Generation of a large-scale homogeneous DBD using polyethylene terephthalate as dielectric material in open air

J Junxia Ran (Engineering Research Center of Zero-carbon Energy Buildings and Measurement Techniques, Ministry of Education 2 , Baoding 071002,) T Tong Su Y Yixun Zhou (College of Physics Science and Technology, Hebei University 1 , Baoding 071002,) T Tianyu Liu (International Collaborative Laboratory of 2D Materials for Optoelectronics Science and Technology of Ministry of Education, Institute of Microscale Optoelectronics) Q Qinyi Chen (State Key Laboratory of Natural Medicines and Jiangsu Key Laboratory of Drug Discovery for Metabolic Diseases, Center of Advanced Pharmaceuticals and Biomaterials) H Han Zhang H Huanxia Sun (Engineering Research Center of Zero-carbon Energy Buildings and Measurement Techniques, Ministry of Education 3 , Baoding 071002,) J Junze Jiang (College of Physics Science and Technology, Hebei University 1 , Baoding 071002,) X Xuexue Zhang J Junyu Chen (School of Marine Sciences, Sun Yat-sen University) M Mo Chen (Obstetrics and Gynecology Hospital of Fudan University Shanghai China) R Ruoqing Su (College of Physics Science and Technology, Hebei University 1 , Baoding 071002,) Q Qing Li X Xuechen Li (Department of Chemistry, State Key Laboratory of Synthetic Chemistry, The University of Hong Kong, Pokfulam Road, Hong Kong, Hong Kong SAR 999077, P. R. China)

Abstract

Dielectric barrier discharge (DBD) in open air usually operates in a filamentary mode, which limits the widespread application of DBD technology in the industrial field. In this Letter, a large-scale homogeneous DBD is obtained by using a wire mesh electrode in open air with a relatively high argon flow velocity. Polyethylene terephthalate (PET) is covered on a quartz plate, and they work together as dielectric materials. There is only one wide pulse of optical signal in each half voltage cycle for the homogeneous discharge. Fast photography reveals that the discharge is uniformly distributed over the entire electrode surface during the discharge period. When argon flow velocity is relatively low, the discharge is filamentous. There are multiple narrow optical signal pulses in each half voltage cycle for the filamentary discharge. Optical emission spectroscopy indicates that electron density (ne), electron temperature (Te), molecular vibrational temperature (Tvib), and gas temperature (Tg) decline in both homogeneous discharge and filamentary discharge with increasing argon flow velocity. Polyvinyl chloride and polypropylene dielectrics behave similar to PET for generating homogeneous discharge, which is of great significance for the uniform surface treatment of various materials.

Article Details

Volume / Issue Vol. 127, Issue 6
Published August 11, 2025
ISSN 0003-6951
Publisher American Institute of Physics

Journal Info

Applied Physics Letters

American Institute of Physics

ISSN: 0003-6951 Physical Sciences

Authors (14)

J

Junxia Ran

Engineering Research Center of Zero-carbon Energy Buildings and Measurement Techniques, Ministry of Education 2 , Baoding 071002,

T

Tong Su

Y

Yixun Zhou

College of Physics Science and Technology, Hebei University 1 , Baoding 071002,

T

Tianyu Liu

International Collaborative Laboratory of 2D Materials for Optoelectronics Science and Technology of Ministry of Education, Institute of Microscale Optoelectronics

Q

Qinyi Chen

State Key Laboratory of Natural Medicines and Jiangsu Key Laboratory of Drug Discovery for Metabolic Diseases, Center of Advanced Pharmaceuticals and Biomaterials

H

Han Zhang

H

Huanxia Sun

Engineering Research Center of Zero-carbon Energy Buildings and Measurement Techniques, Ministry of Education 3 , Baoding 071002,

J

Junze Jiang

College of Physics Science and Technology, Hebei University 1 , Baoding 071002,

X

Xuexue Zhang

J

Junyu Chen

School of Marine Sciences, Sun Yat-sen University

M

Mo Chen

Obstetrics and Gynecology Hospital of Fudan University Shanghai China

R

Ruoqing Su

College of Physics Science and Technology, Hebei University 1 , Baoding 071002,

Q

Qing Li

X

Xuechen Li

Department of Chemistry, State Key Laboratory of Synthetic Chemistry, The University of Hong Kong, Pokfulam Road, Hong Kong, Hong Kong SAR 999077, P. R. China