Plasma (from Ancient Greek πλάσμα, meaning 'moldable substance'[1]) is one of the four fundamental states of matter, and was first described by chemist Irving Langmuir[2] in the 1920s.[3] It consists of a gas of ions – atoms which have some of their orbital electrons removed – and free electrons. Plasma can be artificially generated by heating a neutral gas or subjecting it to a strong electromagnetic field to the point where an ionized gaseous substance becomes increasingly electrically conductive. The resulting charged ions and electrons become influenced by long-range electromagnetic fields, making the plasma dynamics more sensitive to these fields than a neutral gas.[4]
Plasma and ionized gases have properties and behaviours unlike those of the other states, and the transition between them is mostly a matter of nomenclature[2] and subject to interpretation.[5] Based on the temperature and density of the environment that contains a plasma, partially ionized or fully ionized forms of plasma may be produced. Neon signs and lightning are examples of partially ionized plasmas.[6] The Earth's ionosphere is a plasma and the magnetosphere contains plasma in the Earth's surrounding space environment. The interior of the Sun is an example of fully ionized plasma,[7] along with the solar corona[8] and stars.[9]
Positive charges in ions are achieved by stripping away electrons orbiting the atomic nuclei, where the total number of electrons removed is related to either increasing temperature or the local density of other ionized matter. This also can be accompanied by the dissociation of molecular bonds,[10] though this process is distinctly different from chemical processes of ion interactions in liquids or the behaviour of shared ions in metals. The response of plasma to electromagnetic fields is used in many modern technological devices, such as plasma televisions or plasma etching.[11]
Plasma may be the most abundant form of ordinary matter in the universe,[12] although this hypothesis is currently tentative based on the existence and unknown properties of dark matter. Plasma is mostly associated with stars, extending to the rarefied intracluster medium and possibly the intergalactic regions.[13]
History
The word plasma comes from Ancient Greek πλάσμα, meaning 'moldable substance'[1] or 'jelly',[2] and describes the behaviour of the ionized atomic nuclei and the electrons within the surrounding region of the plasma. Very simply, each of these nuclei are suspended in a movable sea of electrons. Plasma was first identified in a Crookes tube, and so described by Sir William Crookes in 1879 (he called it "radiant matter").[14] The nature of this "cathode ray" matter was subsequently identified by British physicist Sir J.J. Thomson in 1897.[15]
The term "plasma" was introduced as a description of ionised gas by Irving Langmuir in 1928.[16] Lewi Tonks and Harold Mott-Smith, both of whom worked with Irving Langmuir in the 1920s, recall that Langmuir first used the word "plasma" in analogy with blood.[17][18] Mott-Smith recalls, in particular, that the transport of electrons from thermionic filaments reminded Langmuir of "the way blood plasma carries red and white corpuscles and germs."[19]
Langmuir described the plasma he observed as follows:
"Except near the electrodes, where there are sheaths containing very few electrons, the ionized gas contains ions and electrons in about equal numbers so that the resultant space charge is very small. We shall use the name plasma to describe this region containing balanced charges of ions and electrons."[16]
Properties and parameters
Artist's rendition of the Earth's plasma fountain, showing oxygen, helium, and hydrogen ions that gush into space from regions near the Earth's poles. The faint yellow area shown above the north pole represents gas lost from Earth into space; the green area is the aurora borealis, where plasma energy pours back into the atmosphere.[20]
Definition
Plasma is a state of matter in which an ionized gaseous substance becomes highly electrically conductive to the point that long-range electric and magnetic fields dominate the behaviour of the matter.[21][22] The plasma state can be contrasted with the other states: solid, liquid, and gas.
Plasma is an electrically neutral medium of unbound positive and negative particles (i.e. the overall charge of a plasma is roughly zero). Although these particles are unbound, they are not "free" in the sense of not experiencing forces. Moving charged particles generate an electric current within a magnetic field, and any movement of a charged plasma particle affects and is affected by the fields created by the other charges. In turn this governs collective behaviour with many degrees of variation.[10][23] Three factors define a plasma:[24][25]
The plasma approximation: The plasma approximation applies when the plasma parameter, Λ,[26] representing the number of charge carriers within a sphere (called the Debye sphere whose radius is the Debye screening length) surrounding a given charged particle, is sufficiently high as to shield the electrostatic influence of the particle outside of the sphere.[21][22]
Bulk interactions: The Debye screening length (defined above) is short compared to the physical size of the plasma. This criterion means that interactions in the bulk of the plasma are more important than those at its edges, where boundary effects may take place. When this criterion is satisfied, the plasma is quasineutral.[27]
Plasma frequency: The electron plasma frequency (measuring plasma oscillations of the electrons) is large compared to the electron-neutral collision frequency (measuring frequency of collisions between electrons and neutral particles). When this condition is valid, electrostatic interactions dominate over the processes of ordinary gas kinetics.[28]
Temperature
Plasma temperature is commonly measured in kelvin or electronvolts and is, informally, a measure of the thermal kinetic energy per particle. High temperatures are usually needed to sustain ionisation, which is a defining feature of a plasma. The degree of plasma ionisation is determined by the electron temperature relative to the ionization energy (and more weakly by the density), in a relationship called the Saha equation. At low temperatures, ions and electrons tend to recombine into bound states—atoms[29]—and the plasma will eventually become a gas.
In most cases the electrons are close enough to thermal equilibrium that their temperature is relatively well-defined; this is true even when there is a significant deviation from a Maxwellian energy distribution function, for example, due to UV radiation, energetic particles, or strong electric fields. Because of the large difference in mass, the electrons come to thermodynamic equilibrium amongst themselves much faster than they come into equilibrium with the ions or neutral atoms. For this reason, the ion temperature may be very different from (usually lower than) the electron temperature. This is especially common in weakly ionized technological plasmas, where the ions are often near the ambient temperature.
Fully vs. partially (weakly) ionized gases
Main article: Degree of ionization
See also: Spitzer resistivity
For plasma to exist, ionisation is necessary. The term "plasma density" by itself usually refers to the "electron density", that is, the number of free electrons per unit volume. The degree of ionisation of a plasma is the proportion of atoms that have lost or gained electrons, and is controlled by the electron and ion temperatures and electron-ion vs electron-neutral collision frequencies. The degree of ionisation, \( \alpha \) , is defined as \( \alpha = \frac{n_i}{n_i + n_n} \), where \( n_{i} \) is the number density of ions and \( n_n \) is the number density of neutral atoms. The electron density is related to this by the average charge state \( \langle Z\rangle \) of the ions through \( n_e = \langle Z\rangle n_i, \) where \( n_{e} \) is the number density of electrons.
