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Mathematical Models for Nano Science - Politecnico di Milano

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Model equations - 3<br />

• Poisson<br />

equation<br />

⎧ ( )<br />

−<strong>di</strong>v ε∇ϕ = −qn in Ω n<br />

( )<br />

−<strong>di</strong>v ε∇ϕ = +q ( p − n ) in Ω ⎪⎨<br />

H<br />

( )<br />

−<strong>di</strong>v ε∇ϕ = +qp in Ω p<br />

ϕ = V appl − V bi<br />

⎪⎩<br />

ϕ = 0<br />

on Γ A<br />

on Γ C<br />

• Applied and bias potential → Dirichlet boundary con<strong>di</strong>tions<br />

• The <strong>di</strong>electric constant ε may vary in the materials<br />

• The electric potential ϕ and the normal component of the<br />

electric <strong>di</strong>splacement field −ε∇ϕ · ν are continuous

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