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David Saintillan

From Wikipedia, the free encyclopedia
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David Saintillan
EducationÉcole Polytechnique
Stanford University
Known forSaintillan–Shelley model
AwardsPi Tau Sigma Gold Medal (2011)
Fellow of the American Physical Society (2018)
Scientific career
FieldsFluid dynamics, soft matter
WorkplacesUniversity of California, San Diego
University of Illinois Urbana-Champaign
Courant Institute of Mathematical Sciences
Eric Shaqfeh
Eric Darve

David Saintillan is an applied mathematician and mechanical engineer whose research is in fluid dynamics and soft matter. He is a professor of mechanical and aerospace engineering at the University of California, San Diego. With Michael J. Shelley, he developed a kinetic theory of active suspensions that subsequently became known as the Saintillan–Shelley model, or Doi–Saintillan–Shelley model. Saintillan was elected a Fellow of the American Physical Society in 2018.

Early life and education

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Saintillan was educated at the École Polytechnique in France, where he obtained an engineering degree in 2001. He then studied mechanical engineering at Stanford University, receiving an M.S. in 2003 and a Ph.D. in 2006.[1] His doctoral research, supervised by Eric Shaqfeh and Eric Darve, received the 2007 Andreas Acrivos Dissertation Award in Fluid Dynamics from the American Physical Society.[2]

Following his Ph.D., Saintillan worked as a research scientist at the Courant Institute of Mathematical Sciences at New York University.[1]

Academic career

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Saintillan joined the faculty at the University of Illinois Urbana-Champaign in 2008 as an assistant professor of mechanical science and engineering.[1] He moved to the University of California, San Diego in 2013, joining the Department of Mechanical and Aerospace Engineering, where he later became a full professor.[1]

Research

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Saintillan's research is in fluid mechanics and soft matter, with an emphasis on dynamics and transport phenomena in complex and biological fluids at small scales. His work has included theoretical and computational studies of active matter and the dynamics of flexible filaments and polymers in viscous flows.[1]

Active suspensions

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Saintillan's early research included work on the collective dynamics of active suspensions, such as suspensions of swimming microorganisms. With Michael J. Shelley, he developed a kinetic theory modeling the coupled dynamics of self-propelled particles and the surrounding fluid. The theory predicted hydrodynamic instabilities in uniformly aligned and isotropic suspensions that can give rise to collective motion and large-scale coherent flows.[3][4]

The kinetic framework developed in this work later became known in the literature as the Saintillan–Shelley model, or more generally the Doi–Saintillan–Shelley model.[5][6][7] The model was subsequently used and extended by independent researchers in the field to study stability, pattern formation, and mathematical properties of active suspensions.[6][8]

Saintillan has also studied the rheology of active fluids, explaining how stresses generated by microorganisms can alter the effective viscosity and transport properties of a suspension.[9]

Flexible filaments

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Saintillan has also studied the dynamics of elastic filaments in viscous fluids. This work has examined how competition between viscous forces and elastic resistance can produce buckling and other morphological transitions. Studies of sedimenting filaments and filaments in straining flow have characterized the onset of elastohydrodynamic buckling and the resulting nonlinear dynamics.[10][11]

In later work combining numerical modeling with microfluidic experiments on actin filaments, Saintillan and collaborators studied morphological transitions of flexible filaments in shear and compressional flows. In shear flow, they identified transitions from tumbling to buckling and to strongly deformed states characterized by localized high-curvature bends propagating along the filament.[12]

Saintillan and collaborators showed that strong compressional flows can cause initially straight, achiral filaments to buckle into three-dimensional helicoidal shapes. The transition arises from the nonlinear interaction of perpendicular planar buckling modes and does not require intrinsic chirality or applied twisting moments.[13]