In a plasma, the electron-ion collision frequency \( {\displaystyle \nu _{ei}} \) is much greater than the electron-neutral collision frequency \({\displaystyle \nu _{en}} \). Therefore, with a weak degree of ionization α {\displaystyle \alpha } \alpha , the electron-ion collision frequency can equal the electron-neutral collision frequency: \( {\displaystyle \nu _{ei}=\nu _{en}} \) is the limit separating a plasma from being partially or fully ionized.
The term fully ionized gas introduced by Lyman Spitzer does not mean the degree of ionization is unity, but only that the plasma is in a Coulomb-collision dominated regime, i.e. when \( {\displaystyle \nu _{ei}>\nu _{en}} \), which can correspond to a degree of ionization as low as 0.01%.[30]
A partially or weakly ionized gas means the plasma is not dominated by Coulomb collisions, i.e. when \({\displaystyle \nu _{ei}<\nu _{en}} \).
Most of "technological" (engineered) plasmas are weakly ionized gases.
Thermal vs. nonthermal (cold) plasmas
Main article: Nonthermal plasma
See also: Anisothermal plasma
Based on the relative temperatures of the electrons, ions and neutrals, plasmas are classified as "thermal" or "non-thermal" (also referred to as "cold plasmas").
Thermal plasmas have electrons and the heavy particles at the same temperature, i.e. they are in thermal equilibrium with each other.
Nonthermal plasmas on the other hand are non-equilibrium ionized gases, with two temperatures: ions and neutrals stay at a low temperature (sometimes room temperature), whereas electrons are much hotter. ( \( T_e \gg T_n) \).[31] A kind of common nonthermal plasma is the mercury-vapor gas within a fluorescent lamp, where the "electrons gas" reaches a temperature of 10,000 kelvins while the rest of the gas stays barely above room temperature, so the bulb can even be touched with hands while operating.
A particular and unusual case of "inverse" nonthermal plasma is the very high temperature plasma produced by the Z machine, where ions are much hotter than electrons.[32][33]
Plasma potential
Lightning as an example of plasma present at Earth's surface: Typically, lightning discharges 30 kiloamperes at up to 100 megavolts, and emits radio waves, light, X- and even gamma rays.[34] Plasma temperatures can approach 30000 K and electron densities may exceed 1024 m−3.
Since plasmas are very good electrical conductors, electric potentials play an important role. The average potential in the space between charged particles, independent of how it can be measured, is called the "plasma potential", or the "space potential". If an electrode is inserted into a plasma, its potential will generally lie considerably below the plasma potential due to what is termed a Debye sheath. The good electrical conductivity of plasmas makes their electric fields very small. This results in the important concept of "quasineutrality", which says the density of negative charges is approximately equal to the density of positive charges over large volumes of the plasma ( \( n_e = \langle Z\rangle n_i) \), but on the scale of the Debye length there can be charge imbalance. In the special case that double layers are formed, the charge separation can extend some tens of Debye lengths.
The magnitude of the potentials and electric fields must be determined by means other than simply finding the net charge density. A common example is to assume that the electrons satisfy the Boltzmann relation:
\( n_{e}\propto e^{e\Phi /k_{B}T_{e}}. \)
Differentiating this relation provides a means to calculate the electric field from the density:
\( \vec{E} = (k_BT_e/e)(\nabla n_e/n_e). \)
It is possible to produce a plasma that is not quasineutral. An electron beam, for example, has only negative charges. The density of a non-neutral plasma must generally be very low, or it must be very small, otherwise, it will be dissipated by the repulsive electrostatic force.[35]
In astrophysical plasmas, Debye screening prevents electric fields from directly affecting the plasma over large distances, i.e., greater than the Debye length. However, the existence of charged particles causes the plasma to generate, and be affected by, magnetic fields. This can and does cause extremely complex behaviour, such as the generation of plasma double layers, an object that separates charge over a few tens of Debye lengths. The dynamics of plasmas interacting with external and self-generated magnetic fields are studied in the academic discipline of magnetohydrodynamics.[36]
Magnetization
Plasma with a magnetic field strong enough to influence the motion of the charged particles is said to be magnetized. A common quantitative criterion is that a particle on average completes at least one gyration around the magnetic field before making a collision, i.e., \( \omega_{\mathrm{ce}} / v_{\mathrm{coll}} > 1 \), where \( \omega_{\mathrm{ce}} \) is the "electron gyrofrequency" and \( v_{\mathrm{coll}} \) is the "electron collision rate". It is often the case that the electrons are magnetized while the ions are not. Magnetized plasmas are anisotropic, meaning that their properties in the direction parallel to the magnetic field are different from those perpendicular to it. While electric fields in plasmas are usually small due to the high conductivity, the electric field associated with a plasma moving in a magnetic field is given by \( \mathbf{E} = -v\times\mathbf{B} \) (where \( \mathbf {E} \) is the electric field, \( \mathbf {v} \) is the velocity, and \( \mathbf {B} \) is the magnetic field), and is not affected by Debye shielding.[37]
Comparison of plasma and gas phases
Plasma is often called the fourth state of matter after solid, liquids and gases, despite plasma typically being an ionized gas.[38][39][40] It is distinct from these and other lower-energy states of matter. Although it is closely related to the gas phase in that it also has no definite form or volume, it differs in a number of ways, including the following:
Property Gas Plasma
Electrical conductivity Very low: Air is an excellent insulator until it breaks down into plasma at electric field strengths above 30 kilovolts per centimeter.[41] Usually very high: For many purposes, the conductivity of a plasma may be treated as infinite.
Independently acting species One: All gas particles behave in a similar way, influenced by gravity and by collisions with one another. Two or three: Electrons, ions, protons and neutrons can be distinguished by the sign and value of their charge so that they behave independently in many circumstances, with different bulk velocities and temperatures, allowing phenomena such as new types of waves and instabilities.
Velocity distribution Maxwellian: Collisions usually lead to a Maxwellian velocity distribution of all gas particles, with very few relatively fast particles. Often non-Maxwellian: Collisional interactions are often weak in hot plasmas and external forcing can drive the plasma far from local equilibrium and lead to a significant population of unusually fast particles.
