The
joint density functional theory (JDFT) is applied in the context
of the grand canonical Kohn–Sham theory to calculate the global
and local softness of pristine and N-substituted graphene structures.
A comparison is established between the different theoretical approaches
to evaluate total capacitance, revealing that the JDFT approach presents
the closest result of this property with experimental data. A model
of series capacitors is used to determine the quantum and nonquantum
contributions of total capacitance, which enables us to determine
the limitations of the rigid band approximation for the studied systems.
It is found that global chemical softness is proportional to the total
capacitance measured in the experiments, when the geometry relaxation
is neglected. In this context, it is possible to obtain quantum and
total capacitance (and consequently softness) from an average number
of electrons vs applied potential plots and the model of series capacitors.
Likewise, the relation of capacitance and softness gives rise to a
new definition of local capacitance within the JDFT formalism. The
evaluation of global and local softness paves the way to analyze electrochemical
surface reactivity as a function of applied potential for a solid-electrolyte
interface.