Honors and awards

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References

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  1. 1 2 3 4 5 "David Saintillan". Jacobs School of Engineering. University of California, San Diego. Retrieved 10 September 2026.
  2. ↑ "2007 Andreas Acrivos Dissertation Award in Fluid Dynamics" (PDF). APS News. American Physical Society. November 2007. p. 5. Retrieved 10 September 2026.
  3. ↑ Saintillan, David; Shelley, Michael J. (2007). "Orientational order and instabilities in suspensions of self-locomoting rods". Physical Review Letters. 99 (5) 058102. Bibcode:2007PhRvL..99e8102S. doi:10.1103/PhysRevLett.99.058102. PMID 17930796.
  4. ↑ Saintillan, David; Shelley, Michael J. (2008). "Instabilities and pattern formation in active particle suspensions: Kinetic theory and continuum simulations". Physical Review Letters. 100 (17) 178103. Bibcode:2008PhRvL.100q8103S. doi:10.1103/PhysRevLett.100.178103. PMID 18518342.
  5. ↑ Chen, Xiuqing; Liu, Jian-Guo (2013). "Global weak entropy solution to Doi–Saintillan–Shelley model for active and passive rod-like and ellipsoidal particle suspensions". Journal of Differential Equations. 254 (7): 2764–2802. Bibcode:2013JDE...254.2764C. doi:10.1016/j.jde.2013.01.005.
  6. 1 2 Coti Zelati, Michele; Dietert, Helge; Gérard-Varet, David (2023). "Orientation Mixing in Active Suspensions". Annals of PDE. 9 (2): 20. doi:10.1007/s40818-023-00163-8.
  7. ↑ Fung, Lloyd; Caldag, Hakan Osman; Bees, Martin A. (2025). "Foundation and challenges in modelling dilute active suspensions". Philosophical Transactions of the Royal Society A. 383 (2304) 20240251. arXiv:2410.08220. Bibcode:2025RSPTA.38340251F. doi:10.1098/rsta.2024.0251. PMC 12423652. PMID 40931659.
  8. ↑ Gérard-Varet, David (2023). "Recent progress in the mathematical analysis of active suspensions". Journées équations aux dérivées partielles: 1–12. doi:10.5802/jedp.676.
  9. ↑ Saintillan, David (2018). "Rheology of Active Fluids". Annual Review of Fluid Mechanics. 50: 563–592. Bibcode:2018AnRFM..50..563S. doi:10.1146/annurev-fluid-010816-060049.
  10. ↑ Li, Lei; Manikantan, Harishankar; Saintillan, David; Spagnolie, Saverio E. (2013). "The sedimentation of flexible filaments". Journal of Fluid Mechanics. 735: 705–736. arXiv:1306.4692. Bibcode:2013JFM...735..705L. doi:10.1017/jfm.2013.512.
  11. ↑ Manikantan, Harishankar; Saintillan, David (2015). "Buckling transition of a semiflexible filament in extensional flow". Physical Review E. 92 (4) 041002. Bibcode:2015PhRvE..92d1002M. doi:10.1103/PhysRevE.92.041002. PMID 26565158.
  12. ↑ Liu, Yanan; Chakrabarti, Brato; Saintillan, David; Lindner, Anke; du Roure, Olivia (2018). "Morphological transitions of elastic filaments in shear flow". Proceedings of the National Academy of Sciences. 115 (38): 9438–9443. arXiv:1803.10979. Bibcode:2018PNAS..115.9438L. doi:10.1073/pnas.1805399115. PMC 6156685. PMID 30181295.
  13. ↑ Chakrabarti, Brato; Liu, Yanan; LaGrone, John; Cortez, Ricardo; Fauci, Lisa; du Roure, Olivia; Saintillan, David; Lindner, Anke (2020). "Flexible filaments buckle into helicoidal shapes in strong compressional flows". Nature Physics. 16 (6): 689–694. arXiv:1910.04558. Bibcode:2020NatPh..16..689C. doi:10.1038/s41567-020-0843-7.
  14. ↑ "Pi Tau Sigma Gold Medal". American Society of Mechanical Engineers. Retrieved 10 September 2026.
  15. ↑ "2018 American Physical Society Fellows Include Four UC San Diegans". UC San Diego Today. University of California, San Diego. 2018. Retrieved 10 September 2026.
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