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x 1<br />

Finite Element Analysis of Membrane Structures 55<br />

x 3<br />

y 2<br />

Fig. 2. Cable reinforced membrane element at(i-j)<br />

4Reinforcement Cables<br />

It is common to place reinforcing cables in membranes to provide added strength or<br />

shape control. The cables are generally very strong in axial load capacity (generally<br />

tension) and weak in bending. Accordingly, they may be modeled by a truss type<br />

member. In the form admitted here it is not necessary for the reinforcement to be<br />

placed at the edges of membrane elements - they may pass through an element as<br />

showninFig 2.<br />

The ends of atypical reinforcement are denoted as i and j in thefigure and have<br />

reference coordinates X i and X j ,respectively. These points may be referred to the<br />

nodal values of themembranebycomputing the values of the natural coordinates<br />

so that<br />

X k = ξ k α X α<br />

for k = i, j (49)<br />

The solution for the two points may be trivially constructed from linear interpolation<br />

on the edges. The results are (for the points intersecting the edges shown in the<br />

figure)<br />

ξ i 2 = X i − X 1 <br />

X 2 − X 1 <br />

ξ j<br />

3 = X j − X 1 <br />

X 3 − X 1 <br />

j<br />

1<br />

3<br />

; ξ i 1 = 1 − ξ i 2 ; ξ i 3 = 0<br />

; ξ i 1 = 1 − ξ i 3 ; ξ i 2 = 0 (50)<br />

Using these values the deformed position of the reinforcement cable may be<br />

written as<br />

i<br />

x<br />

x j<br />

i<br />

ξα I<br />

=<br />

ξ j <br />

˜x<br />

α I<br />

α<br />

(51)<br />

n<br />

i<br />

2<br />

x 2<br />

y 1

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