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:

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:

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:

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:

v → a ⋅ n → = v → i ⋅ n → MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbwvMCKf MBHbqefqvATv2CG4uz3bIuV1wyUbqedmvETj2BSbqefm0B1jxALjhi ov2DaebbnrfifHhDYfgasaacH8srps0lbbf9q8WrFfeuY=Hhbbf9v8 qqaqFr0xc9pk0xbba9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9 q8qqQ8frFve9Fve9Ff0dmeaacaGacmGadaWaaiqacaabaiaafaaake aaceWG2bGbaSaadaWgaaWcbaGaamyyaaqabaGccqGHflY1ceWGUbGb aSaacqGH9aqpceWG2bGbaSaadaWgaaWcbaGaamyAaaqabaGccqGHfl Y1ceWGUbGbaSaaaaa@44D5@