{{#category_index:L|law of tangents}} Electrical current lines at a boundary are bent such that
where ρ 1 {\displaystyle \rho _{1}} , ρ 2 {\displaystyle \rho _{2}} are the resistivities of the two media and α 1 {\displaystyle \alpha _{1}} , α 2 {\displaystyle \alpha _{2}} are the angles that the current flow makes with a normal to the interface.