25,665 research outputs found

    Calculation of subsonic and supersonic steady and unsteady aerodynamic forces using velocity potential aerodynamic elements

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    Expressions for calculation of subsonic and supersonic, steady and unsteady aerodynamic forces are derived, using the concept of aerodynamic elements applied to the downwash velocity potential method. Aerodynamic elements can be of arbitrary out of plane polygon shape, although numerical calculations are restricted to rectangular elements, and to the steady state case in the supersonic examples. It is suggested that the use of conforming, in place of rectangular elements, would give better results. Agreement with results for subsonic oscillating T tails is fair, but results do not converge as the number of collocation points is increased. This appears to be due to the form of expression used in the calculations. The methods derived are expected to facilitate automated flutter analysis on the computer. In particular, the aerodynamic element concept is consistent with finite element methods already used for structural analysis. The method is universal for the complete Mach number range, and, finally, the calculations can be arranged so that they do not have to be repeated completely for every reduced frequency

    Higgs bosons of a supersymmetric E6E_6 model at the Large Hadron Collider

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    It is found that CP symmetry may be explicitly broken in the Higgs sector of a supersymmetric E6E_6 model with two extra neutral gauge bosons at the one-loop level. The phenomenology of the model, the Higgs sector in particular, is studied for a reasonable parameter space of the model, in the presence of explicit CP violation at the one-loop level. At least one of the neutral Higgs bosons of the model might be produced via the WWWW fusion process at the Large Hadron Collider.Comment: 23 pages, 5 figures, JHE

    Explicit CP violation in a MSSM with an extra U(1)′U(1)'

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    We study that a minimal supersymmetric standard model with an extra U(1)′U(1)' gauge symmetry may accommodate the explicit CP violation at the one-loop level through radiative corrections. This model is CP conserving at the tree level and cannot realize the spontaneous CP violation for a wide parameter space at the one-loop level. In explicit CP violation scenario, we calculate the Higgs boson masses and the magnitude of the scalar-pseudoscalar mixings in this model at the one-loop level by taking into account the contributions of top quarks, bottom quarks, exotic quarks, and their superpartners. In particular, we investigate how the exotic quarks and squarks would affect the scalar-pseudoscalar mixings. It is observed that the size of the mixing between the heaviest scalar and pseudoscalar Higgs bosons is changed up to 20 % by a complex phase originated from the exotic quark sector of this model.Comment: 19 pages, 3 figure

    Optical Response of Solid CO2_2 as a Tool for the Determination of the High Pressure Phase

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    We report first-principles calculations of the frequency dependent linear and second-order optical properties of the two probable extended-solid phases of CO2_2--V, i.e. I4ˉ2dI\bar42d and P212121P2_12_12_1. Compared to the parent CmcaCmca phase the linear optical susceptibility of both phases is much smaller. We find that I4ˉ2dI\bar42d and P212121P2_12_12_1 differ substantially in their linear optical response in the higher energy regime. The nonlinear optical responses of the two possible crystal structures differ by roughly a factor of five. Since the differences in the nonlinear optical spectra are pronounced in the low energy regime, i.e. below the band gap of diamond, measurements with the sample inside the diamond anvil cell are feasible. We therefore suggest optical experiments in comparison with our calculated data as a tool for the unambiguous identification of the high pressure phase of CO2_2.Comment: 4 pages 2 fig

    Higgs bosons of a supersymmetric U(1)′U(1)' model at the ILC

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    We study the scalar Higgs sector of the next-to-minimal supersymmetric standard model with an extra U(1), which has two Higgs doublets and a Higgs singlet, in the light leptophobic Z′Z' scenario where the extra neutral gauge boson Z′Z' does not couple to charged leptons. In this model, we find that the sum of the squared coupling coefficients of the three neutral scalar Higgs bosons to ZZZZ, normalized by the corresponding SM coupling coefficient is noticeably smaller than unity, due to the effect of the extra U(1), for a reasonable parameter space of the model, whereas it is unity in the next-to-minimal supersymmetric standard model. Thus, these two models may be distinguished if the coupling coefficients of neutral scalar Higgs bosons to ZZZZ are measured at the future International Linear Collider by producing them via the Higgs-strahlung, ZZZZ fusion, and WWWW fusion processes.Comment: 12 pages, 2 figures, 1 table, PR

    Stabilizing the forming process in unipolar resistance switching using an improved compliance current limiter

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    The high reset current IR in unipolar resistance switching now poses major obstacles to practical applications in memory devices. In particular, the first IR-value after the forming process is so high that the capacitors sometimes do not exhibit reliable unipolar resistance switching. We found that the compliance current Icomp is a critical parameter for reducing IR-values. We therefore introduced an improved, simple, easy to use Icomp-limiter that stabilizes the forming process by drastically decreasing current overflow, in order to precisely control the Icomp- and subsequent IR-values.Comment: 15 pages, 4 figure

    Chaos at the border of criticality

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    The present paper points out to a novel scenario for formation of chaotic attractors in a class of models of excitable cell membranes near an Andronov-Hopf bifurcation (AHB). The mechanism underlying chaotic dynamics admits a simple and visual description in terms of the families of one-dimensional first-return maps, which are constructed using the combination of asymptotic and numerical techniques. The bifurcation structure of the continuous system (specifically, the proximity to a degenerate AHB) endows the Poincare map with distinct qualitative features such as unimodality and the presence of the boundary layer, where the map is strongly expanding. This structure of the map in turn explains the bifurcation scenarios in the continuous system including chaotic mixed-mode oscillations near the border between the regions of sub- and supercritical AHB. The proposed mechanism yields the statistical properties of the mixed-mode oscillations in this regime. The statistics predicted by the analysis of the Poincare map and those observed in the numerical experiments of the continuous system show a very good agreement.Comment: Chaos: An Interdisciplinary Journal of Nonlinear Science (tentatively, Sept 2008

    Learning bodies: What do teachers learn from embodied practice?

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    © 2016, Western Australian Institute for Educational Research Inc. All rights reserved. In this article, we reflect on ways that young adolescents learn through embodied practice, which we define as moments when the body is ‘caught up’ in learning activities. Our observations draw from two workshops conducted as part of the IMC Sky High! program which annually involves over 150 Year 7 and 8 students from schools in low socioeconomic areas of south-west Sydney, Australia. The program is delivered on and off campus by a team at the University of Technology Sydney. In addition to building confidence and skill in curriculum areas, the program aims to introduce young high school students to a tertiary environment and motivate them to engage more actively at school. Paying close attention to a classical music encounter and a trip to a museum, we use ethnographic strategies to consider how looking, doing, listening and proximity facilitate feelings of connection and motivation towards learning. We discuss how an educators’ sensitivity to the listening and speaking body, and the learning and caring body can enhance learning design and opportunities for engagement. Greater awareness of embodiment can enable educators to facilitate rich, sensory learning encounters that are empowering and transformative
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