Ranking general circulation models for India using TOPSIS

Eleven general circulation models/global climate models (GCMs) - BCCR-BCCM2.0, INGV-ECHAM4, GFDL2.0, GFDL2.1, GISS, IPSL-CM4, MIROC3, MRI-CGCM2, NCAR-PCMI, UKMO-HADCM3 and UKMO-HADGEM1 - are evaluated for Indian climate conditions using the performance indicator, skill score (SS). Two climate variables, temperature T (at three levels, i.e. 500, 700, 850 mb) and precipitation rate (Pr) are considered resulting in four SS-based evaluation criteria (T500, T700, T850, Pr). The multicriterion decision-making method, technique for order preference by similarity to an ideal solution, is applied to rank 11 GCMs. Efforts are made to rank GCMs for the Upper Malaprabha catchment and two river basins, namely, Krishna and Mahanadi (covered by 17 and 15 grids of size 2.5 degrees x 2.5 degrees, respectively). Similar efforts are also made for India (covered by 73 grid points of size 2.5 degrees x 2.5 degrees) for which an ensemble of GFDL2.0, INGV-ECHAM4, UKMO-HADCM3, MIROC3, BCCR-BCCM2.0 and GFDL2.1 is found to be suitable. It is concluded that the proposed methodology can be applied to similar situations with ease.

Physical Layer Data Fusion Via Distributed Co-Phasing With General Signal Constellations

This paper studies a pilot-assisted physical layer data fusion technique known as Distributed Co-Phasing (DCP). In this two-phase scheme, the sensors first estimate the channel to the fusion center (FC) using pilots sent by the latter; and then they simultaneously transmit their common data by pre-rotating them by the estimated channel phase, thereby achieving physical layer data fusion. First, by analyzing the symmetric mutual information of the system, it is shown that the use of higher order constellations (HOC) can improve the throughput of DCP compared to the binary signaling considered heretofore. Using an HOC in the DCP setting requires the estimation of the composite DCP channel at the FC for data decoding. To this end, two blind algorithms are proposed: 1) power method, and 2) modified K-means algorithm. The latter algorithm is shown to be computationally efficient and converges significantly faster than the conventional K-means algorithm. Analytical expressions for the probability of error are derived, and it is found that even at moderate to low SNRs, the modified K-means algorithm achieves a probability of error comparable to that achievable with a perfect channel estimate at the FC, while requiring no pilot symbols to be transmitted from the sensor nodes. Also, the problem of signal corruption due to imperfect DCP is investigated, and constellation shaping to minimize the probability of signal corruption is proposed and analyzed. The analysis is validated, and the promising performance of DCP for energy-efficient physical layer data fusion is illustrated, using Monte Carlo simulations.

General framework for acoustic emission during plastic deformation

Despite the long history, so far there is no general theoretical framework for calculating the acoustic emission spectrum accompanying any plastic deformation. We set up a discrete wave equation with plastic strain rate as a source term and include the Rayleigh-dissipation function to represent dissipation accompanying acoustic emission. We devise a method of bridging the widely separated time scales of plastic deformation and elastic degrees of freedom. While this equation is applicable to any type of plastic deformation, it should be supplemented by evolution equations for the dislocation microstructure for calculating the plastic strain rate. The efficacy of the framework is illustrated by considering three distinct cases of plastic deformation. The first one is the acoustic emission during a typical continuous yield exhibiting a smooth stress-strain curve. We first construct an appropriate set of evolution equations for two types of dislocation densities and then show that the shape of the model stress-strain curve and accompanying acoustic emission spectrum match very well with experimental results. The second and the third are the more complex cases of the Portevin-Le Chatelier bands and the Luders band. These two cases are dealt with in the context of the Ananthakrishna model since the model predicts the three types of the Portevin-Le Chatelier bands and also Luders-like bands. Our results show that for the type-C bands where the serration amplitude is large, the acoustic emission spectrum consists of well-separated bursts of acoustic emission. At higher strain rates of hopping type-B bands, the burst-type acoustic emission spectrum tends to overlap, forming a nearly continuous background with some sharp acoustic emission bursts. The latter can be identified with the nucleation of new bands. The acoustic emission spectrum associated with the continuously propagating type-A band is continuous. These predictions are consistent with experimental results. More importantly, our study shows that the low-amplitude continuous acoustic emission spectrum seen in both the type-B and type-A band regimes is directly correlated to small-amplitude serrations induced by propagating bands. The acoustic emission spectrum of the Luders-like band matches with recent experiments as well. In all of these cases, acoustic emission signals are burstlike, reflecting the intermittent character of dislocation-mediated plastic flow.

