Materials And States Of Matter Codexery

Plasma (physics)

Plasma is the fourth state of matter, consisting of ionized gas.

Plasma (physics)

Plasma is a state of matter created when one of the other three classical states—most often a gas—becomes significantly ionized. This means it contains a large number of charged particles, such as ions and electrons. Though plasma is rarely found naturally on Earth, it makes up an estimated 99.9% of all ordinary matter in the universe. Stars are nearly entirely made of plasma, and it also dominates the sparse intracluster and intergalactic mediums. Plasma can be produced artificially by heating a neutral gas or exposing it to a strong electromagnetic field. Because it contains charged particles, plasma is electrically conductive. The behavior of both individual particles and the overall plasma is shaped by collective electromagnetic fields, and it is highly sensitive to any externally applied fields. This response to electromagnetic fields is used in technologies like plasma televisions and plasma etching. Depending on conditions, some neutral particles may remain, creating what is called a partially ionized plasma. Examples include neon signs and lightning. Unlike the clear phase transitions between solids, liquids, and gases, the transition to plasma is not sharply defined. Whether a given level of ionization counts as plasma depends on the specific phenomenon under study. **Etymology** Irving Langmuir introduced the term "plasma" for ionized gas in 1928. He wrote that, except near electrodes where sheaths contain very few electrons, the ionized gas has roughly equal numbers of ions and electrons, resulting in very little space charge. He used "plasma" to describe this region of balanced charges. Colleagues Lewi Tonks and Harold Mott-Smith recalled that Langmuir was inspired by blood plasma—specifically, the way electrons from thermionic filaments reminded him of how blood plasma carries red and white corpuscles and germs. The word "plasma" in blood plasma ultimately comes from the Greek word for the result of forming or molding. **History** Plasma science grew from Langmuir’s work in the 1920s, but its roots lie in the history of electricity. The electric arc was independently discovered by Vasily Petrov and Humphry Davy in 1803. In 1831, Michael Faraday systematically studied electric glow discharge in rarefied gases. Initially, electrical conduction through gases was thought to resemble conduction in liquids. Sir William Crookes, studying low-pressure discharges, proposed a different model and introduced the idea of a fourth state of matter in a well-known 1879 paper. **Definitions**

**The fourth state of matter** Plasma is called the fourth state of matter, after solid, liquid, and gas. In this state, an ionized substance becomes so electrically conductive that long-range electric and magnetic fields dominate its behavior. Plasma is typically electrically quasineutral—its overall charge is roughly zero—consisting of unbound positive and negative particles. Though unbound, these particles are not free from forces; moving charged particles generate electric currents, and each particle’s motion both affects and is affected by the fields created by other charges. This leads to collective behavior with many degrees of variation. Plasma is distinct from the other states. Describing a low-density plasma as merely an "ionized gas" is misleading, even though like a gas it has no definite shape or volume. **Ideal plasma** Three factors define an ideal plasma: 1. The plasma approximation applies when the plasma parameter Λ (the number of charge carriers within the Debye sphere) is much greater than one. This is equivalent to the ratio of plasma electrostatic energy to thermal energy being small; such plasmas are called weakly coupled. 2. The Debye length is much smaller than the physical size of the plasma, meaning interactions in the bulk are more important than boundary effects. When this holds, the plasma is quasineutral. 3. The electron plasma frequency (measuring electron oscillations) is much larger than the electron–neutral collision frequency. When this is true, electrostatic interactions dominate over ordinary gas kinetics; such plasmas are called collisionless. **Non-neutral plasma** Because of the strength and range of the electric force and plasma’s good conductivity, positive and negative charge densities in any sizable region are usually equal (quasineutrality). A plasma with a significant excess of charge—or, in extreme cases, composed of a single species—is called a non-neutral plasma. Here, electric fields dominate. Examples include charged particle beams, an electron cloud in a Penning trap, and positron plasmas. **Dusty plasma** A dusty plasma contains tiny charged dust particles, typically found in space. The dust particles acquire high charges and interact with each other. A plasma with larger particles is called a grain plasma. In laboratory settings, dusty plasmas are also called complex plasmas.

field
Physics
known_for
Fourth state of matter; ionized gas with charged particles; electrically conductive; dominates approximately 99% of ordinary matter in the universe

Lore & Background

Plasma is a state of matter formed when a gas, or another classical state, becomes significantly ionized, meaning a large portion of its atoms have split into charged ions and electrons. This substance is rarely found naturally on Earth, yet it constitutes an estimated 99.9% of all ordinary matter in the universe, forming stars, the intracluster medium, and the intergalactic medium. It can be created artificially by heating a neutral gas or exposing it to a strong electromagnetic field. The defining characteristic of plasma is its electrical conductivity, which arises from the presence of these charged particles. Their movements generate and are governed by collective electromagnetic fields, making plasma highly sensitive to external fields. This property is exploited in technologies like plasma televisions and plasma etching. Plasma is typically quasineutral, meaning its overall charge is roughly zero, though it can exist as a non-neutral plasma composed of a single species, such as in charged particle beams. A dusty plasma contains tiny charged dust particles, often found in space. The transition to plasma is not a sharp phase change like melting or boiling; it is a matter of interpretation, depending on whether the degree of ionization is sufficient for the phenomenon under study. Partially ionized plasmas, which contain some neutral particles, are seen in neon signs and lightning.

