This study aims to study the effect of reactions and temperature on the drag force coefficient in the process of char combustion. For this purpose, two-dimensional fully resolved simulations are performed using the ghost cell immersed boundary method.Heat and mass transfer, together with the corresponding Stefan flow, is accounted for.Reactive particles with different reaction rates, temperatures and diameters are compared with a non-reactive adiabatic particle and a particle with outflow. For a char particle, results show that reactions tend to increase the drag force, which is converse to the effect observed for non-reactive particles with a pure outflow. This discrepancy is due to the fact that species and temperature distribution play an important role, and both of them can affect the property of the fluid. Hence, a reactive particle cannot be simplified as a particle with only outflow. Based on the current study, a new drag force correlation for a single reactive particle is obtained. The correlation shows a good agreement with the simulation results. A posterior analysis is also performed to verify the accuracy of the correlation.
In this work, a fully resolved direct numerical simulation study of the interaction between supersonic turbulent flow and inertial particle is carried out. For the compressible flow, an eighth-order bandwidth optimization weighted essentially nonoscillatory scheme is used for shock capturing, and the central finite difference scheme is used for the spatial discretization of diffusion terms. The three-dimensional ghost zone immersed boundary method is adopted for solid-fluid interface identification. These numerical schemes are integrated in a direct numerical simulation solver, and its validation is demonstrated by comparing to several benchmark cases. Such a developed method is then used to attack the problem of an upstream supersonic turbulent flow over a spherical particle. Three cases with different inflow turbulence intensities are studied. It is shown that with the turbulence intensity increasing the drag force coefficient presents a smaller relative increase compared to the incompressible situation. Analysis of the bow shock-turbulence interaction is also reported. Similar to the normal shock-turbulence interaction, both the Kolmogorov and Taylor scales decrease after being compressed by the shock. Moreover, both the streamwise and transverse Reynolds stresses have a peak at the shock position. These results indicate the significance of taking the effects of shock into consideration when modeling the modulation of a solid particle to the compressible turbulence.
Two methods for solid body representation in flow simulations available in the Pencil Code are the immersed boundary method and overset grids. These methods are quite different in terms of computational cost, flexibility and numerical accuracy. We present here an investigation of the use of the different methods with the purpose of assessing their strengths and weaknesses. At present, the overset grid method in the Pencil Code can only be used for representing cylinders in the flow. For this task it surpasses the immersed boundary method in yielding highly accurate solutions at moderate computational costs. This is partly due to local grid stretching and a body-conformal grid, and partly due to the possibility of working with local time step restrictions on different grids. The immersed boundary method makes up the lack of computational efficiency with flexibility in regards to application to complex geometries, due to a recent extension of the method that allows our implementation of it to represent arbitrarily shaped objects in the flow.
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