Fluid-Structure Interaction (TYPE 1 Interface)

TYPE1 interface is used to model fluid-structure interactions, as shown in Figure 1.


Figure 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:(1)
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:(2)
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:(3)
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:(4)
v a n = v i n MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbwvMCKf MBHbqefqvATv2CG4uz3bIuV1wyUbqedmvETj2BSbqefm0B1jxALjhi ov2DaebbnrfifHhDYfgasaacH8srps0lbbf9q8WrFfeuY=Hhbbf9v8 qqaqFr0xc9pk0xbba9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9 q8qqQ8frFve9Fve9Ff0dmeaacaGacmGadaWaaiqacaabaiaafaaake aaceWG2bGbaSaadaWgaaWcbaGaamyyaaqabaGccqGHflY1ceWGUbGb aSaacqGH9aqpceWG2bGbaSaadaWgaaWcbaGaamyAaaqabaGccqGHfl Y1ceWGUbGbaSaaaaa@44D5@