Interactions Binary: Two-particle collisions are the rule, three-body collisions extremely rare. Collective: Waves, or organized motion of plasma, are very important because the particles can interact at long ranges through the electric and magnetic forces.
Plasmas in space science and astronomy
Further information: Astrophysical plasma, Interstellar medium, and Intergalactic space
See also: Magnetohydrodynamics
Plasmas are by far the most common phase of ordinary matter in the universe, both by mass and by volume.[42]
Above the Earth's surface, the ionosphere is a plasma,[43] and the magnetosphere contains plasma.[44] Within our Solar System, interplanetary space is filled with the plasma expelled via the solar wind, extending from the Sun's surface out to the heliopause. Furthermore, all the distant stars, and much of interstellar space or intergalactic space is also likely filled with plasma, albeit at very low densities. Astrophysical plasmas are also observed in Accretion disks around stars or compact objects like white dwarfs, neutron stars, or black holes in close binary star systems.[45] Plasma is associated with ejection of material in astrophysical jets, which have been observed with accreting black holes[46] or in active galaxies like M87's jet that possibly extends out to 5,000 light-years.[47]
Common plasmas
Plasmas can appear in nature in various forms and locations, which can be usefully broadly summarised in the following Table:
| Artificially produced | Terrestrial plasmas | Space and astrophysical plasmas |
|---|---|---|
|
|
|
Complex plasma phenomena
Although the underlying equations governing plasmas are relatively simple, plasma behaviour is extraordinarily varied and subtle: the emergence of unexpected behaviour from a simple model is a typical feature of a complex system. Such systems lie in some sense on the boundary between ordered and disordered behaviour and cannot typically be described either by simple, smooth, mathematical functions, or by pure randomness. The spontaneous formation of interesting spatial features on a wide range of length scales is one manifestation of plasma complexity. The features are interesting, for example, because they are very sharp, spatially intermittent (the distance between features is much larger than the features themselves), or have a fractal form. Many of these features were first studied in the laboratory, and have subsequently been recognized throughout the universe. Examples of complexity and complex structures in plasmas include:
Filamentation
Striations or string-like structures,[50] also known as Birkeland currents, are seen in many plasmas, like the plasma ball, the aurora,[51] lightning,[52] electric arcs, solar flares,[53] and supernova remnants.[54] They are sometimes associated with larger current densities, and the interaction with the magnetic field can form a magnetic rope structure.[55] High power microwave breakdown at atmospheric pressure also leads to the formation of filamentary structures.[56] (See also Plasma pinch)
Filamentation also refers to the self-focusing of a high power laser pulse. At high powers, the nonlinear part of the index of refraction becomes important and causes a higher index of refraction in the center of the laser beam, where the laser is brighter than at the edges, causing a feedback that focuses the laser even more. The tighter focused laser has a higher peak brightness (irradiance) that forms a plasma. The plasma has an index of refraction lower than one, and causes a defocusing of the laser beam. The interplay of the focusing index of refraction, and the defocusing plasma makes the formation of a long filament of plasma that can be micrometers to kilometers in length.[57] One interesting aspect of the filamentation generated plasma is the relatively low ion density due to defocusing effects of the ionized electrons.[58] (See also Filament propagation)
Non-neutral plasma
The strength and range of the electric force and the good conductivity of plasmas usually ensure that the densities of positive and negative charges in any sizeable region are equal ("quasineutrality"). A plasma with a significant excess of charge density, or, in the extreme case, is composed of a single species, is called a non-neutral plasma. In such a plasma, electric fields play a dominant role. Examples are charged particle beams, an electron cloud in a Penning trap and positron plasmas.[59]
Dusty plasma/grain plasma
A dusty plasma contains tiny charged particles of dust (typically found in space). The dust particles acquire high charges and interact with each other. A plasma that contains larger particles is called grain plasma. Under laboratory conditions, dusty plasmas are also called complex plasmas.[60]
Impermeable plasma
Impermeable plasma is a type of thermal plasma which acts like an impermeable solid with respect to gas or cold plasma and can be physically pushed. Interaction of cold gas and thermal plasma was briefly studied by a group led by Hannes Alfvén in 1960s and 1970s for its possible applications in insulation of fusion plasma from the reactor walls.[61] However, later it was found that the external magnetic fields in this configuration could induce kink instabilities in the plasma and subsequently lead to an unexpectedly high heat loss to the walls.[62] In 2013, a group of materials scientists reported that they have successfully generated stable impermeable plasma with no magnetic confinement using only an ultrahigh-pressure blanket of cold gas. While spectroscopic data on the characteristics of plasma were claimed to be difficult to obtain due to the high pressure, the passive effect of plasma on synthesis of different nanostructures clearly suggested the effective confinement. They also showed that upon maintaining the impermeability for a few tens of seconds, screening of ions at the plasma-gas interface could give rise to a strong secondary mode of heating (known as viscous heating) leading to different kinetics of reactions and formation of complex nanomaterials.[63]
Mathematical descriptions
The complex self-constricting magnetic field lines and current paths in a field-aligned Birkeland current that can develop in a plasma.[64]
Main article: Plasma modeling
To completely describe the state of a plasma, all of the particle locations and velocities that describe the electromagnetic field in the plasma region would need to be written down. However, it is generally not practical or necessary to keep track of all the particles in a plasma. Therefore, plasma physicists commonly use less detailed descriptions, of which there are two main types:
Fluid model
Fluid models describe plasmas in terms of smoothed quantities, like density and averaged velocity around each position (see Plasma parameters). One simple fluid model, magnetohydrodynamics, treats the plasma as a single fluid governed by a combination of Maxwell's equations and the Navier–Stokes equations. A more general description is the two-fluid plasma,[65] where the ions and electrons are described separately. Fluid models are often accurate when collisionality is sufficiently high to keep the plasma velocity distribution close to a Maxwell–Boltzmann distribution. Because fluid models usually describe the plasma in terms of a single flow at a certain temperature at each spatial location, they can neither capture velocity space structures like beams or double layers, nor resolve wave-particle effects.
