Galvani potential

In electrochemistry, the Galvani potential (also called Galvani potential difference, or inner potential difference, Δφ, delta phi) is the electric potential difference between two points in the bulk of two phases. These phases can be two different solids (e.g., two metals joined together), or a solid and a liquid (e.g., a metal electrode submerged in an electrolyte). The Galvani potential is named after Luigi Galvani. First, consider the Galvani potential between two metals. When two metals are electrically isolated from each other, an arbitrary voltage difference may exist between them. However, when two different metals are brought into electronic contact, electrons will flow from the metal with a lower voltage to the metal with the higher voltage until the Fermi level of the electrons in the bulk of both phases are equal. The actual numbers of electrons that passes between the two phases is small (it depends on the capacitance between the objects), and the occupancies of the electron bands are practically unaffected. Rather, this small increase or decrease in charge results in a shift in all the energy levels in the metals. An electrical double layer is formed at the interface between the two phases. The equality of the electrochemical potential between the two different phases in contact can be written as: where: is the electrochemical potential j denotes the species which are the carrier of electric current in the system (which are electrons in metals) (1) and (2) denote phase 1 and phase 2, respectively. Now, the electrochemical potential of a species is defined as a sum of its chemical potential and the local electrostatic potential: where: μ is the chemical potential z is the electrical charge carried by a single charge carrier (unity for electrons) F is the Faraday constant Φ is the electrostatic potential From the two equations above: where the difference on the left-hand side is the Galvani potential difference between the phases (1) and (2).