Journal of Jilin University(Engineering and Technology Edition) ›› 2025, Vol. 55 ›› Issue (12): 3783-3792.doi: 10.13229/j.cnki.jdxbgxb.20240382

   

Effect of discharge parameters on nanosecond pulse multi⁃channel ignition characteristics of NH3/air mixture

Yong XIONG1(),Jie TIAN1,Yong CHENG1(),Qing-wu ZHAO2   

  1. 1.School of Energy and Power Engineering,Shandong University,Jinan 250061,China
    2.School of Mechanical Engineering Sciences,University of Surrey,Guildford GU27XH,UK
  • Received:2024-04-11 Online:2025-12-01 Published:2026-02-03
  • Contact: Yong CHENG E-mail:1193613299@qq.com;cysgd@sdu.edu.cn

Abstract:

The effect of discharge pulse interval and number on the discharge and ignition characteristics of nanosecond pulse surface dielectric barrier discharge (nSDBD) in NH3/air mixture was studied. The experiment is conducted in a constant volume combustion chamber. Discharge characteristic tests show that nSDBD can generate multiple independently distributed discharge filaments, expanding the range of plasma. When using 30 pulse numbers with a pulse interval of 50 μs, at least 12 discharge filaments are excited, with filament lengths exceeding 14 mm. The ignition characteristic test shows that nSDBD has achieved spatial multi-point ignition. When the pulse interval is 50 μs, 180 discharge pulses generate 6 initial flame kernels surrounding the top electrode. In the NH3/air mixture, there is a phenomenon of initial flame kernels dissipating, resulting in a discrepancy between the number of initial flame kernels and the number of stable combustion flame kernels. As the pulse interval or pulse number increases, the area of the initial flame kernels increases, and the number of stable flame kernels gradually increases from 1 to 6. This effectively shortens the ignition delay of NH3/air mixture, with a reduction of up to 30 ms, approximately 55%. The adjustment of pulse interval and pulse number can effectively control the combustion phase of NH3/air mixture.

Key words: power mechanical engineering, surface dielectric barrier discharge, nanosecond pulsed, multi-channel ignition

CLC Number: 

  • TK411

Fig.1

Experimental setup schematic"

Table 1

Experimental plan for nanosecond pulse multi-channel discharge and ignition characteristics"

方案PI/μsPN?

放电

试验

50,60,701201.0
50100,110,140,160,1801.0

点火

试验

50100~2101.0
60100~2001.0
70100~1801.0

Fig.2

Comparison between measured and calculated values of capacitor charging and discharging currents"

Fig.3

Image processing workflow"

Fig.4

Characteristic parameters of the combustion process: FDT and FRT (PI=50 μs, PN=180, initial pressure of 0.1 MPa, ?=1.0 )"

Fig.5

High-frequency repetitive nSDBD multi-filament discharge images in NH3/air mixture (PI=50 μs, PN=30)"

Fig.6

Images of the development of single-pulse discharge filaments in high-frequency nSDBD (PI=50 μs, PN=40, in NH3/air mixture)"

Fig.7

Variation of filament count with discharge pulses in high-frequency nSDBD (PI=50 μs, in NH3/air mixture)"

Fig.8

Variation of discharge filament length with the number of discharge pulses in high-frequency nSDBD (PI=50 μs, in NH3/air mixture)"

Fig.9

Voltage, current, and energy curves of high-frequency nSDBD (PI=50 μs, PN=30, in NH3/air mixture)"

Fig.10

Typical curves of voltage, current, power, and energy for individual pulses in high-frequency nSDBD (PI=50 μs, in NH3/air mixture)"

Fig.11

Energy characteristics of single-pulse discharge in high-frequency nSDBD (in NH3/air mixture)"

Fig.12

Accumulated energy characteristics of high-frequency nSDBD (PN=30, in NH3/air mixture)"

Fig.13

Development process of kernels under different pulse intervals (PN=120, in NH3/air mixture)"

Fig.14

Development process of kernels under different pulse numbers (PI=50 μs, in NH3/air mixture)"

Fig.15

Development process of kernel radius under different pulse intervals (PN=120, in NH3/air mixture)"

Fig.16

Development process of kernel radius under different pulse numbers (PI=50 μs, in NH3/air mixture)"

Fig.17

Impact of discharge parameters on FDT (in NH3/air mixture)"

Fig.18

Influence of discharge parameters on FRT (in NH3/air mixture)"

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