WIDECARS is a dual-pump coherent anti-Stokes Raman Spectroscopy technique that is capable of simultaneously measuring temperature and species mole fractions of N 2 , O 2 , H 2 , C 2 H 4 , CO, and CO 2 . WIDECARS is designed for measurements of all the major species (except water) in supersonic combustion flows fueled with hydrogen and hydrogen/ethylene mixtures.The two lowest rotational energy levels of hydrogen detectable by WIDECARS are H 2 S(3) and H 2 S(4). The detection of these lines gives the system the capability to measure temperature and species concentrations in regions of the flow containing pure hydrogen fuel at room temperature. OCIS codes: 120.1740, 300.6230. https://ntrs.nasa.gov/search.jsp?R=20100017045 2019-04-04T06:21:37+00:00Z
Optical Society of America
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IntroductionThe design of air-breathing supersonic combustion engines is currently being facilitated by creating computational fluid dynamic (CFD) models of turbulent supersonic combustion flow as in Ref [1]. To create and verify CFD models, time-resolved fundamental properties of turbulent supersonic combustion need to be measured. Coherent anti-Stokes Raman spectroscopy (CARS) [2] is a nonintrusive laser-based measurement technique that can measure space-and timeresolved temperature and species concentrations. Studies of hydrogen-fueled supersonic combustion flows were measured with a CARS system design by O'Byrne et al [3]. The CARS system developed by O'Byrne et al. can measure temperature and species mole fractions of nitrogen, oxygen, and hydrogen. Typically CARS systems can only measure relative species concentrations, but because all the major species present in the combustion flow (except water) were measured, absolute concentration measurements could be made as discussed in Ref.3. Future studies are planned to revisit supersonic combustion flow with hydrogen fuel and a mixture of ethylene and hydrogen fuel. To fully characterize these flows, it is desirable to make measurements of as many properties as possible for the full range of conditions within the flow. In these flows, pure, room-temperature fuel is injected into the flow; therefore some regions of the flow will contain only room temperature fuel (hydrogen and or ethylene). The O'Byrne et al. CARS system is incapable of making measurements in pure, room temperature hydrogen as discussed in Ref [4]. The O'Byrne et al. system is not ideal for measuring combustion of an ethylene-hydrogen fuel mixture because it does not have the capability to measure any of the carbon species present in the flow (CO 2 , C 2 H 4 , and CO).Others have designed CARS systems that are closer to the desired measurement attributes for these flows. Kearney et al. [5] and Beyrau et al. [6] have measured many of the major species present in ethylene-and hydrogen-fueled combustion. Additionally, the Kearney et al. system is capable of the needed dynamic temperature range in pure hydrogen. Flores [7] designed a CARS system that can measure all major species in ethylene and hydrogen combustion except...