A variational method for the sheath potential of hypersonic leading edges with space-charge limitations

• Published in: Physics of plasmas 2024-10, Vol.31 (10)
• Main Authors: Ghoniem, Nasr M., Brown, David B., Huang, Yue
• Format: Article
• Language: English
• Subjects: 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; Boundary conditions; Charge efficiency; Cooling; Cooling effects; Critical temperature; Electric potential; Electron emission; Finite element method; Hypersonic aircraft; Leading edges; Plasma density; Poisson equation; Sheath potential, plasma, heat flux, plasma-facing component; Sheaths; Space charge; Sweat cooling; Thermionic emission; Three dimensional analysis; Transition temperature; Transpiration
• ISSN: 1070-664X; 1089-7674
• DOI: 10.1063/5.0222634

Electron transpiration cooling for the leading edges (LE) of hypersonic aircraft utilizes thermionic emission; however, space-charge effects limit the electron emission rate, potentially diminishing the efficiency of this cooling mechanism. We develop a variational weak form of the Poisson equation that describes the sheath potential and then numerically solve it using the finite element method. This formulation has two main benefits: (1) the space-charge limit condition can be incorporated as a constraint and (2) it allows for the analysis of three-dimensional geometries with complex boundary conditions. We demonstrate that the current emitted from the surface of an LE is generally a small fraction of the Child–Langmuir limit due to space charge. We then propose several methods to enhance the emitted current from the surface and to boost the cooling effect of thermionic emission. These include increasing the plasma density, applying a negative surface potential, and using fringe fields under suitable geometric conditions. For a LaB6 emitting LE, the total emitted current is shown to be minimal and independent of the temperature of a surface with floating potential. However, when a negative potential is applied and the surface is heated, the emitted current follows the Richardson–Dushman relationship up to a critical temperature, beyond which it remains constant. At an applied surface potential of −5 V, the critical temperature is around 1700 K.