TYPE1 interface is used to model fluid-structure interactions, as shown in
図 1 .
図 1 . Fluid-Structure Interaction
This interface allows Lagrangian elements (structure) to interact with ALE (Arbitrary
Lagrangian Eulerian) elements, which model a viscous fluid. Full slip conditions are
applied at the boundary between the two domains.
The acceleration of the Lagrange node is computed by:
図 2 .
γ
→
i
=
F
→
i
+
F
→
a
m
+
i
m
a
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbwvMCKf
MBHbqefqvATv2CG4uz3bIuV1wyUbqedmvETj2BSbqefm0B1jxALjhi
ov2DaebbnrfifHhDYfgasaacH8srps0lbbf9q8WrFfeuY=Hhbbf9v8
qqaqFr0xc9pk0xbba9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9
q8qqQ8frFve9Fve9Ff0dmeaacaGacmGadaWaaiqacaabaiaafaaake
aacuaHZoWzgaWcamaaBaaaleaacaWGPbaabeaakiabg2da9maalaaa
baGabmOrayaalaWaaSbaaSqaaiaadMgaaeqaaOGaey4kaSIabmOray
aalaWaaSraaSqaaiaadggaaeqaaaGcbaGaamyBamaaBeaaleaacaWG
PbaabeaakiabgUcaRiaaykW7caWGTbWaaSbaaSqaaiaadggaaeqaaa
aaaaa@482F@
The acceleration of the ALE node is computed by:
図 3 .
γ
→
a
=
F
→
a
m
a
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbwvMCKf
MBHbqefqvATv2CG4uz3bIuV1wyUbqedmvETj2BSbqefm0B1jxALjhi
ov2DaebbnrfifHhDYfgasaacH8srps0lbbf9q8WrFfeuY=Hhbbf9v8
qqaqFr0xc9pk0xbba9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9
q8qqQ8frFve9Fve9Ff0dmeaacaGacmGadaWaaiqacaabaiaafaaake
aacuaHZoWzgaWcamaaBaaaleaacaWGHbaabeaakiabg2da9maalaaa
baGabmOrayaalaWaaSraaSqaaiaadggaaeqaaaGcbaGaamyBamaaBa
aaleaacaWGHbaabeaaaaaaaa@40C0@
The grid velocity of the ALE node is equal to the material velocity of the Lagrange
node:
図 4 .
w
→
a
=
v
→
i
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbwvMCKf
MBHbqefqvATv2CG4uz3bIuV1wyUbqedmvETj2BSbqefm0B1jxALjhi
ov2DaebbnrfifHhDYfgasaacH8srps0lbbf9q8WrFfeuY=Hhbbf9v8
qqaqFr0xc9pk0xbba9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9
q8qqQ8frFve9Fve9Ff0dmeaacaGacmGadaWaaiqacaabaiaafaaake
aaceWG3bGbaSaadaWgaaWcbaGaamyyaaqabaGccqGH9aqpceWG2bGb
aSaadaWgaaWcbaGaamyAaaqabaaaaa@3E2E@
The normal material velocities of Lagrange and ALE nodes are equal.
Therefore:
図 5 .
v
→
a
⋅
n
→
=
v
→
i
⋅
n
→
MathType@MTEF@5@5@+=
feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbwvMCKf
MBHbqefqvATv2CG4uz3bIuV1wyUbqedmvETj2BSbqefm0B1jxALjhi
ov2DaebbnrfifHhDYfgasaacH8srps0lbbf9q8WrFfeuY=Hhbbf9v8
qqaqFr0xc9pk0xbba9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9
q8qqQ8frFve9Fve9Ff0dmeaacaGacmGadaWaaiqacaabaiaafaaake
aaceWG2bGbaSaadaWgaaWcbaGaamyyaaqabaGccqGHflY1ceWGUbGb
aSaacqGH9aqpceWG2bGbaSaadaWgaaWcbaGaamyAaaqabaGccqGHfl
Y1ceWGUbGbaSaaaaa@44D5@