Katherine C. Opacich , Joshua A.T. Gray , Joshua S. Heyne , Timothy M. Ombrello
{"title":"用点火概率表征纳秒脉冲高频和直流电弧放电","authors":"Katherine C. Opacich , Joshua A.T. Gray , Joshua S. Heyne , Timothy M. Ombrello","doi":"10.1016/j.combustflame.2025.114402","DOIUrl":null,"url":null,"abstract":"<div><div>Ignition probability and flame kernel development were measured in methane–air mixtures at equivalence ratios (ϕ) of 0.47 – 0.55 with a flow velocity of 5 m/s using a nanosecond-pulsed high-frequency discharge (NPHFD) exciter and a DC arc discharge (conventional) exciter. The ignition performance of both excitation systems was compared across multiple average power conditions, namely 110, 180, and 375 W. Data was collected at two additional average power conditions (35 and 53 W) for the NPHFD exciter. A novel metric to define a successful ignition event was demonstrated in that ignition probability was based on an area growth rate criterion that must be met within a given amount of time. In total, four minimum growth rate values (0.001, 10, 20, and 30 mm<sup>2</sup>/ms) and four characteristic time intervals (6 – 9, 9 – 12, 12 – 15, and 15 – 18 ms) were utilized to distinguish between an ignition success and failure. At the most lenient definition of a successful ignition event (lowest growth rate criterion in the longest characteristic time interval), the conventional exciter outperformed the NPHFD exciter in terms of ignition probability at leaner equivalence ratios. The poor performance of the NPHFD exciter at lean conditions was due to localized quenching of the flame kernel early in its development from the entrainment of cold reactants between pulses and the onset of jetting motion that further split the reacting region. As the growth rate threshold for a successful ignition event was increased, the ignition probability curves for all test conditions shifted to higher equivalence ratios, indicating that a more reactive mixture was needed to sufficiently grow the kernels to meet the criteria. However, the ignition probability curves for the NPHFD exciter were less sensitive overall to increasing the growth rate threshold for a successful ignition event due to its ability to generate flame kernels with rapid growth rates at higher equivalence ratios. Decreasing the characteristic time interval did not have a large impact on ignition probability for either exciter until the minimum growth rate criterion was increased to 20 mm<sup>2</sup>/ms, upon which the conventional exciter exhibited a greater drop in ignition probability at higher equivalence ratios.</div></div>","PeriodicalId":280,"journal":{"name":"Combustion and Flame","volume":"281 ","pages":"Article 114402"},"PeriodicalIF":6.2000,"publicationDate":"2025-08-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Characterizing nanosecond-pulsed high-frequency and DC Arc discharges in terms of ignition probability\",\"authors\":\"Katherine C. Opacich , Joshua A.T. Gray , Joshua S. Heyne , Timothy M. Ombrello\",\"doi\":\"10.1016/j.combustflame.2025.114402\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Ignition probability and flame kernel development were measured in methane–air mixtures at equivalence ratios (ϕ) of 0.47 – 0.55 with a flow velocity of 5 m/s using a nanosecond-pulsed high-frequency discharge (NPHFD) exciter and a DC arc discharge (conventional) exciter. The ignition performance of both excitation systems was compared across multiple average power conditions, namely 110, 180, and 375 W. Data was collected at two additional average power conditions (35 and 53 W) for the NPHFD exciter. A novel metric to define a successful ignition event was demonstrated in that ignition probability was based on an area growth rate criterion that must be met within a given amount of time. In total, four minimum growth rate values (0.001, 10, 20, and 30 mm<sup>2</sup>/ms) and four characteristic time intervals (6 – 9, 9 – 12, 12 – 15, and 15 – 18 ms) were utilized to distinguish between an ignition success and failure. At the most lenient definition of a successful ignition event (lowest growth rate criterion in the longest characteristic time interval), the conventional exciter outperformed the NPHFD exciter in terms of ignition probability at leaner equivalence ratios. The poor performance of the NPHFD exciter at lean conditions was due to localized quenching of the flame kernel early in its development from the entrainment of cold reactants between pulses and the onset of jetting motion that further split the reacting region. As the growth rate threshold for a successful ignition event was increased, the ignition probability curves for all test conditions shifted to higher equivalence ratios, indicating that a more reactive mixture was needed to sufficiently grow the kernels to meet the criteria. However, the ignition probability curves for the NPHFD exciter were less sensitive overall to increasing the growth rate threshold for a successful ignition event due to its ability to generate flame kernels with rapid growth rates at higher equivalence ratios. Decreasing the characteristic time interval did not have a large impact on ignition probability for either exciter until the minimum growth rate criterion was increased to 20 mm<sup>2</sup>/ms, upon which the conventional exciter exhibited a greater drop in ignition probability at higher equivalence ratios.