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Upward Flame Spread Over an Array of Discrete Thermally-Thin PMMA Plates

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Abstract

Experiments and theoretical analysis were conducted to investigate the upward flame spread over a homogenous PMMA plate and an array of discrete thermally thin PMMA elements. In the experiment, a digital video camera was used to record the flame spread process. An electronic balance and thermocouples were adopted to monitor the mass loss and pyrolysis front position, respectively, as a function of time. In the theoretical analysis, the mass loss rate of PMMA was correlated to the heat transfer during flame spread. The experimental results show that the flame spread rate peaks in the case of discrete PMMA elements with a fuel coverage around 80% rather than 100% (the homogenous case) because the gap with an appropriate spacing between neighboring elements accelerates the flame spread. However, the flame cannot spread over an array of discrete fuels at a coverage of 50% or smaller where the gap is too large to allow effective heat transfer required for flame spread. A smaller coverage of PMMA results in a larger mass loss rate per area since the gaps between elements can entrain more air to promote the burning. A logarithmic relation, that can well describe the mass loss rate as a function of PMMA coverage, was proposed based on the theoretical analysis and the fitting of experimental measurements.

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Abbreviations

A :

Burning area of PMMA plate, m2

B :

Spalding B number

F :

PMMA coverage

F f :

View factor of flame to PMMA surface

g :

Earth normal gravitational acceleration, m s2

h :

Convective heat-transfer coefficient, W m2 K1

H :

Flame height, m

Δh v :

Heat required to convert PMMA at its surface temperature to gas phase, J g1

H p :

Pyrolysis height, m

k :

Thermal conductivity of gas phase, W m1 K1

L :

Length of PMMA plate, m

\(\dot{m}^{\prime \prime }\) :

Mass loss rate per unit area, g s1 m2

Nu :

Nusselt number

Pr :

Prandtl number

\(\dot{q}^{\prime \prime }_{r}\) :

Radiative heat flux from the flame to PMMA surface, J s1 m2

\(\dot{q}_{cv}^{\prime \prime }\) :

Convective heat flux from the flame to PMMA surface, J s1 m2

\(\dot{q}_{rr}^{\prime \prime }\) :

Radiative heat flux lost from PMMA surface to ambient environment, J s1 m2

\(\dot{q}^{\prime \prime }_{misc}\) :

Conductive heat flux from thermal baffle to air, J s1 m2

Ra :

Rayleigh number

S :

Length of spacing, m

t :

Time, s

T f :

Flame temperature, K

T film :

Film temperature, K

T p :

Pyrolysis temperature, K

T :

Ambient temperature, K

V f :

Flame spread rate, m s1

W :

Width of PMMA plate, m

x :

Characteristic length, m

β :

Thermal expansion coefficient, K1

α :

Thermal diffusivity, m2 s1

υ :

Kinematic viscosity, m2 s1

σ :

Stefan-Boltzmann constant

ε f :

Emission coefficient of flame

ε p :

Emission coefficient of PMMA pyrolysis surface

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Acknowledgements

The authors would like to thank the National Natural Science Foundation of China (Grant Nos. 51976210 and 51806208) and the Fundamental Research Funds for the Central Universities (Grant Nos. WK2320000043 and WK2320000048).

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Correspondence to Hua-Hua Xiao or Jin-Hua Sun.

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Gou, FH., Xiao, HH., Jiang, L. et al. Upward Flame Spread Over an Array of Discrete Thermally-Thin PMMA Plates. Fire Technol 57, 1381–1399 (2021). https://doi.org/10.1007/s10694-020-01068-9

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  • DOI: https://doi.org/10.1007/s10694-020-01068-9

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