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Green function and singularities in Stokes flow confined by cylindrical walls

Giuseppe Procopio*

  • *Contact author: giuseppe.procopio@uniroma1.it

Phys. Rev. Fluids 11, 034201 – Published 13 March, 2026

DOI: https://doi.org/10.1103/jt65-63vb

Abstract

In this article, the Green function for the Stokes flow in the interior, exterior, and annular regions bounded by cylindrical walls is derived as a function of the pole position and expressed in an invariant form at both the field and pole points. Specifically, the Green function, assuming no-slip boundary conditions, is obtained using a cylindrical harmonic expansion of the Stokes flow within the bitensorial formulation introduced in Procopio and Giona [Math. Eng. 5, 1 (2022)]. This formulation allows us to obtain higher-order singularities within the same domains and under the same boundary conditions, such as the confined couplet and stresslet, by simply differentiating the Green function at its pole. Moreover, the confined sourcelet (or point source) and its associated multipoles are derived from the Green function through a new method that enforces the reciprocal properties of the Stokes flow. The resulting singularities are then employed to address hydrodynamic problems involving active and passive colloids interacting with cylindrical and planar walls, such as sedimenting particles in an annular cylindrical region and between two parallel plane walls, and the attractive or repulsive hydrodynamic forces exerted by cylindrical boundaries on microswimmers.

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References (87)

