28.01.2013 Views

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

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

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

1<br />

3<br />

3<br />

where n is the boundary normal. <strong>The</strong> above equation can be rewritten for the node I<br />

in Fig. C.1(b) as<br />

ÿ B1<br />

6 …2FI i ‡ F 3 i †n 1 ‡ ÿ B2<br />

6 …2FI i ‡ F 1 i †n 2<br />

…C:6†<br />

where ÿB1 and ÿB2 are appropriate edge lengths.<br />

<strong>The</strong> above equations (C.3) and (C.5) can be reformulated for an edge-based data<br />

st<strong>ru</strong>cture. In such a procedure, Eq. (C.3) can be rewritten as (for an interior node I)<br />

X<br />

…<br />

E 2 I<br />

I<br />

E<br />

1<br />

2<br />

@N I<br />

…N<br />

@xi k F k i † d ˆ Xm s<br />

S ˆ 1<br />

2<br />

(a) (b)<br />

Fig. C.1 Typical patch of linear triangular elements: (a) inside node; (b) boundary node.<br />

X<br />

E 2 II s<br />

A E<br />

3<br />

@N I<br />

@x i E<br />

…F I i ‡ F Is i † …C:7†<br />

where m s is the number of edges in the mesh which are directly connected to the node<br />

I and the summation P E 2 II s extends over those elements that contain the edges II s.<br />

<strong>The</strong> user can readily verify that the above equation is identically equal to the standard<br />

element formulation of Eq. (C.4) if we consider the node I in Fig. C.1(a). <strong>The</strong><br />

inclusion of boundary sides is direct from Eqs (C.5) and (C.6).<br />

3<br />

1<br />

I<br />

2<br />

2<br />

Appendix C 299<br />

1

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!