The Finite Element Method for Fluid Dynamics, Sixth Edition

The only method which adapts itself easily to the treatment of vector variables is that of the Taylor-Galerkin procedure. Here we can repeat the steps of Sec. 2.7 but now addressed to the vector-valued equation with which we started Chapter 2 [Eq. (2.1)]. Noting that now ? has multiple components, expanding ? by a Taylor series in time we have
where ? is a number such that 0 ? ? ? 1.
From Eq. (2.1),
and differentiating
In the above we can write
where A i ? ? F i/ ? ? and if Q = Q( ?, x) and ? Q/ ? ? = S,
We can therefore approximate Eq. (E.1) as
Omitting the second derivatives of G i and interpolating the n + ? between n and n + 1 values we have
At this stage a standard Galerkin approximation is applied which will result in a discrete, semi-implicit, time-stepping scheme. As the explicit form is of particular interest we shall only give the details of the discretization process for ? = 0. Writing as usual
we have
This can be written in a compact matrix form similar to Eq. (2.107) as
in which, with
we have (on omitting the third derivative terms and the effect of S) matrices of the form of Eq. (2.108), i.e.
With ? =...