Experimental study of vertically upward flame spread over polymethyl methacrylate slabs at different altitudes |
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| Authors: | Canjun Liang Xudong Cheng Hui Yang Heping Zhang Kwok Kit Yuen |
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| Affiliation: | 1. State Key Laboratory of Fire Science, University of Science and Technology of China, Hefei, China;2. Department of Civil and Architectural Engineering, City University of Hong Kong, Kowloon Tong, Hong Kong (SAR), China |
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| Abstract: | Experiments of vertically upward flame spread over polymethyl methacrylate slabs were conducted in Hefei (with an altitude of 29.8 m) and Lhasa (with an altitude of 3658.0 m). Measurements were taken for the flame heights, the flame heat flux to the fuel surface and the flame spread rate. Two regions were identified for the dependence of the flame height on the heat release rate per unit width  . When  is less than 22 kW/m, the flame height scales as  while it scales as  , when  is greater than 22 kW/m. The flame heights in Lhasa are approximately 1.34 and 1.25 times, respectively, of those in Hefei for these two regions. The flame heat flux to the fuel surface decreases significantly from the pyrolysis front to the flame tip, whereas it decreases slowly above the flame tip. In both regions, it can be correlated reasonably well with (x ? xp)/(xf ? xp) using the form of  . The flame heat flux to the fuel surface in Lhasa is approximately 0.75 times of that in Hefei. The flame spread process can be divided into three stages, which correspond to a flow region of laminar, transitional, and turbulent, respectively. The transition to a turbulent flow is delayed in Lhasa compared with Hefei. The flame spread rate in Lhasa is about half of that in Hefei because of the lower flame heat flux caused by the lower ambient pressure. Copyright © 2015 John Wiley & Sons, Ltd. |
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| Keywords: | upward flame spread altitude ambient condition PMMA flame spread rate |
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