Kinetic model
Kinetic models describe the particle velocity distribution function at each point in the plasma and therefore do not need to assume a Maxwell–Boltzmann distribution. A kinetic description is often necessary for collisionless plasmas. There are two common approaches to kinetic description of a plasma. One is based on representing the smoothed distribution function on a grid in velocity and position. The other, known as the particle-in-cell (PIC) technique, includes kinetic information by following the trajectories of a large number of individual particles. Kinetic models are generally more computationally intensive than fluid models. The Vlasov equation may be used to describe the dynamics of a system of charged particles interacting with an electromagnetic field. In magnetized plasmas, a gyrokinetic approach can substantially reduce the computational expense of a fully kinetic simulation.
Artificial plasmas
Most artificial plasmas are generated by the application of electric and/or magnetic fields through a gas. Plasma generated in a laboratory setting and for industrial use can be generally categorized by:
The type of power source used to generate the plasma—DC, AC (typically with radio frequency (RF)) and microwave
The pressure they operate at—vacuum pressure (< 10 mTorr or 1 Pa), moderate pressure (≈1 Torr or 100 Pa), atmospheric pressure (760 Torr or 100 kPa)
The degree of ionisation within the plasma—fully, partially, or weakly ionized
The temperature relationships within the plasma—thermal plasma ( \( T_e = T_i = T_{gas}) \), non-thermal or "cold" plasma ( \( T_e \gg T_i = T_{gas}) \)
The electrode configuration used to generate the plasma
The magnetization of the particles within the plasma—magnetized (both ion and electrons are trapped in Larmor orbits by the magnetic field), partially magnetized (the electrons but not the ions are trapped by the magnetic field), non-magnetized (the magnetic field is too weak to trap the particles in orbits but may generate Lorentz forces)
Generation of artificial plasma
Simple representation of a discharge tube - plasma.png
Artificial plasma produced in air by a Jacob's Ladder
Artificial plasma produced in air by a Jacob's Ladder
Just like the many uses of plasma, there are several means for its generation. However, one principle is common to all of them: there must be energy input to produce and sustain it.[66] For this case, plasma is generated when an electric current is applied across a dielectric gas or fluid (an electrically non-conducting material) as can be seen in the adjacent image, which shows a discharge tube as a simple example (DC used for simplicity).
The potential difference and subsequent electric field pull the bound electrons (negative) toward the anode (positive electrode) while the cathode (negative electrode) pulls the nucleus.[67] As the voltage increases, the current stresses the material (by electric polarization) beyond its dielectric limit (termed strength) into a stage of electrical breakdown, marked by an electric spark, where the material transforms from being an insulator into a conductor (as it becomes increasingly ionized). The underlying process is the Townsend avalanche, where collisions between electrons and neutral gas atoms create more ions and electrons (as can be seen in the figure on the right). The first impact of an electron on an atom results in one ion and two electrons. Therefore, the number of charged particles increases rapidly (in the millions) only "after about 20 successive sets of collisions",[68] mainly due to a small mean free path (average distance travelled between collisions).
Electric arc
Cascade process of ionisation. Electrons are "e−", neutral atoms "o", and cations "+".
Avalanche effect between two electrodes. The original ionisation event liberates one electron, and each subsequent collision liberates a further electron, so two electrons emerge from each collision: the ionising electron and the liberated electron.
With ample current density and ionisation, this forms a luminous electric arc (a continuous electric discharge similar to lightning) between the electrodes.[Note 1] Electrical resistance along the continuous electric arc creates heat, which dissociates more gas molecules and ionises the resulting atoms (where degree of ionisation is determined by temperature), and as per the sequence: solid-liquid-gas-plasma, the gas is gradually turned into a thermal plasma.[Note 2] A thermal plasma is in thermal equilibrium, which is to say that the temperature is relatively homogeneous throughout the heavy particles (i.e. atoms, molecules and ions) and electrons. This is so because when thermal plasmas are generated, electrical energy is given to electrons, which, due to their great mobility and large numbers, are able to disperse it rapidly and by elastic collision (without energy loss) to the heavy particles.[69][Note 3]
Examples of industrial/commercial plasma
Because of their sizable temperature and density ranges, plasmas find applications in many fields of research, technology and industry. For example, in: industrial and extractive metallurgy,[69][70] surface treatments such as plasma spraying (coating), etching in microelectronics,[71] metal cutting[72] and welding; as well as in everyday vehicle exhaust cleanup and fluorescent/luminescent lamps,[66] fuel ignition, while even playing a part in supersonic combustion engines for aerospace engineering.[73]
Low-pressure discharges
Glow discharge plasmas: non-thermal plasmas generated by the application of DC or low frequency RF (<100 kHz) electric field to the gap between two metal electrodes. Probably the most common plasma; this is the type of plasma generated within fluorescent light tubes.[74]
Capacitively coupled plasma (CCP): similar to glow discharge plasmas, but generated with high frequency RF electric fields, typically 13.56 MHz. These differ from glow discharges in that the sheaths are much less intense. These are widely used in the microfabrication and integrated circuit manufacturing industries for plasma etching and plasma enhanced chemical vapor deposition.[75]
Cascaded Arc Plasma Source: a device to produce low temperature (≈1eV) high density plasmas (HDP).
Inductively coupled plasma (ICP): similar to a CCP and with similar applications but the electrode consists of a coil wrapped around the chamber where plasma is formed.[76]
Wave heated plasma: similar to CCP and ICP in that it is typically RF (or microwave). Examples include helicon discharge and electron cyclotron resonance (ECR).[77]
Atmospheric pressure
Arc discharge: this is a high power thermal discharge of very high temperature (≈10,000 K). It can be generated using various power supplies. It is commonly used in metallurgical processes. For example, it is used to smelt minerals containing Al2O3 to produce aluminium.
Corona discharge: this is a non-thermal discharge generated by the application of high voltage to sharp electrode tips. It is commonly used in ozone generators and particle precipitators.
