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

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Beam <strong>Element</strong>s - Strong Form to Weak Form<br />

Arrive at <strong>the</strong> weak <strong>for</strong>m<br />

(W)<br />

Note:<br />

1. <strong>The</strong> spaces are C 1 continuous, i.e. <strong>the</strong> derivative must also be<br />

continuous<br />

Note:<br />

1. <strong>The</strong> spaces are C 1 continuous, i.e. <strong>the</strong> derivative must also be<br />

continuous<br />

2. <strong>The</strong> left side is symmetric in w <strong>and</strong> υ (bi-linear <strong>for</strong>m:<br />

a(υ, w)=a(w, υ)) this will lead to a symmetric Stiffness Matrix<br />

2. <strong>The</strong> left side is symmetric in w <strong>and</strong> v (bi-linear <strong>for</strong>m: a(v,w)=a(w,v)<br />

this will lead to symmetric stiffness matrix<br />

Institute <strong>of</strong> Structural Engineering <strong>Method</strong> <strong>of</strong> <strong>Finite</strong> <strong>Element</strong>s II 20

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