Abstract
We refer to the fourth state of matter as plasma, indicating ionized, electrically quasi-neutral gas. Electrical discharge in a gas medium is a normal and easy way of turning the gas into plasma in a moderate pressure condition. The electron temperature, electron density, and gas temperature characterize a quality of plasma. Particularly in the domain in terms of the electron temperature and gas temperature, we have room to design discharges to be a thermal plasma (both electron and gas temperature are in equilibrium) or non-thermal plasma (a couple of orders magnitude higher electron temperature than gas temperature). This indicates that the plasma chemistry, consisting of electron impact reactions and thermochemistry governed by the electron temperature and gas temperature, respectively, can be tailored to a certain extent. In this regard, we believe that plasma technology can be considered as a versatile reaction platform, which can replace and reinforce conventional combustion and catalyst-based ones in an electrified future. This perspective particularly highlights the opportunities for the combustion community in the field of low-temperature plasma technology, elaborating on the leashed potential of plasma chemistry and its similarities with combustion studies.
A Blistering History of Fire
Numerous mythologies from around the world have undoubtedly shown us the importance of fire throughout humankind’s history. The acquisition, control, or theft of fire has been a recurring theme in many cultures across the globe. The importance of fire in mythology and its divine connotations are hardly surprising. Today, we are all too aware that early human’s ability to wield fire can be considered one of the pivotal moments that ignited the course of human history.
Fire provided our ancestors with the means for cooking, heating, hunting, and protecting, as well as for art and tool-making. Over time control over fire lit the path for three major socio-technological revolutions. Fire became the cornerstone of civilization, beginning with the Neolithic revolution (10,000 B.C.), followed by humankind’s first innovative manufacturing waves during the Bronze (3000–1200 B.C.) and Iron Age (1200–500 B.C.), which are both defined by humankind’s ability to control fire. The third major innovation was the replacement of manpower with man-made power through the development of the steam engine, followed by the invention of the internal combustion engine (late 19th C). These innovations sparked the Industrial Revolution (1760–1840) fueled by coal and oil, and combustion processes became the foundation of power generation, transportation, smelting, and material processing. Advances in petrochemistry rapidly followed, which expanded the applications of oil far beyond combustion, producing fertilizers, materials (like plastics, fiber, and rubber), food, medicine, household goods, and much more. Today almost everything in our day-to-day lives relies on fire and fossil fuels, in terms of the applied science of combustion and petrochemistry.
Although fire has powered unprecedented advancements in society, the devastating effects of unchecked CO2 emissions on our planet’s climate and environment opened a Pandora’s box, releasing fear of a gloomy future on a scorched earth. However, hope arises through our pursuit of promising and logical solutions, such as renewable energy and carbon-free or carbon-neutral fuels (hydrogen, ammonia, biomass, solar fuels, etc.). Even though we cannot abandon fossil fuels entirely just yet because of current energy demands (), a controlled transition from the era of fire to an electrified future appears imperative.
Since the first commercial power generator, electricity has superseded combustion in many of its initial breakthrough areas. For example, lighting has long since become fully electric, and domestic heating and gas-based cooking appliances have been gradually supplanted by their electric counterparts. Even in the transport sector, the market for electric vehicles (both battery and fuel-cell-based) is growing rapidly. Additionally, the IEA (International Energy Agency) forecasts that electricity will be the primary source of energy for the fourth industrial revolution. Hence, the transition toward an electrified future is already kindling all around us, and we must prepare ourselves for both the challenges and opportunities that electrification presents.
A new era With Plasma
Is it simply a curious coincidence that this modern transition from fire to electricity bears a resemblance to mythology? The Greek God Zeus, who punished Prometheus for giving fire to humankind, symbolized his might through lightning—his ultimate source of power—which, of course, is electricity! And lightning moreover is one of the most common natural plasmas on Earth. Is the use of plasma technology in an electrified future predestined? In fact, low-pressure plasma technology was an unsung hero behind the Information Revolution fabricating IC (Integrated Circuit) chips.
The term ‘plasma’ refers to ionized gas that is in an electrically quasi-neutral state, considered to be the fourth state of matter. The key element to sustain a plasma is the multiplication of its highly energetic electrons through electron impact reactions, which result in the formation of a large variety of species, such as ions, atoms, molecules, radicals, and excited species, often making plasma a highly reactive and complex physicochemical cocktail ().
We can distinguish two groups of man-made plasma: fully ionized plasmas, such as thermonuclear fusion plasmas (; ), and partially ionized plasmas (10−4–10–6) or so-called gas discharges, which are the focus of several disrupting innovations (Figure 1) (; ; ). Since plasma is a multicomponent system, it can exhibit multiple temperatures. When the temperature of all the species is the same in a localized area, the plasma is said to be in ‘local thermodynamic equilibrium’ (LTE). When the temperature of all the species (particularly electrons, Te, and neural species, Tgas) is characterized by multiple different temperatures, it is said to be in ‘non-local thermodynamic equilibrium’ (non-LTE). The former type of plasmas is usually called “thermal plasmas” and the latter ‘non-thermal plasmas’ (; ; ).
