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The ideal gas law is the equation of state for an ideal gas, given by: = where P is the pressure; V is the volume; n is the amount of substance of the gas (in moles) T is the absolute temperature; R is the gas constant, which must be expressed in units consistent with those chosen for pressure, volume and temperature.
A physical situation where the chemical potential for photons can differ from zero are material-filled optical microcavities, with spacings between cavity mirrors in the wavelength regime. In such two-dimensional cases, photon gases with tuneable chemical potential, much reminiscent to gases of material particles, can be observed. [22]
Isotherms of an ideal gas for different temperatures. The curved lines are rectangular hyperbolae of the form y = a/x. They represent the relationship between pressure (on the vertical axis) and volume (on the horizontal axis) for an ideal gas at different temperatures: lines that are farther away from the origin (that is, lines that are nearer to the top right-hand corner of the diagram ...
Chemical potential (of component i in a mixture) ... Ideal gas equations Physical situation Nomenclature Equations Ideal gas law: p = pressure; V = volume of container;
The equation of state is the ideal gas law ... For a single component system, the chemical potential equals the Gibbs energy per amount of substance, ...
The relative activity of a species i, denoted a i, is defined [4] [5] as: = where μ i is the (molar) chemical potential of the species i under the conditions of interest, μ o i is the (molar) chemical potential of that species under some defined set of standard conditions, R is the gas constant, T is the thermodynamic temperature and e is the exponential constant.
Equation of state; Ideal gas; Real gas; State of matter; Phase (matter) Equilibrium; Control volume; Instruments; ... where μ is the chemical potential. In addition ...
For an ideal gas the equation of state can be written as =, where R is the ideal gas constant.The differential change of the chemical potential between two states of slightly different pressures but equal temperature (i.e., dT = 0) is given by = = = , where ln p is the natural logarithm of p.