[Development and performance testing of a high-sensitivity pulsed flame photometric detector].

Jun-Bin Chen, Hao-Yuan Cai, Zhi-Han Deng, Yu-Jie Jin, Jian-Hai Sun
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The detector consisted of five functional modules: the combustion and ignition module, the gas supply module, the optical collection and detection module, the temperature-control module, and the mechanical support and sealing module. The combustion zone consisted of a vertically mounted quartz chamber. The chamber had an outer diameter of 4 mm. Its inner diameter was 2 mm. Its total length was 17.5 mm. The effective combustion length was 12 mm. The calculated chamber volume was 37.68 mm<sup>3</sup>. Numerical simulation was used to examine flame propagation and self-extinction. A 12 mm effective length maintained a stable finger-shaped flame front. The flame was self-terminated near the lower limiting orifice at about 1.97 ms. The hydroxyl radical mass fraction decreased close to baseline within 5 ms, whereas the temperature decayed more gradually and approached its initial level at approximately 30 ms. These results supported the chamber design for periodic pulsed combustion. The optical unit used a quartz light guide and a BG-12 band-pass filter. The filter matched the sulfur emission band near 394 nm. A photomultiplier tube (PMT) recorded the time-resolved emission signal. Two electronic pneumatic control (EPC) units were used for gas regulation. One unit controlled hydrogen and air for the ignition chamber. The other unit controlled hydrogen and air for the combustion chamber. This design separated ignition conditions from analytical combustion conditions. It also reduced uncertainty caused by coupled gas adjustment. The optimization started with the ignition chamber. Then the combustion chamber was optimized under the fixed ignition baseline. Finally, detector temperature and PMT voltage were evaluated. Peak area, sensitivity, and signal-to-noise ratio (SNR) were used as indicators. Gas chromatographic tests used a sulfur-specific quartz capillary column. Nitrogen was used as the carrier gas. The gate delay was 6 ms. The gate width was 18 ms. The trigger level was 500 mV. A stable pulsed flame was obtained at an ignition-chamber hydrogen flow of 8.0 mL/min. The corresponding ignition-chamber air flow was 19.0 mL/min. Under this ignition baseline, the combustion chamber was further adjusted. A higher sulfur response was obtained at 5.0 mL/min hydrogen. The corresponding air flow was 3.7 mL/min. Detector temperature also affected the delayed sulfur emission. The response was low at 110-130 ℃. At about 150 ℃, the delayed sulfur signal was higher. Peak area and sulfur sensitivity were also higher at this temperature. Higher temperatures from 170 to 250 ℃ reduced the peak area and sensitivity. PMT voltage affected signal amplitude, SNR, and waveform fidelity. Increasing the voltage from 590 to 710 V improved the SNR. At 730 V, the delayed emission plateau showed peak clipping. This behavior indicated saturation or nonlinear response in the detection chain. Dynamic dilutions of a 10 μmol/mol hydrogen sulfide (H₂S) standard gas were used to evaluate the linear range. A 1.1 μmol/mol H₂S standard gas was used for the quantitative repeatability test and, after 30-fold dynamic dilution, for determination of the sulfur detection limit. The quantitative repeatability, evaluated from the peak areas of seven consecutive injections, was 0.37%. The sulfur detection limit was 4.1×10⁻<sup>1</sup>³ g/s, and the linear range spanned approximately two orders of magnitude. The developed PFPD showed stable pulsed combustion behavior. It also provided reliable quantitative response for trace sulfur detection. The dual-EPC design helped clarify the relationship between ignition and analytical combustion. 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引用次数: 0

