Introduction xi
Mhamed SOULI
Chapter 1. Introduction to ArbitraryLagrangian-Eulerian in Finite Element Methods 1
David J. BENSON
1.1. Introduction 1
1.2. Governing equations 3
1.3. Operator splitting 4
1.4. The Lagrangian step 7
1.5. Mesh relaxation 25
1.6. The Eulerian step 27
1.7. Future research directions 44
1.8. Bibliography 45
Application to Dynamic Problems 51
Mhamed SOULI
2.1. Introduction 51
2.2. General ALE description of Navier-Stokes equations54
2.3. Fluid-structure interaction 57
2.4. Numerical applications 72
Chapter 2. Fluid-Structure Interaction: Application toDynamic Problems 51
Mhamed SOULI
2.5. Conclusion 104
2.6. Acknowledgments 104
2.7. Bibliography 105
Chapter 3. Implicit Partitioned Coupling inFluid-Structure Interaction 109
Michael SCHÄFER
3.1. Introduction 109
3.2. Computational fluid mechanics 110
3.3. Computational structural mechanics 121
3.4. Fluid-structure interaction algorithms 136
3.5. Results and applications 150
3.6. Bibliography 161
Chapter 4. Avoiding Instabilities Caused by Added MassEffects in Fluid-Structure Interaction Problems165
Sergio IDELSOHN, Facundo DEL PIN and Riccardo ROSSI
4.1. Introduction 165
4.2. The discretized equations to be solved in a FSI problem169
4.3. Monolithic solution of the FSI equations by pressuresegregation 174
4.4. Static condensation of the pressure 176
4.5. Evaluation of the Laplace matrix for FSI problems 187
4.6. The partitioned (or staggered) scheme 189
4.7. Numerical examples 195
4.8. Conclusions 215
4.9. Acknowledgments 216
4.10. Bibliography 216
Chapter 5. Multidomain Finite Element Computations:Application to Multiphasic Problems 221
Thierry COUPEZ, Hugues DIGONNET, Elie HACHEM, Patrice LAURE, LuisaSILVA, Rudy VALETTE
5.1. Introduction 221
5.2. Characterization of different phases 228
5.3. Stabilized finite element formulations 240
5.4. Multiphasic problems with fluid-air andfluid-fluid interface 256
5.5. Immersion of solid bodies in fluid 264
5.6. Conclusion 281
5.7. Acknowledgements 282
5.8. Bibliography 282
List of Authors 291
Index 293
