Reduction of breakdown threshold by metal nanoparticle seeding in a DC microdischarge
© Sawyer et al.; licensee Springer. 2015
Received: 20 October 2014
Accepted: 23 December 2014
Published: 28 January 2015
Significant reduction of the breakdown threshold in a DC microdischarge via seeding metal nanoparticles has been demonstrated. Compared to standard Paschen curves in dry air, reductions in the breakdown voltage of 5% to 25% were obtained for PD values (the product of pressure and electrode gap distance) ranging from 20 to 40 Torr-cm by seeding aluminum and iron nanoparticles with mean sizes of 75 nm and 80 nm, respectively. No secondary energy source was required to achieve this breakdown threshold reduction. From high-speed chemiluminescence imaging of the discharge evolution, breakdown was shown to be initiated at reduced voltages. Following breakdown, the increase in temperature ignited some of the nanoparticles near the cathode. Results suggest that possible charging of the nanoparticles within the gap may reduce the effective transient distance, leading to the threshold reduction.
KeywordsMicrodischarge Metal nanoparticles Threshold
The mechanisms for breakdown in gas discharges have been studied extensively for over a century . It is well known that the voltage required to initiate breakdown of a gaseous DC discharge depends strongly on the pressure P multiplied by the distance D of the gap between the electrodes, PD, as described by Paschen's Law . For a gas at atmospheric pressure, by limiting the inter-electrode separation to a distance of less than a millimeter, it is possible to produce a stable ‘normal-glow’ microdischarge . Although such a microdischarge is spatially confined compared to a traditional low-pressure discharge, the normal glow properties of a nonthermal discharge still apply, such as an electron temperature, Te, which is several orders of magnitude larger than the gas temperature, Tg [3-5]. Many applications have been explored to exploit this excess electron energy and drive optical or chemical processes such as vacuum-ultraviolet light sources , biomedical systems [7,8], nanoparticle synthesis [9,10], and plasma ignition . However in atmospheric air, even with a small inter-electrode separation of less than 1 mm, a sizeable voltage (upwards of 4 to 5 kV) may still be required to initiate breakdown.
A significant reduction of the breakdown threshold within a microdischarge could be a breakthrough that enables numerous applications. Such a breakdown voltage reduction could allow for the use of smaller, cheaper, and safer power supplies. One method of reducing the voltage required to initiate breakdown is to generate seed electrons into the discharge region. Breakdown under these conditions is termed ‘under-voltage breakdown’. Previously studied techniques for achieving under-voltage breakdown have included electron seeding by illumination of the cathode by ultraviolet (UV) light [12-14], resonance enhanced multi-photon ionization (REMPI) by UV pulsed lasers [15,16], and the use of secondary electrodes or spark plugs . The major limitation of these methods is that they all require a secondary energy source in order to produce the seed electrons which can increase the overall cost, complexity, and weight of the microdischarge system.
On the other hand, the effect of solid particle contamination, whether intentionally introduced or not, on the breakdown process in air gaps has been explored previously. Unwanted solid particle contaminants in commercial electrical systems can lead to arcing and failure of transmission lines and gas insulation systems. Sand and dust with particle sizes above several tens of microns were shown to initiate breakdown across gap lengths of several centimeters [18,19]. The previous works concluded that the sand and dust particles in the inter-electrode gap played a negligible role in the volume processes during breakdown; however, the formation of a thin contaminant layer on the cathode enhanced secondary electron emission and significantly reduced the breakdown voltage in some circumstances. Other works have shown that larger (100 s of microns to 100 s mms) conductive particles in an inter-electrode air gap can play a significant role in reducing breakdown voltage, time-lag of impulses, and breakdown probability [20-22]. These previous works have concluded that the degree of influence that the solid particles have on the breakdown process depends on both the discharge properties, namely polarity and field uniformity, as well as properties of the particles such as conductivity, shape, size, concentration, and position relative to the electrodes.
In this study, aluminum and iron nanoparticles were seeded into a DC microdischarge at a very low flow speed. Experimental results indicate that breakdown thresholds of dry air with nanoparticle seeding were significantly reduced compared to standard Paschen law. High-speed chemiluminescence images reveal that the nanoparticles had a major influence in inducing breakdown and subsequent heating that eventually ignited the nanoparticles.
