似文献   

9.
The crystalline structure, redox stability and electrical conductivity of LaCrO3, (La1−xMx)CrO3 (M = Mg, Ca, Ba for x = 0.3 and M = Sr for x = 0.25), and (La0.75Sr0.25)(Cr0.5Mn0.5)O3 (LSCM) perovskites are studied from 500 to 800 °C in both oxidizing and reducing atmospheres. Dopability, redox stability and electrical conductivity are compared and examined. A-site doping with alkaline elements is found to improve significantly the electrical conductivity, particularly if properly doped. The highest conductivity is obtained with Ca- and Sr-doped LaCrO3. A-site doping also reduces the activation energy of the electrical conductivity, particularly under a reducing environment. Preliminary electrochemical results indicate that Ca-doped LaCrO3 shows promise as a cathode for solid oxide fuel cells.  相似文献   

10.
The electrochemical properties of mixed-conducting ceramic-ceramic (cer-cer) composites for proton-conducting solid oxide fuel cells (PC-SOFCs) based on La0.995Ca0.005NbO4−δ (LCN) have been investigated. Different ratios of La0.8Sr0.2MnO3−δ/La0.995Ca0.005NbO4−δ (LSM/LCN) composites have been tested as cathodes in symmetrical cells based on La0.995Ca0.005NbO4−δ dense electrolytes while two different electrode sintering temperatures (1050 and 1150 °C) have been studied. Additionally, different LCN doped materials (Pr, Ce and Mn), which present a different conduction behavior, have been used as components in composite cathodes (mixtures of LSM/doped-LCN 50/50 vol.%). Electrochemical impedance spectroscopy analysis has been carried out in the temperature range 700-900 °C under moist (2.5%) atmospheres. Different oxygen partial pressures (pO2) have been employed in order to characterize the processes (surface reaction and charge transport) occurring at the composite electrode under oxidizing conditions. The main outcome of the present study is that the mixture of LSM (electronic phase) and LCN (protonic phase) enables to decrease substantially the electrode polarization resistance. This is ascribed to the increase in the three-phase-boundary length and therefore it allows electrochemical reactions to occur in a larger region (thickness) of the electrode.  相似文献   

11.
In the present work, we have explored novel Nd2WO6-type structure Sm2−xAxM1−yByO6−δ (A = Ca, Sr; M = Mo, W; B = Ce, Ni) as precursor for the development of solid oxide fuel cells (SOFCs) anodes. The formation of single-phase monoclinic structure was confirmed by powder X-ray diffraction (PXRD) for the A- and B-doped Sm2MO6 (SMO). Samples after AC measurements under wet H2 up to 850 °C changed from Nd2WO6-type structure into Sm2MoO5 due to the reduction of MoVI that was confirmed by PXRD and is consistent with literature. The electrical conductivity was determined using 2-probe AC impedance and DC method and was compared with 4-probe DC method. The total electrical conductivity obtained from these two different techniques was found to vary within the experimental error over the investigated temperature of 350-650 °C. Ionic and electronic conductivity were studied using electron-blocking electrodes technique. Among the samples studied, Sm1.8Ca0.2MoO6−δ exhibits total conductivity of 0.12 S cm−1 at 550 °C in wet H2 with an activation energy of 0.06 eV. Ca-doped SMO appears to be chemically stable against reaction with YSZ electrolyte at 800 °C for 24 h in wet H2. The ionic transference number (ti) of Sm1.9Ca0.1MoO6−δ in wet H2 at 550 °C (pO2 = 10−25.5 atm) was found to be about 0.012 after subtraction of electrical lead resistance from the 2-probe AC data and showed predominate electronic conductors.  相似文献   

12.
Sr2−xLaxMnO4+δ (x = 0.4, 0.5, 0.6) oxides were studied as the cathode material for solid oxide fuel cells (SOFC). The reactivity tests indicated that no reaction occurred between Sr2−xLaxMnO4+δ and CGO at annealing temperature of 1000 °C, and the electrode formed good contact with the electrolyte after being sintered at 1000 °C for 4 h. The total electrical conductivity, which has strong effect on the electrode properties, was determined in a temperature range from 100 to 800 °C. The maximum value of 5.7 S cm−1 was found for the x = 0.6 phase at 800 °C in air. The cathode polarization and AC impedance results showed that Sr1.4La0.6MnO4+δ exhibited the lowest cathode overpotential. The area specific resistance (ASR) was 0.39 Ω cm2 at 800 °C in air. The charge transfer process is the rate-limiting step for oxygen reduction reaction on Sr1.4La0.6MnO4+δ electrode.  相似文献   

