Influence of Rise Time of Pulse Voltage on the Pulsed Plasma Conversion of Methane

Recently, the authors developed a high-frequency pulsed plasma for methane conversion to acetylene and hydrogen. Such a pulsed plasma is potentially competitive to the commercial acetylene production processes. For the industrialization of this plasma technology, the influence of some factors, such...

Full description

Saved in:
Bibliographic Details
Published inEnergy & fuels Vol. 15; no. 5; pp. 1300 - 1303
Main Authors Yao, S. L, Suzuki, E, Meng, N, Nakayama, A
Format Journal Article
LanguageEnglish
Published Washington, DC American Chemical Society 01.09.2001
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:Recently, the authors developed a high-frequency pulsed plasma for methane conversion to acetylene and hydrogen. Such a pulsed plasma is potentially competitive to the commercial acetylene production processes. For the industrialization of this plasma technology, the influence of some factors, such as the pulse voltage, rise time of pulse voltage, pulse frequency, kind of background gases, temperature of the background gases, and electrode geometries, on methane conversion and the development of a pulse power supply should be cleared. In this study, the influence of the rise time of the pulse voltage on methane conversion has been investigated using a coaxial cylindrical type of reactor. The pulsed streamer/spark discharge occurred more easily with a pulse voltage of short rise time than with that of long rise time. The energy injection rate into the discharge space decreased with increasing the rise time of the pulse voltage. The rise time of the pulse voltage did not remarkably influence the methane conversion efficiency and selectivity of each product at pulse frequencies higher than 2 kPPS.
Bibliography:This paper was published at the AIChE 2001 Spring National Meeting, Houston, TX, April 22−26, 2001.
ark:/67375/TPS-5G7QNGSK-T
istex:A8118204629C5BB104902D163F51B126EA2F157C
ISSN:0887-0624
1520-5029
DOI:10.1021/ef0100909