Some studies on a solid state sulphur probe for coal gasification system

Measurements on the solid electrolyte cell(Ar -b H2 ~ H2S/CaS + CaF2 ~- ( P t ) / / C a F 2 / / ( P t )-~- CaF2 ~ CaS/H2S ~- H2 ~- At) show that the emf of the cell is directly related through the Nernst equation to the difference in sulfur potentials established at the two Ar ~- H2 ~ H2S/electrode interfaces. The electrodes are designed to convert the sulfur potential gradient across the calcium fluoride electrolyte into an equivalent fluorine potential gradient with the aid of the reaction, CaF2(s) ~ 1~ S2(g)-e CaS(s) ~- F2(g). The response time of the probe varies from approximately 9 hr at 990~ to 2.5 hr at 1225~ The conversion of calcium sulfide and/or calcium fluoride into calcium oxide should not be a problem in anticipated commercial coal gasification systems. Suggestions are presented for improving the cell for such commercial applications.

Hierarchical Clustering Algorithm for Land Cover Mapping Using Satellite Images

This paper presents hierarchical clustering algorithms for land cover mapping problem using multi-spectral satellite images. In unsupervised techniques, the automatic generation of number of clusters and its centers for a huge database is not exploited to their full potential. Hence, a hierarchical clustering algorithm that uses splitting and merging techniques is proposed. Initially, the splitting method is used to search for the best possible number of clusters and its centers using Mean Shift Clustering (MSC), Niche Particle Swarm Optimization (NPSO) and Glowworm Swarm Optimization (GSO). Using these clusters and its centers, the merging method is used to group the data points based on a parametric method (k-means algorithm). A performance comparison of the proposed hierarchical clustering algorithms (MSC, NPSO and GSO) is presented using two typical multi-spectral satellite images - Landsat 7 thematic mapper and QuickBird. From the results obtained, we conclude that the proposed GSO based hierarchical clustering algorithm is more accurate and robust.

Substrate integrated Lead-Carbon hybrid ultracapacitor with flooded, absorbent glass mat and silica-gel electrolyte configurations

Lead-Carbon hybrid ultracapacitors (Pb-C HUCs) with flooded, absorbent-glass-mat (AGM) and silica-gel sulphuric acid electrolyte configurations are developed and performance tested. Pb-C HUCs comprise substrate-integrated PbO2 (SI-PbO2) as positive electrodes and high surface-area carbon with graphite-sheet substrate as negative electrodes. The electrode and silica-gel electrolyte materials are characterized by XRD, XPS, SEM, TEM, Rheometry, BET surface area, and FTIR spectroscopy in conjunction with electrochemistry. Electrochemical performance of SI-PbO2 and carbon electrodes is studied using cyclic voltammetry with constant-current charge and discharge techniques by assembling symmetric electrical-double-layer capacitors and hybrid Pb-C HUCs with a dynamic Pb(porous)/PbSO4 reference electrode. The specific capacitance values for 2 V Pb-C HUCs are found to be 166 F/g, 102 F/g and 152 F/g with a faradaic efficiency of 98%, 92% and 88% for flooded, AGM and gel configurations, respectively.

HIGH-RESOLUTION IMAGING OF THE ATLBS REGIONS: THE RADIO SOURCE COUNTS

The Australia Telescope Low-brightness Survey (ATLBS) regions have been mosaic imaged at a radio frequency of 1.4 GHz with 6 `' angular resolution and 72 mu Jy beam(-1) rms noise. The images (centered at R. A. 00(h)35(m)00(s), decl. -67 degrees 00'00 `' and R. A. 00(h)59(m)17(s), decl. -67.00'00 `', J2000 epoch) cover 8.42 deg(2) sky area and have no artifacts or imaging errors above the image thermal noise. Multi-resolution radio and optical r-band images (made using the 4 m CTIO Blanco telescope) were used to recognize multi-component sources and prepare a source list; the detection threshold was 0.38 mJy in a low-resolution radio image made with beam FWHM of 50 `'. Radio source counts in the flux density range 0.4-8.7 mJy are estimated, with corrections applied for noise bias, effective area correction, and resolution bias. The resolution bias is mitigated using low-resolution radio images, while effects of source confusion are removed by using high-resolution images for identifying blended sources. Below 1 mJy the ATLBS counts are systematically lower than the previous estimates. Showing no evidence for an upturn down to 0.4 mJy, they do not require any changes in the radio source population down to the limit of the survey. The work suggests that automated image analysis for counts may be dependent on the ability of the imaging to reproduce connecting emission with low surface brightness and on the ability of the algorithm to recognize sources, which may require that source finding algorithms effectively work with multi-resolution and multi-wavelength data. The work underscores the importance of using source lists-as opposed to component lists-and correcting for the noise bias in order to precisely estimate counts close to the image noise and determine the upturn at sub-mJy flux density.

