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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The values for the thermal properties of the steel <strong>and</strong> geometry of the shape are<br />
averaged values <strong>and</strong> not necessarily exactly what the member will be when constructed<br />
in place. This means that high accuracy is unnecessary <strong>and</strong> often inappropriate when<br />
many other factors, such as the temperature of the fire are also estimated.<br />
The advantages of the spreadsheet programme are that the computer software that is<br />
required for it is a spreadsheet programme such as Microsoft Excel, which is installed<br />
in most office computers. For computer programmes such as SAFIR, files such as<br />
beam sizes, are required as well as the three units of the programme. With the<br />
estimations <strong>and</strong> assumptions made in fire design <strong>and</strong> analysis ,the 5 % difference<br />
found between the two methods can not show that one is more accurate than the other.<br />
Since the spreadsheet method usually gives higher temperatures than the SAFIR <strong>and</strong><br />
other finite element programmes, the results are acceptable to use in design with four<br />
sided exposure <strong>and</strong> when analysing the temperature elevation of simply supported<br />
members.<br />
2.1.2 Unprotected Steel:<br />
The temperature of unprotected steel is found from the following method, (Buchanan,<br />
1999):<br />
Time Steel Temp Fire Temp T f – T s h t ∆T s<br />
T s<br />
T f<br />
t 1 = ∆t Initial steel Fire Temp at T f - T so Eqn 2.2 with Eqn 2.1<br />
temp, T so ∆t/2<br />
T s <strong>and</strong> T f<br />
from this row<br />
t 2 = t 1 +∆t T s +∆T s from Fire Temp at T f - T s Eqn 2.2 with Eqn 2.1<br />
previous row t 1 +∆t/2<br />
T s <strong>and</strong> T f<br />
from this row<br />
etc etc etc etc etc etc<br />
Figure 2.1: Spreadsheet calculation for heat transfer in unprotected steel members, (Buchanan, 1999)<br />
The difference in temperature of the steel over the time period is calculated from:<br />
∆T<br />
s<br />
H<br />
p <br />
ht<br />
<br />
=<br />
<br />
A<br />
<br />
<br />
sc<br />
<br />
<br />
ρ<br />
s <br />
( T − T ) ∆t<br />
where H p /A is the section factor of the beam (m -1 )<br />
20<br />
f<br />
s<br />
2.1