“…This technique has the broad applicability to physical and chemical systems modeled by PDEs. The models that include the solution of mixed systems of algebraic equations, the resolution of steep moving fronts, parameter estimation and optimal control, other problems such as delay differential equations [34], two-dimensional sine-Gordon equation [2], the Boussinesq equation [3], coupled generalized Kortoweg de Vries and quintic regularized long wave equations [32], the Nwogu's one-dimensional extended Boussinesq equation [31], partial differential equation describing nonlinear wave phenomena, e.g., a fully nonlinear third order Korteweg-de Vries (KdV) equation, the fourth-order Boussinesq equation, the fifth order Kaup-Kupershmidt equation and an extended KdV5 equation [39], non-linear inverse heat conduction problem [42], interface problem [33], multi-component atmospheric pollutant propagation model with pollutants phase transformation consideration [28], a Bingham problem in cylindrical pipes [43], a mathematical model for capillary formation [29,36], 3-D transient radiative transfer equation [1], elliptic partial differential equations which describe steady-state mass and energy transport in solids [41] and many other physical problems. Some of the options available for time integration when using a moving grid MOL code is surveyed in [11].…”