Hydrothermal synthesis of Gd2O3:Eu3+ nanophosphors: Effect of surfactant on structural and luminescence properties

Various morphologies of Eu3+ activated gadolinium oxide have been prepared by hydrothermal method using hexadecylamine (HDA) as surfactant at different experimental conditions. The powder X-ray diffraction studies reveal as-formed product is hexagonal Gd(OH)(3):Eu3+ phase and subsequent heat treatment at 350 and 600 degrees C transforms to monoclinic GdOOH:Eu3+ and cubic Gd2O3:Eu3+ phases respectively. SEM pictures of without surfactant show irregular shaped rods along with flakes. However, in the presence of HDA surfactant, the particles are converted into rods of various sizes. The temperature dependent morphological evolution of Gd2O3:Eu3+ without and with HDA surfactant is studied. TEM micrographs of Gd(OH)(3):Eu3+ sample with HDA confirms smooth nanorods with various diameters in the range 20-100 nm. FTIR studies reveal that HDA surfactant plays an important role in conversion of cubic to hexagonal phases. Among these three phases, cubic phase Gd2O3:Eu3+ (lambda(ex) = 254 nm) show red emission at 612 nm corresponding to D-5(0)-> F-7(2) and is more efficient host than the monoclinic counterpart. The band gap for hexagonal Gd(OH)(3):Eu3+ is more when compared to monoclinic GdOOH:Eu3+ and cubic Gd2O3:Eu3+. (C) 2013 Elsevier B. V. All rights reserved.

Measurement of in-plane and out-of-plane displacements and strains using digital holographic moire

The paper proposes a non-destructive method for simultaneous measurement of in-plane and out-of-plane displacements and strains undergone by a deformed specimen from a single moire fringe pattern obtained on the specimen in a dual beam digital holographic interferometry setup. The moire fringe pattern encodes multiple interference phases which carry the information on multidimensional deformation. The interference field is segmented in each column and is modeled as multicomponent quadratic/cubic frequency-modulated signal in each segment. Subsequently, the product form of modified cubic phase function is used for accurate estimation of phase parameters. The estimated phase parameters are further utilized for direct estimation of the unwrapped interference phases and phase derivatives. The simulation and experimental results are provided to validate the effectiveness of the proposed method.

Approaches toward (eta(2)-HX) (X = H, SiR (R = Me-3 or Me2Ph), CH3) sigma-complexes of ruthenium

Two new Ru(II)-complexes RuH(Tpms)(PPh3)(2)] 1 (Tpms - (C3H3N2)(3)CSO3, tris-(pyrazolyl) methane sulfonate) and Ru(OTf)(Tpms)(PPh3)(2)] 2 (OTf = CF3SO3) have been synthesized and characterized wherein Ru-H and Ru-OTf are the key reactive centers. Reaction of 1 with HOTf results in the Ru(eta(2)-H-2)(Tpms)(PPh3)(2)]OTf] complex 3, whereas reaction of 1 with Me3SiOTf affords the dihydrogen complex 3 and complex 1 through an unobserved sigma-silane intermediate. In addition, an attempt to characterize the sigma methane complex via reaction of complex 1 with CH3OTf yields complex 2 and free methane. On the other hand, reaction of Ru(OTf)(Tpms)(PPh3)(2)] 2 with H-2 and PhMe2SiH at low temperature resulted in sigma-H-2, 3 and a probable sigma-silane complexes, respectively. However, no sigma-methane complex was observed for the reaction of complex 2 with methane even at low temperature. (C) 2014 Elsevier B. V. All rights reserved.

Time resolved terahertz spectroscopy of low frequency electronic resonances and optical pump-induced terahertz photoconductivity in reduced graphene oxide membrane

Towards ultrafast optoelectronic applications of single and a few layer reduced graphene oxide (RGO), we study time domain terahertz spectroscopy and optical pump induced changes in terahertz conductivity of self-supported RGO membrane in the spectral window of 0.5-3.5 THz. The real and imaginary parts of conductivity spectra clearly reveal low frequency resonances, attributed to the energy gaps due to the van Hove singularities in the density of states flanking the Dirac points arising due to the relative rotation of the graphene layers. Further, optical pump induced terahertz conductivity is positive, pointing to the dominance of intraband scattering processes. The relaxation dynamics of the photo-excited carriers consists of three cooling pathways: the faster (similar to 450 fs) one due to optical phonon emission followed by disorder mediated large momentum and large energy acoustic phonon emission with a time constant of a few ps (called the super-collision mechanism) and a very large time (similar to 100 ps) arising from the deep trap states. The frequency dependence of the dynamic conductivity at different delay times is analyzed in term of Drude-Smith model. (C) 2014 Published by Elsevier Ltd.