  1. J. Happel and H. Brenner, Low Reynolds Number Hydrodynamics: With Special Applications to Particulate Media (Martinus Nijhoff Publisher, The Hague, 1983).
  2. É. Guazzelli and J. F. Morris, A Physical Introduction to Suspension Dynamics (Cambridge University Press, Cambridge UK, 2012).
  3. A. Hochstetter, R. Vernekar, R. H. Austin, H. Becker, J. P. Beech, D. A. Fedosov, G. Gompper, S.-C. Kim, J. T. Smith, G. Stolovitzky, et al., Deterministic lateral displacement: Challenges and perspectives, ACS Nano 14, 10784 (2020).
  4. A. M. Striegel and A. K. Brewer, Hydrodynamic chromatography, Annu. Rev. Anal. Chem. 5, 15 (2012).
  5. R. Edam, S. Eeltink, D. J. Vanhoutte, W. T. Kok, and P. J. Schoenmakers, Hydrodynamic chromatography of macromolecules using polymer monolithic columns, J. Chromatogr., A 1218, 8638 (2011).
  6. J. Hansing and R. R. Netz, Hydrodynamic effects on particle diffusion in polymeric hydrogels with steric and electrostatic particle–gel interactions, Macromolecules 51, 7608 (2018).
  7. D. Mangal, J. C. Conrad, and J. C. Palmer, Nanoparticle dispersion in porous media: Effects of hydrodynamic interactions and dimensionality, AIChE J. 67, e17147 (2021).
  8. J. Mo, A. Simha, and M. G. Raizen, Broadband boundary effects on Brownian motion, Phys. Rev. E 92, 062106 (2015).
  9. J. Mo, Short timescale brownian motion and applications, Ph.D. thesis, The University of Texas at Austin, 2015.
  10. O. Sipos, K. Nagy, R. Di Leonardo, and P. Galajda, Hydrodynamic trapping of swimming bacteria by convex walls, Phys. Rev. Lett. 114, 258104 (2015).
  11. E. Secchi, A. Vitale, G. L. Miño, V. Kantsler, L. Eberl, R. Rusconi, and R. Stocker, The effect of flow on swimming bacteria controls the initial colonization of curved surfaces, Nat. Commun. 11, 2851 (2020).
  12. A. Théry, A. Zambrano, E. Lauga, and R. Zenit, Helical locomotion in dilute suspensions, Phys. Rev. Fluids 10, 013101 (2025).
  13. D. Leighton and A. Acrivos, The shear-induced migration of particles in concentrated suspensions, J. Fluid Mech. 181, 415 (1987).
  14. T. Wang, A. Shapiro, and S. I. Andersen, Movement of oil droplets against salt concentration gradients in thin capillaries, Chem. Eng. Sci. 304, 120983 (2025).
  15. S. Kim and S. J. Karrila, Microhydrodynamics: Principles and Selected Applications (Dover, Mineola, NY, 2005).
  16. C. Pozrikidis, Boundary Integral and Singularity Methods for Linearized Viscous Flow (Cambridge University Press, New York, 1992).
  17. J. R. Blake and A. T. Chwang, Fundamental singularities of viscous flow: Part I: The image systems in the vicinity of a stationary no-slip boundary, J. Eng. Math. 8, 23 (1974).
  18. The dichotomy couplet and stresslet have been introduced by Batchelor [19] with reference to the disturbance flow due to an infinitesimal immersed particle in a linear flow. Specifically, the couplet refers to the disturbance flow due to a nonrotating particle in the ambient flow (hence, introducing an additional torque to the fluid), and the stresslet refers to the disturbance flow due to a rigid particle in the fluid (hence, introducing and additional stress). Alternatively to the term couplet, the term rotlet have been introduced, in the field of active particles, by Chwan and Wu [20] for indicating the flow induced by a rotating infinitesimal particle in the fluid. Following this logic, it would be more appropriate to refer to a singularity as a strainlet when it describes the infinitesimal deformation introduced by an active particle in the fluid, in dichotomy with its antisymmetric counterpart, the rotlet.
  19. G. K. Batchelor, The stress system in a suspension of force-free particles, J. Fluid Mech. 41, 545 (1970).
  20. A. T. Chwang and T. Y. Wu, A note on the helical movement of micro-organisms, Proc. R. Soc. Lond. B Biol. Sci. 178, 327 (1971).
  21. H. A. Lorentz, Abhandlungen über Theoretische Physik (B. G. Teubner, Leipzig, 1907).
  22. A. Einstein, Eine neue Bestimmung der Moleküldimensionen, Ann. Phys. 324, 289 (1906).
  23. A. Einstein, Berichtigung zu meiner Arbeit: “Eine neue Bestimmung der Moleküldimensionen,” Ann. Phys. 339, 591 (1911).
  24. J. M. Burgers, On the motion of small particles of elongated form suspended in a viscous liquid, in Selected Papers of J. M. Burgers, edited by F. T. M.  Nieuwstadt and J. A. Steketee (Springer Science+Business Media, Dordrecht, 1938), p. 209.
  25. T. J. Pedley and J. O. Kessler, A new continuum model for suspensions of gyrotactic micro-organisms, J. Fluid Mech. 212, 155 (1990).