Dielectric barrier discharge (DBD): this is a non-thermal discharge generated by the application of high voltages across small gaps wherein a non-conducting coating prevents the transition of the plasma discharge into an arc. It is often mislabeled 'Corona' discharge in industry and has similar application to corona discharges. A common usage of this discharge is in a plasma actuator for vehicle drag reduction.[78] It is also widely used in the web treatment of fabrics.[79] The application of the discharge to synthetic fabrics and plastics functionalizes the surface and allows for paints, glues and similar materials to adhere.[80] The dielectric barrier discharge was used in the mid-1990s to show that low temperature atmospheric pressure plasma is effective in inactivating bacterial cells.[81] This work and later experiments using mammalian cells led to the establishment of a new field of research known as plasma medicine. The dielectric barrier discharge configuration was also used in the design of low temperature plasma jets. These plasma jets are produced by fast propagating guided ionisation waves known as plasma bullets.[82]
Capacitive discharge: this is a nonthermal plasma generated by the application of RF power (e.g., 13.56 MHz) to one powered electrode, with a grounded electrode held at a small separation distance on the order of 1 cm. Such discharges are commonly stabilized using a noble gas such as helium or argon.[83]
"Piezoelectric direct discharge plasma:" is a nonthermal plasma generated at the high-side of a piezoelectric transformer (PT). This generation variant is particularly suited for high efficient and compact devices where a separate high voltage power supply is not desired.
MHD converters
Main articles: magnetohydrodynamic converter, magnetohydrodynamic generator, and magnetohydrodynamic drive
See also: Electrothermal instability
A world effort was triggered in the 1960s to study magnetohydrodynamic converters in order to bring MHD power conversion to market with commercial power plants of a new kind, converting the kinetic energy of a high velocity plasma into electricity with no moving parts at a high efficiency. Research was also conducted in the field of supersonic and hypersonic aerodynamics to study plasma interaction with magnetic fields to eventually achieve passive and even active flow control around vehicles or projectiles, in order to soften and mitigate shock waves, lower thermal transfer and reduce drag.
Such ionized gases used in "plasma technology" ("technological" or "engineered" plasmas) are usually weakly ionized gases in the sense that only a tiny fraction of the gas molecules are ionized.[84] These kinds of weakly ionized gases are also nonthermal "cold" plasmas. In the presence of magnetics fields, the study of such magnetized nonthermal weakly ionized gases involves resistive magnetohydrodynamics with low magnetic Reynolds number, a challenging field of plasma physics where calculations require dyadic tensors in a 7-dimensional phase space. When used in combination with a high Hall parameter, a critical value triggers the problematic electrothermal instability which limited these technological developments.
Research
Plasmas are the object of study of the academic field of plasma science or plasma physics,[85] including sub-disciplines such as space plasma physics. It currently involves the following fields of active research and features across many journals, whose interest includes:
Plasma theory
Plasma equilibria and stability
Plasma interactions with waves and beams
Guiding center
Adiabatic invariant
Debye sheath
Coulomb collision
Plasmas in nature
Astrophysical plasma
Northern and southern (polar) lights
The Earth's ionosphere
Interplanetary medium
Planetary magnetospheres
Space plasma
Industrial plasmas
Plasma chemistry
Plasma processing
Plasma spray
Plasma display
Plasma sources
Dusty plasmas
Plasma diagnostics
Thomson scattering
Langmuir probe
Ball-pen probe
Faraday cup
Spectroscopy
Interferometry
Ionospheric heating
Incoherent scatter radar
Plasma applications
Dielectric barrier discharge
Enhanced oil recovery
Fusion power
Plasma Actuator (e.g. Serpentine geometry plasma actuator [86]
Magnetic fusion energy (MFE) —
Tokamak
Stellarator
Reversed field pinch
Magnetic mirror
Dense plasma focus
Inertial confinement fusion (ICF)
Plasma weapons
Ion implantation
Ion thruster
MAGPIE (Implosion experiments)
Plasma ashing
Food processing
Nonthermal plasma or "cold plasma"
Plasma arc waste disposal, recycling.
Plasma acceleration
Plasma medicine (e. g. Dentistry[87])
Plasma window
Research examples
Hall effect thruster. The electric field in a plasma double layer is so effective at accelerating ions that electric fields are used in ion drives.
File:Wispy 'Plasma Dancer' on the limb of the Sun.ogvPlay media
Solar plasma
Plasma spraying
Tokamak plasma in nuclear fusion research
Argon Plasma in the Hawkeye Linearly Magnetized Experiment (HLMX) at the University of Iowa
See also
Plasma torch
Ambipolar diffusion
Hannes Alfvén Prize
Plasma channel
Plasma parameters
Plasma nitriding
Magnetohydrodynamics (MHD)
Magnetohydrodynamic converter
Electrically powered spacecraft propulsion
Plasma propulsion engine
Electric field screening
List of plasma physicists
List of plasma physics articles
Important publications in plasma physics
IEEE Nuclear and Plasma Sciences Society
LULI
Quark-gluon plasma
Nikola Tesla
Space physics
Total electron content
Plasma display
Aurora
| To | |||||
|---|---|---|---|---|---|
| Solid | Liquid | Gas | Plasma | ||
| From | Solid | Melting | Sublimation | ||
| Liquid | Freezing | Vaporization | |||
| Gas | Deposition | Condensation | Ionization | ||
| Plasma | Recombination | ||||
Notes
The material undergoes various "regimes" or stages (e.g. saturation, breakdown, glow, transition and thermal arc) as the voltage is increased under the voltage-current relationship. The voltage rises to its maximum value in the saturation stage, and thereafter it undergoes fluctuations of the various stages; while the current progressively increases throughout.[68]
Across literature, there appears to be no strict definition on where the boundary is between a gas and plasma. Nevertheless, it is enough to say that at 2,000°C the gas molecules become atomized, and ionized at 3,000 °C and "in this state, [the] gas has a liquid like viscosity at atmospheric pressure and the free electric charges confer relatively high electrical conductivities that can approach those of metals."[69]
Note that non-thermal, or non-equilibrium plasmas are not as ionized and have lower energy densities, and thus the temperature is not dispersed evenly among the particles, where some heavy ones remain "cold".
References
πλάσμα Archived 18 June 2013 at the Wayback Machine, Henry George Liddell, Robert Scott, A Greek English Lexicon, on Perseus
Goldston, R.J.; Rutherford, P.H. (1995). Introduction to Plasma Physics. Taylor & Francis. p. 1−2. ISBN 978-0-7503-0183-1.
Morozov, A.I. (2012). Introduction to Plasma Dynamics. CRC Press. p. 17. ISBN 978-1-4398-8132-3.
Morozov, A.I. (2012). Introduction to Plasma Dynamics. CRC Press. p. 30. ISBN 978-1-4398-8132-3.
Morozov, A.I. (2012). Introduction to Plasma Dynamics. CRC Press. p. 4−5. ISBN 978-1-4398-8132-3.