FIGURE 1
Regardless of these categorizations, the cascade of energy transfers from the highly energetic electrons to all the other species through collisions leads to an increase in gas temperature. Depending on the conditions, this increase can range from several Kelvin up to temperatures that are more than one order of magnitude greater than what can be achieved through the conventional combustion of fossil fuel (see Figure 2 and Table 1). Particularly, non-thermal plasmas operating at atmospheric pressure, such as Dielectric Barrier Discharges (DBD) () and Nanosecond Repetitively Pulsed (NRP) discharges (; ), generate highly energetic electrons with only a minimal increase in the gas temperature (Te >> Tgas). Arc discharges, on the other hand, representing thermal plasmas, typically demonstrate Te = Tgas (∼ 10,000 K) at their core. Between these opposites, elongated arc (including gliding arc) discharges () and microwave (MW) discharges () can bridge the wide gap in Tgas, from room temperature up to several thousand Kelvin. It should be also noted that a local Tgas in the discharge channel of NRP discharges can go up to a couple of thousand Kelvin.
FIGURE 2
TABLE 1
| Temperature | Characteristics | Application | |
|---|---|---|---|
| Dielectric Barrier Discharge (DBD) | Te = up to 30 eV | • Large discharge volume | • Ozone generation |
| Tgas = up to 500 K (; ) | • Entire flow can be treated | • Surface coating | |
| • Low power density | • Fundamental kinetic study | ||
| • Electron-driven chemistry prevails | |||
| Nanosecond Repetitively Pulsed (NRP) discharge | Te = ∼4 eV at 200 torr with He; 150 ns pulse duration; 9 kV () | • Compatible with pulsed corona and DBD configurations | • Plasma assisted combustion |
| Tgas at the discharge channel: 300–2,600 K (; ) | • Higher Te due to stronger breakdown field | • In-liquid discharges | |
| • Te should be higher than DBD due to stronger breakdown field () | • Severe EMI | • Fundamental kinetic study | |
| • Bulk gas temperature should be similar to that of DBD. | |||
| Gliding arc | Te = 1.4–2.1 eV | • Relatively easy to treat high flow rate | • Fuel reformer |
| Tgas = 1,000–3,000 K (; ) | • Relatively higher bulk temperature | • Chemical conversion | |
| • Requiring special design to increase effective plasma volume | |||
| • Corrosion of metallic electrodes | |||
| Arc torch | Te = Tgas | • High gas temperature | • Welding |
| ∼8,000–14,000 K (; ) | • High power density | • Surface coating | |
| • Indirect mixing required to treat high flow rate | • Waste-to-energy | ||
| • Corrosion of electrodes | |||
| Microwave (MW) discharge | Te = 0.4–0.9 eV | • High gas temperature | • Fuel reforming |
| Tgas = 2,000–6,000 K (; ) | • High power density | • Chemical conversion | |
| • No corrosion of metallic electrodes |
Characteristics of the main atmospheric pressure discharges.
These properties place plasma in a unique position in an electrified future by providing two almost independent ways to control chemical reactions, allowing for energetic electron-driven chemistry, (extreme) heat-driven chemistry, and any possible combination of the two. Low-pressure non-thermal plasma-based nanoscale semiconductor fabrication is a perfect example of electron-driven chemistry, which has already led us to the dawn of the fourth industrial revolution (; ), whereas thermal plasma-based arc welding and waste treatment well represents heat-driven plasma processes (; ).
A Versatile Platform for Electrically Driven Chemical Synthesis
Currently, we burn chemicals (in the form of fossil fuels or biological matter) to generate electrical energy. Plasma has the potential to be a key technology to transform electrical energy into chemical energy, and thus efficiently store electrical energy in a chemical form by synthesizing chemicals and fuels of interest (). Plasma technology provides us with the opportunity to utilize the full potential of electrical energy. Energy production is already shifting away from fossil fuels to renewable sources. In the same way, a similar shift from conventional energy sources towards electricity in industrial processes might be envisioned.
Plasmas have already been investigated for hydrocarbon reforming processes, such as partial oxidation, dry reforming, steam reforming, and conversion of pure hydrocarbons (; ; ). The conversion of CO2, through pure CO2 splitting, CO2 hydrogenation, and artificial photosynthesis have also been studied (; ; ; ). However, despite the wide variety of plasma devices invented, plasma chemistry for higher hydrocarbons (even C2 and C3) with CO2, O2, H2O, and N2 remains a mostly undiscovered domain.