Necessary and sufficient conditions for optimality in constrained general sum stochastic games

In this paper we first derive a necessary and sufficient condition for a stationary strategy to be the Nash equilibrium of discounted constrained stochastic game under certain assumptions. In this process we also develop a nonlinear (non-convex) optimization problem for a discounted constrained stochastic game. We use the linear best response functions of every player and complementary slackness theorem for linear programs to derive both the optimization problem and the equivalent condition. We then extend this result to average reward constrained stochastic games. Finally, we present a heuristic algorithm motivated by our necessary and sufficient conditions for a discounted cost constrained stochastic game. We numerically observe the convergence of this algorithm to Nash equilibrium. (C) 2015 Elsevier B.V. All rights reserved.

Ancilla-assisted measurements on quantum ensembles: general protocols and applications in NMR quantum information processing

Quantum ensembles form easily accessible architectures for studying various phenomena in quantum physics, quantum information science and spectroscopy. Here we review some recent protocols for measurements in quantum ensembles by utilizing ancillary systems. We also illustrate these protocols experimentally via nuclear magnetic resonance techniques. In particular, we shall review noninvasive measurements, extracting expectation values of various operators, characterizations of quantum states and quantum processes, and finally quantum noise engineering.

General relativity and relativistic astrophysics

Einstein established the theory of general relativity and the corresponding field equation in 1915 and its vacuum solutions were obtained by Schwarzschild and Kerr for, respectively, static and rotating black holes, in 1916 and 1963, respectively. They are, however, still playing an indispensable role, even after 100 years of their original discovery, to explain high energy astrophysical phenomena. Application of the solutions of Einstein's equation to resolve astrophysical phenomena has formed an important branch, namely relativistic astrophysics. I devote this article to enlightening some of the current astrophysical problems based on general relativity. However, there seem to be some issues with regard to explaining certain astrophysical phenomena based on Einstein's theory alone. I show that Einstein's theory and its modified form, both are necessary to explain modern astrophysical processes, in particular, those related to compact objects.

The time finite element as a robust general scheme for solving nonlinear dynamic equations including chaotic systems

Schemes that can be proven to be unconditionally stable in the linear context can yield unstable solutions when used to solve nonlinear dynamical problems. Hence, the formulation of numerical strategies for nonlinear dynamical problems can be particularly challenging. In this work, we show that time finite element methods because of their inherent energy momentum conserving property (in the case of linear and nonlinear elastodynamics), provide a robust time-stepping method for nonlinear dynamic equations (including chaotic systems). We also show that most of the existing schemes that are known to be robust for parabolic or hyperbolic problems can be derived within the time finite element framework; thus, the time finite element provides a unification of time-stepping schemes used in diverse disciplines. We demonstrate the robust performance of the time finite element method on several challenging examples from the literature where the solution behavior is known to be chaotic. (C) 2015 Elsevier Inc. All rights reserved.

The time finite element as a robust general scheme for solving nonlinear dynamic equations including chaotic systems

Schemes that can be proven to be unconditionally stable in the linear context can yield unstable solutions when used to solve nonlinear dynamical problems. Hence, the formulation of numerical strategies for nonlinear dynamical problems can be particularly challenging. In this work, we show that time finite element methods because of their inherent energy momentum conserving property (in the case of linear and nonlinear elastodynamics), provide a robust time-stepping method for nonlinear dynamic equations (including chaotic systems). We also show that most of the existing schemes that are known to be robust for parabolic or hyperbolic problems can be derived within the time finite element framework; thus, the time finite element provides a unification of time-stepping schemes used in diverse disciplines. We demonstrate the robust performance of the time finite element method on several challenging examples from the literature where the solution behavior is known to be chaotic. (C) 2015 Elsevier Inc. All rights reserved.

