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FIRE DESIGN OF STEEL MEMBERS - Civil and Natural Resources ...

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1 <br />

T<br />

s, cr<br />

= 39.19ln<br />

−1<br />

+ 482<br />

3. 833 <br />

3.7a<br />

<br />

0.9674µ<br />

0 <br />

or, for values of µ 0<br />

from 0.22 to 0.80, the limiting temperature has been<br />

calculated <strong>and</strong> entered in a table. The degree of utilisation is a factor giving the<br />

ratio of design load to load bearing capacity of the member at elevated<br />

temperatures, <strong>and</strong> the same effecitve factor as r f in NZS 3404.<br />

When this equation is rearranged to produce a formula in terms of µ 0<br />

, this<br />

becomes:<br />

− 1<br />

3.833<br />

T − 482 <br />

µ<br />

0<br />

= 0.96741<br />

+ exp<br />

<br />

3.7b<br />

39.19 <br />

Fitting the results from this equation against those in Figure 3.2 gives a curve that<br />

fits the data points included in the table in EC3. This is expected, as the<br />

calculation of the limiting temperature in NZS 3404 is a direct rearrangement of<br />

the yield stress formulas also.<br />

3.1.4 Temperature rise of unprotected steel:<br />

According to NZS 3404:1997<br />

The time (t)at which the limiting temperature is attained shall be calculated<br />

for:<br />

a. Three sided exposure as follows:<br />

0.433T<br />

l <br />

t = −5 .2 + 0.0221T<br />

l<br />

+ <br />

3.8<br />

SF <br />

b. Four sided exposure as follows:<br />

0.203T<br />

l <br />

t = −4 .7 + 0.0263T<br />

l<br />

+ <br />

3.9<br />

SF <br />

H <br />

where: SF is the section factor of the steel member p<br />

, m<br />

A<br />

-1 .<br />

<br />

These formulas have limitations for the steel temperature <strong>and</strong> the section factor of<br />

the beam. These are:<br />

500 < T l < 850 °C in NZS 3404, <strong>and</strong> 500 < T l < 750 °C in AS 4100<br />

43

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