116 research outputs found

    Structural Disorder, Octahedral Coordination, and 2-Dimensional Ferromagnetism in Anhydrous Alums

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    The crystal structures of the triangular lattice, layered anhydrous alums KCr(SO4)2, RbCr(SO4)2 and KAl(SO4)2 are characterized by X-ray and neutron powder diffraction at temperatures between 1.4 and 773 K. The compounds all crystallize in the space group P-3, with octahedral coordination of the trivalent cations. In all cases, small amounts of disorder in the stacking of the triangular layers of corner sharing MO6 octahedra and SO4 tetrahedra is seen, with the MO6-SO4 network rotated in opposite directions between layers. The electron diffraction study of KCr(SO4)2 supports this model, which on average can be taken to imply trigonal prismatic coordination for the M3+ ions; as was previously reported for the prototype anhydrous alum KAl(SO4)2. The temperature dependent magnetic susceptibilities for ACr(SO4)2 (A = K,Rb,Cs) indicate the presence of predominantly ferromagnetic interactions. Low temperature powder neutron diffraction reveals that the magnetic ordering is ferromagnetic in-plane, with antiferromagnetic ordering between planes below 3 K.Comment: Accepted to the Journal of Solid State Chemistr

    K0.8Ag0.2Nb4O9AsO4

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    The title compound, potassium silver tetra­niobium nona­oxide arsenate, K0.8Ag0.2Nb4O9AsO4, was prepared by a solid-state reaction at 1183 K. The structure consists of infinite (Nb2AsO14)n chains parallel to the b axis and cross-linked by corner sharing via pairs of edge-sharing octa­hedra. Each pair links together four infinite chains to form a three-dimensional framework. The K+ and Ag+ ions partially occupy several independent close positions in the inter­connected cavities delimited by the framework. K0.8Ag0.2Nb4O9AsO4 is likely to exhibit fast alkali-ion mobility and ion-exchange properties. The Wyckoff symbols of special positions are as follows: one Nb 8e, one Nb 8g, As 4c, two K 8f, one Ag 8f, one Ag 4c, one O 8g, one O 4c

    Vanadium(V) oxide arsenate(V), VOAsO4

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    The vanadyl arsenate, VOAsO4, has been isolated by a solid-state reaction. The structure consists of distorted VO6 octa­hedra and AsO4 tetra­hedra sharing corners to build up VAsO7 layers parallel to ac linked by edge-sharing of VO6 octa­hedra, forming a three-dimensional framework

    AgNa2Mo3O9AsO4

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    The title compound, silver disodium trimolybdenum(VI) nonaoxide arsenate, AgNa2Mo3O9AsO4, was prepared by a solid-state reaction at 808 K. The structure consists of an infinite (Mo3AsO13)n ribbon, parallel to the c axis, composed of AsO4 tetra­hedra and MoO6 octa­hedra sharing edges and corners. The Na and Ag ions partially occupy several independent close positions, with various occupancies, in the inter-ribbon space delimited by the one-dimensional framework. The composition was refined to Ag1.06(1)Na1.94(1)Mo3O9AsO4

    La variĂ©tĂ© ÎČ-NaMoO2(AsO4)

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    The title compound, sodium dioxidomolybdenum(VI) arsenate(V), ÎČ-NaMoO2AsO4, was prepared by solid-state reaction at 953 K. In the crystal structure, the AsO4 tetra­hedra and MoO6 octa­hedra (both with m symmetry) share corner atoms to form a three-dimensional framework that delimits cavities parallel to [010] where disordered six-coordinated sodium cations (half-occupation) are located. Structural relationships between the different orthoarsenates of the AMoO2AsO4 series (A = Ag, Li, Na, K and Rb) are discussed

    ChemInform Abstract: Cobalt Lithium Orthoborate, LiCoBO3.

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    Conception d’observateurs pour la commande d’un systĂšme pile Ă  combustible embarquĂ© en vue d’optimiser performances et durabilitĂ©

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    Fuel cells are considered as a promising source of energy for the future, thanks to their non-polluting aspect. However, the deployment of these solutions on a large scale is still conditioned by the improvement of their performance and especially of their durability in order to guarantee a low cost industrialization. The transport application also imposes a variable power demand, which complicates the improvement of performance and durability. The approach adopted for this work consists of the design of a system management law that generates the optimal operating conditions to be applied to the stack (pressures, temperature, current, stoichiometries) as a function of the power demand, the state of health (active surface loss) and current humidity. Optimality is understood in the sense of increasing system efficiency and decreasing the degradation of the membrane and the platinum dissolution. This law is based on degradation and performance models of a fuel cell system. This management law requires in real time the data of the state of health of the fuel cell and the humidity rate. The assessment of the state of health is already the subject of many diagnostic work. On the other hand, the humidity rate must be estimated by a state observer because the humidity sensors are not reliable for a transport application. Therefore, a state observer was developed to estimate the relative humidities in the stack channels and also the membrane water content, the hydrogen at the anode as well as the nitrogen saturation at the anode. This last data makes it possible to propose a purge strategy for a dead-end architecture, based on nitrogen saturation, which limits the losses in hydrogen and reduces the damage associated with this architecture.Les piles Ă  combustibles sont considĂ©rĂ©es comme une Ă©nergie d’avenir, notamment grĂące Ă  leur caractĂšre non polluant Ă  l’usage. Cependant, le dĂ©ploiement de ces solutions Ă  grande Ă©chelle est encore conditionnĂ© par l’amĂ©lioration de leurs performances et surtout de leur durabilitĂ© afin de garantir une industrialisation Ă  faible coĂ»t. L’application de la pile Ă  combustible au domaine des transports impose en plus un fonctionnement Ă  puissance variable, ce qui complique l’amĂ©lioration des performances et de la durabilitĂ©. L’approche retenue pour ces travaux consiste en la conception d’une loi de gestion du systĂšme qui gĂ©nĂšre les conditions opĂ©ratoires optimales Ă  appliquer au stack (pressions, tempĂ©rature, courant, stoechiomĂ©tries) en fonction de la demande en puissance, de l’état de santĂ© de la pile (perte de surface active) et du taux d’humiditĂ© actuel. L’optimalitĂ© est entendue au sens de l’augmentation du rendement systĂšme et de la diminution des dĂ©gradations du platine et de la membrane. Cette loi se base sur des modĂšles de dĂ©gradations et de performances d’un systĂšme pile Ă  combustible. Cette loi de gestion requiert pour fonctionner les donnĂ©es de l’état de santĂ© de la pile et du taux d’humiditĂ©. L’évaluation de l’état de santĂ© de la pile fait dĂ©jĂ  l’objet de nombreux travaux de diagnostic. En revanche, le taux d’humiditĂ© doit ĂȘtre estimĂ© par un observateur d’état car les capteurs d’humiditĂ© ne sont pas fiables pour une application transport. Pour cela, un observateur d’état a Ă©tĂ© dĂ©veloppĂ© pour estimer les humiditĂ©s relatives dans les canaux du stack et aussi le chargement en eau de la membrane, la quantitĂ© d’hydrogĂšne Ă  l’anode ainsi que la saturation d’azote Ă  l’anode. Cette derniĂšre donnĂ©e permet de proposer une stratĂ©gie de purge pour une architecture dead-end basĂ©e sur la saturation d’azote, qui limite les pertes en hydrogĂšne et rĂ©duit les dĂ©gradations liĂ©es Ă  cette architecture
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