10,429 research outputs found

    Rayleigh-Brillouin light scattering spectroscopy of nitrous oxide (N2_2O)

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    High signal-to-noise and high-resolution light scattering spectra are measured for nitrous oxide (N2_2O) gas at an incident wavelength of 403.00 nm, at 90∘^\circ scattering, at room temperature and at gas pressures in the range 0.5−40.5-4 bar. The resulting Rayleigh-Brillouin light scattering spectra are compared to a number of models describing in an approximate manner the collisional dynamics and energy transfer in this gaseous medium of this polyatomic molecular species. The Tenti-S6 model, based on macroscopic gas transport coefficients, reproduces the scattering profiles in the entire pressure range at less than 2\% deviation at a similar level as does the alternative kinetic Grad's 6-moment model, which is based on the internal collisional relaxation as a decisive parameter. A hydrodynamic model fails to reproduce experimental spectra for the low pressures of 0.5-1 bar, but yields very good agreement (<1< 1\%) in the pressure range 2−42-4 bar. While these three models have a different physical basis the internal molecular relaxation derived can for all three be described in terms of a bulk viscosity of ηb∼(6±2)×10−5\eta_b \sim (6 \pm 2) \times 10^{-5} Pa⋅\cdots. A 'rough-sphere' model, previously shown to be effective to describe light scattering in SF6_6 gas, is not found to be suitable, likely in view of the non-sphericity and asymmetry of the N-N-O structured linear polyatomic molecule

    Analysis of Mesostructure Unit Cells Comprised of Octet-truss Structures

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    A unit truss finite element analysis method allowing non-linear deformation is employed to analyze a unit cell comprised of n 3 octet-truss structures for their stiffness and displacement compared to their relative density under loading. Axial, bending, shearing, and torsion effects are included in the analysis for each strut in the octet-truss structure which is then related to the mesostructure level (unit cell). The versatility of additive manufacturing allows for the fabrication of these complex unit cell truss structures which can be used as building blocks for macro-scale geometries. The finite element calculations are compared to experimental results for samples manufactured on a Stereolithography Apparatus (SLA) out of a standard resin.Mechanical Engineerin

    Nonlinear Aerodynamic and Aeroelastic Model Reduction using a Discrete Empirical Interpolation Method

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    First-principles predicted low-energy structures of NaSc(BH4)4

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    According to previous interpretations of experimental data, sodium-scandium double-cation borohydride NaSc(BH4_4)4_4 crystallizes in the crystallographic space group CmcmCmcm where each sodium (scandium) atom is surrounded by six scandium (sodium) atoms. A careful investigation of this phase based on \textit{ab initio} calculations indicates that the structure is dynamically unstable and gives rise to an energetically and dynamically more favorable phase with C2221C222_1 symmetry and nearly identical x-ray diffraction pattern. By additionally performing extensive structural searches with the minima-hopping method we discover a class of new low-energy structures exhibiting a novel structural motif in which each sodium (scandium) atom is surrounded by four scandium (sodium) atoms arranged at the corners of either a rectangle with nearly equal sides or a tetrahedron. These new phases are all predicted to be insulators with band gaps of 7.9−8.27.9-8.2 eV. Finally, we estimate the influence of these structures on the hydrogen-storage performance of NaSc(BH4_4)4_4.Comment: Version publishe

    Frustrated multiband superconductivity

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    We show that a clean multiband superconductor may display one or several phase transitions with increasing temperature from or to frustrated configurations of the relative phases of the superconducting order parameters. These transitions may occur when more than two bands are involved in the formation of the superconducting phase and when the number of repulsive interband interactions is odd. These transitions are signalled by slope changes in the temperature dependence of the superconducting gaps.Comment: 5 pages, 3 figure
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