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中国物理学会期刊

四边形石英网格介质阻挡放电中斑图的研究

Study on patterns in square quartz grid dielectric barrier discharge

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  • 本工作通过设计一种四边形石英网格介质阻挡放电装置,首次观察到了四边形点框架阵列斑图和四边形十字点晕阵列斑图.通过求解拉普拉斯方程发现气隙中外加电场呈四边形阵列分布.采用光电倍增管和高速照相机对上述两种斑图进行时空分辨测量,结果表明:四边形点框架阵列斑图由四角点和四边形框架两个子结构组成,四角点比四边形框架先放电;四边形十字点晕阵列斑图包含中心点、四角点和菱形框架三个子结构,并按顺序依次放电.值得指出的是,上述斑图子结构在每个石英网孔中的放电具有同时性.使用光谱仪对结构更复杂的四边形十字点晕阵列斑图的发射光谱进行测量,发现其子结构均处于不同的等离子体状态.理论上,通过求解泊松方程对其进一步研究,结果很好地解释了实验现象,并给出了斑图的形成机制.

     

    In this study, a square quartz grid dielectric barrier discharge device is designed, in which a square dot frame lattice pattern and a square cross dot halo lattice pattern are observed for the first time. These plasma patterns, combined with the quartz grid, constitute a plasma photonic crystal with a square lattice arrangement. Solving the Laplace equation reveals that the applied electric field in the gas gap exhibits a square lattice distribution. The spatiotemporal evolution of the above two patterns is characterized using two photomultiplier tubes and an intensified charge coupled device. Results indicate that the square dot frame lattice pattern consists of two substructures: corner dots and square frame. The corner dots discharge before the square frame. The emission intensities of the corner dots and square frame differ significantly, with a brightness ratio of approximately 8:5. The square cross dot halo lattice pattern consists of three substructures: central dots, corner dots, and rhombic frame. The discharge sequence is central dots→corner dots→rhombic frame. The brightness ratio among the three substructures is approximately 17:16:4. This variation indicates that the intensity of electron avalanches differs across distinct substructure locations. Notably, the pattern substructures discharge synchronously across all holes of the quartz grid. The emission spectra of the square cross dot halo lattice pattern are measured using a spectrograph. The vibrational temperatures at the central dot, corner dot, and rhombic frame are 2527±55 K, 2559±57 K, and 2611±59 K, respectively. It indicates a non-uniform vibrational temperature distribution within each grid hole. Specifically, the relative populations of nitrogen molecules across different vibrational energy levels vary among distinct substructures. It reveals that the substructures of the pattern are in different plasma states. Theoretically, the electric field distributions of the square cross dot halo lattice pattern at different times are simulated by solving the Poisson equation. It effectively elucidates the formation mechanism of the pattern in the square quartz grid dielectric barrier discharge device. This work not only advances the study of pattern dynamics but also provides a new approach for the design of plasma photonic crystals.

     

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