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首页> 外文期刊>Experiments in Fluids: Experimental Methods and Their Applications to Fluid Flow >Combined phosphor and CARS thermometry at the wall-gas interface of impinging flame and jet systems
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Combined phosphor and CARS thermometry at the wall-gas interface of impinging flame and jet systems

机译:撞击火焰和喷射系统的壁-气界面处的荧光粉和CARS组合测温

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For the determination of surface normal temperature gradients, a generic system was built up consisting of two opposed, vertical nozzles impinging onto a flat, horizontal copper plate. From below, the plate was heated by non-reacting, turbulent air jets (Re = 5,000) and by a laminar flame (lambda = 0.7, Re = 350), respectively. For well-defined boundary conditions, the plate was cooled by a turbulent cold jet from above in both cases. Wall temperature as well as gas temperature distributions within and outside of the thermal boundary layer of the hot side of the system were determined. The radial surface temperature profile of the plate was measured by coating it with thermographic phosphors (TP), materials whose phosphorescence decay time is dependent on their temperature. The TP was excited electronically by a frequency-tripled Nd:YAG laser (355 nm). The temporal decay of the phosphorescence intensity was measured pointwise by a photomultiplier tube. In this case, the 659 nm emission line of Mg4FGeO6:Mn was monitored. Non-intrusive point measurements of the gas temperature close to the surface were performed by rovibrational coherent anti-Stokes Raman spectroscopy (CARS) of diatomic nitrogen. Beams from a seeded, frequency-doubled Nd:YAG laser (532 nm) and from a modeless broadband dye laser (607 nm) were phase-matched into a surface-parallel, planar-boxcars configuration. The temperature data could be collected as close as 300 mu m to the surface. Thermographic phosphors as well as CARS proved to be consistent for wall temperature and boundary layer measurements in all test cases. The results and challenges of this approach are discussed.
机译:为了确定表面正常温度梯度,建立了一个通用系统,该系统由两个相对的垂直喷嘴撞击到平坦的水平铜板上。从下方,分别通过无反应的湍流空气喷嘴(Re = 5,000)和层流火焰(λ= 0.7,Re = 350)加热板。对于界限分明的边界条件,在两种情况下均通过湍流冷射流从上方冷却板。确定了系统热侧的热边界层内部和外部的壁温以及气体温度分布。通过用热成像磷光体(TP)涂覆该板来测量其径向表面温度分布,该材料的磷光衰减时间取决于其温度。 TP由三倍频的Nd:YAG激光(355 nm)电激发。用光电倍增管逐点测量磷光强度的时间衰减。在这种情况下,监测了Mg4FGeO6:Mn的659 nm发射线。通过双原子氮的振动相干反斯托克斯拉曼光谱法(CARS)对靠近表面的气体温度进行非侵入式测量。来自播种的,倍频Nd:YAG激光(532 nm)和来自无模宽带染料激光(607 nm)的光束进行相位匹配,以形成平行于表面的平面棚车配置。可以收集到距离地面300微米的温度数据。在所有测试案例中,热成像荧光粉和CARS在壁温和边界层测量中均被证明是一致的。讨论了这种方法的结果和挑战。

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