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Variation of turbulent burning rate of methane, methanol, and iso-octane air mixtures with equivalence ratio at elevated pressure

机译:甲烷,甲醇和异辛烷空气混合物湍流燃烧速率随高压当量比的变化

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摘要

Turbulent burning velocities for premixed methane, methanol, and iso-octane/air mixtures have been experimentally determined for an rms turbulent velocity of 2 m/s and pressure of 0.5 MPa for a wide range of equivalence ratios. Turbulent burning velocity data were derived using high-speed schlieren photography and transient pressure recording; measurements were processed to yield a turbulent mass rate burning velocity, utr. The consistency between the values derived using the two techniques, for all fuels for both fuel-lean and fuel-rich mixtures, was good. Laminar burning measurements were made at the same pressure, temperature, and equivalence ratios as the turbulent cases and laminar burning velocities and Markstein numbers were determined. The equivalence ratio (φ) for peak turbulent burning velocity proved not always coincident with that for laminar burning velocity for the same fuel; for isooctane, the turbulent burning velocity unexpectedly remained high over the range φ = 1 to 2. The ratio of turbulent to laminar burning velocity proved remarkably high for very rich iso-octane/air and lean methane/air mixtures.
机译:已通过实验确定了预混合甲烷,甲醇和异辛烷/空气混合物的湍流燃烧速度,其均方根湍流速度为2 m / s,压力为0.5 MPa,适用于广泛的当量比。湍流燃烧速度数据是通过高速schlieren摄影和瞬态压力记录得出的。对测量值进行处理以产生湍流质量速率燃烧速度​​utr。对于贫燃料和富燃料混合物的所有燃料,使用两种技术得出的值之间的一致性很好。在与湍流情况相同的压力,温度和当量比下进行层流燃烧测量,并确定层流燃烧速度和马克斯坦数。对于相同的燃料,湍流燃烧峰值速度的当量比(φ)并不总是与层流燃烧速度的当量比(coincide†)始终一致。对于异辛烷,湍流燃烧速度出乎意料地保持在φ= 1至2的范围内。对于非常浓的异辛烷/空气和稀甲烷/空气混合物,湍流与层流燃烧速度之比非常高。

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