Hi all,
About the SPREAD_RATE, the FDS User guide says "It should not be used to mimic a t-squared fire growth rate".Β
However there is a CFD best practice paper that recommeds to use the
spread_rate using the formula:
πππ πΈπ΄π·_π π΄ππΈ=sqrt((πΌ/π)β(1/π»π π πππ΄)) whereΒ Ξ± = Alfaβt2 growth rate (kW/s2)
Β
So my question is : why the πππ πΈπ΄π·_π π΄ππΈ should not be used to mimic a t-squared fire growth rate?
Thank you
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Thanks blackarrow90,
I didn't know it's that complex to share a published material.
On 28 Nov 2017 7:32 am, "blackarrow90" <bojan...@gmail.com> wrote:
It is actually a conference paper from Daniel Rosberg, there is also the whole presentation here:Β https://www.thunderheadeng.com/2014/10/femtc2014_d1-d-2_rosberg/If the cells of the burner are modeled properly, I would say it is more realistic to use spread, otherwise you would have the activation of all fire cells immediately which is not hot fire behaves.
On Tuesday, November 21, 2017 at 6:34:37 PM UTC+1, enzo.d...@gmail.com wrote:Hi all,
About the SPREAD_RATE, the FDS User guide says "It should not be used to mimic a t-squared fire growth rate".Β
However there is a CFD best practice paper that recommeds to use the spread_rate using the formula:
πππ πΈπ΄π·_π π΄ππΈ=sqrt((πΌ/π)β(1/π»π π πππ΄)) whereΒ Ξ± = Alfaβt2 growth rate (kW/s2)
Β
So my question is : why the πππ πΈπ΄π·_π π΄ππΈ should not be used to mimic a t-squared fire growth rate?
Thank you
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Hello,
From my point of view it depends on what you are analyzing. I only use spreading rate when I need heat flux or flame height during the growing phase.
For other applications, when I need to explore steady state, I use a negative TAU_Q.
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