• Title/Summary/Keyword: DFT topology

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Magnetic Coupling in Oxoverdazyl-Benzene-Oxoverdazyl Diradical Systems: A DFT Study

  • Park, Young Geun;Ko, Kyoung Chul
    • Proceeding of EDISON Challenge
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    • 2013.04a
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    • pp.25-35
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    • 2013
  • The intramolecular magnetic coupling constant (J) values of diradical-based magnet models (S1-S5) were studied using unrestricted density functional theory. The model systems were designed with series of oxoverdazyl radicals (o-Ver(N) and o-Ver(C)) linked through a benzene coupler. They were divided according to either connectivity of the radical (C or N) or geometrical topology (meta- and para-) of benzene coupler. Reasonable relationship was found between spin density distribution and sign of J value. With our results we determined ferromagnetic (positive J value) and antiferromagnetic (negative J value) interactions. J values were also calculated along the twisting movement by the scan of dihedral angles between the radical and the coupler. An overall trend was found as absolute value of J decreased over increasing torsion angles.

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NUMERICAL SIMULATIONS OF LOW- AND HIGH-FREQUENCY BUZZ AROUND AN AXISYMMETRIC SUPERSONIC INLET (축대칭 초음속 흡입구 주위의 저주파수 및 고주파수 버즈(Buzz)에 대한 수치모사)

  • Kwak, E.;Lee, N.;Gong, H.;Lee, S.
    • Journal of computational fluids engineering
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    • v.18 no.2
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    • pp.78-84
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    • 2013
  • In this paper, numerical simulations of both low- and high-frequency buzz phenomena at the throttle ratios (T.R.) in Nagashima's experiment are performed. The dominant frequencies of the low-and high-frequency buzz in the experiment are about 109 Hz with T.R.=0.97 and 376 Hz with T.R.=0.55, respectively. An axisymmetric solver with the S-A turbulence model is used for the simulations, and DFT(Discrete Fourier Transform) on pressure histories is conducted for the buzz frequency analysis. In the present simulations, the free-stream Mach number and the Reynolds number based on the inlet diameter are 2 and $10^7$, respectively. Both the low- and high-frequency buzz phenomena are accomplished without the changes in the grid topology. The dominant frequency of the simulation is about 125 Hz with T.R.=0.97, while it is 399 Hz with T.R.=0.55.