Slip conditions
DESCRIPTION
Three different slipping law can be selected :
where vs is the tangential velocity
of the fluid
vwall is the tangential velocity of the wall
fslip and exslip are materials properties
Note : full slip is obtained for fslip = 0
the law is linear when exslip = 0, corresponds to a power law when exslip
< 0
- fslip ( vs - vwall )
vs - vwall < yc / fslip
fs =
- yc - fslip2 ( vs - vwall - (yc/fslip) )
vs - vwall >= yc / fslip
where fslip and fslip2 are two different slip coefficients.
The Asymptotic law :
fs = -fslip [ 1 - exp( (vs - vwall )
/ vc ) ]
fs = F(v) * H(T)
where F(v) is one of the 3 laws described here above
H(T) can be the Arrhenius law or Arrhenius approximate law.
H(T) = exp ( alpha/(T-T0) - alpha/(Talpha - T0) )
where alpha is the energy of activation
Talpha is the reference temperature at which H(T) = 1
T0 is the temperature offset, T0 = 0 by default
Arrhenius approximate law :
H(T) = exp ( - alpha/(T - Talpha) )
| -2 | Define constraints on wall normals |
| Allows for specifying the wall normals that will be used for the calculation of normal tangential components. | |
| -1 | Upper level menu |
| Accepts the current setup | |
| 0 | Define v_wall, the velocity of the wall |
| Allows for specifying the magnitude of the tangential velocity of the wall | |
| 1 | F(v) = Generalized Navier's law |
| Switches to Generalized Navier's slipping law | |
| 2 | F(v) = Threshold law |
| Switches to Threshold slipping law | |
| 3 | F(v) = Asymptotic law |
| Switches to Asymptotic slipping law | |
| 4 | H(T) = 1 (temperature independent) |
| for non-isothermal flows, switches to temperature independent law | |
| 5 | H(T) = Arrhenius approximate law |
| for non-isothermal flows, switches to Arrhenius approximate law | |
| 6 | H(T) = Arrhenius law |
| for non-isothermal flows, switches to Arrhenius law |
NOTES
For many non-linear
flow problems, it is interesting to increase the slip coefficient from
a low to its nominal value.
This can be done by
means of an evolution scheme. The current task should then be of the evolution
type.
When the boundary set
on which the slip condition is applied presents large discontinuities of
the normal direction, the user should split it up into smaller parts in
order to avoid 'leakages' around the corners. These leakages are due to
the single normal and tangent defined at the corner; this mean tangent
is not really tangent to the flow domain boundary and some fluid goes out
of the flow region.