For Example 16.1, show that the element stiffness equations for the isotropic case are given by relations

Question:

For Example 16.1, show that the element stiffness equations for the isotropic case are given by relations (16.4.1) and (16.4.2).

Data from example 16.1

Consider the plane stress problem of an isotropic elastic plate under uniform tension with zero body forces,

y 4 3 1 1 (2) 2 3 3 2 2 T -X

The element mesh is labeled as shown with local node numbers within each element and global node numbers

In similar fashion for element 2, 61 = 0, B2 = 1, B3 =  1, y1 = -1, Y2 = 0, Y3 = 1, A1 = 1/2, and the element

These individual element equations are to be assembled to model the plate, and this is carried out using the

K+K KQ+K2 K KQ K+K K(! +K() K!! K(!) K16 K +K(2) K + K K K K K 33 K34 (1) 44 K+K 35 (1) K56 (1) U1 V U V U3

where U, and V; are the global x and y nodal displacements, and K and K are the local stiffness components

Equation 16.4.1

E 2(1-1) [1 0 -1 -V 1-v V 0  V   . 0 V -1 0 3 (1) 4 (1) 1x ly 2x !!! TO) (16.4.1)

Equation 16.4.2

E 2(1-1)  O 1 -V -  0 1 0 1 - v 2  V -1  3-v 1 - -1 V |2 3-P 2 (2) (2) Wi (2) (2) uz Co (2) 2x IM (16.4.2)

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