"How Lightning Works". HowStuffWorks. April 2000. Archived from the original on 7 April 2014.
Phillips, K. J. H. (1995). Guide to the Sun. Cambridge University Press. p. 295. ISBN 978-0-521-39788-9. Archived from the original on 15 January 2018.
Aschwanden, M. J. (2004). Physics of the Solar Corona. An Introduction. Praxis Publishing. ISBN 978-3-540-22321-4.
Piel, A. (2010). Plasma Physics: An Introduction to Laboratory, Space, and Fusion Plasmas. Springer. pp. 4–5. ISBN 978-3-642-10491-6. Archived from the original on 5 January 2016.
Sturrock, Peter A. (1994). Plasma Physics: An Introduction to the Theory of Astrophysical, Geophysical & Laboratory Plasmas. Cambridge University Press. ISBN 978-0-521-44810-9.
Chu, P.K.; Lu, XinPel (2013). Low Temperature Plasma Technology: Methods and Applications. CRC Press. ISBN 978-1-4665-0990-0.
Chu, P.K.; Lu, XinPel (2013). Low Temperature Plasma Technology: Methods and Applications. CRC Press. p. 3. ISBN 978-1-4665-0990-0.
Chiuderi, C.; Velli, M. (2015). Basics of Plasma Astrophysics. Springer. p. 17. ISBN 978-88-470-5280-2.
Crookes presented a lecture to the British Association for the Advancement of Science, in Sheffield, on Friday, 22 August 1879 "Archived copy". Archived from the original on 9 July 2006. Retrieved 24 May 2006. "Radiant Matter". Archived from the original on 13 June 2006. Retrieved 24 May 2006.
Announced in his evening lecture to the Royal Institution on Friday, 30 April 1897, and published in Thomson, J. J. (1897). "J. J. Thomson (1856–1940)". Philosophical Magazine. 44 (269): 293–316. doi:10.1080/14786449708621070. Archived from the original on 12 August 2015.
Langmuir, I. (1928). "Oscillations in Ionized Gases". Proceedings of the National Academy of Sciences. 14 (8): 627–637. Bibcode:1928PNAS...14..627L. doi:10.1073/pnas.14.8.627. PMC 1085653. PMID 16587379.
Tonks, Lewi (1967). "The birth of "plasma"". American Journal of Physics. 35 (9): 857–858. Bibcode:1967AmJPh..35..857T. doi:10.1119/1.1974266.
Brown, Sanborn C. (1978). "Chapter 1: A Short History of Gaseous Electronics". In Hirsh, Merle N.; Oskam, H. J. (eds.). Gaseous Electronics. 1. Academic Press. ISBN 978-0-12-349701-7. Archived from the original on 23 October 2017.
Mott-Smith, Harold M. (1971). "History of "plasmas"". Nature. 233 (5316): 219. Bibcode:1971Natur.233..219M. doi:10.1038/233219a0. PMID 16063290.
Plasma fountain Source Archived 6 September 2008 at the Wayback Machine, press release: Solar Wind Squeezes Some of Earth's Atmosphere into Space Archived 20 March 2009 at the Wayback Machine
Chen, Francis F. (1984). Introduction to Plasma Physics and controlled fusion. Springer International Publishing. pp. 2–3. ISBN 9781475755954. Archived from the original on 15 January 2018.
Freidberg, Jeffrey P. (2008). Plasma Physics and Fusion Energy. Cambridge University Press. p. 121. ISBN 9781139462150. Archived from the original on 24 December 2016.
Hazeltine, R.D.; Waelbroeck, F.L. (2004). The Framework of Plasma Physics. Westview Press. ISBN 978-0-7382-0047-7.
Dendy, R. O. (1990). Plasma Dynamics. Oxford University Press. ISBN 978-0-19-852041-2. Archived from the original on 15 January 2018.
Hastings, Daniel & Garrett, Henry (2000). Spacecraft-Environment Interactions. Cambridge University Press. ISBN 978-0-521-47128-2.
1929-, Chen, Francis F. (1984). Introduction to plasma physics and controlled fusion. Chen, Francis F., 1929- (2nd ed.). New York: Plenum Press. ISBN 978-0306413322. OCLC 9852700. Archived from the original on 15 January 2018.
"Quasi-neutrality - The Plasma Universe theory (Wikipedia-like Encyclopedia)". www.plasma-universe.com. Archived from the original on 26 October 2017. Retrieved 25 October 2017.
Merlino, Robert L. (3 October 2012). "Plasma Oscillations— An application of electrostatics and classical mechanics". homepage.physics.uiowa.edu. pp. See October 3 notes. Archived from the original on 26 October 2017. Retrieved 25 October 2017.
Nicholson, Dwight R. (1983). Introduction to Plasma Theory. John Wiley & Sons. ISBN 978-0-471-09045-8.
Chapman, Brian (25 September 1980). "Chapter 3: Plasmas". Glow Discharge Processes: Sputtering and Plasma Etching. New York: John Wiley & Sons. p. 49. ISBN 978-0471078289.
von Engel, A. and Cozens, J.R. (1976) "Flame Plasma" in Advances in electronics and electron physics, L. L. Marton (ed.), Academic Press, ISBN 978-0-12-014520-1, p. 99 Archived 2 December 2016 at the Wayback Machine
Haines, M. G.; LePell, P. D.; Coverdale, C. A.; Jones, B.; Deeney, C.; Apruzese, J. P. (23 February 2006). "Ion Viscous Heating in a Magnetohydrodynamically Unstable Pinch at Over 2 × 109 Kelvin" (PDF). Physical Review Letters. 96 (7): 075003. Bibcode:2006PhRvL..96g5003H. doi:10.1103/PhysRevLett.96.075003. PMID 16606100.
Petit, J.-P. "The Z Machine: Over two billion degrees! Malcolm Haines' paper" (PDF). Retrieved 7 April 2018.
See Flashes in the Sky: Earth's Gamma-Ray Bursts Triggered by Lightning Archived 7 July 2014 at the Wayback Machine
Plasma science : from fundamental research to technological applications. National Research Council (U.S.). Panel on Opportunities in Plasma Science and Technology. Washington, D.C.: National Academy Press. 1995. p. 51. ISBN 9780309052313. OCLC 42854229.
Dorch, Søren (13 April 2007). "Magnetohydrodynamics". Scholarpedia. 2 (4): 2295. Bibcode:2007SchpJ...2.2295D. doi:10.4249/scholarpedia.2295. ISSN 1941-6016.