Reader's Guide

Plasma is distinct from the other states of matter. In particular, describing a low-density plasma as merely an 'ionized gas' is wrong and misleading, even though it is similar to the gas phase in that both assume no definite shape or volume. The presence of charged particles makes plasma electrically conductive, with the dynamics of individual particles and macroscopic plasma motion governed by collective electromagnetic fields and very sensitive to externally applied fields. The response of plasma to electromagnetic fields is used in many modern devices and technologies, such as plasma televisions or plasma etching. Unlike the phase transitions between the three other classical states of matter, the transition to plasma is not well defined and is a matter of interpretation and context. Whether a given degree of ionization suffices to call a substance 'plasma' depends on the specific phenomenon being considered. Plasma is typically an electrically quasineutral medium of unbound positive and negative particles. Although these particles are unbound, they are not 'free' in the sense of not experiencing forces. Moving charged particles generate electric currents, and any movement of a charged plasma particle affects and is affected by the fields created by the other charges.

Did You Know?

Formation and Fundamental Composition

Plasma emerges when matter is subjected to sufficiently high temperatures or intense electromagnetic fields, conditions under which atoms shed their electrons and become ionized. This process sets plasma apart from the three classical states of matter—solid, liquid, and gas—which dominate under ordinary pressure and temperature conditions. While a gas consists of neutral atoms drifting relatively independently, plasma is populated by a significant population of free electrons alongside their parent ionized atoms, creating a fundamentally different kind of material. The distinction is not merely one of degree but of kind: the presence of mobile charged particles transforms the collective behavior of the substance entirely. In the broader landscape of matter, plasma occupies a position beyond the traditional triad, belonging to the vast family of distinct states that arise when external conditions push atoms beyond their familiar configurations. It is one of the infinite ways that matter can organize itself when the usual constraints of moderate temperature and pressure no longer apply.

Collective Electromagnetic Identity

What most sharply distinguishes plasma from a neutral gas is its electromagnetic personality. Because the medium is riddled with free electrons and ionized atoms, it does not behave as a collection of isolated particles. Instead, plasma can self-generate magnetic fields and sustain electric currents within itself, phenomena that a simple gas cannot produce on its own. Furthermore, when external electromagnetic forces are applied, the response is not local or individual; it is strong and collective, with the charged constituents acting in concert as a coupled system. This collective responsiveness means that a disturbance in one region of the plasma can propagate and influence distant regions through the self-generated fields, giving the state a kind of internal coherence that neutral matter simply lacks. In the taxonomy of states of matter, this electromagnetic self-organization is what elevates plasma from a mere hot gas to a genuinely distinct phase with fundamentally different properties, placing it alongside liquid crystals, superconductors, and magnetic phases as a state defined by emergent collective behavior rather than by the arrangement of neutral atoms alone.

Plasma in the Infinite Taxonomy of Matter

Plasma does not exist in isolation; it is one thread in an extraordinarily rich tapestry of material states. Beyond the familiar solid, liquid, and gas, matter can organize in an infinite number of ways, each yielding fundamentally different properties. Complex molecules give rise to mesophases such as liquid crystals, which flow like liquids yet maintain long-range orientational order. At cryogenic temperatures, electrons in solids can condense into superconducting states with vanishing resistivity, or arrange their spins into patterns of ferromagnetism and antiferromagnetism. Under the extreme conditions inside certain stars or in the early universe, atoms themselves break apart into degenerate matter or quark matter. Plasma, formed by ionization at high temperatures or under strong electromagnetic fields, sits among this diverse company as a state defined by its charged, collectively responsive constituents. The identification of each of these states—from Bose-Einstein condensates to spin glasses to ferroelectric phases—reflects the depth of modern physics in cataloguing the many faces that matter can wear under the right conditions.

The Twentieth-Century Cataloguing of States

The recognition of plasma as a distinct state of matter is part of a broader twentieth-century scientific revolution in understanding how matter organizes itself. As physicists deepened their grasp of atomic and subatomic properties, an ever-growing catalogue of material phases emerged, each with its own defining characteristics. The list stretches from conventional and unconventional superconductors to fermionic condensates, from spin-density waves to quantum spin liquids, from ferroelectric and antiferroelectric states to altermagnetism with its spin-split electronic bands. Plasma, with its free electrons, ionized atoms, self-generated fields, and collective electromagnetic response, occupies a prominent place in this catalogue. The theoretical framework of Landau theory, which treats different structural phases of polymorphic materials as distinct states, provided a unifying lens through which these diverse phenomena could be compared. Plasma's inclusion among these notable examples underscores that the classical triad of solid, liquid, and gas was never the complete story—merely the most accessible chapter in a far longer narrative about the possibilities of matter.

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