Galvanic Cell

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H. Näfe - One of the best experts on this subject based on the ideXlab platform.

V Venugopal - One of the best experts on this subject based on the ideXlab platform.

  • synergistic use of knudsen effusion quadrupole mass spectrometry solid state Galvanic Cell and differential scanning calorimetry for thermodynamic studies on lithium aluminates
    Journal of Solid State Chemistry, 2008
    Co-Authors: S K Rakshit, Y P Naik, S C Parida, Smruti Dash, Ziley Singh, V Venugopal
    Abstract:

    Abstract Three ternary oxides LiAl 5 O 8 (s), LiAlO 2 (s) and Li 5 AlO 4 (s) in the system Li–Al–O were prepared by solid-state reaction route and characterized by X-ray powder diffraction method. Equilibrium partial pressure of CO 2 (g) over the three-phase mixtures {LiAl 5 O 8 (s)+Li 2 CO 3 (s)+5Al 2 O 3 (s)}, {LiAl 5 O 8 (s)+5LiAlO 2 (s)+2Li 2 CO 3 (s)} and {LiAlO 2 (s)+Li 5 AlO 4 (s)+2Li 2 CO 3 (s)} were measured using Knudsen effusion quadrupole mass spectrometry (KEQMS). Solid-state Galvanic Cell technique based on calcium fluoride electrolyte was used to determine the standard molar Gibbs energies of formations of these aluminates. The standard molar Gibbs energies of formation of these three aluminates calculated from KEQMS and Galvanic Cell measurements were in good agreement. Heat capacities of individual ternary oxides were measured from 127 to 868 K using differential scanning calorimetry. Thermodynamic tables representing the values of Δ f H 0 (298.15 K), S 0 (298.15 K) S 0 ( T ), C p 0 ( T ), H 0 ( T ), { H 0 ( T )– H 0 (298.15 K)}, G 0 ( T ), Δ f H 0 ( T ), Δ f G 0 ( T ) and free energy function (fef) were constructed using second law analysis and FACTSAGE thermo-chemical database software.

  • standard molar gibbs energies of formation of the ternary compounds in the la co o system using solid oxide Galvanic Cell method
    Journal of Alloys and Compounds, 1999
    Co-Authors: S C Parida, Smruti Dash, Ziley Singh, R Prasad, V Venugopal
    Abstract:

    Abstract The standard molar Gibbs energies of formation of the ternary oxide compounds; LaCoO 3 (s), La 4 Co 3 O 10 (s) and La 2 CoO 4 (s) in the La-Co-O system have been determined by a solid oxide Galvanic Cell method using 15 mole% calcia stabilized zirconia as the solid electrolyte. The corresponding expressions for the Δ f G m °(T) are given as: Δ f G m °(LaCoO 3 , s, T) (kJ mol −1 ) (±0.6)=−1234.2+0.272T ( K ) (1002 K ≤T≤1204 K ), Δ f G m °(La 4 Co 3 O 10 , s, T) (kJ mol −1 ) (±3.2)=−4663.8+0.969T (K) (1009 K≤T≤1238 K) and Δ f G m °(La 2 CoO 4 , s, T) (kJ mol −1 )(±1.1)=−2017.1+0.347T (K) (1004 K≤T≤1171 K).

  • molar gibbs free energy of formation of rb2u4o11 s by solid oxide electrolyte Galvanic Cell
    Journal of Alloys and Compounds, 1996
    Co-Authors: V S Iyer, K Jayanthi, S K Sali, S Sampath, V Venugopal
    Abstract:

    Abstract The molar Gibbs' free energy of formation of Rb 2 U 4 O 11 was determined by measuring the oxygen potentials over the Rb 2 U 4 O 11 + Rb 2 U 4 O 12 system using a solid oxide electrolyte Galvanic Cell with Ni + NiO as reference electrode in the temperature range 985–1186 K. It was found by X-ray diffraction analysis that Rb 2 U 4 O 11 coexists with Rb 2 U 4 O 12 up to 1300 K. The molar Gibbs' free energy formation of Rb 2 U 4 O 11 is calculated from the e.m.f. values and can be given by: Δ f G ° (kJ mol −1 ) ± 0.65 = −5348.87 + 1.076 T (K). The kinetics of oxidation of Rb 2 U 4 O 11 in air, studied by thermogravimetry indicated that the reaction is phase boundary controlled with an activation energy of 123.6 kJ mol −1 .

Jian Bi - One of the best experts on this subject based on the ideXlab platform.

  • oxidant assisted preparation of camoo4 thin film using an irreversible Galvanic Cell method
    Thin Solid Films, 2010
    Co-Authors: Ping Cheng, Jian Bi
    Abstract:

    Abstract CaMoO4 thin films were prepared by an irreversible Galvanic Cell method at room temperature; the crystalline phase structure, surface morphology, chemical composition and room temperature photoluminescence property were characterized by X-ray diffraction, Raman spectroscopy, scanning electronic microscopy, X-ray photoelectron spectroscopy as well as photoluminescence spectroscopy. Our results reveal that it is very difficult to directly deposit dense and uniform CaMoO4 thin films in saturated Ca(OH)2 solution at room temperature by the irreversible Galvanic Cell method. After adding some oxidant (NaClO solution or H2O2 solution), the growth of CaMoO4 grains has been promoted, and well-crystallized, dense, and uniform CaMoO4 films were obtained. The as-prepared CaMoO4 films exhibit a good green photoluminescence, with the excitation of various wavelengths (220 nm, 230 nm, 240 nm, 250 nm and 270 nm) of ultraviolet irradiation.