Richard Fitzpatrick, Introduction to Plasma Physics, Magnetized plasmas Archived 1 March 2006 at the Wayback Machine
Frank-Kamenetskii, David A. (1972) [1961–1963]. Plasma-The Fourth State of Matter (3rd ed.). New York: Plenum Press. ISBN 9781468418965. Archived from the original on 15 January 2018.
Yaffa Eliezer, Shalom Eliezer, The Fourth State of Matter: An Introduction to the Physics of Plasma, Publisher: Adam Hilger, 1989, ISBN 978-0-85274-164-1, 226 pages, page 5
Bittencourt, J.A. (2004). Fundamentals of Plasma Physics. Springer. p. 1. ISBN 9780387209753. Archived from the original on 2 February 2017.
Hong, Alice (2000). Elert, Glenn (ed.). "Dielectric Strength of Air". The Physics Factbook. Retrieved 6 July 2018.
It is assumed that more than 99% the visible universe is made of some form of plasma.Gurnett, D. A. & Bhattacharjee, A. (2005). Introduction to Plasma Physics: With Space and Laboratory Applications. Cambridge, UK: Cambridge University Press. p. 2. ISBN 978-0-521-36483-6. Scherer, K; Fichtner, H & Heber, B (2005). Space Weather: The Physics Behind a Slogan. Berlin: Springer. p. 138. ISBN 978-3-540-22907-0..
Kelley, M. C. (2009). The Earth's Ionosphere: Plasma Physics and Electrodynamics (2nd ed.). Academic Press. ISBN 9780120884254.
Russell, C.T. (1990). "The Magnetopause". Physics of Magnetic Flux Ropes. Geophysical Monograph Series. 58: 439–453. Bibcode:1990GMS....58..439R. doi:10.1029/GM058p0439. ISBN 0-87590-026-7. Archived from the original on 3 May 2012. Retrieved 25 August 2018.
Mészáros, Péter (2010) The High Energy Universe: Ultra-High Energy Events in Astrophysics and Cosmology, Publisher: Cambridge University Press, ISBN 978-0-521-51700-3, p. 99 Archived 2 February 2017 at the Wayback Machine.
Raine, Derek J. and Thomas, Edwin George (2010) Black Holes: An Introduction, Publisher: Imperial College Press, ISBN 978-1-84816-382-9, p. 160 Archived 2 December 2016 at the Wayback Machine
Nemiroff, Robert and Bonnell, Jerry (11 December 2004) Astronomy Picture of the Day Archived 18 October 2012 at the Wayback Machine, nasa.gov
IPPEX Glossary of Fusion Terms Archived 8 March 2008 at the Wayback Machine. Ippex.pppl.gov. Retrieved on 2011-11-19.
Helmenstine, Anne Marie. "What is the State of Matter of Fire or Flame? Is it a Liquid, Solid, or Gas?". About.com. Retrieved 21 January 2009.
Dickel, J. R. (1990). "The Filaments in Supernova Remnants: Sheets, Strings, Ribbons, or?". Bulletin of the American Astronomical Society. 22: 832. Bibcode:1990BAAS...22..832D.
Grydeland, T. (2003). "Interferometric observations of filamentary structures associated with plasma instability in the auroral ionosphere". Geophysical Research Letters. 30 (6): 1338. Bibcode:2003GeoRL..30.1338G. doi:10.1029/2002GL016362.
Moss, G. D.; Pasko, V. P.; Liu, N.; Veronis, G. (2006). "Monte Carlo model for analysis of thermal runaway electrons in streamer tips in transient luminous events and streamer zones of lightning leaders". Journal of Geophysical Research. 111 (A2): A02307. Bibcode:2006JGRA..111.2307M. doi:10.1029/2005JA011350.
Doherty, Lowell R.; Menzel, Donald H. (1965). "Filamentary Structure in Solar Prominences". The Astrophysical Journal. 141: 251. Bibcode:1965ApJ...141..251D. doi:10.1086/148107.
"Hubble views the Crab Nebula M1: The Crab Nebula Filaments". Archived from the original on 5 October 2009. Retrieved 26 January 2017.. The University of Arizona
Zhang, Y. A.; Song, M. T.; Ji, H. S. (2002). "A rope-shaped solar filament and a IIIb flare". Chinese Astronomy and Astrophysics. 26 (4): 442–450. Bibcode:2002ChA&A..26..442Z. doi:10.1016/S0275-1062(02)00095-4.
Boeuf, J. P.; Chaudhury, B.; Zhu, G. Q. (2010). "Theory and Modeling of Self-Organization and Propagation of Filamentary Plasma Arrays in Microwave Breakdown at Atmospheric Pressure". Physical Review Letters. 104 (1): 015002. Bibcode:2010PhRvL.104a5002B. doi:10.1103/PhysRevLett.104.015002. PMID 20366367.
Chin, S. L. (2006). Some Fundamental Concepts of Femtosecond Laser Filamentation (PDF). Journal of the Korean Physical Society. Springer Series in Chemical Physics. 49. p. 281. Bibcode:2008pui3.book..243C. doi:10.1007/978-3-540-73794-0_12. ISBN 978-3-540-73793-3.
Talebpour, A.; Abdel-Fattah, M.; Chin, S. L. (2000). "Focusing limits of intense ultrafast laser pulses in a high pressure gas: Road to new spectroscopic source". Optics Communications. 183 (5–6): 479–484. Bibcode:2000OptCo.183..479T. doi:10.1016/S0030-4018(00)00903-2.
Greaves, R. G.; Tinkle, M. D.; Surko, C. M. (1994). "Creation and uses of positron plasmas". Physics of Plasmas. 1 (5): 1439. Bibcode:1994PhPl....1.1439G. doi:10.1063/1.870693.
Morfill, G. E.; Ivlev, Alexei V. (2009). "Complex plasmas: An interdisciplinary research field". Reviews of Modern Physics. 81 (4): 1353–1404. Bibcode:2009RvMP...81.1353M. doi:10.1103/RevModPhys.81.1353.
Alfvén, H.; Smårs, E. (1960). "Gas-Insulation of a Hot Plasma". Nature. 188 (4753): 801–802. Bibcode:1960Natur.188..801A. doi:10.1038/188801a0. S2CID 26797662.
