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