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Effects of Combined Surface and In-Depth Absorption on Ignition of PMMA.

作者信息

Gong Junhui, Chen Yixuan, Li Jing, Jiang Juncheng, Wang Zhirong, Wang Jinghong

机构信息

College of Safety Science and Engineering, Nanjing Tech University, Nanjing, Jiangsu 210009, China.

Department of Fire Science & Professional Studies, University of New Haven, West Haven, CT 06516, USA.

出版信息

Materials (Basel). 2016 Oct 5;9(10):820. doi: 10.3390/ma9100820.

DOI:10.3390/ma9100820
PMID:28773940
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5456632/
Abstract

A one-dimensional numerical model and theoretical analysis involving both surface and in-depth radiative heat flux absorption are utilized to investigate the influence of their combination on ignition of PMMA (Polymethyl Methacrylate). Ignition time, transient temperature in a solid and optimized combination of these two absorption modes of black and clear PMMA are examined to understand the ignition mechanism. Based on the comparison, it is found that the selection of constant or variable thermal parameters of PMMA barely affects the ignition time of simulation results. The linearity between t and heat flux does not exist anymore for high heat flux. Both analytical and numerical models underestimate the surface temperature and overestimate the temperature in a solid beneath the heat penetration layer for pure in-depth absorption. Unlike surface absorption circumstances, the peak value of temperature is in the vicinity of the surface but not on the surface for in-depth absorption. The numerical model predicts the ignition time better than the analytical model due to the more reasonable ignition criterion selected. The surface temperature increases with increasing incident heat flux. Furthermore, it also increases with the fraction of surface absorption and the radiative extinction coefficient for fixed heat flux. Finally, the combination is optimized by ignition time, temperature distribution in a solid and mass loss rate.

摘要
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/5be5d9039941/materials-09-00820-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/92ff2d1c1ba8/materials-09-00820-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/ae2d099f5d39/materials-09-00820-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/8f3afd049676/materials-09-00820-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/8ebd85034fd3/materials-09-00820-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/5c4309a83253/materials-09-00820-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/10169ab7eafc/materials-09-00820-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/91b9f3fab7cd/materials-09-00820-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/9d31ecbdc880/materials-09-00820-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/5be5d9039941/materials-09-00820-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/92ff2d1c1ba8/materials-09-00820-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/ae2d099f5d39/materials-09-00820-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/8f3afd049676/materials-09-00820-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/8ebd85034fd3/materials-09-00820-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/5c4309a83253/materials-09-00820-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/10169ab7eafc/materials-09-00820-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/91b9f3fab7cd/materials-09-00820-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/9d31ecbdc880/materials-09-00820-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/44de/5456632/5be5d9039941/materials-09-00820-g009.jpg

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