53 research outputs found

    Sixth Drag Prediction Workshop Results Using FUN3D with k-kL-MEAH2015 Turbulence Model

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    The Common Research Model wing-body configuration is investigated with the k-kL-MEAH2015 turbulence model implemented in FUN3D. This includes results presented at the Sixth Drag Prediction Workshop and additional results generated after the workshop with a nonlinear Quadratic Constitutive Relation (QCR) variant of the same turbulence model. The workshop provided grids are used, and a uniform grid refinement study is performed at the design condition. A large variation between results with and without a reconstruction limiter is exhibited on medium grid sizes, indicating that the medium grid size is too coarse for drawing conclusions in comparison with experiment. This variation is reduced with grid refinement. At a fixed angle of attack near design conditions, the QCR variant yielded decreased lift and drag compared with the linear eddy-viscosity model by an amount that was approximately constant with grid refinement. The k-kL-MEAH2015 turbulence model produced wing root junction flow behavior consistent with wind tunnel observations

    Symbiotic modeling: Linguistic Anthropology and the promise of chiasmus

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    Reflexive observations and observations of reflexivity: such agendas are by now standard practice in anthropology. Dynamic feedback loops between self and other, cause and effect, represented and representamen may no longer seem surprising; but, in spite of our enhanced awareness, little deliberate attention is devoted to modeling or grounding such phenomena. Attending to both linguistic and extra-linguistic modalities of chiasmus (the X figure), a group of anthropologists has recently embraced this challenge. Applied to contemporary problems in linguistic anthropology, chiasmus functions to highlight and enhance relationships of interdependence or symbiosis between contraries, including anthropology’s four fields, the nature of human being and facets of being human

    Long-term modification of cortical synapses improves sensory perception

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    Synapses and receptive fields of the cerebral cortex are plastic. However, changes to specific inputs must be coordinated within neural networks to ensure that excitability and feature selectivity are appropriately configured for perception of the sensory environment. Long-lasting enhancements and decrements to rat primary auditory cortical excitatory synaptic strength were induced by pairing acoustic stimuli with activation of the nucleus basalis neuromodulatory system. Here we report that these synaptic modifications were approximately balanced across individual receptive fields, conserving mean excitation while reducing overall response variability. Decreased response variability should increase detection and recognition of near-threshold or previously imperceptible stimuli, as we found in behaving animals. Thus, modification of cortical inputs leads to wide-scale synaptic changes, which are related to improved sensory perception and enhanced behavioral performance

    Planck intermediate results: II. Comparison of sunyaev-zeldovich measurements from planck and from the arcminute microkelvin imager for 11 galaxy clusters

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    Spectacular sulfides from the Merelani tanzanite deposit, Lelatema Mountains, Manyara Region, Tanzania

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    Outstanding specimens of several sulfide minerals from the Merelani tanzanite deposit have recently become available, including rare wurtzite in giant, deep red-brown, partially gemmy, well-formed crystals, lustrous black alabandite and form-rich pyrite with exceptional luster. Other sulfides identified include sphalerite, chalcopyrite, millerite, stannite, tennantite-tetrahedrite, sharp microcrystals of clausthalite and rare colusite-germanocolusite

    Lead-tellurium oxysalts from Otto Mountain near Baker, California: VII. Chromschieffelinite, Pb_(10)Te_6O_(20)(OH)_(14)(CrO_4)(H_2O)_5, the chromate analog of schieffelinite

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    Chromschieffelinite, Pb-(10)Te_6O_(20)(OH)_(14)(CrO_4)(H_2O)_5, is a new tellurate from Otto Mountain near Baker, California, named as the chromate analog of schieffelinite, Pb_(10)Te_6O_(20)(OH)_(14)(SO_4)(H_2O)_5. The new mineral occurs in a single 1 mm vug in a quartz vein. Associated mineral species include: chalcopyrite, chrysocolla, galena, goethite, hematite, khinite, pyrite, and wulfenite. Chromschieffelinite is orthorhombic, space group C222_1, a = 9.6646(3), b = 19.4962(8), c = 10.5101(7) Å, V = 1980.33(17) Å3, and Z = 2. Crystals are blocky to tabular on {010} with striations parallel to [001]. The forms observed are {010}, {210}, {120}, {150}, {180}, {212}, and {101}, and crystals reach 0.2 mm in maximum dimension. The color and streak are pale yellow and the luster is adamantine. The Mohs hardness is estimated at 2. The new mineral is brittle with irregular fracture and one perfect cleavage on {010}. The calculated density based on the ideal formula is 5.892 g/cm^3. Chromschieffelinite is biaxial (−) with indices of refraction α = 1.930(5), β = 1.960(5), and γ = 1.975(5), measured in white light. The measured 2V is 68(2)°, the dispersion is strong, r < v, and the optical orientation is X = b, Y = c, Z = a. No pleochroism was observed. Electron microprobe analysis provided: PbO 59.42, TeO_3 29.08, CrO_3 1.86, H_2O 6.63 (structure), total 96.99 wt%; the empirical formula (based on 6 Te) is Pb_(9.65)Te_6O_(19.96)(OH)_(14.04)(CrO_4)_(0.67)(H_2O)_(6.32). The strongest powder X-ray diffraction lines are [d_(obs) in Å (hkl) I]: 9.814 (020) 100, 3.575 (042,202) 41, 3.347 (222) 44, 3.262 (241,060,113) 53, 3.052 (311) 45, 2.9455 (152,133) 55, 2.0396 (115,353) 33, and 1.6500 (multiple) 33. The crystal structures of schieffelinite (R_1 = 0.0282) and chromschieffelinite (R_1 = 0.0277) contain isolated Te^(6+)O_6 octahedra and Te_2^(6+)O_(11) corner-sharing dimers, which are linked into a three-dimensional framework via bonds to Pb2+ atoms. The framework has large channels along c, which contain disordered SO_4 or CrO_4 groups and H_2O. The lone-electron pair of each Pb^(2+) is stereochemically active, resulting in one-sided Pb-O coordination arrangements. The short Pb-O bonds of the Pb^(2+) coordinations are all to Te^(6+)O_6 octahedra, resulting in strongly bonded layers parallel to {010}, which accounts for the perfect {010} cleavage
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