13.
We have studied the structure and proton conductivity of rhombohedral La6?xMoO12?δ (x = 0.5, 0.6, 0.7, 1) lanthanum molybdates prepared via mechanical activation of lanthanum and molybdenum oxides, followed by thermal annealing at 1650 °C. The La6?xMoO12?δ (x = 0.5, 0.6) materials were phase-pure and had a complex rhombohedral structure (R1). An increase in the molybdenum concentration leads to a decrease in the degree of rhombohedral distortion and proton conductivity in the La6?xMoO12?δ (x = 0.5, 0.6, 0.7, 1) series. The proton conductivity at the optimal composition La6?xMoO12?δ (x = 0.5) is ~4.0 × 10?5 S/cm at 500 °C in wet air.A comparative analysis shows that, in the Ln6?xMoO12?δ (Ln = La, Nd, Sm, Gd, Dy, Ho, Er, Tm, Yb; x = 0–1) series, proton conductivity decreases with the Ln ionic radii decreasing regardless of the structural type. Because of this, the high proton conductivity is demostrated by the stable La6?xMoO12?δ (x = 0.5, 0.6) materials, with an inherently deficient oxygen sublattice, which crystallize in a large-volume, complex rhombohedral cell (R1).  相似文献   

14.
The misfit compounds Ca3−xBixCo4O9−δ (x = 0.1–0.5) were successfully synthesized via conventional solid state reaction and evaluated as cathode materials for intermediate temperature-solid oxide fuel cells. The powders were characterized by X-ray diffraction, scanning emission microscopy, X-ray photoelectron spectroscopy, thermogravimetry analysis and oxygen-temperature programmed desorption. The monoclinic Ca3−xBixCo4O9−δ powders exhibit good thermal stability and chemical compatibility with Ce0.8Sm0.2O2−γ electrolyte. Among the investigated single-phase samples, Ca2.9Bi0.1Co4O9−δ shows the maximal conductivity of 655.9 S cm−1 and higher catalytic activity compared with other Ca3−xBixCo4O9−δ compositions. Ca2.9Bi0.1Co4O9−δ also shows the best cathodic performance and its cathode polarization resistance can be further decreased by incorporating 30 wt.% Ce0.8Sm0.2O2−γ. The maximal power densities of the NiO/Ce0.8Sm0.2O2−γ anode-supported button cells fabricated with the Ce0.8Sm0.2O2−γ electrolyte and Ca2.9Bi0.1Co4O9−δ + 30 wt.% Ce0.8Sm0.2O2−γ cathode reach 430 and 320 mW cm−2 at 700 and 650 °C respectively.  相似文献   

15.
Oxides of composition SrMo1−xCrxO3−δ (x = 0.1, 0.2) have been prepared, characterized and tested as anode materials in single solid-oxide fuel cells, yielding output powers higher than 700 mW cm−2 at 850 °C with pure H2 as a fuel. All the materials are suggested to present mixed ionic–electronic conductivity (MIEC) from neutron powder diffraction (NPD) experiments, complemented with transport measurements; the presence of a Mo4+/Mo5+ mixed valence at room temperature, combined with a huge metal-like electronic conductivity, as high as 340 S cm−1 at T = 50 °C for x = 0.1, could make these oxides good materials for solid-oxide fuel cells. The magnitude of the electronic conductivity decreases with increasing Cr-doping content. The reversibility of the reduction–oxidation between the oxidized Sr(Mo,Cr)O4−δ scheelite and the reduced Sr(Mo,Cr)O3 perovskite phases was studied by thermogravimetric analysis, which exhibit the required cyclability for fuel cells. An adequate thermal expansion coefficient, without abrupt changes, and a chemical compatibility with electrolytes make these oxides good candidates for anodes in intermediate-temperature SOFC (IT-SOFCs).  相似文献   

16.
Ce0.8Sm0.15R0.05O2−δ (R = Sm, Mg, Ca, Sr, and Ba) specimens were successfully prepared using a solid-state reaction, and they were used in an intermediate temperate solid oxide fuel cell (IT-SOFC) electrolyte. This study focused on the effects of co-doping and an aging treatment for the conductivities and microstructures of CeO2-based ceramics and also analyzed the variation of the conductivity in the reducing atmosphere. The study showed that the conductivities of the CeO2-based materials have a higher conductivity at 500–800 °C by the co-doping aliovalent cations Sm and R. The conductivity increased with the increasing oxygen vacancies that were induced from charge compensation. The XRD and EDS analyses showed that the MgO and BaCeO3 phases appeared in the Ce0.8Sm0.15Mg0.05O2−δ and Ce0.8Sm0.15Ba0.05O2−δ specimens, respectively. The conductivity of the Ce0.8Sm0.15Ca0.05O2−δ specimens was higher, approximately 0.0837 S/cm at 800 °C in the air. The thermal expansion coefficient (TEC) in all samples was ca. 11–15 × 10−6/°C at 200–800 °C. After an aging treatment at 700 °C for a holding time of 1000 h, the conductivities of all samples showed almost no change. However, the conductivity in Ce0.8Sm0.15Ca0.05O2−δ decreased from 0.0837 to 0.0581 S/cm, and the grain size increased. The conductivities of the CeO2-based specimens were also measured under a 5%H2–95%N2 atmosphere, and the conductivity greatly increased in the reducing atmosphere because the Ce4+ ions reduced to Ce3+ ions.  相似文献   