Instabilities in a fluid overlying an inclined anisotropic and inhomogeneous porous layer

In this paper, linear stability analysis on a Newtonian fluid film flowing under the effect of gravity over an inclined porous medium saturated with the same fluid in isothermal condition is carried out. The focus is placed on the effect of the anisotropic and inhomogeneous variations in the permeability of the porous medium on the shear mode and surface mode instabilities. The fluid-porous system is modelled by a coupled two-dimensional Navier-Stokes/Darcy problem. The perturbation equations are solved numerically using the Chebyshev collocation method. Detailed stability characteristics as a function of the depth ratio (the ratio of the depth of the fluid layer to that of the porous layer), the anisotropic parameter (the ratio of the permeability in the direction of the basic flow to that in the direction transverse to the basic flow) and the inhomogeneity functions are presented.

An analysis on overall crack-number-density of short-fatigue-cracks

The evolution of dispersed short-fatigue-cracks is analysed based on the equilibrium of crack-number-density (CND). By separating the mean value and the stochastic fluctuation of local CND, the equilibrium equation of overall CND is derived. Comparing with the mean-field equilibrium equation, the equilibrium equation of overall CND has different forms in the expression of crack-nucleation-rate or crack-growth-rate. The simulation results are compared with experimental measurements showing the stochastic analyses provide consistent tendency with experiments. The discrepancy in simulation results between overall CND and mean-field CND is discussed.

Estudio del crecimiento del camarón de agua dulce (M rosenbergu), en condiciones semi-intensivas en la comunidad de Alos Encuentros, Municipio de Limay, Esteli

Con el propósito de determinar el comportamiento de rasgos de crecimiento del camarón de agua dulce M. rosenbergii. Se montó un ensayo en la comunidad de los Encuentros, municipio de Limay, Estelí. Para tal efecto se utilizaron tres estanques de tierra de 200m 3 c/u en los que se sembraron 5 post larvas/m2. La alimentación fue a base de concentrado con 35%, 25%, 20% de proteína respectivamente de manera igual para los tres estanques. Se efectuaron muestreos, de talla, peso con respecto a la edad siendo estos el primer muestreo al momento de la siembra el segundo a los 30 días y los restantes cada 20 días, hasta los 190 días que culminó el ensayo, para determinar el crecimiento de los camarones de agua dulce M. rosenhergií mediante análisis estadísticos se empleó el modelo no lineal sugerido por Pearl-read (1923) y = k/1+bea:. Para realizar un menor ajuste de los datos se procedió a linealizarlos por medio de una regresión con la ecuación: Ln (k/y)-1 = Lnb±ax. Para el primer estanque se construyó el modelo Ln(k/y)-1 = 6.69459 = 0.97948 (cm), el error estándar para Lnb y a son de 0.338010.57300 respectivamente, laPr> ltl iguala 1.0001con r2 = 0.976605 y C.V= 29.66412. En el segundo estanque se obtuvo Ln(kly)-1 = 6.53469- 0.89897 (cm) el error standard para Lnb y a son de 0.4235;0.6858. La Pr > ltl para ambos son de 0.0001 con r1 = 0.96084 y C.V= 36.20477, para el tercer estanque se tiene valores de Ln (k/y)-1 = 6.93459- 1.116595 (cm) con error standard de Lnb y a = 1.04923; 0.180752 y para Pr > ltl fue de 0.0003;0.0005 con un r2= 0.8450 y C.V = 126.7102, al hacer un análisis de regresión combinando los tres estanques se obtuvo valores deLn(k/y)-1 = 5.5224-0.8068 (cm) con errores standard de Lnb y a= O.2878; 0.480 y para Pr > ltl fue de 0.0001 con un r2=; 0.9700 y C.V = 31.489, el comportamiento de crecimiento de los camarones de agua dulce M. rosenbergii sometidos a estudio bajo las mismas condiciones de cultivo tuvieron diferencias de talla y peso siendo éstas de 0.331 cm; 2.S02 g. del estanque 2 vs estanque 1; 1.093 cm, 4.3500 g del estanque 2 vs estanque 3 y 0.762 cm; 1.848 g para el estanque 1 vs estanque 3, sin embargo para los estanques en estudio se observó un aumento de talla y peso entre los 110-130 días de edad.

Efecto de diferentes leguminosas como cultivos antecesores sobre el crecimiento, desarrollo y rendimiento del sorgo (Sorghum bicolor (L) Moench) y maíz (Zea mays L.)

