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The nodal displacements u 1 , u 2 , u 3 , v 1 , v 2 and v 3 can then be expressed by the six inter-
polation coeffi cients a 1 , a 2 , a 3 , b 1 , b 2 and b 3 as follows:
(10.2)
From these six linear equations a 1 , a 2 , a 3 , b 1 , b 2 and b 3 can be evaluated as functions of
the nodal coordinates and nodal displacements:
(10.3)
where A is the area of the triangular element.
Assuming elastic, isotropic stress--strain behavior strains and stresses within the ele-
ment can be derived from the two-dimensional formulation of the compatibility equa-
tions and Hooke's law:
(10.4)
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