研究目的
Investigating the use of picosecond laser-induced breakdown spectroscopy (ps-LIBS) for the determination of local equivalence ratios in atmospheric-pressure adiabatic methane–air flames and examining the stability of the ps-LIBS signal in a high-pressure nitrogen cell.
研究成果
The study demonstrates the potential of picosecond-duration pulses for improving LIBS-based equivalence-ratio measurements in both atmospheric- and high-pressure combustion environments. Higher laser energies and shorter camera delay times (~20 ns) were found favorable for accurate and precise measurements. The ps-LIBS plasma emission and spatial position were stable at elevated pressures, indicating advantages over traditional ns-LIBS for high-pressure applications.
研究不足
The study acknowledges the presence of continuum emission in the spectrum of the picosecond laser-induced plasma, albeit to a lesser degree than in nanosecond plasma. The stochastic nature of the LIBS plasma and chaotic evolution of the plasma introduce measurement fluctuations, particularly at longer time delays.
1:Experimental Design and Method Selection:
The study employed a diode-pumped high-energy picosecond laser for LIBS measurements in methane–air flames and a high-pressure nitrogen cell. The methodology focused on optimizing the signal-to-noise ratio (S/N) and minimizing measurement uncertainties by analyzing the dependence of the plasma emission ratio Hα (656 nm)/NII (568 nm) on laser energy and time-delay.
2:Sample Selection and Data Sources:
Premixed, laminar methane–air flames at atmospheric pressure and a high-pressure nitrogen cell were used as samples. Data acquisition involved spectral emissions from the laser-induced plasma.
3:List of Experimental Equipment and Materials:
A diode-pumped high-energy picosecond laser (Ekspla, PL2330), a spectrometer (Princeton Instruments, SpectraPro 2300i), and an ICCD (Princeton Instrument, PI-Max 4) were used. The setup included a Hencken burner for flame studies.
4:Experimental Procedures and Operational Workflow:
The laser was focused on the sample to create a plasma, and the emitted light was collected and analyzed. The study varied laser energy and time delays to optimize measurements.
5:Data Analysis Methods:
Spectral data processing involved background subtraction and curve fitting to remove continuum emission contributions, focusing on the Hα (656 nm)/NII (568 nm) ratio for equivalence ratio determination.
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