here, un is the solution at time
tn,
k is the time step, and
R(un) the weak form

of the DG scheme (compare to the weak formulation of
Equation 16-11), which includes the numerical flux.
The basic idea with local time stepping is as follows. First, the elements are divided into groups, based on their size. Typically, the groups are constructed such that the time steps k,
k/2,
k/4, and so forth are stable time steps for each group of elements and where any coupling between groups is disregarded. This allows for easy synchronization of the solution at every full step. The right-hand-side vectors