Skip to main content
Log in

Dynamic simulations of an encapsulated microbubble translating in a tube at low capillary and Reynolds numbers

  • Published:
Journal of Engineering Mathematics Aims and scope Submit manuscript

Abstract

The dynamic translation of a micron-sized encapsulated bubble is investigated numerically inside a horizontal tube where liquid flows under constant pressure drop, when the effect of gravity is neglected. The coating of the bubble is treated as an infinitesimally thin viscoelastic shell with bending resistance. The Galerkin Finite Element Methodology is employed to solve the axisymmetric flow configuration combined with the spine or elliptic mesh generation techniques for updating the mesh. The microbubble is initially elongated and the Reynolds number of the flow is relatively small, i.e. \(\hbox {Re}< 5\). Benchmark simulations for long free bubbles robustly recover the scaling of the film thickness with the 2/3 power of the capillary number based on surface tension. In the case of encapsulated bubbles, for a sufficiently small capillary number and after a short transient period, the bubble acquires a Bretherton type shape that slowly expands in order to accommodate changes in the liquid pressure. The speed of translation is nearly constant, close to the mean velocity of the flow, and does not depend on surface tension, shell elasticity or bending resistance. Fluid motion in the thin film “contact” region that forms in the gap between the tube and the shell is seen to be a stable flow arrangement that entails a mixture of pressure driven and shear driven flow, with the latter greatly affected by the area dilatation modulus via the tangential stress balance. By introducing a modified capillary number based on the area dilatational modulus, rather than surface tension, it is seen that the dimensionless film thickness that occupies the region between the bubble and the tube wall increases with the 1/3 power of the modified capillary number with increasing area dilatation. Simulations when surface tension is absent indicate that tangential shear generated due to variation of the membrane stress in the transition region that joins the bulk of the flow configuration with the contact region, leads to film thinning via the 5/7 power of the modified capillary number. Variations in the transverse shear of the viscoelastic shell generate large lubrication overpressures in the thin film region between the tube and the shell that are exerted radially on the shell and are conjectured to be responsible for the onset of 3d buckled shapes. The latter are often observed experimentally in similar flow configurations of capsules and are characterized by wrinkles that develop in the azimuthal direction around the shell equator.

This is a preview of subscription content, log in via an institution to check access.

Access this article

Price excludes VAT (USA)
Tax calculation will be finalised during checkout.

Instant access to the full article PDF.

Fig. 1
Fig. 2
Fig. 3
Fig. 4
Fig. 5
Fig. 6
Fig. 7
Fig. 8
Fig. 9
Fig. 10
Fig. 11
Fig. 12
Fig. 13
Fig. 14
Fig. 15
Fig. 16

Similar content being viewed by others

References

  1. Frinking PJ, Bouakaz A, Kirkhorn J, Ten Cate FJ, de Jong N (2000) Ultrasound contrast imaging: current and new potential methods. Ultrasound Med Biol 26(6):965–97

    Article  Google Scholar 

  2. Cosgrove D (2006) Ultrasound contrast agents: an overview. Eur J Radiol 60(3):324–330

    Article  Google Scholar 

  3. Ferrara K, Pollard R, Borden M (2007) Ultrasound microbubble contrast agents: fundamentals and application to gene and drug delivery. Annu Rev Biomed Eng 9(1):415–444

    Article  Google Scholar 

  4. Kaufmann BA, Wei K, Lindner JR (2007) Contrast echocardiography. Curr Probl Cardiol 32(2):51–96

    Article  Google Scholar 

  5. Efthymiou K, Pelekasis N, Butler MB, Thomas DH, Sboros V (2018) The effect of resonance on transient microbubble acoustic response: experimental observations and numerical simulations. J Acoust Soc Am 143(3):1392–1406

    Article  Google Scholar 

  6. Taniyama Y, Tachibana K, Hiraoka K, Namba T, Yamasaki K, Hashiya N, Aoki M, Ogihara T, Yasufumi K, Morishita R (2002) Local delivery of plasmid DNA into rat carotid artery using ultrasound. Circulation 105(10):1233–1239

