A Third Order Accurate Cellwise Relaxation Implicit Discontinuous Galerkin Scheme for Unstructured Hybrid Meshes

<table class="table-group" width="800px"><tr class="fig-image" id="a"><td><img alt="176752.fig.0017a" src="https://static.hindawi.com/articles/mpe/volume-2014/176752/figures/176752.fig.0017a.jpg"/></td></tr><tr class="fig-caption"><td align="center"><table><tr><td><b>(a) </b>2nd order</td></tr></table></td></tr><tr class="fig-image" id="b"><td><img alt="176752.fig.0017b" src="https://static.hindawi.com/articles/mpe/volume-2014/176752/figures/176752.fig.0017b.jpg"/></td></tr><tr class="fig-caption"><td align="center"><table><tr><td><b>(b) </b>3rd order</td></tr></table></td></tr></table>

<table>Convergence histories for computing the turbulent boundary layer flow; (a) 2nd order and (b) 3rd order.</table>

Mathematical Problems in Engineering

fig17

Figure 17

Figure 17: A Third Order Accurate Cellwise Relaxation Implicit Discontinuous Galerkin Scheme for Unstructured Hybrid Meshes 