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Development of advanced laser systems and spectroscopic techniques for combustion diagnostic applications.

机译:为燃烧诊断应用开发先进的激光系统和光谱技术。

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Single-longitudinal-mode, narrowband, injection-seeded, pulsed optical parametric (OP) systems have been developed, characterized, and applied for high-resolution spectroscopy of nitric oxide (NO). The OP systems were injection seeded at the idler wavelength using a near-infrared distributed feedback (DFB) diode laser. In the optical parametric generator (OPG) version, two counter-rotating, beta-barium borate (beta-BBO) crystals were pumped by the third-harmonic output of an injection-seeded Nd:YAG laser. An optical parametric oscillator (OPO) version has also been developed by incorporating a feedback cavity at the signal wavelength. The cavity length was not actively controlled. The output signal beam from OPG or OPO was amplified using an optical parametric amplifier (OPA) stage. In both the OPG and OPO, the signal and idler frequency bandwidths are nearly Fourier transform limited and were measured to be 220 MHz. The temporal pulses were smooth and near-Gaussian. The frequency-doubled signal output of the OPO/OPA system was used for single-photon, laser-induced fluorescence (LIF) and laser-induced polarization spectroscopy (LIPS) of NO. The signal output of the OPG/OPA system was also used for sub-Doppler, two-photon LIF of NO.; A detailed investigation was also performed for electronic-resonance-enhanced coherent anti-Stokes Raman spectroscopy (ERE-CARS) of NO. In the ERE-CARS scheme, an ultraviolet probe-laser beam is tuned to an electronic resonance, resulting in a huge resonance enhancement of the ERE-CARS signal. The effect of drastic variations in electronic quenching rate on the NO ERE-CARS signal was investigated experimentally. In contrast to LIF, the ERE-CARS signal was nearly unaffected by the quenchers O2 and CO2. The ERE-CARS signal intensity was also found to increase rapidly between pressures of 0.1-2 bars and remain nearly constant thereafter up to 8 bars, whereas the NO LIF signal drops with increasing pressure. We have also detected NO down to 50 ppm in H2/air flames using ERE-CARS. NO ERE-CARS signals were also recorded in heavily sooting C2H2/air flames with minimal background interferences. These findings are very significant for the development of ERE-CARS as a technique for measuring NO concentrations in high-pressure combustion environments.
机译:已经开发,表征了单纵模,窄带,注入种子,脉冲光学参量(OP)系统,并将其用于一氧化氮(NO)的高分辨率光谱。使用近红外分布反馈(DFB)二极管激光器以空载波长注入OP系统。在光学参量发生器(OPG)版本中,通过注入种子的Nd:YAG激光器的三次谐波输出泵浦了两个反向旋转的硼酸钡钡(β-BBO)晶体。光学参量振荡器(OPO)版本还通过在信号波长处加入反馈腔而开发。腔体长度未得到积极控制。来自OPG或OPO的输出信号束使用光参量放大器(OPA)级进行放大。在OPG和OPO中,信号和惰轮频率带宽几乎都受到傅立叶变换的限制,测量的带宽为220 MHz。时间脉冲是平滑且接近高斯的。 OPO / OPA系统的倍频信号输出用于NO的单光子,激光诱导荧光(LIF)和激光诱导偏振光谱(LIPS)。 OPG / OPA系统的信号输出也用于NO的亚多普勒双光子LIF;还对NO的电子共振相干反斯托克斯拉曼光谱法(ERE-CARS)进行了详细研究。在ERE-CARS方案中,紫外线探测激光束被调谐到电子共振,从而导致ERE-CARS信号的共振大大增强。实验研究了电子猝灭速率急剧变化对NO ERE-CARS信号的影响。与LIF相比,ERE-CARS信号几乎不受淬灭剂O2和CO2的影响。还发现ERE-CARS信号强度在0.1-2 bar的压力之间迅速增加,此后几乎保持恒定,直到8 bar,而NO LIF信号随压力增加而下降。我们还使用ERE-CARS在氢气/空气火焰中检测到低至50 ppm的NO。在严重吹灰的C2H2 /空气火焰中,也没有记录到ERE-CARS信号,且背景干扰最小。这些发现对于开发ERE-CARS作为一种在高压燃烧环境中测量NO浓度的技术非常重要。

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