A key theorem in non-equilibrium thermodynamics, these relations express the equality of certain cross-coefficients between coupled flows of energy and matter. They state that in the absence of a magnetic field, the matrix of transport coefficients is symmetric: [latex]L_{\alpha\beta} = L_{\beta\alpha}[/latex]. This links seemingly unrelated transport phenomena, such as the Seebeck Und Peltier effects in thermoelectricity.