Timing Calculations for a General N-Level Dodecagonal Space Vector Structure Using Only Reference Phase Voltages

Multilevel inverters with dodecagonal (12-sided polygon) voltage space vector (SV) structures have advantages like extension of linear modulation range, elimination of fifth and seventh harmonics in phase voltages and currents for the full modulation range including extreme 12-step operation, reduced device voltage ratings, lesser dv/dt stresses on devices and motor phase windings resulting in lower EMI/EMC problems, and lower switching frequency-making it more suitable for high-power drive applications. This paper proposes a simple method to obtain pulsewidth modulation (PWM) timings for a dodecagonal voltage SV structure using only sampled reference voltages. In addition to this, a carrier-based method for obtaining the PWM timings for a general N-level dodecagonal structure is proposed in this paper for the first time. The algorithm outputs the triangle information and the PWM timing values which can be set as the compare values for any carrier-based hardware PWM module to obtain SV PWM like switching sequences. The proposed method eliminates the need for angle estimation, computation of modulation indices, and iterative search algorithms that are typical in multilevel dodecagonal SV systems. The proposed PWM scheme was implemented on a five-level dodecagonal SV structure. Exhaustive simulation and experimental results for steady-state and transient conditions are presented to validate the proposed method.

General Relationship Between Contact Stiffness, Contact Depth, and Mechanical Properties for Indentation in Linear Viscoelastic Solids Using Axisymmetric Indenters of Arbitrary Profiles

We derive a relationship between the initial unloading slope, contact depth, and the instantaneous relaxation modulus for indentation in linear viscoelastic solids by a rigid indenter with an arbitrary axisymmetric smooth profile. Although the same expression is well known for indentation in elastic and in elastic-plastic solids, we show that it is also true for indentation in linear viscoelastic solids, provided that the unloading rate is sufficiently fast. Furthermore, the same expression holds true for both fast loading and unloading. These results should provide a sound basis for using the relationship for determining properties of viscoelastic solids using indentation techniques.

General Solution to Two-Dimensional Nonslipping JKR Model with a Pulling Force in an Arbitrary Direction

In this paper, a generalized JKR model is investigated, in which an elastic cylinder adhesively contacts with an elastic half space and the contact region is assumed to be perfect bonding. An external pulling force is acted on the cylinder in an arbitrary direction. The contact area changes during the pull-off process, which can be predicted using the dynamic Griffith energy balance criterion as the contact edge shifts. Full coupled solution with an oscillatory singularity is obtained and analyzed by numerical calculations. The effect of Dundurs' parameter on the pull-off process is analyzed, which shows that a nonoscillatory solution can approximate the general one under some conditions, i.e., larger pulling angle (pi/2 is the maximum value), smaller a/R or larger nondimensional parameter value of Delta gamma/E*R. Relations among the contact half width, the external pulling force and the pulling angle are used to determine the pull-off force and pull-off contact half width explicitly. All the results in the present paper as basic solutions are helpful and applicable for experimenters and engineers.

Efecto de diferentes frecuencias de corte sobre la producción de materia seca del pasto Brachiaria brizantha cv. Marandú CIAT 6780, en época de verano, zona del Pacífico de Nicaragua.(Managua)

