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Zienkiewicz O.C., Taylor R.L. Vol. 3. The finite - tiera.ru

Zienkiewicz O.C., Taylor R.L. Vol. 3. The finite - tiera.ru

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u � � ���������<br />

u � ��<br />

�h<br />

��� ��������<br />

��� �����������<br />

�h<br />

��� �������� ��������<br />

it can be written as (see reference 22 for details)<br />

h<br />

e ˆ ÿ h ˆ ch 2 d 2<br />

u � �� � ��<br />

u � �� � ��<br />

Fig. 4.10 Flow past a backward facing step. Exercise on exit boundary conditions, Re ˆ 100.<br />

dx2 ch 2 2 h<br />

d<br />

dx2 …4:21†<br />

where<br />

h<br />

is the ®nite element solution and c is a constant.<br />

If, for instance, we further assume that ˆ h at the nodes, i.e. that the nodal error<br />

is zero, then e represents the values on a parabola with a curvature of d 2 h =dx 2 . This<br />

allows c, the unknown constant, to be determined, giving for instance the maximum<br />

��� �����������<br />

��� �������� ��������<br />

Fig. 4.11 Flow past a backward facing step. Solution with a longer domain, Re ˆ 100.<br />

��h<br />

Adaptive mesh re®nement 105<br />

t n ��<br />

u � ��

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