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Here, we choose (h=1/16), (tau=0.01), and the finite element space is a Taylor-Hood finite element space.
Now we turn to the three inverse properties of the finite element space (V_{h}^{k}).
To this end, now we introduce the basis functions of the finite element space.
Let (V_{h}) denote the standard piecewise linear finite element space.
The Morley element space (S^{h}subset L_{2}(Omega)), (S^{h}notsubset H^{1}(Omega)).
Ausas, F.S. Sousa, G.C. Buscaglia, An improved finite element space for discontinuous pressures, Comput.
The models were built in a 3-dimensional finite element space.
In the present paper, we use the extended finite element space (XFEM), presented in [N.
To simplify our presentation we here only consider the piecewise constant finite element space for the approximation of the control.
We first build a finite element space V 0 h, which will be further discussed in the next section.
We assume V h ( Ω i ) be the bilinear conforming element space associated with the partition T h ( Ω i ).
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