Abstract

To examine the plasma-assisted combustion of a scramjet, a microwave-enhanced gliding arc plasma method was proposed in this study, and the flame structure and combustion instability were observed. The mechanism of plasma-assisted combustion was obtained via a Bunsen experiment, and then the influence on supersonic combustion was obtained on a direct-connected scramjet. The active species of the flame was determined via optical emission spectroscopy, and the flame temperature was measured with a thermocouple. The luminous intensity of the OH radicals in the flame increased ninefold when the flame temperature was increased to 1573 K, but the luminous intensity of CH* and C2 was not obviously changed with the excitation of arc plasma. Moreover, the DC arc plasma had no effect on the rotation and the vibration temperature of OH radicals under these experimental conditions. In the range of microwave energy less than 800 W, there was no typical change in the intensity of the radicals; however, when the microwave power was up to 1000 W, the effect became obvious. When plasma was applied to the scramjet, the plasma caused the pre-combustion shock train to move forward, and the initial and stable position of the flame was transferred from the cavity shear layer to the front of the fuel jet. These results clearly show that plasma free radical mechanisms cause changes to combustion modes.

Highlights

  • Ignition and flame stabilization is challenging work in a scramjet [1,2,3]

  • Traditional passive flame stabilization methods stabilize a flame in a vortex structure to achieve the purpose of stable combustion, which is dominated by supersonic inflow and formed passively

  • Analysis of Flame Emission Spectra Influenced by Arc Plasma

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Summary

Introduction

Ignition and flame stabilization is challenging work in a scramjet [1,2,3]. The residence time of air in a combustor (tflow ≈ 0.5 ms) is even shorter than the typical self-ignition time of fuel (tig ≈ 1–2 ms) [4,5,6]. Traditional passive flame stabilization methods (such as cavity and plate flame stabilization) stabilize a flame in a vortex structure to achieve the purpose of stable combustion, which is dominated by supersonic inflow and formed passively. The interaction between the instability of the inflow and the combustion affects the flame structure [7,8,9,10,11]. A more effective flame stabilization method is needed in order to stabilize flames actively so that the flame structure can be accurately controlled In the process of acceleration, it has been pointed out that the combustor inlet flow acceleration will lead to the transition of the flame mode [12,13].

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