By H. Oh
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And Chakravarthy, S. “Uniformly High Order Accurate Essentially Non-Oscillatiry Schemes III”, J. Comput. Phys, 71, (1987), pp. 231-303. M. “On the mutual threading of vortex rings”, Proceedings of the Royal Society of London A 10 (1922) 111–131. , “Numerical computation of internal and external flows”, vol. 2, John Wiley & Sons, 1998. , “The generation of sound by aerodynamic sources in an inhomogeneous steady flow”, J. , Vol 67, No. 3, 1975, pp. 597-610. Inoue, O “Sound generation by the leapfrogging between two coaxial vortex rings”, Physics of Fluids 14 (9) (2002) 3361–3364.
Aw can be represented by: Aw MAX C w ,0 Dw (21) In the second order one, quantities at cell faces are computed using a multidimensional linear reconstruction approach (Jespersen and Barth 1989). In this approach, higher-order accuracy is achieved at cell faces through a Taylor series expansion of the cell-centered solution about the cell centroid.
The face value (Φw) are equal to the cell-center value of Φ in the upstream cell. v dA vw AwW C wW (20) Where, Cw is the west face convective coefficient. Aw can be represented by: Aw MAX C w ,0 Dw (21) In the second order one, quantities at cell faces are computed using a multidimensional linear reconstruction approach (Jespersen and Barth 1989). In this approach, higher-order accuracy is achieved at cell faces through a Taylor series expansion of the cell-centered solution about the cell centroid.