Laminar burning speeds and flame structures of mixtures of difluoromethane (HFC-32) and 1,1-difluoroethane (HFC-152a) with air at elevated temperatures and pressures

Ali Moghaddas, Casey Bennett, Emad Rokni, H. Metghalchi
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引用次数: 21

Abstract

Laminar burning speeds and flame structures of difluoromethane (HFC-32)/air and 1,1-difluoroethane (HFC-152a)/air mixtures have been studied. Experiments have been carried out in constant-volume spherical and cylindrical vessels coupled with a schlieren/shadowgraph system and high-speed complementary metal-oxide-semiconductor (CMOS) camera. Laminar burning speed was determined using a thermodynamic model that employs the pressure rise history of the combustion process. Experiments were conducted for different initial conditions over a wide range of equivalence ratios. Laminar burning speeds of HFC-152a/air mixtures have been measured over the temperature range of 298 K to 580 K and pressure range of 1 to 8 bar. Laminar burning speeds of HFC-32/air mixtures have been measured for the temperature range of 350 K to 475 K and pressure range of 2 to 6.8 bar. Correlations have been developed for laminar burning speeds of HFC-32 and HFC-152a to demonstrate the temperature and pressure dependency of laminar burning speeds of these two refrigerants.
二氟甲烷(HFC-32)和1,1-二氟乙烷(HFC-152a)混合物在高温高压下与空气的层流燃烧速度和火焰结构
研究了二氟甲烷(HFC-32)/空气和1,1-二氟乙烷(HFC-152a)/空气混合物的层流燃烧速度和火焰结构。实验在等体积的球形和圆柱形容器中进行,并与纹影/阴影系统和高速互补金属氧化物半导体(CMOS)相机耦合。层流燃烧速度是用热力学模型确定的,该模型采用了燃烧过程的压力上升历史。在不同的初始条件下,在较宽的等效比范围内进行了实验。在298 ~ 580 K的温度范围和1 ~ 8 bar的压力范围内,测量了HFC-152a/空气混合物的层流燃烧速度。在350 ~ 475 K的温度范围和2 ~ 6.8 bar的压力范围内,测量了HFC-32/空气混合物的层流燃烧速度。建立了HFC-32和HFC-152a层流燃烧速度的关系式,以证明这两种制冷剂层流燃烧速度的温度和压力依赖性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
HVAC&R Research
HVAC&R Research 工程技术-工程:机械
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