Butler-Volmer Current-Potential Characteristic

The Butler-Volmer equation is typically used in electrochemistry applications to model the relationship between the electric current and the electric potential at an electrode, where cathodic and anodic reactions occur.

At a boundary, or interface, the over-potential η is defined as:

Figure 1. EQUATION_DISPLAY
η=ϕ1-ϕ0-ϕEJnR
(4295)

where R is a user-defined electrical resistance and Jn is the specific electric current (see Eqn. (4283)). For an interface, ϕ0 and ϕ1 denote the potential at boundary 0 and boundary 1 of the interface, respectively. For a boundary, ϕ0 denotes the potential solution computed at the boundary, whereas ϕ1 denotes the potential prescribed at the boundary. ϕE denotes the zero electric current potential.

The Butler-Volmer equation defines the relationship between the specific electric current Jn and the over-potential η , as:

Figure 2. EQUATION_DISPLAY
Jn(η)=j0(eαaFη/(RuT)-e-αcFη/(RuT))
(4296)

where:

  • α a is the anodic apparent transfer coefficient
  • α c is the cathodic apparent transfer coefficient
  • j0 is the specific electric exchange current
  • F=9.648525879×107C kmol-1 is the Faraday constant
  • Ru=8.3144621×103J kmol-1K-1 is the universal gas constant

When Simcenter STAR-CCM+ solves the energy equation (Eqn. (658)), the temperature T is automatically computed. Otherwise, Simcenter STAR-CCM+ applies a default temperature of T=293K . Large variations of temperature between two sides of an interface should be avoided.

For an over-potential η = 0 , the specific current prescribed by Eqn. (4296) is Jn=0 .