17.
The anode materials La0.3Sr0.7Ti1−xCrxO3−δ (LSTC, x = 0, 0.1, 0.2) with cubic structure were prepared via solid state reaction route. The influence of Cr content on the properties of LSTC as anode and interconnect materials for solid oxide fuel cells (SOFCs) was investigated. The Cr-doping decreased the lattice parameter while increased the sinterability of LSTC materials. The total electrical conductivity decreased with Cr doping level, from 230 S cm−1 for x = 0 to 53 S cm−1 for x = 0.2. The total electrical conductivity exhibited good stability and recoverability in alternative atmospheres of air and 5% H2/Ar, showing excellent redox stability. The cell testing showed that the anode performance of LSTC was enhanced somewhat by Cr doping. The present results indicated that the prepared La0.3Sr0.7Ti1−xCrxO3−δ can be potential anode and interconnect materials for SOFCs.  相似文献   

18.
K2NiF4-type structural Nd2−xSrxCoO4+δ (x = 0.8, 1.0, 1.2) was synthesized and evaluated as cathodes for intermediate-temperature solid oxide fuel cell (IT-SOFC). The crystal structure, thermal expansion, electrical conductivity and electrochemical properties were investigated by X-ray diffraction, dilatometry, DC four-probe method, AC impedance and polarization techniques. It is found that the electrochemical properties were remarkably improved with the increasing of Sr in the experiment range. Nd0.8Sr1.2CoO4+δ showed the highest electrical conductivity of 212 S cm−1 at 800 °C, the lowest polarization resistance and cathodic overpotential, 0.40 Ωcm2 at 700 °C and 35.6 mV at a current density of 0.1 A cm−2 at 700 °C, respectively. The chemical compatibility experiment revealed that Nd0.8Sr1.2CoO4+δ cathode was chemically stable with the SDC electrolyte. The thermal expansion coefficient also increased with the Sr content.  相似文献   

19.
Determining the relationship between electrical conductivity and doping level in high temperature proton conductors is of great significance to accelerate their process of practicality and develop new applications. In this work, BaCe1-xSmxO3-δ (x = 0.01-0.50) was synthesized via citric-nitrate method and their electrical conduction behavior in 5% H2/Ar in the intermediate temperature range was investigated. The solubility of Sm in BaCeO3 was between 0.30 and 0.40. Both the bulk and the grain boundary conductivity increased with Sm content up to x = 0.20 and then decreased. The infrared spectra results indicated that the degree of hydrogen bonding decreased with Sm content (x = 0.20-0.30), which should be responsible for the descending bulk conductivity of samples with x = 0.25 and 0.30. BaCe0.80Sm0.20O3-δ, with electrical conductivity of 0.017 S cm−1 at 600 °C, was a promising electrolyte for intermediate temperature solid oxide fuel cells.  相似文献   

20.
Perovskite oxide Ba1.0Co0.7Fe0.2Nb0.1O3−δ has been reported as oxygen transport membrane and cathode material for solid oxide fuel cells (SOFCs). In this study, the effects of A-site cation deficiency and B-site iron doping concentration on the crystal structure, thermal expansion coefficient (TEC), electrical conductivity and electrochemical performance of Ba1−xCo0.9−yFeyNb0.1O3−δ (x = 0-0.15, y = 0-0.9) have been systematically evaluated. Ba1−xCo0.9−yFeyNb0.1O3−δ (x = 0-0.10, y = 0.2 and x = 0.10, y = 0.2-0.6) can be indexed to a cubic structure. Increased electrical conductivity and decreased cathode polarization resistance have been achieved by A-site deficiency. No obvious variation can be observed in TEC by A-site deficiency. The electrical conductivity and TEC of Ba0.9Co0.9−yFeyNb0.1O3−δ decrease while the cathode polarization resistance increases with the increase in iron doping concentration. The highest conductivity of 13.9 S cm−1 and the lowest cathode polarization resistance of 0.07 Ω cm2 have been achieved at 700 °C for Ba0.9Co0.7Fe0.2Nb0.1O3−δ. The composition Ba0.9Co0.3Fe0.6Nb0.1O3−δ shows the lowest TEC value of 13.2 × 10−6 °C−1 at 600 °C and can be a potential cathode material for SOFCs.  相似文献   

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