In

_{m}'' = ''R''(''T_{C}'' + 267) (with temperature expressed in degrees Celsius), where ''R'' is the gas constant. However, later work revealed that the number should actually be closer to 273.2, and then the Celsius scale was defined with $0~^\backslash mathrm\; =\; 273.15~\backslash mathrm$, giving:$$pV\_m\; =\; R\; \backslash left(T\_C\; +\; 273.15\backslash \; ^\backslash circ\backslash text\backslash right).$$In 1873, J. D. van der Waals introduced the first

_{B}''T'') where ''μ'' is the chemical potential, Li is the polylogarithm, ζ is the Riemann zeta function, and ''T''_{''c''} is the critical temperature at which a Bose–Einstein condensate begins to form.

Link to Archiv e-print**Link to Hal e-print**

/ref> * Anton-Schmidt equation of state

physics
Physics is the natural science that studies matter, its Elementary particle, fundamental constituents, its motion and behavior through Spacetime, space and time, and the related entities of energy and force. "Physical science is that depar ...

, chemistry
Chemistry is the scientific study of the properties and behavior of matter. It is a natural science that covers the elements that make up matter to the compounds made of atoms, molecules and ions: their composition, structure, properties ...

, and thermodynamics
Thermodynamics is a branch of physics that deals with heat, Work (thermodynamics), work, and temperature, and their relation to energy, entropy, and the physical properties of matter and radiation. The behavior of these quantities is governed b ...

, an equation of state is a thermodynamic equation relating state variables, which describe the state of matter under a given set of physical conditions, such as pressure
Pressure (symbol: ''p'' or ''P'') is the force applied perpendicular to the surface of an object per unit area over which that force is distributed. Gauge pressure (also spelled ''gage'' pressure)The preferred spelling varies by country and e ...

, volume
Volume is a measure of occupied three-dimensional space. It is often quantified numerically using SI derived units (such as the cubic metre and litre) or by various imperial or US customary units (such as the gallon, quart, cubic inch). ...

, temperature
Temperature is a physical quantity that expresses quantitatively the perceptions of hotness and coldness. Temperature is measurement, measured with a thermometer.
Thermometers are calibrated in various Conversion of units of temperature, temp ...

, or internal energy
The internal energy of a thermodynamic system is the total energy contained within it. It is the energy necessary to create or prepare the system in its given internal state, and includes the contributions of potential energy and internal kinet ...

. Most modern equations of state are formulated in the Helmholtz free energy. Equations of state are useful in describing the properties of pure substances and mixtures in liquids, gases, and solid
Solid is one of the State of matter#Four fundamental states, four fundamental states of matter (the others being liquid, gas, and Plasma (physics), plasma). The molecules in a solid are closely packed together and contain the least amount o ...

states as well as the state of matter in the interior of star
A star is an astronomical object comprising a luminous spheroid of plasma (physics), plasma held together by its gravity. The List of nearest stars and brown dwarfs, nearest star to Earth is the Sun. Many other stars are visible to the naked ...

s.
Overview

At present, there is no single equation of state that accurately predicts the properties of all substances under all conditions. An example of an equation of state correlates densities of gases and liquids to temperatures and pressures, known as theideal gas law
The ideal gas law, also called the general gas equation, is the equation of state of a hypothetical ideal gas. It is a good approximation of the behavior of many gases under many conditions, although it has several limitations. It was first s ...

, which is roughly accurate for weakly polar gases at low pressures and moderate temperatures. This equation becomes increasingly inaccurate at higher pressures and lower temperatures, and fails to predict condensation from a gas to a liquid.
The general form of an equation of state may be written as
$$f(p,\; V,\; T)\; =\; 0$$
where $p$ is the pressure, $V$ the volume, and $T$ the temperature of the system. Yet also other variables may be used in that form. It is directly related to Gibbs phase rule, that is, the number of independent variables depends on the number of substances and phases in the system.
An equation used to model this relationship is called an equation of state. In most cases this model will comprise some empirical parameters that are usually adjusted to measurement data. Equations of state can also describe solids, including the transition of solids from one crystalline state to another. Equations of state are also used for the modeling of the state of matter in the interior of stars, including neutron star
A neutron star is the Gravitational collapse, collapsed Stellar structure, core of a massive supergiant star, which had a total mass of between 10 and 25 solar masses, possibly more if the star was especially Metallicity, metal-rich. Except fo ...

