DeltaDualCoreβ„’ Panel Awning Systems 
 
Revision 1-12 
40 
 
Appendix A 
  Assessment of Heat Conduction Through a 
Steel Member 
A.1  Introduction 
A one-dimensional finite difference heat transfer calculation is undertaken to determine the temperature 
distribution through a steel purlin (approximated as a solid steel rod) when exposed on one face to a H3V3 
fire source feature on the site boundary. The simplified model is shown in Figure 5-1.  
The aim of the assessment is to establish whether conduction through a steel member along the non-
combustible portion of the DeltaDualCoreβ„’ system may result in ignition of the EPS-FR component of the 
roof system. 
 
 
Figure 5-1. Finite Difference Heat Transfer Analysis Paths to assess heat transfer through a steel 
member via conduction. 
 
A.2  Methodology 
The finite difference heat transfer equation used for calculating the temperature distribution through the 
steel rod is given below: 
π‘‡π‘œβ€² = [π‘˜π‘ π΄(π‘‡π‘›βˆ’1 βˆ’π‘‡π‘›)
𝛿π‘₯𝑛,π‘›βˆ’1
+ π‘˜π‘ π΄(𝑇𝑛+1 βˆ’π‘‡π‘›)
𝛿π‘₯𝑛+1,𝑛
βˆ’β„Žπ΄(π‘‡π‘œβˆ’20) βˆ’πœ€πœŽπ΄(π‘‡π‘œ4 βˆ’2934)] Γ—
𝛿𝑑
πœŒπ‘π΄π›Ώπ‘₯π‘œ
+ π‘‡π‘œ 
 
For the above equation the notation is defined as follows: 
variables: 
 
One-dimensional heat path 
through steel rod showing 
nodes used for heat 
transfer analysis 
(βˆ†x = 0.1 m) 
AXONOMETRIC VIEW FROM ABOVE 
AXONOMETRIC VIEW FROM BELOW 
Rate of conduction is proportional to 
cross-sectional area i.e. a higher rate of 
conduction is expected through a thick 
gauge steel member than through thin 
steel sheeting. As such, conduction is 
assessed through a steel purlin which is 
approximated as a steel rod. 
Solid cross-sectional area 
0.008 m2 
Face exposed to heat 
900mm 
Non-combustible 
portion within 
900 mm of site 
boundary 
Non-combustible 
portion within 
900 mm of site 
boundary 

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