  26. T. J. Pedley and J. O. Kessler, Hydrodynamic phenomena in suspensions of swimming microorganisms, Annu. Rev. Fluid Mech. 24, 313 (1992).
  27. K. Drescher, J. Dunkel, L. H. Cisneros, S. Ganguly, and R. E. Goldstein, Fluid dynamics and noise in bacterial cell–cell and cell–surface scattering, Proc. Natl. Acad. Sci. USA 108, 10940 (2011).
  28. E. Lauga, The Fluid Dynamics of Cell Motility (Cambridge University Press, Singapore, 2020).
  29. J. R. Blake, A note on the image system for a stokeslet in a no-slip boundary, Math. Proc. Camb. Phil. Soc. 70, 303 (1971).
  30. T. Bickel, Hindered mobility of a particle near a soft interface, Phys. Rev. E 75, 041403 (2007).
  31. D. Lopez and E. Lauga, Dynamics of swimming bacteria at complex interfaces, Phys. Fluids 26, 071902 (2014).
  32. G. Procopio and M. Giona, Bitensorial formulation of the singularity method for stokes flows, Math. Eng. 5, 1 (2022).
  33. H. Hasimoto, M.-U. Kim, and T. Miyazaki, The effect of a semi-infinite plane on the motion of a small particle in a viscous fluid, J. Phys. Soc. Jpn. 52, 1996 (1983).
  34. N. Liron and S. Mochon, Stokes flow for a stokeslet between two parallel flat plates, J. Eng. Math. 10, 287 (1976).
  35. W. W. Hackborn, Asymmetric Stokes flow between parallel planes due to a rotlet, J. Fluid Mech. 218, 531 (1990).
  36. S. Bhattacharya and J. Bławzdziewicz, Image system for Stokes-flow singularity between two parallel planar walls, J. Math. Phys. 43, 5720 (2002).
  37. A. J. T. M. Mathijssen, A. Doostmohammadi, J. M. Yeomans, and T. N. Shendruk, Hydrodynamics of micro-swimmers in films, J. Fluid Mech. 806, 35 (2016).
  38. A. Daddi-Moussa-Ider, M. Lisicki, A. J. T. M. Mathijssen, C. Hoell, S. Goh, J. Bławzdziewicz, A. M. Menzel, and H. Löwen, State diagram of a three-sphere microswimmer in a channel, J. Phys.: Condens. Matter 30, 254004 (2018).
  39. G. T. Fortune, E. Lauga, and R. E. Goldstein, Biophysical fluid dynamics in a Petri dish, Phys. Rev. Fluids 9, 083101 (2024).
  40. O. Sono and H. Hasimoto, Slow motion of a spherical particle in a viscous fluid bounded by two perpendicular walls, J. Phys. Soc. Jpn. 40, 884 (1976).
  41. O. Sano and H. Hasimoto, The effect of two plane walls on the motion of a small sphere in a viscous fluid, J. Fluid Mech. 87, 673 (1978).
  42. M.-U. Kim, The effect of a salient wedge on the motion of a small particle in a viscous fluid, J. Phys. Soc. Jpn. 52, 3790 (1983).
  43. J. Dauparas and E. Lauga, Leading-order Stokes flows near a corner, IMA J. Appl. Math. 83, 590 (2018).
  44. A. R. Sprenger and A. M. Menzel, Microswimming under a wedge-shaped confinement, Phys. Fluids 35, 123119 (2023).
  45. C. W. Oseen, Neuere Methoden und Ergebnisse in der Hydrodynamik (Akademische Verlagsgesellschaft, Leipzig, 1927).
  46. Y. O. Fuentes, S. Kim, and D. J. Jeffrey, Mobility functions for two unequal viscous drops in Stokes flow. I. Axisymmetric motions, Phys. Fluids 31, 2445 (1988).
  47. R. Shail and S. H. Onslow, Some Stokes flows exterior to a spherical boundary, Mathematika 35, 233 (1988).
  48. Y. O. Fuentes, S. Kim, and D. J. Jeffrey, Mobility functions for two unequal viscous drops in Stokes flow. II. Asymmetric motions, Phys. Fluids 1, 61 (1989).
  49. R. Usha and S. D. Nigam, Flow in a spherical cavity due to a stokeslet, Fluid Dyn. Res. 11, 75 (1993).
  50. C. Maul and S. Kim, Image systems for a stokeslet inside a rigid spherical container, Phys. Fluids 6, 2221 (1994).
  51. V. A. Shaik and A. M. Ardekani, Point force singularities outside a drop covered with an incompressible surfactant: Image systems and their applications, Phys. Rev. Fluids 2, 113606 (2017).
  52. A. Chamolly and E. Lauga, Stokes flow due to point torques and sources in a spherical geometry, Phys. Rev. Fluids 5, 074202 (2020).
  53. A. R. Sprenger, V. A. Shaik, A. M. Ardekani, M. Lisicki, A. J. T. M. Mathijssen, F. Guzmán-Lastra, H. Löwen, A. M. Menzel, and A. Daddi-Moussa-Ider, Towards an analytical description of active microswimmers in clean and in surfactant-covered drops, Eur. Phys. J. E 43, 58 (2020).
  54. M.-U. Kim, Slow viscous flow due to the motion of a sphere on the axis of a circular cone, J. Phys. Soc. Jpn. 47, 1670 (1979).
  55. M.-U. Kim, Slow viscous rotation of a sphere on the axis of a circular cone, Phys. Fluids 23, 1268 (1980).
  56. I. V. Blinova, K. N. Kyz'yurova, and I. Y. Popov, Stokes flow driven by a stokeslet in a cone, Acta Mech. 225, 3115 (2014).
  57. A. Daddi-Moussa-Ider, A. R. Sprenger, Y. Amarouchene, T. Salez, C. Schönecker, T. Richter, H. Löwen, and A. M. Menzel, Axisymmetric Stokes flow due to a point-force singularity acting between two coaxially positioned rigid no-slip disks, J. Fluid Mech. 904, A34 (2020).
