16,489 research outputs found

    Integral-method analysis for a hypersonic viscous shock layer with mass injection

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    Integral method analysis for hypersonic viscous shock layer with mass injectio

    Writing-skills Intervention Programming and Its Being a Component of Response to Intervention

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    For a struggling writer, step-by-step instruction can be a helpful means to manage organizing and producing elaborate text. This mixed-methods project offered four struggling writers a mnemonic strategy called Ask, Reflect, Text (ART) in 45-minute sessions over 22 days. The second- and fourth-grade students attended a public school in the US Pacific Northwest. As a parallel component to the project, the students' teachers and intervention specialist met with the author for 4 one-hour sessions to discuss: 1) the children's intervention programming and progress, and 2) the paradigm of response to intervention (RTI) and their thoughts about its feasibility in classrooms. The end-of-project assessment data demonstrated that the children made progress with writing skills, but the teachers and intervention specialist felt that support personnel would be needed to manage RTI-type intervention programming in general education classrooms

    Photon signature analysis using template matching

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    We describe an approach to detect improvised explosive devices (IEDs) by using a template matching procedure. This approach relies on the signature due to backstreaming ? photons from various targets. In this work we have simulated cylindrical targets of aluminum, iron, copper, water and ammonium nitrate (nitrogen-rich fertilizer). We simulate 3.5 MeV source photons distributed on a plane inside a shielded area using Monte Carlo N-Particle (MCNP TM) code version 5 (V5). The 3.5 MeV source gamma rays yield 511 keV peaks due to pair production and scattered gamma rays. In this work, we simulate capture of those photons that backstream, after impinging on the target element, toward a NaI detector. The captured backstreamed photons are expected to produce a unique spectrum that will become part of a simple signal processing recognition system based on the template matching method. Different elements were simulated using different sets of random numbers in the Monte Carlo simulation. To date, the sum of absolute differences (SAD) method has been used to match the template. In the examples investigated, template matching was found to detect all elements correctly

    On the Use of Group Theoretical and Graphical Techniques toward the Solution of the General N-body Problem

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    Group theoretic and graphical techniques are used to derive the N-body wave function for a system of identical bosons with general interactions through first-order in a perturbation approach. This method is based on the maximal symmetry present at lowest order in a perturbation series in inverse spatial dimensions. The symmetric structure at lowest order has a point group isomorphic with the S_N group, the symmetric group of N particles, and the resulting perturbation expansion of the Hamiltonian is order-by-order invariant under the permutations of the S_N group. This invariance under S_N imposes severe symmetry requirements on the tensor blocks needed at each order in the perturbation series. We show here that these blocks can be decomposed into a basis of binary tensors invariant under S_N. This basis is small (25 terms at first order in the wave function), independent of N, and is derived using graphical techniques. This checks the N^6 scaling of these terms at first order by effectively separating the N scaling problem away from the rest of the physics. The transformation of each binary tensor to the final normal coordinate basis requires the derivation of Clebsch-Gordon coefficients of S_N for arbitrary N. This has been accomplished using the group theory of the symmetric group. This achievement results in an analytic solution for the wave function, exact through first order, that scales as N^0, effectively circumventing intensive numerical work. This solution can be systematically improved with further analytic work by going to yet higher orders in the perturbation series.Comment: This paper was submitted to the Journal of Mathematical physics, and is under revie

    Estimates of nonequilibrium ionization phenomena in the inviscid Apollo plasma sheath

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    Nonequilibrium ionization in asymmetric plasma sheath determined for Apollo spacecraft at superorbital velocity reentr

    Vacuum-UV negative photoion spectroscopy of CF3Cl, CF3Br and CF3I

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    Using synchrotron radiation negative ions have been detected by mass spectrometry following vacuum-UV photoexcitation of trifluorochloromethane (CF3_3Cl), trifluorobromomethane (CF3_3Br) and trifluoroiodomethane (CF3_3I). The anions F^-, X^-, F2_2^-, FX^-, CF^-, CF2_2^- and CF3_3^- were observed from all three molecules, where X = Cl, Br or I, and their ion yields recorded in the range 8-35 eV. With the exception of Br^- and I^-, the anions observed show a linear dependence of signal with pressure, showing that they arise from unimolecular ion-pair dissociation. Dissociative electron attachment, following photoionization of CF3_3Br and CF3_3I as the source of low-energy electrons, is shown to dominate the observed Br^- and I^- signals, respectively. Cross sections for ion-pair formation are put on to an absolute scale by calibrating the signal strengths with those of F^- from both SF6_6 and CF4_4. These anion cross sections are normalized to vacuum-UV absorption cross sections, where available, and the resulting quantum yields are reported. Anion appearance energies are used to calculate upper limits to 298 K bond dissociation energies for D0D^0(CF3_3-X) which are consistent with literature values. We report new data for D0D^0(CF2_2I^--F) ≤ 2.7 ± 0.2 eV and ΔfH2980\Delta_fH^0_{298} (CF2_2I+^+) ≤ (598 ± 22) kJ mol1^{-1}. No ion-pair formation is observed below the ionization energy of the parent molecule for CF3_3Cl and CF3_3Br, and only weak signals (in both I^- and F^-) are detected for CF3_3I. These observations suggest neutral photodissociation is the dominant exit channel to Rydberg state photoexcitation at these lower energies
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