s, dense matter ( quark–gluon plasmas) and radiation fields. A related concept is the perfect fluid equation of state used in cosmology.
Equations of state are applied in many fields such as process engineering
Process engineering is the understanding and application of the fundamental principles and Scientific law, laws of nature that allow humans to transform raw material and energy into products that are useful to society, at an industrial level. By t ...

and petroleum industry as well as pharmaceutical industry.
Any consistent set of units may be used, although SI units are preferred. Absolute temperature refers to the use of the Kelvin (K), with zero being absolute zero.
*$n$, number of moles of a substance
*$V\_m$, $\backslash frac$, molar volume, the volume of 1 mole of gas or liquid
*$R$, ideal gas constant ≈ 8.3144621J/mol·K
*$p\_c$, pressure at the critical point
*$V\_c$, molar volume at the critical point
*$T\_c$, absolute temperature at the critical point
Historical background

Boyle's law was one of the earliest formulation of an equation of state. In 1662, the Irish physicist and chemist Robert Boyle performed a series of experiments employing a J-shaped glass tube, which was sealed on one end. Mercury was added to the tube, trapping a fixed quantity of air in the short, sealed end of the tube. Then the volume of gas was measured as additional mercury was added to the tube. The pressure of the gas could be determined by the difference between the mercury level in the short end of the tube and that in the long, open end. Through these experiments, Boyle noted that the gas volume varied inversely with the pressure. In mathematical form, this can be stated as:$$pV\; =\; \backslash mathrm.$$The above relationship has also been attributed to Edme Mariotte and is sometimes referred to as Mariotte's law. However, Mariotte's work was not published until 1676. In 1787 the French physicist Jacques Charles found that oxygen, nitrogen, hydrogen, carbon dioxide, and air expand to roughly the same extent over the same 80-kelvin interval. This is known today as Charles's law. Later, in 1802, Joseph Louis Gay-Lussac published results of similar experiments, indicating a linear relationship between volume and temperature:$$\backslash frac\; =\; \backslash frac.$$ Dalton's law (1801) of partial pressure states that the pressure of a mixture of gases is equal to the sum of the pressures of all of the constituent gases alone. Mathematically, this can be represented for $n$ species as:$$p\_\backslash text\; =\; p\_1\; +\; p\_2\; +\; \backslash cdots\; +\; p\_n\; =\; \backslash sum\_^n\; p\_i.$$In 1834, Émile Clapeyron combined Boyle's law and Charles' law into the first statement of the ''ideal gas law
The ideal gas law, also called the general gas equation, is the equation of state of a hypothetical ideal gas. It is a good approximation of the behavior of many gases under many conditions, although it has several limitations. It was first s ...

''. Initially, the law was formulated as ''pVequation of state
In physics, chemistry, and thermodynamics, an equation of state is a thermodynamic equations, thermodynamic equation relating state variables, which describe the state of matter under a given set of physical conditions, such as pressure, Volume ( ...

derived by the assumption of a finite volume occupied by the constituent molecules. His new formula revolutionized the study of equations of state, and was the starting point of cubic equations of state, which most famously continued via the Redlich–Kwong equation of state and the Soave modification of Redlich-Kwong.
The van der Waals equation of state can be written as
:$\backslash left(P+a\backslash frac1\backslash right)(V\_m-b)=R\; T$
where $a$ is a parameter describing the attractive energy between particles and $b$ is a parameter describing the volume of the particles.
Ideal gas law

Classical ideal gas law

The classicalideal gas law
The ideal gas law, also called the general gas equation, is the equation of state of a hypothetical ideal gas. It is a good approximation of the behavior of many gases under many conditions, although it has several limitations. It was first s ...

may be written
$$pV\; =\; nRT.$$
In the form shown above, the equation of state is thus
$$f(p,\; V,\; T)\; =\; pV\; -\; nRT\; =\; 0.$$
If the calorically perfect gas approximation is used, then the ideal gas law may also be expressed as follows
$$p\; =\; \backslash rho(\backslash gamma\; -\; 1)e$$
where $\backslash rho$ is the density, $\backslash gamma\; =\; C\_p/C\_v$ is the (constant) adiabatic index ( ratio of specific heats), $e\; =\; C\_v\; T$ is the internal energy per unit mass (the "specific internal energy"), $C\_v$ is the constant specific heat at constant volume, and $C\_p$ is the constant specific heat at constant pressure.
Quantum ideal gas law