  58. I. Tanasijević and E. Lauga, Hydrodynamic interactions between a point force and a slender filament, Phys. Rev. Fluids 6, 124101 (2021).
  59. H. Hasimoto, Slow motion of a small sphere in a cylindrical domain, J. Phys. Soc. Jpn. 41, 2143 (1976).
  60. J. R. Blake, On the generation of viscous toroidal eddies in a cylinder, J. Fluid Mech. 95, 209 (1979).
  61. Md. Shamsul Alam, K. Ishii, and H. Hasimoto, Slow motion of a small sphere outside of a circular cylinder, J. Phys. Soc. Jpn. 49, 405 (1980).
  62. Y. Fukumoto, Slow motion of a small sphere in a viscous fluid between two concentric circular cylinders, J. Phys. Soc. Jpn. 54, 1322 (1985).
  63. N. Liron and R. Shahar, Stokes flow due to a stokeslet in a pipe, J. Fluid Mech. 86, 727 (1978).
  64. A. Daddi-Moussa-Ider, M. Lisicki, and S. Gekle, Hydrodynamic mobility of a sphere moving on the centerline of an elastic tube, Phys. Fluids 29, 111901 (2017).
  65. See Supplemental Material at http://link.aps.org/supplemental/10.1103/jt65-63vb for a revision of the results obtained in Ref. [62].
  66. G. Procopio and M. Giona, On the Hinch–Kim dualism between singularity and Faxén operators in the hydromechanics of arbitrary bodies in Stokes flows, Phys. Fluids 36, 032016 (2024).
  67. G. Procopio and M. Giona, On the theory of body motion in confined Stokesian fluids, J. Fluid Mech. 1000, A11 (2024).
  68. D. Takagi, J. Palacci, A. B. Braunschweig, M. J. Shelley, and J. Zhang, Hydrodynamic capture of microswimmers into sphere-bound orbits, Soft Matter 10, 1784 (2014).
  69. M. Jalaal, B. Ten Hagen, H. Le The, C. Diddens, D. Lohse, and A. Marin, Interfacial aggregation of self-propelled Janus colloids in sessile droplets, Phys. Rev. Fluids 7, 110514 (2022).
  70. S. E. Spagnolie, G. R. Moreno-Flores, D. Bartolo, and E. Lauga, Geometric capture and escape of a microswimmer colliding with an obstacle, Soft Matter 11, 3396 (2015).
  71. A. Daddi-Moussa-Ider, H. Löwen, and B. Liebchen, Hydrodynamics can determine the optimal route for microswimmer navigation, Commun. Phys. 4, 15 (2021).
  72. H. Brenner and J. Happel, Slow viscous flow past a sphere in a cylindrical tube, J. Fluid Mech. 4, 195 (1958).
  73. J. L. Synge and A. Schild, Tensor Calculus (Dover, New York, 1978).
  74. E. Poisson, A. Pound, and I. Vega, The motion of point particles in curved spacetime, Living Rev. Relativ. 14, 7 (2011).
  75. R. P. Kanwal, Generalized Functions: Theory and Applications, 3rd ed. (Springer Science+Business Media, New York, 2004).
  76. O. A. Ladyzhenskaia, The Mathematical Theory of Viscous Incompressible Flow, revised English edition (Martino, Mansfield Centre, CT, 2014).
  77. J. Synge, Relativity: The General Theory (North-Holland, Amsterdam, 1960).
  78. G. N. Watson, A Treatise on the Theory of Bessel Functions, 2nd ed. (Cambridge University Press, Cambridge, UK, 1944).
  79. The Brenner expressions reported in Refs. [2, 71] are represented in terms of the physical components of the velocity, while in this work the contravariant components are used. If vθ(x) is the physical component along the angular direction used in Refs. [2, 71], then the relation v2(x)=vθ(x)/R holds. See Ref. [ [72], pp. 142–149] for a detailed discussion.
  80. P. F. Papkovich, Solution générale des équations differentielles fondamentales d'élasticité exprimée par trois fonctions harmoniques, C.R. Acad. Sci. Paris 195, 513 (1932).
  81. V. H. Neuber, Ein neuer ansatz zur lösung räumlicher probleme der elastizitätstheorie. der hohlkegel unter einzellast als beispiel, J. Appl. Math. Mech. 14, 203 (1934).
  82. D. Bernstein, Scalar, Vector, and Matrix Mathematics: Theory, Facts, and Formulas (Princeton University Press, Princeton, NJ, 2018).
  83. A. P. Berke, L. Turner, H. C. Berg, and E. Lauga, Hydrodynamic attraction of swimming microorganisms by surfaces, Phys. Rev. Lett. 101, 038102 (2008).
  84. J. W. Swan and J. F. Brady, Particle motion between parallel walls: Hydrodynamics and simulation, Phys. Fluids 22, 103301 (2010).
  85. https://doi.org/10.5281/zenodo.18526478.
  86. M. Giona, G. Procopio, and R. Mauri, Hydrodynamic Green functions: Paradoxes in unsteady Stokes conditions and infinite propagation velocity in incompressible viscous models, Meccanica 57, 1055 (2022).
  87. E. De Souza Sánchez Filho, Tensor Calculus for Engineers and Physicists (Springer International, Cham, 2016).

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