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Van Leer, 1979), for enhancing linear wave properties of the solution away from the largesolution gradients discontinuities. g, Hirsch, 2007). , Direct Numerical Simulations of Compressible Vortex Flow Problems 23 1975). By enforcing the TVD property on the solution, the limiter functions introduce implicit numerical dissipation. , 1987). The nonoscillatory methods are very attractive for computing flows with shocks. , selectively use the non-oscillatory methods only for strong discontinuities.

Wu et al. 2008; Heindel, Gray, and Jensen 2008) (Du, Warsito, and Fan 2005; Kumar, Moslemian, and Milorad P. Dudukovic 1995; Tan et al. 2007; Thatte et al. 2004; Veluswamy et al. 2011; H. G Wang et al. 2008) Radioactive Particle Tracking (RPT) Technique to measure velocity field and turbulent parameters of multiphase flow. This is based on the principle of tracking the motion of a single tracer particle as a marker of the solids phase. The tracer particle contains a radioactive element emitting γrays.

101–116. M. “Balanced characteristic method for systems of hyperbolic conservation laws”, Doklady. Mathematics, 2005, vol. 72, no1, pp. 619-62313. , 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.

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