    Article  Google Scholar 

  7. Marmottant P, Hilgenfeldt S (2003) Controlled vesicle deformation and lysis by single oscillating bubbles. Nature 423:153–156

    Article  Google Scholar 

  8. Doinikov AA, Bouakaz A (2014) Effect of a distant rigid wall on microstreaming generated by an acoustically driven gas bubble. J Fluid Mech 742:425–445

    Article  MathSciNet  MATH  Google Scholar 

  9. Chen H, Dong E, Li J, Stone HA (2013) Adhesion of moving droplets in microchannels. Appl Phys Lett 103:131605

    Article  Google Scholar 

  10. Lin H, Chen J, Chen C (2016) A novel technology: microfluidic devices for microbubble ultrasound contrast agent generation. Med Biol Eng Comput 54:1317–1330

    Article  Google Scholar 

  11. Kok MP, Segers T, Versluis M (2015) Bubble sorting in pinched microchannels for ultrasound contrast agent enrichment. Lab Chip 15:3716–3722

    Article  Google Scholar 

  12. Segers T, de Rond L, de Jong N, Borden M, Versluis M (2016) Stability of monodisperse phospholipid-coated microbubbles formed by flow-focusing at high production rates. Langmuir 32(16):3937–3944

    Article  Google Scholar 

  13. Lignel S, Salsac AV, Drelich A, Leclerc E, Pezron I (2017) Water-in-oil droplet formation in a flow-focusing microsystem using pressure- and flow rate-driven pumps. Colloids Surf A 531:164–172

    Article  Google Scholar 

  14. Ryskin G, Leal LG (1984) Numerical solution of free-boundary problems in fluid mechanics. Part 2. Buoyancy-driven motion of a gas bubble through a quiescent liquid. J Fluid Mech 148:19–35

    Article  MATH  Google Scholar 

  15. Bonometti T, Magnaudet J (2006) Transition from spherical cap to toroidal bubbles. Phys Fluids 18:052102

    Article  Google Scholar 

  16. Bretherton FP (1961) The motion of long bubbles in tubes. J Fluid Mech 10:166–188

    Article  MathSciNet  MATH  Google Scholar 

  17. Lamstaes C, Eggers J (2017) Arrested bubble rise in a narrow tube. J Stat Phys 167:656–682

    Article  MathSciNet  MATH  Google Scholar 

  18. Magnini M, Khodaparast S, Matar OK, Stone HA, Thome JR (2019) Dynamics of long gas bubbles rising in a vertical tube in a cocurrent liquid flow. Phys Rev Fluids 4:02360

    Article  Google Scholar 

  19. Yu YE, Magnini M, Zhu L, Shim S, Stone HA (2021) Non-unique bubble dynamics in a vertical capillary with an external flow. J Fluid Mech 911(A34):10.1017

    MathSciNet  MATH  Google Scholar 

  20. Dhaouadi W, Kolinski JM (2019) Bretherton’s buoyant bubble. Phys Rev Fluids 4:123601

  21. Feng JQ (2007) A spherical-cap bubble moving at terminal velocity in a viscous liquid. J Fluid Mech 579:347–371

    Article  MathSciNet  MATH  Google Scholar 

  22. Feng JQ (2010) Steady axisymmetric motion of a small bubble in a tube with flowing liquid. Proc R Soc A 466:549–562

    Article  MATH  Google Scholar 

  23. Schwartz LW, Princen HM, Kiss AD (1986) On the motion of bubbles in capillary tubes. J Fluid Mech 172:259–27

    Article  Google Scholar 

  24. Stebe KJ, Barthes-Biesel D (1995) Marangoni effects of adsorption-desorption controlled surfactants on the leading end of an infinitely long bubble in a capillary. J. Fluid Mech 286:25–48

    Article  MATH  Google Scholar 

  25. Olgac U, Muradoglu M (2013) Effects of surfactant on liquid film thickness in the Bretherton problem. Int J Multiphase Flow 48:58–70