Abstract

The conventional flame photometric detector (FPD) is widely used for sulfur-selective gas chromatography. However, the FPD is sensitive to hydrocarbon backgrounds. Its sulfur response also depends strongly on flame stability. These factors limit stable trace sulfur determination in complex matrices. A pulsed flame photometric detector (PFPD) provides a time-resolved approach to this problem. Sulfur emission appears later than most hydrocarbon background emissions after pulsed combustion. A suitable acquisition window can therefore improve sulfur selectivity. In this study, a high-sensitivity single-channel PFPD was designed and tested. The aim was to establish reproducible operating conditions for trace sulfur analysis. The detector consisted of five functional modules: the combustion and ignition module, the gas supply module, the optical collection and detection module, the temperature-control module, and the mechanical support and sealing module. The combustion zone consisted of a vertically mounted quartz chamber. The chamber had an outer diameter of 4 mm. Its inner diameter was 2 mm. Its total length was 17.5 mm. The effective combustion length was 12 mm. The calculated chamber volume was 37.68 mm3. Numerical simulation was used to examine flame propagation and self-extinction. A 12 mm effective length maintained a stable finger-shaped flame front. The flame was self-terminated near the lower limiting orifice at about 1.97 ms. The hydroxyl radical mass fraction decreased close to baseline within 5 ms, whereas the temperature decayed more gradually and approached its initial level at approximately 30 ms. These results supported the chamber design for periodic pulsed combustion. The optical unit used a quartz light guide and a BG-12 band-pass filter. The filter matched the sulfur emission band near 394 nm. A photomultiplier tube (PMT) recorded the time-resolved emission signal. Two electronic pneumatic control (EPC) units were used for gas regulation. One unit controlled hydrogen and air for the ignition chamber. The other unit controlled hydrogen and air for the combustion chamber. This design separated ignition conditions from analytical combustion conditions. It also reduced uncertainty caused by coupled gas adjustment. The optimization started with the ignition chamber. Then the combustion chamber was optimized under the fixed ignition baseline. Finally, detector temperature and PMT voltage were evaluated. Peak area, sensitivity, and signal-to-noise ratio (SNR) were used as indicators. Gas chromatographic tests used a sulfur-specific quartz capillary column. Nitrogen was used as the carrier gas. The gate delay was 6 ms. The gate width was 18 ms. The trigger level was 500 mV. A stable pulsed flame was obtained at an ignition-chamber hydrogen flow of 8.0 mL/min. The corresponding ignition-chamber air flow was 19.0 mL/min. Under this ignition baseline, the combustion chamber was further adjusted. A higher sulfur response was obtained at 5.0 mL/min hydrogen. The corresponding air flow was 3.7 mL/min. Detector temperature also affected the delayed sulfur emission. The response was low at 110-130 ℃. At about 150 ℃, the delayed sulfur signal was higher. Peak area and sulfur sensitivity were also higher at this temperature. Higher temperatures from 170 to 250 ℃ reduced the peak area and sensitivity. PMT voltage affected signal amplitude, SNR, and waveform fidelity. Increasing the voltage from 590 to 710 V improved the SNR. At 730 V, the delayed emission plateau showed peak clipping. This behavior indicated saturation or nonlinear response in the detection chain. Dynamic dilutions of a 10 μmol/mol hydrogen sulfide (H₂S) standard gas were used to evaluate the linear range. A 1.1 μmol/mol H₂S standard gas was used for the quantitative repeatability test and, after 30-fold dynamic dilution, for determination of the sulfur detection limit. The quantitative repeatability, evaluated from the peak areas of seven consecutive injections, was 0.37%. The sulfur detection limit was 4.1×10⁻1³ g/s, and the linear range spanned approximately two orders of magnitude. The developed PFPD showed stable pulsed combustion behavior. It also provided reliable quantitative response for trace sulfur detection. The dual-EPC design helped clarify the relationship between ignition and analytical combustion. The optimized conditions provide an experimental basis for self-developed PFPD systems.

[高灵敏度脉冲火焰光度检测器的研制与性能测试]。
传统的火焰光度检测器(FPD)广泛应用于硫选择气相色谱。然而,FPD对碳氢化合物背景很敏感。它的硫反应也很大程度上取决于火焰稳定性。这些因素限制了复杂基质中稳定痕量硫的测定。脉冲火焰光度检测器(PFPD)为这一问题提供了一种时间解决方法。脉冲燃烧后硫排放比大多数碳氢化合物本底排放出现得晚。因此,合适的获取窗口可以提高硫的选择性。本研究设计并测试了一种高灵敏度单通道PFPD。目的是建立可重复的操作条件的痕量硫分析。探测器由五个功能模块组成:燃烧与点火模块、供气模块、光采集与检测模块、温控模块、机械支撑与密封模块。燃烧区由一个垂直安装的石英室组成。该腔室外径为4毫米。其内径为2mm。全长17.5 mm。有效燃烧长度为12 mm。计算腔体体积为37.68 mm3。采用数值模拟方法研究了火焰的传播和自灭。12毫米的有效长度维持了稳定的指状火焰前缘。火焰在约1.97 ms时在下限孔附近自行终止。羟基自由基质量分数在5 ms内下降到接近基线的水平,而温度则在30 ms左右逐渐下降到接近初始水平。这些结果支持了周期性脉冲燃烧的燃烧室设计。光学单元使用石英光导和BG-12带通滤波器。滤光片匹配394 nm附近的硫发射波段。光电倍增管(PMT)记录了时间分辨发射信号。两个电子气动控制(EPC)单元用于气体调节。一个单元控制点火室的氢气和空气。另一个单元控制燃烧室的氢气和空气。该设计将点火条件与分析燃烧条件分开。它还减少了耦合气体调节引起的不确定性。优化从点火室开始。然后在固定点火基线下对燃烧室进行了优化。最后,对探测器温度和PMT电压进行了评估。以峰面积、灵敏度、信噪比(SNR)为指标。气相色谱测试使用硫专用石英毛细管柱。氮气被用作载气。栅极延迟为6毫秒。栅极宽度为18 ms。触发电平为500mv。在点火室氢气流量为8.0 mL/min时,获得了稳定的脉冲火焰。相应的点火室空气流量为19.0 mL/min。在此点火基准下,进一步调整燃烧室。在5.0 mL/min氢气条件下,硫反应较高。相应的空气流量为3.7 mL/min。探测器温度对硫延迟排放也有影响。110 ~ 130℃时反应较弱。在150℃左右,延迟硫信号较高。峰面积和硫敏感性在此温度下也较高。温度从170到250℃降低了峰面积和灵敏度。PMT电压影响信号幅度、信噪比和波形保真度。将电压从590 V提高到710 V,提高了信噪比。在730v时,延迟发射平台出现峰削。这种行为表明在检测链中存在饱和或非线性响应。采用10 μmol/mol硫化氢(H₂S)标准气体的动态稀释来评估线性范围。采用1.1 μmol/mol H₂S标准气体进行定量重复性试验,经30倍动态稀释后测定硫的检出限。从连续7次注射的峰面积评价,定量重复性为0.37%。硫的检出限为4.1×10⁻1³g/s,线性范围约为两个数量级。所研制的PFPD具有稳定的脉冲燃烧性能。为痕量硫的检测提供了可靠的定量响应。双epc设计有助于澄清点火和分析燃烧之间的关系。优化条件为自行研制PFPD系统提供了实验依据。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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