A custom-made particle seeder, which included a particle container, inlet and outlet tubes, was used to seed the flow with various nanoenergetic materials. Mass measurements, before and after each run, were used to estimate the particle flow rates. Usually about 5 g of aluminum or iron nanoenergetics (nominal diameters of 70 nm, purchased from NanoAmor Inc., Houston, USA, without further treatment) were placed along the flow path inside the particle container. The particle seeder inlet tube was submerged below the surface of the piles to generate particle suspensions inside the container. The height of the inlet and outlet were offset to ensure roughly uniform seeding in the flow through the discharge tube. Standard breathing dry air was used as the gas supply. A flow controller (FMA 5400, Omega, Stamford, USA) regulated the flow rate in the system to 1 ± 0.1 standard liters per minute (slpm). A three-way valve allowed the flow to be switched between the nanoparticle seeder and a bypass line. If particle seeding was desired, the three-way valve and needle valve were opened to allow flow through the seeder. Otherwise, the three-way valve and needle valve were closed to isolate the particle seeder. The pressure in the system was monitored downstream of the cell by a piezoelectric pressure sensor (Series 910, Kurt J. Lesker Company, Jefferson Hills, USA), and the desired pressure was obtained by adjusting the needle valve upstream of the vacuum pump.
The high-voltage system included a high-voltage power supply, high-voltage probes, and data acquisition systems. The output of the high-voltage power supply was controlled via Labview™ software on a personal computer. The positive terminal was connected to a 1 MΩ ballast resistor used to limit the current through the discharge circuit. When a sufficient positive voltage was applied to the anode, breakdown occurred within the air between the two electrodes, with the resulting current spike traveling through the circuit to the grounded cathode. The supply voltage was linearly increased until breakdown was achieved. Two high-voltage probes were used to monitor the voltage drop across the electrode gap and across the ballast resistor. The voltage drop across the electrode gap, V 1, was determined directly by measuring the potential at junctions before the anode and after the cathode. The current in the system was obtained by measuring the potential drop across the ballast resistor and electrode gap sequentially. The total applied potential across the ballast and gap could be expressed as V 2 = V 1 + V R. Rearranging and dividing by the resistance of the ballast resistor, R, the current in the circuit was determined by Ohm's Law to be I = (V 2 − V 1)/R.
A high-speed camera (HS1200, Cooke Corporation, Kelheim, Germany) was used to track the chemiluminescence from the plasma initiation and nanoparticle ignition events. The 2D chemiluminescence images were acquired with a 1 ms exposure time. Because of the nature of the volume-averaged chemiluminescence images, the measurements can be regarded as an average over the line of sight across the discharge.
Results and discussions
Based on the experimental observations, the mechanisms for reducing the breakdown threshold may be due to possible charging of the nanoparticles within the gap, which may reduce the effective distance. Since the current across the gap does not vary with and without nanoparticle seeding, the increased conductivity due to the presence of metal nanoparticles is small. Additionally nanoparticles do not start to combust before the breakdown. The Joule heating due to the presence of metal nanoparticles is slow compared to breakdown generation. However, evidence of charging of the metal nanoparticles within the gap has been observed in these experiments. For example in Figure 5, the attraction of the nanoparticles to the cathode and the subsequent ignition near the cathode region indicate that the nanoparticles were positively charged. In addition, the chemiluminescence image at 2 ms shows a brighter glow near the cathode, which suggests that the evolution of the breakdown started from anode and turned toward the cathode. The nanoparticles charging and shifting toward the cathode might allow the nanoparticles to serve as effective electrodes within the gap, which could mimic a reduction in the gap distance. It is speculated that the Paschen curve may still hold for the particle laden flow with the addition of the conducting nanoparticles near the cathode leading to an effective reduction in distance between the electrodes, i.e., the PD values on the x axis are reduced.
In this work, the seeding of metal nanoparticles was shown to reduce the voltage required to initiate breakdown in an air DC microdischarge. Reductions in the breakdown voltage were seen to be as high as 25% for a PD scaling of 40 Torr-cm. High-speed chemiluminescence imaging of the discharge region revealed that the breakdown process was enhanced by a reduction in the required voltage from nanoparticle seeding, and then heating from the discharge led to ignition of some of the nanoparticles as they flowed through the discharge region. The use of SEM imaging gave detailed information regarding the particle size, shape, and oxidation distributions. Further use of ex situ diagnostic techniques, such as SEM analyses, could allow for the development of empirical correlations between particle characteristics and reduction in the breakdown voltage. Visual evidence of particle charging being the most likely mechanism for breakdown voltage reduction and subsequent reduction of the effective distance between the electrodes has been presented.
We acknowledge support from the AFOSR and NSF CBET - 1346944.
