Description🔗
The electrostaticDeposition
is a boundary condition to
calculate electric potential (V
) on a given boundary
based on film thickness (h
) and film resistance (R
) fields
which are updated based on a given patch-normal current density
field (jn
), Coulombic efficiency and film resistivity.
Usage🔗
The condition requires entries in both the boundary
and field files.
Boundary file🔗
<patchName>
{
type patch;
...
}
Field file🔗
<patchName>
{
// Mandatory entries
type electrostaticDeposition;
h <scalarField>;
CoulombicEfficiency <PatchFunction1>;
resistivity <PatchFunction1>;
// Conditional mandatory entries
// Option-1: single-phase
sigma <scalar>;
// Option-2: multiphase
phases
{
alpha.air
{
sigma <scalar>;
}
alpha.water
{
sigma <scalar>;
}
alpha.mercury
{
sigma <scalar>;
}
...
}
// Optional entries
jMin <scalar>;
qMin <scalar>;
Rbody <scalar>;
Vi <scalar>;
Vanode <scalar>;
qCumulative <scalarField>;
// Inherited entries
...
}
where:
Property | Description | Type | Required | Default |
---|---|---|---|---|
type |
Type name: electrostaticDeposition
|
word | yes | - |
h |
Film thickness | scalarField | yes | - |
CoulombicEfficiency |
Coulombic efficiency | PatchFunction1<scalar> | yes | - |
resistivity |
Isotropic film resistivity | PatchFunction1<scalar> | yes | - |
sigma |
Isotropic electrical conductivity of phase | scalar | yes | - |
jMin |
Minimum current density for deposition onset | scalar | no | 0 |
qMin |
Minimum accumulative specific charge for deposition onset | scalar | no | 0 |
Rbody |
Resistance due to main body and/or pretreatment layers | scalar | no | 0 |
Vi |
Initial electric potential | scalar | no | 0 |
Vanode |
Anode electric potential | scalar | no | GREAT |
qCumulative |
Accumulative specific charge [A s/m^2] | scalarField | no | 0 |
The inherited entries are elaborated in:
- fixedValueFvPatchFields.H
-
PatchFunction1.H
- Depletion or abrasion of material due to negative current is not allowed.
- When accumulative specific charge (
qCumulative
) is less than minimum accumulative specific charge (qMin
), no deposition occurs. - Boundary-condition updates are not allowed during outer corrections to prevent spurious accumulation of film thickness.
-
resistivity
,jMin
,qMin
andRbody
are always non-negative.
Method🔗
\[j_n = - \sigma \nabla^\perp_p V = - \sigma (\vec{n}\cdot(\nabla V)_p)\] \[\frac{dh}{dt} = C_{eff} (j_n - j_{min})\] \[\frac{dR}{dt} = \rho \frac{dh}{dt} = \rho C_{eff} (j_n - j_{min})\] \[V_{film}^n = V_{film}^o + j_n R_\Delta\] \[V_{body} = j_n R_{body}\] \[V_p^n = V_i + V_{body} + V_{film}^n\]where:
Property | Description |
---|---|
\(j_n\) | Patch-normal current density [A/m^2] |
\(V_p^n\) | Electric potential on film-fluid interface [volt = kg m^2/(A s^3)] |
\(V_p^o\) | Previous time-step electric potential on the interface [volt] |
\(V_{film}\) | Electric potential due to film resistance [volt] |
\(V_{body}\) | Electric potential due to body resistance [volt] |
\(V_i\) | Initial electric potential [volt] |
\(R_\Delta\) | Film resistance (finite increment) [ohm m^2 = kg m^4/(A^2 s^3)] |
\(R_{body}\) | Body resistance [ohm m^2 = kg m^4/(A^2 s^3)] |
\(\rho\) | Isotropic film resistivity [ohm m = kg m^3/(A^2 s^3)] |
\(h\) | Film thickness [m] |
\(C_{eff}\) | Volumetric Coulombic efficiency [m^3/(A s)] |
\(j_{min}\) | Minimum current density for deposition onset [A/m^2] |
\(\sigma\) | Isotropic conductivity of mixture [S/m = A^2 s^3/(kg m^3)] |
\(\vec{n}\) | Patch-normal unit vector [-] |
Further information🔗
Tutorial:
Source code:
API:
History:
- Introduced in version v2112