While plasmas excel at initiating reactions, tuning the selectivity remains a major challenge. Recent studies have revealed that while the electron impact reactions can initiate a chemical reaction regardless of initial conditions, the thermochemistry (governed by the gas temperature) has a dominant effect on the product selectivity and thus final product composition (). Another study showed that despite the non-thermodynamic equilibrium nature of non-thermal plasmas, it is possible to influence the product selectivity by changing the inlet composition or adding specific reaction products to shift the chemical equilibrium (). Combining plasma with a catalyst is another route to affect the process selectivity. This approach creates synergistic effects that increase selectivity and yield and/or decrease the light-off temperature (; ; ; ). The mechanism of this synergy highly depends on the chemical process, the plasma properties and the type of catalyst; the catalyst can be activated by a combination of heat and/or the species (charges, photons, radicals, intermediates) generated by the plasma.
Future efforts should continue in this direction, focusing on rigorous, fundamental investigations into the plasma chemistry (and possible catalyst interactions), with a final goal to design and develop plasma systems based on knowledge and understanding, where we can optimize the conditions (such as electron temperature and gas temperature) for any target process. Special attention should be given to processes for the production of carbon-free fuels such as hydrogen and ammonia (), and the production of feedstock (petro)chemicals like methanol, aldehydes, C2-C3 hydrocarbons (such as ethylene and propylene).
Once control over the product formation and selectivity for plasma processes is fully understood—and further exploited, this can pave the way for using plasmas as a highly flexible platform for the on-demand production of tailored chemicals and fuels using (renewable) electricity. Also, the potential for chemically reactive plasma processes in the future will not remain limited to chemical synthesis and energy applications. Plasmas are already found in several applications in materials science (e.g., coating deposition, surface modification, nanomaterial fabrication), the microelectronics industry (for microchip manufacturing), as light sources, lasers and displays (owing to their light-emitting characteristics), as well as for many emerging environmental (waste, gas and water treatment), food, agriculture, and even medical applications (such as sterilization, wound treatment and even cancer treatment) (; ).
Plasma: Our new Fire?
This perspective shares our views on the unique opportunity to expand the combustion community’s horizons into the electrified future. There are, in fact, many analogies between combustion and plasma processes, especially considering how plasma can be defined as an electrically sustained reacting flow with heat and mass transport, while combustion processes are a thermally sustained reacting flow with heat and mass transport. As a result, they not only share fundamental properties, but they also rely on similar methodologies for their scientific exploration, such as laser diagnostics, chemical kinetics modeling, multi-physics simulation, and much more. If we recall that spark-ignition in fact utilizes plasma, we realize the enormous potential plasma has in complementing combustion (). Recent advancements in the area of plasma-assisted combustion reveal how we can effectively use plasma to support existing combustion applications (; ). In particular, plasma-generated radicals and ozone have been found to be crucial in igniting both premixed and non-premixed conditions, by supporting the chain-branching combustion chemistry to jump-start in extreme conditions, yielding extended lean-limits, reduced ignition delay, and increased ignition probability.
Faced with the realities of climate change, the combustion community is fully aware of the major challenges that lie ahead for the energy industry and energy technology (). As the transition towards an electrified future has already begun in earnest, we could not think of a better time for the combustion community to consider plasma as another, more adaptive, form of fire, and to explore plasma’s potential far beyond its assisted function in combustion. Looking at the similarities in the chemistry between combustion and plasma, and the unexpected as well as expected synergies that are awaiting further exploration, we are convinced that the emerging field of plasma technology has a lot to offer the mature field of energy and combustion science and—perhaps more importantly—vice versa.
Statements
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The original contributions presented in the study are included in the article/Supplementary Material, further inquiries can be directed to the corresponding author.
Author contributions
MC and RS equally contributed to the preparation of the manuscript.
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
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Summary
Keywords
plasma chemistry, thermal plasma, nonthermal plasma, combustion, reacting flow
Citation
Cha MS and Snoeckx R (2022) Plasma Technology–Preparing for the Electrified Future. Front. Mech. Eng 8:903379. doi: 10.3389/fmech.2022.903379
Received
24 March 2022
Accepted
28 April 2022
Published
12 May 2022
Volume
8 - 2022
Edited by
Joseph K. Lefkowitz, Technion Israel Institute of Technology, Israel
Reviewed by
Mariana Amorim Fraga, Federal University of São Paulo, Brazil
Timothy Ombrello, Air Force Research Laboratory, United States
Updates
Copyright
© 2022 Cha and Snoeckx.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Min Suk Cha, minsuk.cha@kaust.edu.sa
This article was submitted to Engine and Automotive Engineering, a section of the journal Frontiers in Mechanical Engineering
Disclaimer
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article or claim that may be made by its manufacturer is not guaranteed or endorsed by the publisher.