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The Finite Element Method for the Analysis of Non-Linear and ...

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Simple Bar Example - Revisited<br />

Load step 1: t = 1:<br />

( K + K ) Δ u = R− F − F<br />

0 0 (1) 1 1 (0) 1 (0)<br />

a b a b<br />

⇓<br />

2×<br />

10<br />

Δ u = = 6.6667×<br />

10<br />

7 1 1<br />

10 ( + )<br />

10 5<br />

Iteration 1: ( i = 1)<br />

4<br />

(1) −3<br />

u = u +Δ u = 6.6667×<br />

10<br />

1 (1) 1 (0) (1) −3<br />

1 (1)<br />

1 (1) −4<br />

εa<br />

= = ×<br />

La<br />

1 (1)<br />

b<br />

u<br />

b<br />

6.6667 10 < ε (elastic section!)<br />

1 (1)<br />

u<br />

−3<br />

ε = = 1.3333×<br />

10 < εY<br />

(elastic section!)<br />

L<br />

F<br />

= 6.6667× 10 ; F = 1.3333×<br />

10<br />

1 (1) 3 1 (1) 4<br />

a<br />

b<br />

0 0 (2) 1 1 (1) 1 (1)<br />

( Ka Kb) u R Fa Fb<br />

0<br />

Y<br />

Convergence in one iteration!<br />

1 −3<br />

+ Δ = − − = u = 6.6667×<br />

`10<br />

Institute <strong>of</strong> Structural Engineering <strong>Method</strong> <strong>of</strong> <strong>Finite</strong> <strong>Element</strong>s II 30

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