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Second International Workshop Structures in Fire – Christchurch – March 2002 .<br />

1. Initial Input<br />

STRUCTURAL<br />

RESPONSE MODEL<br />

2. Input <strong>of</strong> Temperature<br />

Distribution in the Wall<br />

3. Determine Stiffnesses <strong>of</strong>:<br />

Elements<br />

Members<br />

Supports<br />

Frame<br />

Increment<br />

Time Step<br />

4. Determine Unbalanced Actions<br />

5. Undertake Frame Analysis to<br />

Determine Displacements<br />

6. Test Failure<br />

Yes<br />

failure<br />

No<br />

not<br />

converged<br />

yet<br />

Yes<br />

convergence achieved<br />

No<br />

no failure<br />

7. Test Convergence<br />

8. Output<br />

Figure 21. Flowchart showing overview <strong>of</strong> structural response model [6].<br />

CONCLUSIONS<br />

Creep <strong>of</strong> <strong>wood</strong> specimens h<strong>as</strong> been me<strong>as</strong>ured for a range <strong>of</strong> loads, <strong>moisture</strong> contents <strong>and</strong><br />

temperatures. The significant types <strong>of</strong> creep observed were:<br />

• Creep due to the presence <strong>of</strong> <strong>moisture</strong>, heat <strong>and</strong> <strong>stress</strong> in the temperature range 20°-<br />

100°C.<br />

• Creep due to heat <strong>and</strong> <strong>stress</strong> in the temperature range 100°-300°C.<br />

Experimentation involving desorption <strong>of</strong> <strong>moisture</strong> in <strong>wood</strong> specimens did not reveal significant<br />

creep due to mechano-sorptive effects.<br />

The first type <strong>of</strong> creep mentioned above w<strong>as</strong> sufficient for explaining the difference between the<br />

el<strong>as</strong>tic modulus obtained by calibration <strong>and</strong> direct me<strong>as</strong>urement.<br />

The relationships for the el<strong>as</strong>tic modulus <strong>of</strong> <strong>wood</strong> in <strong>compression</strong> obtained by several<br />

researchers through the calibration <strong>of</strong> models to full scale experiments represent simple el<strong>as</strong>tocreep<br />

models for predicting the effects <strong>of</strong> creep <strong>of</strong> light-timber structures in fire. The models are<br />

limited to applications in which the <strong>wood</strong> is subjected to temperatures, <strong>moisture</strong>s <strong>and</strong> <strong>stress</strong>es<br />

similar to values that occurred in the experiments.<br />

240

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