High Order Weighted Essentially Non-oscillation Schemes for Two-Dimensional Detonation Wave Simulations

  • Authors:
  • Zhen Gao;Wai Sun Don;Zhiqiu Li

  • Affiliations:
  • Key Laboratory of Marine Environment & Ecology, Ministry of Education, and School of Mathematical Sciences, Ocean University of China, Qingdao, China 266100;Department of Mathematics, Hong Kong Baptist University, Hong Kong, China;Department of Mathematics, Hong Kong Baptist University, Hong Kong, China

  • Venue:
  • Journal of Scientific Computing
  • Year:
  • 2012

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Abstract

In this paper, we demonstrate the detailed numerical studies of three classical two dimensional detonation waves by solving the two dimensional reactive Euler equations with species with the fifth order WENO-Z finite difference scheme (Borges et al. in J. Comput. Phys. 227:3101---3211, 2008) with various grid resolutions. To reduce the computational cost and to avoid wave reflection from the artificial computational boundary of a truncated physical domain, we derive an efficient and easily implemented one dimensional Perfectly Matched Layer (PML) absorbing boundary condition (ABC) for the two dimensional unsteady reactive Euler equation when one of the directions of domain is periodical and inflow/outflow in the other direction. The numerical comparison among characteristic, free stream, extrapolation and PML boundary conditions are conducted for the detonation wave simulations. The accuracy and efficiency of four mentioned boundary conditions are verified against the reference solutions which are obtained from using a large computational domain. Numerical schemes for solving the system of hyperbolic conversation laws with a single-mode sinusoidal perturbed ZND analytical solution as initial conditions are presented. Regular rectangular combustion cell, pockets of unburned gas and bubbles and spikes are generated and resolved in the simulations. It is shown that large amplitude of perturbation wave generates more fine scale structures within the detonation waves and the number of cell structures depends on the wave number of sinusoidal perturbation.