  • Analysis of Galvanic Cell deposition process in preparation of BaMoO4 films
    Journal of Materials Science, 2009
    Co-Authors: Chunyan Wu, Bo Li, Jian Bi
    Abstract:

    The Galvanic Cell method has been used for the synthesis of BaMoO4 double oxide film in barium hydroxide aqueous solutions. This method could resolve the repulsion of the electric field on the anode and favor the mass transfer of cations. The crystal growth in the solution is easier compared with the traditional electrochemical deposition with applied power. The deposition process of the Galvanic Cell technique has been investigated by deposition time, pH, and ion concentration, and the basic features of this method are discussed.

  • Room temperature synthesis of crystallized luminescent SrWO4 films by an adjustable Galvanic Cell method
    Journal of Crystal Growth, 2008
    Co-Authors: Jian Bi
    Abstract:

    Abstract Highly crystallized luminescent SrWO 4 films were prepared directly on tungsten substrate in strontium hydroxide aqueous solution by a Galvanic Cell method without impressed current at room temperature. It is noteworthy that the driving force of Galvanic Cell method is adjustable by adding different concentrations of oxidant. The X-ray diffraction (XRD) and scanning electron microscopy (SEM) results reveal that the crystallized films have a scheelite-type tetragonal structure and homogeneous surface. The film showed single blue emissions at 447 nm with excitation lights of 220, 230, 250, 260 and 270 nm at room temperature, respectively.

  • morphology and crystal phase control in preparation of highly crystallized bawo4 film via Galvanic Cell method
    Journal of Alloys and Compounds, 2008
    Co-Authors: Jian Bi, Keqing Zhao
    Abstract:

    Abstract Highly crystallized BaWO 4 films have been prepared by a Galvanic Cell method without impressed current on tungsten substrates at room temperature. The surface morphology, grain size and crystal phase of BaWO 4 films have been controlled effectively by adjusting ion-concentration, pH and even adding adequate surfactant. The BaWO 4 films are characterized by scanning electron microscopy (SEM), X-ray diffraction (XRD). The results indicate that the films have single phase and uniform surfaces. The grain size was changed under different treatment conditions.

  • room temperature preparation of highly crystallized cawo4 film by a Galvanic Cell method
    Materials Letters, 2008
    Co-Authors: Jian Bi
    Abstract:

    Abstract Highly crystallized CaWO 4 film has been prepared directly by a Galvanic Cell method on tungsten substrates in calcium hydroxide aqueous solution without impressed current at room temperature (25 °C). The scanning electron microscopy (SEM) and X-ray diffraction (XRD) results reveal that the crystallized film has a scheelite-type tetragonal structure, uniform and homogeneous surface. The film shows only the blue emission of 447.5 nm with the excitation light of 250 nm at room temperature. The formation mechanism of CaWO 4 film under the simple electrochemical process has been discussed. This method could resolve the repulsion of the electric field on the anode for the mass transfer. The crystal growth in the solution is freer.

Seshadri Seetharaman - One of the best experts on this subject based on the ideXlab platform.

Pekka Taskinen - One of the best experts on this subject based on the ideXlab platform.

  • thermodynamic properties of ag3ause2 from 300 to 500 k by a solid state Galvanic Cell
    Journal of Alloys and Compounds, 2014
    Co-Authors: Dawei Feng, Pekka Taskinen
    Abstract:

    Abstract The numerical values of the standard thermodynamic functions of Ag 3 AuSe 2 (fischesserite) in the Ag–Au–Se system were determined by the electromotive force (EMF) method in a solid state Galvanic Cell with RbAg 4 I 5 as the solid electrolyte below 500 K. Ag 3 AuSe 2 was synthesized from pure elements in stoichiometric composition by evacuated ampoules made of quartz glass. On the basis of EMF vs. temperature experimental data, the analytical equations were obtained, from which the temperature dependent relationships of the Gibbs energy in the relevant reactions and the standard thermodynamic functions of Ag 3 AuSe 2 within the temperature range of 300–500 K were calculated. The results show that there is possible a new polymorphic transformation around 350 K.

  • thermodynamic stability of ag2se from 350 to 500 k by a solid state Galvanic Cell
    Solid State Ionics, 2013
    Co-Authors: Dawei Feng, Pekka Taskinen, Fiseha Tesfaye
    Abstract:

    Abstract The numerical values on the standard thermodynamic functions of Ag 2 Se (naumannite) were determined by the electromotive force (EMF) method in a solid-state Galvanic Cell with superionic conductor RbAg 4 I 5 as the solid electrolyte. Ag 2 Se was synthesized from pure elements in evacuated quartz glass ampoules and examined to be homogenous by SEM and EDS. According to the experimental data on the EMF versus temperature, the analytical equations were obtained for the polymorphic forms of Ag 2 Se. The temperature-dependent relationships of the Gibbs energy of formation of Ag 2 Se in its polymorphic forms and the standard thermodynamic functions of compounds within the temperature range of 350–500 K were also evaluated. The temperature of phase transformation from α-Ag 2 Se to β-Ag 2 Se is determined experimentally to be 407.7 K and the enthalpy of phase transformation is 6.06 kJ mol − 1 .