</div></div>\",\"PeriodicalId\":280,\"journal\":{\"name\":\"Combustion and Flame\",\"volume\":\"281 \",\"pages\":\"Article 114402\"},\"PeriodicalIF\":6.2000,\"publicationDate\":\"2025-08-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Combustion and Flame\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0010218025004390\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ENERGY & FUELS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Combustion and Flame","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0010218025004390","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENERGY & FUELS","Score":null,"Total":0}
Characterizing nanosecond-pulsed high-frequency and DC Arc discharges in terms of ignition probability
Ignition probability and flame kernel development were measured in methane–air mixtures at equivalence ratios (ϕ) of 0.47 – 0.55 with a flow velocity of 5 m/s using a nanosecond-pulsed high-frequency discharge (NPHFD) exciter and a DC arc discharge (conventional) exciter. The ignition performance of both excitation systems was compared across multiple average power conditions, namely 110, 180, and 375 W. Data was collected at two additional average power conditions (35 and 53 W) for the NPHFD exciter. A novel metric to define a successful ignition event was demonstrated in that ignition probability was based on an area growth rate criterion that must be met within a given amount of time. In total, four minimum growth rate values (0.001, 10, 20, and 30 mm2/ms) and four characteristic time intervals (6 – 9, 9 – 12, 12 – 15, and 15 – 18 ms) were utilized to distinguish between an ignition success and failure. At the most lenient definition of a successful ignition event (lowest growth rate criterion in the longest characteristic time interval), the conventional exciter outperformed the NPHFD exciter in terms of ignition probability at leaner equivalence ratios. The poor performance of the NPHFD exciter at lean conditions was due to localized quenching of the flame kernel early in its development from the entrainment of cold reactants between pulses and the onset of jetting motion that further split the reacting region. As the growth rate threshold for a successful ignition event was increased, the ignition probability curves for all test conditions shifted to higher equivalence ratios, indicating that a more reactive mixture was needed to sufficiently grow the kernels to meet the criteria. However, the ignition probability curves for the NPHFD exciter were less sensitive overall to increasing the growth rate threshold for a successful ignition event due to its ability to generate flame kernels with rapid growth rates at higher equivalence ratios. Decreasing the characteristic time interval did not have a large impact on ignition probability for either exciter until the minimum growth rate criterion was increased to 20 mm2/ms, upon which the conventional exciter exhibited a greater drop in ignition probability at higher equivalence ratios.
期刊介绍:
The mission of the journal is to publish high quality work from experimental, theoretical, and computational investigations on the fundamentals of combustion phenomena and closely allied matters. While submissions in all pertinent areas are welcomed, past and recent focus of the journal has been on:
Development and validation of reaction kinetics, reduction of reaction mechanisms and modeling of combustion systems, including:
Conventional, alternative and surrogate fuels;
Pollutants;
Particulate and aerosol formation and abatement;
Heterogeneous processes.
Experimental, theoretical, and computational studies of laminar and turbulent combustion phenomena, including:
Premixed and non-premixed flames;
Ignition and extinction phenomena;
Flame propagation;
Flame structure;
Instabilities and swirl;
Flame spread;
Multi-phase reactants.
Advances in diagnostic and computational methods in combustion, including:
Measurement and simulation of scalar and vector properties;
Novel techniques;
State-of-the art applications.
Fundamental investigations of combustion technologies and systems, including:
Internal combustion engines;
Gas turbines;
Small- and large-scale stationary combustion and power generation;
Catalytic combustion;
Combustion synthesis;
Combustion under extreme conditions;
New concepts.