Gas-flow rate and reynolds number in a tube of plasma jet device

Sehwan Jhin, Yunjung Kim, Won Young Lee, D. Jin, Hong-Keun Yu, Hyunchul Kim, J. Koo, G. Cho
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引用次数: 3

Abstract

Summary form only given. For flow in a pipe or tube, the Reynolds number (Re) is generally defined with fluid velocity, tube diameter, and kinematic viscosity. With a certain value of Re, the flow will become unstable and turbulent. This instability occurs with different fluids, usually when Re is over 2000. The laminar flow is stable if Re is less than 2000. In the interval between 2000 and 4000, laminar and turbulent flows are possible and are called "transition" flows, depending on other factors, such as pipe roughness and flow uniformity. In an atmospheric plasma jet of pencil type, a glass tube is used to insert the discharge gas. The property of plasma jet depends on the gas flow velocity which is given by the tube diameter and the volumetric gas flow rate. However, there exists an optimal flow velocity to obtain a stable plasma jet. The dependence of flow velocity on the instability of discharge plasma can be analyzed with Reynolds number which defines the stability of flow such as the stable laminar flow and the turbulent flow in hydro-kinetics. In this report the optimum flow velocity in a glass tube of plasma jet is investigated according to the stability of discharge plasma with the variation of Reynolds number. In the range of stable discharge where the laminar flow is sustained, the length of plasma jet column and plume is increased and the operational discharge voltage is decreased as the flow velocity is increased in the glass tube. However, if the gas flow velocity is increased to be over the critical value of turbulent flow, the length of plasma jet column as well as the plasma current varies unstably. In the conclusion the flow velocity has the limited value to keep the laminar flow inside the glass tube for the stable discharge of plasma jet.
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等离子体射流装置管内气体流速和雷诺数
只提供摘要形式。对于管道或管中的流动,雷诺数(Re)通常用流体速度、管径和运动粘度来定义。当Re值一定时,流动将变得不稳定和湍流。这种不稳定性发生在不同的流体中,通常在Re大于2000时。当Re小于2000时,层流是稳定的。在2000年至4000年之间,层流和湍流流动是可能的,被称为“过渡”流动,这取决于其他因素,如管道粗糙度和流动均匀性。在铅笔型大气等离子体射流中,用玻璃管插入放电气体。等离子体射流的特性取决于气体流速,而气体流速是由管径和气体体积流速决定的。然而,要获得稳定的等离子体射流,存在一个最佳流速。流速对放电等离子体不稳定性的依赖关系可以用雷诺数来分析,雷诺数定义了流体动力学中稳定层流和湍流等流动的稳定性。本文根据放电等离子体随雷诺数变化的稳定性,研究了玻璃管内等离子体射流的最佳流速。在维持层流的稳定放电范围内,随着玻璃管内流速的增大,等离子体射流柱和羽流的长度增大,放电电压降低。但是,当气体流速增加到湍流的临界值以上时,等离子体射流柱的长度和等离子体电流的变化都不稳定。结果表明,为了保证等离子体射流的稳定放电,在玻璃管内保持层流存在一定的流速限制值。
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