En el presente ensayo se evaluaron los efectos de cuatro frecuencias de corte (27, 32, 37, 42 días) sobre la producción de materia seca Brachiaria brizantha cv. Marandú CIAT 6780, durante la época de verano, sin fertilizar, como una forma de generar información a los productores que manejan sus pasturas en todo el País. El ensayo se realizó en el Centro Nacional de Investigación Agropecuaria CNIA/INTA entre Septiembre 1996 y Abril 1997, en el Departamento de Managua. Se utilizó un Diseño experimental de Bloques Completos al Azar. Los resultados del análisis de varianza y prueba de rangos múltiples (Tukey y Duncan) mostraron que las frecuencias de corte no tuvieron diferencias estadísticas (0.01>P<0.05) sobre la producción de materia seca , número de macolla, diámetro de macolla y materia verde. El mejor rendimiento de materia seca se obtuvo en el tratamiento de mayor frecuencia (42 días) con 2512.1 kg en todo el periodo evaluado, lo que se atribuye a que el pasto de mayor edad está más lignificado. El análisis de varianza y prueba de rangos múltiples (Tukey y Duncan), (0.01>P<0.05) reflejó que la variable altura de macolla tuvo diferencias estadísticas significativas para las diferentes frecuencias de corte evaluados. La producción total de materia seca (kg/ha) en este periodo de evaluación fue de 2512.1, 2403.1, 2383.1 y 2333.9 para los tratamientos de 42, 32, 27 y 37 días respectivamente. Es importante resaltar que para determinar el momento óptimo de corte es necesario realizar un análisis bromatológico y de digestibilidad de la materia seca del pasto en estudio.

Valor nutritivo del pasto pangola (Digitaria decumbens stent.) vr. transvala a distintos niveles de fertilización y diversas edades de corte

Este estudio Se desarrolló en el periodo de julio a diciembre de 1990 en el Centro de Investigación Zootecnia “La Polvosa” de la UCA (Universidad Centroamericana), situada en el km 23 112 de la carretera nueva a León, depto. de Managua. El centro se ubica a una elevación de 40 msnrn a 1 2 grados 12 minutos, Latitud norte y 86 grados 22 minutos, longitud oeste registra temperaturas promedio anuales de 32 grados centígrados los y unos 8OO mm de precipitación media por año, por lo cual, es posible calificar su zona agroecológica como de trópico seco se evaluó la respuesta en términos de valor nutritivo del pasto Pangola (Digitaria decumbens Stent.) vr. Transvala, utilizándose un diseño experimental en bloques completos al azar (BCA) con arreglo factorial, se estudió el efecto de dos factores (Niveles de fertilizantes-edades de cortes) con cuatro repeticiones, formándose un total de 16 tratamientos El ensayo contó con un área experimental total de 357.75 mt2 para la toma de muestras, se empleó el método del metro cuadrado realizándose en las parcelas un muestreo sin reemplazo para cada frecuencia en estudio. Previo al momento experimental, se efectúo una poda de control procediéndose después a aplicar de una sola vez los respectivos niveles de fertizante. El estudio estadístico contempló el uso del análisis de varianza (ANDEVA), se hizo una separción de medias por Tukey, y se midió la influencia porcentual (Individual y asociada) de 4 niveles de fertilizante (0, 50,100 y150 kg urea (46%N2) / mz) y 4 edades de corte (15, 30.. 45y 60 días), sobre nueve variables o componentes bromatológicos (MS, PB,FC, ELN, EE, EB (Kcal/ 100g), Cz, Ca y P). Todos los componentes bromatológicos evaluados excepto el EE.. presentaron una variación significativa (P<0.05), bajo el efecto de los factores en estudio. Los niveles de fertilizante influyeron ios valores de mayor mérito con la dosis •150 kg urea / rnz, observando la PB.. 9.76% ;el ELN, 56.54 y la EB,190.97 Kcal ,' 100 g. En tanto que los 50 kg1mz mostraron !os mayores índices en FC (28.88), EE (2.75) y Cz. (11.:39) las parcelas no fertilizadas brindaron los porcentajes más altos de MS (23.78) y Ca (0.60),y el nivel 100 kg/ mz El mejor en P (0.39) y el más bajo en FC (26.61). A su vez con O kg / mz_. Observaron sus níveles minimos la PB (6.91), el ELN (53.58). el valor energético (175.45 Kcal/ 100 g) y el P (O.28), y con 100 kg/ mz los menores en MS y Cz (25.08 y 10.38 respectivamente), a. los 150kg/mz el EE (2.29) y el Ca (0.49), rindieron sus índices más bajos. En cuanto a la frecuencia de corte, la edad 15 días presentó los máximos contenidos en PH (11.95), ELN (56.45),EB (202.40 Kcal/ 100g), EE (2.65) y el mínimo en FC (27.09). Observando el corte a los 60 días, las mayores proporciones en MS (30.91) Cz (12.43) )'Ca (0.58),en tanto que con 30 y 45 días se dieron los más altos valores de P (0.34) FC (28.55) respectivamente los índices más bajos de PB (6.48),ELN (52.63), Ca (0.47)y P (0.30), se obtuvieron a los 45 días de madurez mientras que la MS (22.88) y la Cz (9.56),alcanzaron sus valores más pequeños con 15 días de corte a los 60 días, la EB (175. 42 Kcal ./ 100g) y el EE (2.20) respondieron con sus por cientos más bajos. Para los tratamientos resultantes de la combinación de un nivel de fertilizante y una edad de corte, la interacción 50 kg/mz-60 días reportó el mayor contenido en MS (32.72), sobresaliendo el tratamiento 150 kg / mz-15 días al presentar los valores más altos en EB (214.39 Kcal/100g), PB (14.30) y ELN (59.02), aunque la combinación 50 kg/mz-30 días brindó igual valor en ELN y el máximo en Cz (13.10) con aplicaciones de 100 kg/mz y frecuencia de 15 días se obtuvieron los menores índices en FC (24.82) y Cz (9.37). Consiguiéndose en O kg / mz-15 días el valor más alto en Ca (0.76) y el menor en P (0.22), observando la MS su índice más bajo (18.37) con el tratamiento 100 kg / mz-15 días. Finalmente, en las interacciones que incluyen la frecuencia 45 días, se encontró que las parcelas no fertilizadas presentaron los menores contenidos en PB (5.02), ELN (48.95) y EB (165.44 Kcal/ 1oo g). en cambio al aplicar 100 kg /rnz, se obtuvieron (para la misma interacción) los valores más bajos en EE (1.72), Ca (0.43) y el mayor en P (0.44),en tanto los niveles 50 y 150 kg / mz influyeron los índices más altos en EE (3.85) y FC (30.75) respectivamente.

