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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

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