Braams, C.M. (1966). "Stability of Plasma Confined by a Cold-Gas Blanket". Physical Review Letters. 17 (9): 470–471. Bibcode:1966PhRvL..17..470B. doi:10.1103/PhysRevLett.17.470.
Yaghoubi, A.; Mélinon, P. (2013). "Tunable synthesis and in situ growth of silicon-carbon mesostructures using impermeable plasma". Scientific Reports. 3: 1083. Bibcode:2013NatSR...3E1083Y. doi:10.1038/srep01083. PMC 3547321. PMID 23330064.
See Evolution of the Solar System Archived 25 December 2017 at the Wayback Machine, 1976
Roy, S., and Pandey, B. "Roy S. and Pandey, B.P. Numerical Investigation of a Hall Thruster Plasma, Physics of Plasmas, 9 (9) pp. 4052-60 (2002): https://doi.org/10.1063/1.1498261.
Hippler, R.; Kersten, H.; Schmidt, M.; Schoenbach, K.M., eds. (2008). "Plasma Sources". Low Temperature Plasmas: Fundamentals, Technologies, and Techniques (2nd ed.). Wiley-VCH. ISBN 978-3-527-40673-9.
Chen, Francis F. (1984). Plasma Physics and Controlled Fusion. Plenum Press. ISBN 978-0-306-41332-2. Archived from the original on 15 January 2018.
Leal-Quirós, Edbertho (2004). "Plasma Processing of Municipal Solid Waste". Brazilian Journal of Physics. 34 (4B): 1587–1593. Bibcode:2004BrJPh..34.1587L. doi:10.1590/S0103-97332004000800015.
Gomez, E.; Rani, D. A.; Cheeseman, C. R.; Deegan, D.; Wise, M.; Boccaccini, A. R. (2009). "Thermal plasma technology for the treatment of wastes: A critical review". Journal of Hazardous Materials. 161 (2–3): 614–626. doi:10.1016/j.jhazmat.2008.04.017. PMID 18499345.
Szałatkiewicz, J. (2016). "Metals Recovery from Artificial Ore in Case of Printed Circuit Boards, Using Plasmatron Plasma Reactor". Materials. 9 (8): 683–696. Bibcode:2016Mate....9..683S. doi:10.3390/ma9080683. PMC 5512349. PMID 28773804.
National Research Council (1991). Plasma Processing of Materials : Scientific Opportunities and Technological Challenges. National Academies Press. ISBN 978-0-309-04597-1.
Nemchinsky, V. A.; Severance, W. S. (2006). "What we know and what we do not know about plasma arc cutting". Journal of Physics D: Applied Physics. 39 (22): R423. Bibcode:2006JPhD...39R.423N. doi:10.1088/0022-3727/39/22/R01.
Peretich, M.A.; O'Brien, W.F.; Schetz, J.A. (2007). "Plasma torch power control for scramjet application" (PDF). Virginia Space Grant Consortium. Archived from the original (PDF) on 29 June 2010. Retrieved 12 April 2010.
Stern, David P. "The Fluorescent Lamp: A plasma you can use". Archived from the original on 30 May 2010. Retrieved 19 May 2010.
Sobolewski, M.A.; Langan & Felker, J.G. & B.S. (1997). "Electrical optimization of plasma-enhanced chemical vapor deposition chamber cleaning plasmas" (PDF). Journal of Vacuum Science and Technology B. 16 (1): 173–182. Bibcode:1998JVSTB..16..173S. doi:10.1116/1.589774. Archived from the original (PDF) on 18 January 2009.
Okumura, T. (2010). "Inductively Coupled Plasma Sources and Applications". Physics Research International. 2010: 1–14. doi:10.1155/2010/164249.
Plasma Chemistry. Cambridge University Press. 2008. p. 229. ISBN 9781139471732. Archived from the original on 2 February 2017.
Roy, S.; Zhao, P.; Dasgupta, A.; Soni, J. (2016). "Dielectric barrier discharge actuator for vehicle drag reduction at highway speeds". AIP Advances. 6 (2): 025322. Bibcode:2016AIPA....6b5322R. doi:10.1063/1.4942979.
Leroux, F.; Perwuelz, A.; Campagne, C.; Behary, N. (2006). "Atmospheric air-plasma treatments of polyester textile structures". Journal of Adhesion Science and Technology. 20 (9): 939–957. doi:10.1163/156856106777657788. S2CID 137392051.
Leroux, F. D. R.; Campagne, C.; Perwuelz, A.; Gengembre, L. O. (2008). "Polypropylene film chemical and physical modifications by dielectric barrier discharge plasma treatment at atmospheric pressure". Journal of Colloid and Interface Science. 328 (2): 412–420. Bibcode:2008JCIS..328..412L. doi:10.1016/j.jcis.2008.09.062. PMID 18930244.
Laroussi, M. (1996). "Sterilization of contaminated matter with an atmospheric pressure plasma". IEEE Transactions on Plasma Science. 24 (3): 1188–1191. Bibcode:1996ITPS...24.1188L. doi:10.1109/27.533129.
Lu, X.; Naidis, G.V.; Laroussi, M.; Ostrikov, K. (2014). "Guided ionization waves: Theory and experiments". Physics Reports. 540 (3): 123. Bibcode:2014PhR...540..123L. doi:10.1016/j.physrep.2014.02.006.
Park, J.; Henins, I.; Herrmann, H. W.; Selwyn, G. S.; Hicks, R. F. (2001). "Discharge phenomena of an atmospheric pressure radio-frequency capacitive plasma source". Journal of Applied Physics. 89 (1): 20. Bibcode:2001JAP....89...20P. doi:10.1063/1.1323753.
Plasma scattering of electromagnetic radiation : theory and measurement techniques. Froula, Dustin H. (1st ed., 2nd ed.). Burlington, MA: Academic Press/Elsevier. 2011. p. 273. ISBN 978-0080952031. OCLC 690642377.
University of Colorado, Plasma Physics, Overview
"Wrangling flow to quiet cars and aircraft," EurekAlert, http://www.eurekalert.org/pub_releases/2013-10/aiop-wft101813.php, viewed on 1/20/2014.
"High-tech dentistry – "St Elmo's frier" – Using a plasma torch to clean your teeth". The Economist print edition. 17 June 2009. Archived from the original on 20 June 2009. Retrieved 7 September 2009.
External links
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