![]() | ||
In thermodynamics, the Onsager reciprocal relations express the equality of certain ratios between flows and forces in thermodynamic systems out of equilibrium, but where a notion of local equilibrium exists.
Contents
- The fundamental equation
- The continuity equations
- The phenomenological equations
- The rate of entropy production
- The Onsager reciprocal relations
- Abstract formulation
- Proof
- References
"Reciprocal relations" occur between different pairs of forces and flows in a variety of physical systems. For example, consider fluid systems described in terms of temperature, matter density, and pressure. In this class of systems, it is known that temperature differences lead to heat flows from the warmer to the colder parts of the system; similarly, pressure differences will lead to matter flow from high-pressure to low-pressure regions. What is remarkable is the observation that, when both pressure and temperature vary, temperature differences at constant pressure can cause matter flow (as in convection) and pressure differences at constant temperature can cause heat flow. Perhaps surprisingly, the heat flow per unit of pressure difference and the density (matter) flow per unit of temperature difference are equal. This equality was shown to be necessary by Lars Onsager using statistical mechanics as a consequence of the time reversibility of microscopic dynamics (microscopic reversibility). The theory developed by Onsager is much more general than this example and capable of treating more than two thermodynamic forces at once, with the limitation that "the principle of dynamical reversibility does not apply when (external) magnetic fields or Coriolis forces are present", in which case "the reciprocal relations break down".
Though the fluid system is perhaps described most intuitively, the high precision of electrical measurements makes experimental realisations of Onsager's reciprocity easier in systems involving electrical phenomena. In fact, Onsager's 1931 paper refers to thermoelectricity and transport phenomena in electrolytes as well-known from the 19th century, including "quasi-thermodynamic" theories by Thomson and Helmholtz respectively. Onsager's reciprocity in the thermoelectric effect manifests itself in the equality of the Peltier (heat flow caused by a voltage difference) and Seebeck (electrical current caused by a temperature difference) coefficients of a thermoelectric material. Similarly, the so-called "direct piezoelectric" (electrical current produced by mechanical stress) and "reverse piezoelectric" (deformation produced by a voltage difference) coefficients are equal. For many kinetic systems, like the Boltzmann equation or chemical kinetics, the Onsager relations are closely connected to the principle of detailed balance and follow from them in the linear approximation near equilibrium.
Experimental verifications of the Onsager reciprocal relations were collected and analyzed by D. G. Miller for many classes of irreversible processes, namely for thermoelectricity, electrokinetics, transference in electrolytic solutions, diffusion, conduction of heat and electricity in anisotropic solids, thermomagnetism and galvanomagnetism. In this classical review, chemical reactions are considered as "cases with meager" and inconclusive evidence. Further theoretical analysis and experiments support the reciprocal relations for chemical kinetics with transport.
For his discovery of these reciprocal relations, Lars Onsager was awarded the 1968 Nobel Prize in Chemistry. The presentation speech referred to the three laws of thermodynamics and then added "It can be said that Onsager's reciprocal relations represent a further law making a thermodynamic study of irreversible processes possible." Some authors have even described Onsager's relations as the "Fourth law of thermodynamics".
The fundamental equation
The basic thermodynamic potential is internal energy. In a simple fluid system, neglecting the effects of viscosity the fundamental thermodynamic equation is written:
where U is the internal energy, T is temperature, S is entropy, P is the hydrostatic pressure, V is the volume,
For non-fluid or more complex systems there will be a different collection of variables describing the work term, but the principle is the same. The above equation may be solved for the entropy density:
The above expression of the first law in terms of entropy change defines the entropic conjugate variables of
The continuity equations
The conservation of mass is expressed locally by the fact that the flow of mass density
where
where
Since we are interested in a general imperfect fluid, entropy is locally not conserved and its local evolution can be given in the form of entropy density
where
The phenomenological equations
In the absence of matter flows, Fourier's law is usually written:
where k is the thermal conductivity. However, this law is just a linear approximation, and holds only for the case where
In the absence of heat flows, Fick's law of diffusion is usually written:
where D is the coefficient of diffusion. Since this is also a linear approximation and since the chemical potential is monotonically increasing with density at a fixed temperature, Fick's law may just as well be written:
where, again, D' is a function of thermodynamic state parameters, but not their gradients or time rate of change. For the general case in which there are both mass and energy fluxes, the phenomenological equations may be written as:
or, more concisely,
where the entropic "thermodynamic forces" conjugate to the "displacements"
The rate of entropy production
From the fundamental equation, it follows that:
and
Using the continuity equations, the rate of entropy production may now be written:
and, incorporating the phenomenological equations:
It can be seen that, since the entropy production must be greater than zero, the Onsager matrix of phenomenological coefficients
The Onsager reciprocal relations
Onsager's contribution was to demonstrate that not only is
The rate of entropy production for the above simple example uses only two entropic forces, and a 2x2 Onsager phenomenological matrix. The expression for the linear approximation to the fluxes and the rate of entropy production can very often be expressed in an analogous way for many more general and complicated systems.
Abstract formulation
Let
where we are using Einstein summation convention and
Using the quasi-stationary equilibrium approximation, that is, assuming that the system is only slightly non-equilibrium, we have
Suppose we define thermodynamic conjugate quantities as
Thus, we can write
The principle of symmetry of kinetic coefficients or the Onsager's principle states that
Proof
Define mean values
Symmetry of fluctuations under time reversal implies that
or, with
Differentiating with respect to
Putting
It can be easily shown from the definition that