Producción de biomasa de Cratylia argentea bajo diferentes densidades de siembra y frecuencias de corte en el trópico seco de Nicaragua

El presente estudio se realizó en la finca "Santa Rosa" propiedad de la Universidad Nacional Agraria, localizada geográficamente a 12°08'15" de latitud Norte y 86°09'36" de longitud Este, en el departamento de Managua, en los meses de octubre 2001 a septiembre 2002, se utilizó un diseño de Bloques completamente al azar, con arreglo en parcelas divididas. Se evaluaron los efectos de tres densidades de siembra (40,000, 20,000 y 10,000 Plantas/ha) y tres frecuencias de corte (8, 12 y 16 semanas) sobre la producción de Biomasa de Cratylia argentea. Las variables evaluadas fueron Materia Fresca Total (MFT), Materia Fresca Fracción Fina (MFFF), Materia Fresca Fracción Gruesa (MFFG), Porcentaje de Materia Seca (PMS), Materia Seca Total (MST), Materia Seca Fracción Fina (MSFF), Altura, Tasa de Crecimiento (TC) y Ceniza. Se realizó análisis de varianza y comparaciones con la Prueba de Tukey utilizando MINITAB, versión 13.0. Los resultados en el análisis de varianza (P<0,05) mostraron que la densidad de siembra de 40,000pl/ba presentó los mayores resultados sobre las variables, MFT (59.93 Ton/ha/Año), MFFF (43.5 Ton/ha/Afio), MFFG (13.34 Ton/ha/Año), MST (14.86 Ton MS ha/Año), MSFF (10.59 Ton MS ha/Año) y TC (52.33 Kg MS ha/día), las densidades de siembra no afectaron las variables altura, TC y PMS, la frecuencia de corte de 16 semanas mostró los mejores resultados para las variables MFT (59.58 Ton/ha/Año), MFFG (15.45 Ton/ha/Año), %MS (28.51 %), MST (16.15 Ton MS ha/Año), MSFF (8.75 Ton MS/ha/Año), altura (147.74 cm), Ceniza (12.92 %) y TC (60.06 kg MS ha/día), excepto para MFFF.