Experimental investigation and numerical modeling of the effect of voltage parameters on the characteristics of low-pressure argon dielectric barrier discharges
Abstract:In this paper, we have presented the experimental and modeling results of the effect of voltage parameters on the characteristics of the low-pressure Ar dielectric barrier discharge. The frequency and amplitude range was set at 5–19 kHz and 255–370 V, respectively. Our investigations showed that the voltage parameters such as amplitude and frequency have large impact on the discharge behavior. Increase in applied voltage amplitude leads to an increase in discharge current. It is also shown that with increasing… Show more
“…Based on pure air gap discharge simulation [28], the cathode secondary electron emission coefficient is set to 0.004. According to description of secondary electron from material surface reference DBD simulation [11], secondary electron emission of PI surface is set to 0.5; the average energy of secondary electrons ɛ = 2.5 eV [29]. The flux boundary for species k considers a flux contribution due to migration and an inward or outward mass flux determined by surface reactions.…”
Section: Wall Boundary Conditionmentioning
confidence: 99%
“…With the leap of computer computing and storage capacity and development of numerical simulation methods, it is possible to simulate micro‐parameters, such as electric field and charge distribution, in discharge process. At present, the simulation of discharge mostly focuses on air gap discharge [9, 10] between needle‐plate electrodes and dielectric barrier discharge (DBD) between plate electrodes [11, 12]. Compared with surface discharge, the effect of solid insulation on the discharge process need not be considered in the air gap discharge process.…”
A surface discharge non-equilibrium plasma model of air-polyimide under pulsed electrical stress is established, by considering the reaction of charged particles on the dielectric surface and the secondary electron emission caused by the condition that high-energy particles bombard the material surface. The model defines the chemical reaction of air discharge by using simplified set of reactions, which greatly reduces the complexity of the model. To avoid the negative value of particle density in the process of solution, the logarithmic finite-element method is used to solve the model established, so as to implement the dynamic simulation of the surface discharge process. Also, the temporal and spatial evolution of the microparameters such as charge and electric field distribution during discharge are obtained, and the reliability of the model is verified by experiments in terms of discharge development pattern and surface charge accumulation. By comparing the development process of surface discharge under single pulse and repetitive pulses, it can be seen that surface discharge develops from needle electrode to ground electrode under both repetitive pulses and single pulse stress, but the relationship between the discharge propagation time under repetitive pulses and pulse repetition rate is a 'u' curve, and the inflection point moves to higher repetition rate region with the increase of voltage.
“…Based on pure air gap discharge simulation [28], the cathode secondary electron emission coefficient is set to 0.004. According to description of secondary electron from material surface reference DBD simulation [11], secondary electron emission of PI surface is set to 0.5; the average energy of secondary electrons ɛ = 2.5 eV [29]. The flux boundary for species k considers a flux contribution due to migration and an inward or outward mass flux determined by surface reactions.…”
Section: Wall Boundary Conditionmentioning
confidence: 99%
“…With the leap of computer computing and storage capacity and development of numerical simulation methods, it is possible to simulate micro‐parameters, such as electric field and charge distribution, in discharge process. At present, the simulation of discharge mostly focuses on air gap discharge [9, 10] between needle‐plate electrodes and dielectric barrier discharge (DBD) between plate electrodes [11, 12]. Compared with surface discharge, the effect of solid insulation on the discharge process need not be considered in the air gap discharge process.…”
A surface discharge non-equilibrium plasma model of air-polyimide under pulsed electrical stress is established, by considering the reaction of charged particles on the dielectric surface and the secondary electron emission caused by the condition that high-energy particles bombard the material surface. The model defines the chemical reaction of air discharge by using simplified set of reactions, which greatly reduces the complexity of the model. To avoid the negative value of particle density in the process of solution, the logarithmic finite-element method is used to solve the model established, so as to implement the dynamic simulation of the surface discharge process. Also, the temporal and spatial evolution of the microparameters such as charge and electric field distribution during discharge are obtained, and the reliability of the model is verified by experiments in terms of discharge development pattern and surface charge accumulation. By comparing the development process of surface discharge under single pulse and repetitive pulses, it can be seen that surface discharge develops from needle electrode to ground electrode under both repetitive pulses and single pulse stress, but the relationship between the discharge propagation time under repetitive pulses and pulse repetition rate is a 'u' curve, and the inflection point moves to higher repetition rate region with the increase of voltage.