- Townsend J. Electricity in gases. Oxford: Clarendon; 1915.Google Scholar
- Paschen F. Ueber die zum Funkenübergang in Luft, Wasserstoff und Kohlensäure bei verschiedenen Drucken erforderliche Potentialdifferenz. Ann Phys. 1889;273:69–96.View ArticleGoogle Scholar
- Foest R, Schmidt M, Becker K. Microplasmas, an emerging field of low-temperature plasma science and technology. Int J Mass Spectrom. 2006;248:87–102.View ArticleGoogle Scholar
- Sawyer J, Wu Y, Zhang Z, Adams SF. O2 rotational temperature measurements in an atmospheric air microdischarge by radar resonance-enhanced multiphoton ionization. J Appl Phys. 2013;113:233304.View ArticleGoogle Scholar
- Laux CO, Spence TG, Kruger CH, Zare RN. Optical diagnostics of atmospheric pressure air plasmas. Plasma Sources Sci Technol. 2003;12:125.View ArticleGoogle Scholar
- Ren'an B, Mingdong S, Zhongrui W, Jing J, Wenbo H, Feng Q, et al. Development of 146 nm vacuum UV light source. Phys Procedia. 2012;32:477–81.View ArticleGoogle Scholar
- Goree J, Bin L, Drake D, Stoffels E. Killing of S. mutans bacteria using a plasma needle at atmospheric pressure. Plasma Sci IEEE Trans. 2006;34:1317–24.View ArticleGoogle Scholar
- Kim JY, Wei Y, Li J, Kim S-O. 15-μm-sized single-cellular-level and cell-manipulatable microplasma jet in cancer therapies. Biosens Bioelectron. 2010;26:555–9.View ArticleGoogle Scholar
- Chiang W-H, Sankaran RM. Microplasma synthesis of metal nanoparticles for gas-phase studies of catalyzed carbon nanotube growth. Appl Phys Lett. 2007;91:121503–3.View ArticleGoogle Scholar
- Richmonds C, Sankaran RM. Plasma-liquid electrochemistry: rapid synthesis of colloidal metal nanoparticles by microplasma reduction of aqueous cations. Appl Phys Lett. 2008;93:131501–3.View ArticleGoogle Scholar
- Pancheshnyi SV, Lacoste DA, Bourdon A, Laux CO. Ignition of propane-air mixtures by a repetitively pulsed nanosecond discharge. Plasma Sci IEEE Trans. 2006;34:2478–87.View ArticleGoogle Scholar
- Frechette MF, Bouchelouh N, Larocque RY. Laser-induced undervoltage breakdown in atmospheric N2 correlated with time-resolved avalanches. In: Electrical insulation, 1994, Conference Record of the 1994 IEEE International Symposium on; 5–8 Jun 1994. 1994. p. 515–7.Google Scholar
- Kluckow R. Über den zeitlichen Verlauf des Stromes einer Gasentladung in Wasserstoff. Z Physik. 1961;161:353–69.View ArticleGoogle Scholar
- Varney RN. Liberation of electrons by positive-ion impact on the cathode of a pulsed Townsend discharge tube. Phys Rev. 1954;93:1156–60.View ArticleGoogle Scholar
- Cooley JE, Choueiri EY. Threshold criteria for undervoltage breakdown. J Appl Phys. 2008;103:093305.View ArticleGoogle Scholar
- Cooley JE. Fundamentals of undervoltage breakdown through the Townsend mechanism. 2008Google Scholar
- Hong T, Scuka V. The breakdown mechanism of a mid-plane triggered spark gap trigatron. Dielectrics Electric Insulation IEEE Trans. 1996;3:843–8.View ArticleGoogle Scholar
- Al-Arainy AA. The influence of dust particles on the DC breakdown voltage of rod-rod air gaps. In: Electrical Insulating Materials, 1995 International Symposium on; 17–20 Sep 1995. 1995. p. 303–6.Google Scholar
- Al-Arainy AA, Malik NH, Qureshi MI. Influence of sand/dust contamination on the breakdown of asymmetrical air gaps under lightning impulses. Electric Insulation IEEE Trans. 1992;27:193–206.View ArticleGoogle Scholar
- Kubuki M, Yoshimoto R, Yoshizumi K, Tsuru S, Hara M. Estimation of DC breakdown mechanisms in air gaps containing floating metallic particles. Dielectrics Electric Insulation IEEE Trans. 1997;4:92–101.View ArticleGoogle Scholar
- Hara M, Akazaki M. A method for prediction of gaseous discharge threshold voltage in the presence of a conducting particle. J Electrostat. 1977;2:223–39.View ArticleGoogle Scholar
- Hara M, Negara Y, Setoguchi M, Kurihara T, Suehiro J, Haashi N. Particle-triggered pre-breakdown phenomena in atmospheric air gap under AC voltage. Dielectrics Electric Insulation IEEE Trans. 2005;12:1071–81.View ArticleGoogle Scholar
- Chong X, Abboud J, Zhang Z. Plasmonics resonance enhanced active photothermal effects of aluminum and iron nanoparticles. J Nanosci Nanotechnol. 2015;15:2234–40.View ArticleGoogle Scholar
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