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Opposed Jet Burner Approach for Characterizing Flameholding Potentials of Hydrocarbon Scramjet Fuels

机译:对立的喷气燃烧器方法,用于表征碳氢超燃发动机燃料的阻焰潜力

摘要

Opposed Jet Burner (OJB) tools have been used extensively by the authors to measure Flame Strength (FS) extinction limits of laminar H2/N2 air and (recently) hydrocarbon (HC) air Counterflow Diffusion Flames (CFDFs) at one atm. This paper details normalization of FSs of N2- diluted H2 and HC systems to account for effects of fuel composition, temperature, pressure, jet diameter, inflow Reynolds number, and inflow velocity profile (plug, contoured nozzle; and parabolic, straight tube). Normalized results exemplify a sensitive accurate means of validating, globally, reduced chemical kinetic models at approx. 1 atm and the relatively low temperatures approximating the loss of non-premixed idealized flameholding, e.g., in scramjet combustors. Laminar FS is defined locally as maximum air input velocity, U(sub air), that sustains combustion of a counter-jet of g-fuel at extinction. It uniquely characterizes a fuel. And global axial strain rate at extinction (U(sub air) normalized by nozzle or tube diameter, D(sub n or (sub t)) can be compared directly with computed extinction limits, determined using either a 1-D Navier Stokes stream-function solution, using detailed transport and finite rate chemistry, or (better yet) a detailed 2-D Navier Stokes numerical simulation. The experimental results define an idealized flameholding reactivity scale that shows wide ranging (50 x) normalized FS s for various vaporized-liquid and gaseous HCs, including, in ascending order: JP-10, methane, JP-7, n-heptane, n-butane, propane, ethane, and ethylene. Results from H2 air produce a unique and exceptionally strong flame that agree within approx. 1% of a recent 2-D numerically simulated FS for a 3 mm tube-OJB. Thus we suggest that experimental FS s and/or FS ratios, for various neat and blended HCs w/ and w/o additives, offer accurate global tests of chemical kinetic models at the Ts and Ps of extinction. In conclusion, we argue the FS approach is more direct and fundamental, for assessing, e.g., idealized scramjet flameholding potentials, than measurements of laminar burning velocity or blowout in a Perfectly Stirred Reactor, because the latter characterize premixed combustion in the absence of aerodynamic strain. And FS directly measures a chemical kinetic characteristic of non-premixed combustion at typical flameholding temperatures. It mimics conditions where gfuels are typically injected into a subsonic flameholding recirculation zone that captures air, where the effects of aerodynamic strain and associated multi-component diffusion become important.
机译:作者已广泛使用对置喷射燃烧器(OJB)工具在一个大气压下测量层流H2 / N2空气和(最近)碳氢化合物(HC)空气逆流扩散火焰(CFDF)的火焰强度(FS)消光极限。本文详细介绍了N2稀释的H2和HC系统的FS标准化,以说明燃料成分,温度,压力,射流直径,流入雷诺数和流入速度曲线(塞子,轮廓喷嘴;抛物线,直管)的影响。归一化结果举例说明了一种灵敏的准确方法,可在大约190℃下全局验证还原的化学动力学模型。例如,在超燃式燃烧器中,温度为1atm,相对较低的温度近似于未预混合理想化火焰保持的损失。层流FS在本地定义为最大空气输入速度U(次空气),该速度在熄火时维持g燃料反向喷射的燃烧。它独特地表征了燃料。并且可以将消光的总轴向应变率(通过喷嘴或管径归一化的U(sub air),D(sub n或(sub t)))与计算的消光极限直接进行比较,该极限由一维Navier Stokes流确定-功能解,使用详细的传输和有限速率化学,或(更好的是)详细的二维Navier Stokes数值模拟实验结果定义了理想的阻焰反应性标度,该标度显示了各种汽化的宽范围(50 x)归一化FS液态和气态HC,按升序排列包括:JP-10,甲烷,JP-7,正庚烷,正丁烷,丙烷,乙烷和乙烯H2空气产生的独特火焰异常强烈3 mm管OJB的最新二维数值模拟FS的大约1%,因此我们建议,对于各种纯净和混合HC(不含添加剂)的实验FS和/或FS比,可以提供准确的灭绝的Ts和Ps处的化学动力学模型的整体测试。因此,我们认为FS方法比完全搅拌反应堆中层流燃烧速度或爆燃的测量方法更直接,更基础,例如用于评估理想的超燃冲压火焰保持潜力,因为后者的特点是在没有空气动力应变的情况下进行预混燃烧。 FS直接测量典型的火焰保持温度下非预混燃烧的化学动力学特性。它模仿了通常将燃料注入捕获空气的亚音速火焰保持再循环区域的情况,其中空气动力应变和相关的多组分扩散的影响变得很重要。

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