Since for atomic and molecular gases, the classical ideal gas law is well suited in most cases, let us describe the equation of state for elementary particles with mass $m$ and spin $s$ that takes into account of quantum effects. In the following, the upper sign will always correspond to Fermi–Dirac statistics and the lower sign to Bose–Einstein statistics. The equation of state of such gases with $N$ particles occupying a volume $V$ with temperature $T$ and pressure $p$ is given by $$p=\; \backslash frac\backslash int\_0^\backslash infty\backslash frac$$ where $k\_\backslash text$ is the Boltzmann constant and $\backslash mu(T,N/V)$ the chemical potential is given by the following implicit function $$\backslash frac=\backslash frac\backslash int\_0^\backslash infty\backslash frac.$$ In the limiting case where $e^\backslash ll\; 1$, this equation of state will reduce to that of the classical ideal gas. It can be shown that the above equation of state in the limit $e^\backslash ll\; 1$ reduces to $$pV\; =\; N\; k\_\backslash text\; T\backslash left;\; href="/html/ALL/s/\backslash pm\backslash frac\_\backslash frac+\backslash cdots\backslash right.html"\; ;"title="\backslash pm\backslash frac\; \backslash frac+\backslash cdots\backslash right">\backslash pm\backslash frac\; \backslash frac+\backslash cdots\backslash right$$Fermi gas
An ideal Fermi gas is a state of matter which is an ensemble of many non-interacting fermions. Fermions are subatomic particle, particles that obey Fermi–Dirac statistics, like electrons, protons, and neutrons, and, in general, particles with ...

, an increase in the value for pressure from its classical value implying an effective repulsion between particles (this is an apparent repulsion due to quantum exchange effects not because of actual interactions between particles since in ideal gas, interactional forces are neglected) and in Bose gas, a decrease in pressure from its classical value implying an effective attraction. The quantum nature of this equation is in it dependence on s and ħ.
Cubic equations of state

Cubic equations of state are called such because they can be rewritten as a cubic function of $V\_m$. Cubic equations of state originated from van der Waals equation of state. Hence, all cubic equations of state can be considered 'modified van der Waals equation of state'. There is a very large number of such cubic equations of state. For process engineering, cubic equations of state are today still highly relevant, e.g. the Peng Robinson equation of state or the Soave Redlich Kwong equation of state.Virial equations of state

Virial equation of state

$$\backslash frac\; =\; A\; +\; \backslash frac\; +\; \backslash frac\; +\; \backslash frac\; +\; \backslash cdots$$ Although usually not the most convenient equation of state, the virial equation is important because it can be derived directly from statistical mechanics. This equation is also called the Kamerlingh Onnes equation. If appropriate assumptions are made about the mathematical form of intermolecular forces, theoretical expressions can be developed for each of the coefficients. ''A'' is the first virial coefficient, which has a constant value of 1 and makes the statement that when volume is large, all fluids behave like ideal gases. The second virial coefficient ''B'' corresponds to interactions between pairs of molecules, ''C'' to triplets, and so on. Accuracy can be increased indefinitely by considering higher order terms. The coefficients ''B'', ''C'', ''D'', etc. are functions of temperature only.The BWR equation of state

$$p\; =\; \backslash rho\; RT\; +\; \backslash left(B\_0\; RT\; -\; A\_0\; -\; \backslash frac\; +\; \backslash frac\; -\; \backslash frac\backslash right)\; \backslash rho^2\; +\; \backslash left(bRT\; -\; a\; -\; \backslash frac\backslash right)\; \backslash rho^3\; +\; \backslash alpha\backslash left(a\; +\; \backslash frac\backslash right)\; \backslash rho^6\; +\; \backslash frac\backslash left(1\; +\; \backslash gamma\backslash rho^2\backslash right)\backslash exp\backslash left(-\backslash gamma\backslash rho^2\backslash right)$$ where *$p$ is pressure *$\backslash rho$ is molar density Values of the various parameters can be found in reference materials. The BWR equation of state has also frequently been used for the modelling of the Lennard-Jones fluid. There are several extensions and modifications of the classical BWR equation of state available. The Benedict–Webb–Rubin–Starling equation of state is a modified BWR equation of state and can be written as $$p=\backslash rho\; RT\; +\; \backslash left(B\_0\; RT-A\_0\; -\; \backslash frac\; +\; \backslash frac\; -\; \backslash frac\backslash right)\; \backslash rho^2\; +\; \backslash left(bRT-a-\backslash frac\; +\; \backslash frac\backslash right)\; \backslash rho^3\; +\; \backslash alpha\backslash left(a+\backslash frac\backslash right)\; \backslash rho^6$$ Note that in this virial equation, the fourth and fifth virial terms are zero. The second virial coefficient is monotonically decreasing as temperature is lowered. The third virial coefficient is monotonically increasing as temperature is lowered. The Lee–Kesler equation of state is based on the corresponding states principle, and is a modification of the BWR equation of state. $$p\; =\; \backslash frac\; \backslash left(\; 1\; +\; \backslash frac\; +\; \backslash frac\; +\; \backslash frac\; +\; \backslash frac\; \backslash left(\; \backslash beta\; +\; \backslash frac\; \backslash right)\; \backslash exp\; \backslash left(\; \backslash frac\; \backslash right)\; \backslash right)$$Physically-based equations of state