“…The literature [17] considered 12 kinds of particles and 31 kinds of chemical reactions to establish a surface discharge model in N 2 /O 2 environment and obtained the distribution rule of surface charge. Although some progress has been made in these studies, the current simulation of gas discharge is mostly concentrated on the DBD between the plate electrodes [18,19] or the surface discharge under the needle-plate electrode, while the simulation of partial discharge is still in the exploratory stage. Therefore, it is necessary to carry out simulation research on partial discharge of insulation defects of the epoxy interface under the excitation of highfrequency sinusoidal voltage.…”
High‐frequency sinusoidal voltage excitation is proposed as a feasible method to solve the difficulty of partial discharge detection at the epoxy interface. In order to study the development process of partial discharge under high‐frequency stress, a two‐dimensional plasma simulation model of partial discharge for a needle‐plate electrode structure is established by coupling particle transport equation, Poisson equation and plasma chemical reaction. The model adopts a reaction set to reduce the difficulty of modelling generation, transport and disappearance of charged particles. It realises dynamic simulation of the partial discharge at the epoxy interface. The spatial–temporal distribution characteristics of microscopic parameters such as electron density, electron temperature and surface charge are obtained. Based on this simulation model, the partial discharge characteristics of the epoxy interface at different frequencies are further studied in this work. The results show that with the increase of applied voltage frequency, the electron temperature shows an increasing trend, but its increasing rate gradually slows down; while surface charge accumulation decreases uniformly with the increase of applied voltage frequency. These two factors make the partial discharge severest under the frequency of 10 kHz. The results of the model are verified from two aspects of discharge form and discharge intensity by experimental means.
“…With the advancement of computer technology and storage capacity and the establishment of numerical simulation methodologies, it is now possible to measure micro‐parameters in the discharge process, such as the electric field and charge distribution. Air gap discharge between needle‐plate electrodes and dielectric barrier discharge (DBD) between plate electrodes are the two most common discharge simulations at the moment [6, 7]. Edmiston et al.…”
Section: Introductionmentioning
confidence: 99%
“…With the advancement of computer technology and storage capacity and the establishment of numerical simulation methodologies, it is now possible to measure micro-parameters in the discharge process, such as the electric field and charge distribution. Air gap discharge between needle-plate electrodes and dielectric barrier discharge (DBD) between plate electrodes are the two most common discharge simulations at the moment [6,7]. Edmiston et al [8] showed a correspondence between pressure, pulse amplitude, microwave frequency, and the delay time of destructive discharge on the surface within a large range of experimental parameters by using high-power microwave (HPM) surface-flashover experiments.…”
The high‐frequency power transformer (HFPT) has become a vital component of the power system. For HFPT insulations, surface discharge is a serious problem. Polyimide (PI) is a widely used insulating material for HFPT's. A needle‐plate electrode structure‐based experimental setup was developed to produce and measure the surface discharge. This paper first time used the fluid‐kinetic model by adopting the finite element simulation method to address the micro‐level study of surface discharge. This paper aimed at the discharge phenomenon of the PI under the direct action of high‐frequency sinusoidal voltage and has not considered the overvoltage phenomenon caused by the waveform parameters that is the actual high‐frequency action on the PI material. The development of surface discharge at various stages was analysed. Particle densities and electric field distributions versus discharge time were determined. Frequency, temperature, and air pressure have a significant effect on surface discharge behaviour. As a result, the applied voltage reaches its peak value at high‐frequency, so the flashover time of surface discharge is reduced under the high frequency. The electron density of the streamer development increases as the temperature rises, and the time to flashover the channel becomes shorter. The higher the electron density and the longer the discharge channel develops while the gas pressure is lower. The simulation results have high accuracy and good agreement with experimental data.
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