Con la finalidad de estudiar el comportamiento del crecimiento, desarrollo y rendimiento de los cultivos de sorgo (Sorghum bicolor. L. Moench) híbrido D-55 y maíz (Zea mays L) variedad NB-30, bajo los efectos de diferentes cultivos leguminosos: Maní (Arachis hypogaea L. ), caupí (Vigna unguiculata L. Walp), soya (Glycine max L. Merril) y frijol común ( Phaseolus vulgaris L.) como cultivos antecesores, se realizó un experimento de campo, utilizando un diseño de Bloques Completos al Azar con doce tratamientos y cuatro repeticiones realizados durante la siembra de primera y postrera de 1991, en el Centro Experimental La Compañía; Carazo, cuyo suelos son de topografía plana, textura media, franco limoso ( Typic Durandept ). De los resultados obtenidos se llegó a la conclusión que los diferentes cultivos leguminosos influyeron sobre el crecimiento, desarrollo y rendimiento de los cultivos de sorgo y maíz, ya que estos fueron afectados de manera significativa por los cultivos antecesores. Por otro lado se comprobó que el sorgo y el maíz, cuando tienen como cultivo antecesor a las leguminosas, sus rendimientos fueron superiores que cuando se tiene al sorgo y al maíz como cultivo antecesor. De las leguminosas, el cultivo de maní tuvo un mayor efecto sobre el rendimiento del sorgo y maíz. (4,391 y 1,675 kg/ha respectivamente). Se comprobó cuantitativamente el efecto negativo de utilizar a los cultivos de sorgo y maíz como cultivos antecesores a su mismo cultivo, ya que los rendimientos disminuyen considerablemente, siendo estos los siguientes: sorgo-sorgo obtuvo 2,170 kg/ha., maíz-sorgo dio un rendimiento de 2,373 kg/ha, maíz-maíz presentó 762 kg/ha, y finalmente el tratamiento sorgo-maíz rindió 674 kg/ha.

Efecto de fertilizantes orgánicos y sintéticos en el crecimiento y rendimiento del cultivo de soya (Glycine max (L) merrill), El Plantel, Masaya, 2009

El ensayo fue establecido en la finca El Plantel, propiedad de la Universidad Nacional Agraria, kilómetro 42 ½ de la carretera Masaya – Tipitapa. C on el objetivo de evaluar el efecto de los abonos orgánicos y sintéticos sobr e el crecimiento y rendimiento del cultivo de soya. El material vegetal utilizado fue la variedad CEA-CH-86. Se utilizó un diseño experimental de parcelas apareadas, el cual cons iste en el establecimiento de dos tratamientos con cuatro sub repeticiones po r tratamiento, con un área de 84m 2 por subrepetición. La fertilización orgánica se realizó con compost, hum us de lombriz y biofertilizante en dosis de 10,000 kg ha -1 , 4,488 kg ha -1 y 4,762 l ha -1 , respectivamente, el fertilizante sintético aplicado fue completo (12-30-10) y ureá 46% en dosis de 382 y 119.04 kg ha -1 , respectivamente. Las variables de crecimiento evaluada s fueron, días a emergencia (%), altura de la planta (cm) y diámetro del tallo (mm). Al momento de la cos echa; altura de inserción de la primera vaina (cm), número de vainas por planta, número de granos por vainas, peso de mil granos (g), rendimiento del grano en kg ha -1 . Las variables evaluadas fueron sometidas a un análisis de varianza (ANDEVA) y análisis de correlación entre el rendimient o y sus componentes a través del programa estadístico JMP 7 y se realizó un aná lisis económico para ev aluar la rentabilidad de los tratamientos y de esta forma ofrecer alternativas económicas a pequeños y medianos productores. En base a los resultados obtenid os, se concluye que no existe diferencia significativa en cuanto a la ap licación de los tratamientos con fertilizantes orgánicos y sintéticos, sobre las variables evaluadas. El mayor rendimiento lo presentó el tratamiento orgánico con 1,816.61 kg ha -1 , seguido del tratamiento sintético con 1,318.38kg ha -1 sin ser estadísticamente diferentes. El análisis económic o indica que el tratamiento con fertilizantes sintéticos presenta el menor costo variable (C$ 9,021.8) y el mayor beneficio neto con (C$ 2,843.6)

Deflections and curvatures of a film-substrate structure with the presence of gradient stress in MEMS applications

The close form solutions of deflections and curvatures for a film-substrate composite structure with the presence of gradient stress are derived. With the definition of more precise kinematic assumption, the effect of axial loading due to residual gradient stress is incorporated in the governing equation. The curvature of film-substrate with the presence of gradient stress is shown to be nonuniform when the axial loading is nonzero. When the axial loading is zero, the curvature expressions of some structures derived in this paper recover the previous ones which assume the uniform curvature. Because residual gradient stress results in both moment and axial loading inside the film-substrate composite structure, measuring both the deflection and curvature is proposed as a safe way to uniquely determine the residual stress state inside a film-substrate composite structure with the presence of gradient stress.