There is a large number of physically-based equations of state available today. Most of those are formulated in theHelmholtz free energy
In thermodynamics, the Helmholtz free energy (or Helmholtz energy) is a thermodynamic potential that measures the useful work (thermodynamics), work obtainable from a closed system, closed thermodynamic system at a constant temperature (Isotherma ...

as a function of temperature, density (and for mixtures additionally the composition). The Helmholtz energy is formulated as a sum of multiple terms modelling different types of molecular interaction or molecular structures, e.g. the formation of chains or dipolar interactions. Hence, physically-based equations of state model the effect of molecular size, attraction and shape as well as hydrogen bonding and polar interactions of fluids. In general, physically-based equations of state give more accurate results than traditional cubic equations of state, especially for systems containing liquids or solids. Most physically-based equations of state are built on monomer term describing the Lennard-Jones fluid or the Mie fluid.
Perturbation theory-based models

Perturbation theory
In mathematics and applied mathematics, perturbation theory comprises methods for finding an approximation theory, approximate solution to a problem, by starting from the exact solution (equation), solution of a related, simpler problem. A crit ...

is frequently used for modelling dispersive interactions in an equation of state. There is a large number of perturbation theory based equations of state available today, e.g. for the classical Lennard-Jones fluid. The two most important theories used for these types of equations of state are the Barker-Henderson perturbation theory and the Weeks–Chandler–Andersen perturbation theory.
Statistical associating fluid theory (SAFT)

An important contribution for physically-based equations of state is the statistical associating fluid theory (SAFT) that contributes the Helmholtz energy that describes the association (a.k.a. hydrogen bonding) in fluids, which can also be applied for modelling chain formation (in the limit of infinite association strength). The SAFT equation of state was developed using statistical mechanical methods (in particular theperturbation theory
In mathematics and applied mathematics, perturbation theory comprises methods for finding an approximation theory, approximate solution to a problem, by starting from the exact solution (equation), solution of a related, simpler problem. A crit ...

of Wertheim) to describe the interactions between molecules in a system. The idea of a SAFT equation of state was first proposed by Chapman et al. in 1988 and 1989. Many different versions of the SAFT models have been proposed, but all use the same chain and association terms derived by Chapman et al.
Multiparameter equations of state

Multiparameter equations of state are empirical equations of state that can be used to represent pure fluids with high accuracy. Multiparameter equations of state are empirical correlations of experimental data and are usually formulated in the Helmholtz free energy. The functional form of these models is in most parts not physically motivated. They can be usually applied in both liquid and gaseous states. Empirical multiparameter equations of state represent the Helmholtz energy of the fluid as the sum of ideal gas and residual terms. Both terms are explicit in temperature and density: $$\backslash frac\; =\; \backslash frac$$ with $$\backslash tau\; =\; \backslash frac,\; \backslash delta\; =\; \backslash frac$$ The reduced density $\backslash rho\_r$ and reduced temperature $T\_r$ are in most cases the critical values for the pure fluid. Because integration of the multiparameter equations of state is not required and thermodynamic properties can be determined using classical thermodynamic relations, there are few restrictions as to the functional form of the ideal or residual terms. Typical multiparameter equations of state use upwards of 50 fluid specific parameters, but are able to represent the fluid's properties with high accuracy. Multiparameter equations of state are available currently for about 50 of the most common industrial fluids including refrigerants. The IAPWS95 reference equation of state for water is also a multiparameter equations of state. Mixture models for multiparameter equations of state exist, as well. Yet, multiparameter equations of state applied to mixtures are known to exhibit artifacts at times. One example of such an equation of state is the form proposed by Span and Wagner. $$a^\backslash mathrm\; =\; \backslash sum\_^8\; \backslash sum\_^\; n\_\; \backslash delta^i\; \backslash tau^\; +\; \backslash sum\_^5\; \backslash sum\_^\; n\_\; \backslash delta^i\; \backslash tau^\; \backslash exp\; \backslash left(\; -\backslash delta\; \backslash right)\; +\; \backslash sum\_^5\; \backslash sum\_^\; n\_\; \backslash delta^i\; \backslash tau^\; \backslash exp\; \backslash left(\; -\backslash delta^2\; \backslash right)\; +\; \backslash sum\_^4\; \backslash sum\_^\; n\_\; \backslash delta^i\; \backslash tau^\; \backslash exp\; \backslash left(\; -\backslash delta^3\; \backslash right)$$ This is a somewhat simpler form that is intended to be used more in technical applications. Equations of state that require a higher accuracy use a more complicated form with more terms.List of further equations of state

Stiffened equation of state

When considering water under very high pressures, in situations such as underwater nuclear explosions, sonic shock lithotripsy, and sonoluminescence, the stiffened equation of state is often used: $$p\; =\; \backslash rho(\backslash gamma\; -\; 1)e\; -\; \backslash gamma\; p^0\; \backslash ,$$ where $e$ is the internal energy per unit mass, $\backslash gamma$ is an empirically determined constant typically taken to be about 6.1, and $p^0$ is another constant, representing the molecular attraction between water molecules. The magnitude of the correction is about 2 gigapascals (20,000 atmospheres). The equation is stated in this form because the speed of sound in water is given by $c^2\; =\; \backslash gamma\backslash left(p\; +\; p^0\backslash right)/\backslash rho$. Thus water behaves as though it is an ideal gas that is ''already'' under about 20,000 atmospheres (2 GPa) pressure, and explains why water is commonly assumed to be incompressible: when the external pressure changes from 1 atmosphere to 2 atmospheres (100 kPa to 200 kPa), the water behaves as an ideal gas would when changing from 20,001 to 20,002 atmospheres (2000.1 MPa to 2000.2 MPa). This equation mispredicts thespecific heat capacity
In thermodynamics, the specific heat capacity (symbol ) of a substance is the heat capacity of a sample of the substance divided by the mass of the sample, also sometimes referred to as massic heat capacity. Informally, it is the amount of heat t ...

of water but few simple alternatives are available for severely nonisentropic processes such as strong shocks.
Ultrarelativistic equation of state

An ultrarelativistic fluid has equation of state $$p\; =\; \backslash rho\_m\; c\_s^2$$ where $p$ is the pressure, $\backslash rho\_m$ is the mass density, and $c\_s$ is thespeed of sound
The speed of sound is the distance travelled per unit of time by a sound wave as it propagates through an elasticity (solid mechanics), elastic medium. At , the speed of sound in air is about , or one kilometre in or one mile in . It depends ...

.
Ideal Bose equation of state

The equation of state for an ideal Bose gas is $$p\; V\_m\; =\; RT~\backslash frac\; \backslash left(\backslash frac\backslash right)^\backslash alpha$$ where ''α'' is an exponent specific to the system (e.g. in the absence of a potential field, α = 3/2), ''z'' is exp(''μ''/''k''Jones–Wilkins–Lee equation of state for explosives (JWL equation)

The equation of state from Jones–Wilkins–Lee is used to describe the detonation products of explosives. $$p\; =\; A\; \backslash left(\; 1\; -\; \backslash frac\; \backslash right)\; \backslash exp(-R\_1\; V)\; +\; B\; \backslash left(\; 1\; -\; \backslash frac\; \backslash right)\; \backslash exp\backslash left(-R\_2\; V\backslash right)\; +\; \backslash frac$$ The ratio $V\; =\; \backslash rho\_e\; /\; \backslash rho$ is defined by using $\backslash rho\_e$, which is the density of the explosive (solid part) and $\backslash rho$, which is the density of the detonation products. The parameters $A$, $B$, $R\_1$, $R\_2$ and $\backslash omega$ are given by several references. In addition, the initial density (solid part) $\backslash rho\_0$, speed of detonation $V\_D$, Chapman–Jouguet pressure $P\_$ and the chemical energy of the explosive $e\_0$ are given in such references. These parameters are obtained by fitting the JWL-EOS to experimental results. Typical parameters for some explosives are listed in the table below.Others

* Tait equation for water and other liquids. Several equations are referred to as the Tait equation. * Murnaghan equation of state * Birch–Murnaghan equation of state * Stacey–Brennan–Irvine equation of state * Modified Rydberg equation of state * Adapted polynomial equation of state * Johnson–Holmquist equation of state * Mie–Grüneisen equation of stateS. Benjelloun, "Thermodynamic identities and thermodynamic consistency of Equation of States"Link to Archiv e-print

/ref> * Anton-Schmidt equation of state

See also

* Gas laws * Departure function * Table of thermodynamic equations * Real gas * Cluster expansionReferences

External links

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