    Article  Google Scholar 

  26. Yu YE, Zhu L, Shim S, Eggers J, Stone HA (2018) Time-dependent motion of a confined bubble in a tube: transition between two steady states. J Fluid Mech 857(R4):10.101

    MathSciNet  MATH  Google Scholar 

  27. Balestra G, Zhu L, Gallaire F (2018) Viscous Taylor droplets in axisymmetric and planar tubes: from Bretherton‘s theory to empirical models. Microfluid Nanofluid 22:67mydo

    Article  Google Scholar 

  28. Pozrikidis C (1992) Boundary integral and singularity methods for linearized viscous flow. Cambridge University Pres, Cambridge

    Book  MATH  Google Scholar 

  29. Barthes-Biesel D, Rallison M (1981) The time-dependent deformation of a capsule freel suspended in a linear shear flow. J Fluid Mech 113:251–267

    Article  MATH  Google Scholar 

  30. Li XZ, Barthes-Biesel D, Helmy A (1988) Large deformations and burst of a capsule freely suspended in an elongational flow. J Fluid Mech 187:179–196

    Article  MATH  Google Scholar 

  31. Pozrikidis C (1995) Finite deformation of liquid capsules enclosed by elastic membranes in simple shear flow. J Fluid Mech 297:12–152

    Article  MATH  Google Scholar 

  32. Ramanujan S, Pozrikidis C (1998) Deformation of liquid capsules enclosed by elastic membranes in simple shear flow: large deformations and the effect of fluid viscosities. J Fluid Mech 361:11–143

    Article  MathSciNet  MATH  Google Scholar 

  33. Pozrikidis C (2001) Effect of membrane bending stiffness on the deformation of capsules in simpl shear flow. J Fluid Mech 440:26–291

    Article  MATH  Google Scholar 

  34. Diaz A, Pelekasis N, Barthes-Biesel D (2000) Transient response of a capsule subjected to varying flow conditions: effect of internal fluid viscosity and membrane elasticity. Phys Fluids 12:94–957

    Article  MATH  Google Scholar 

  35. Lac E, Barthes-Biesel D, Pelekasis N, Tsamopoulos J (2004) Spherical capsules in three-dimensional unbounded Stokes flows: effect of the membrane constitutive law and the onset of buckling. J Fluid Mech 516:303–334

    Article  MathSciNet  MATH  Google Scholar 

  36. Barthes-Biesel D, Diaz A, Dhenin E (2002) Effect of constitutive laws for two-dimensional membranes on flow-induced capsule deformation. J Fluid Mech 460:211–222

    Article  MATH  Google Scholar 

  37. Qin S, Ferrara KW (2007) The natural frequency of non-linear oscillation of ultrasound contrast agents in microvessels. Ultrasound in Med & Biol 33(7):1140–114

    Article  Google Scholar 

  38. Chen C, Gu Y, Tu J, Guo X, Zhang D (2016) Microbubble oscillating in a microvessel filled with viscous fluid: a finite element modeling study. Ultrasonics 66:5–64

    Article  Google Scholar 

  39. Vlachomitrou M, Pelekasis N (2021) Numerical study of the interaction between a pulsating coated microbubble and a rigid wall. I. Translational motion. Phys Rev Fluids 6:013601

    Article  Google Scholar 

  40. Vlachomitrou M, Pelekasis N (2021) Numerical study of the interaction between a pulsating coated microbubble and a rigid wall. II. Trapped pulsation. Phys Rev Fluids 6:01360

    Google Scholar 

  41. Sarkar K, Shi WT, Chatterjee D, Forsberg F (2005) Characterization of ultrasound contrast microbubbles using in vitro experiments and viscous and viscoelastic interface models for encapsulation. J. Acoust Soc Am 118(1):539–550

    Article  Google Scholar 

  42. Marmottant P, van der Meer S, Emmer M, Versluis M, de Jong N, Hilgenfeldt S, Lohse D (2005) A model for large amplitude oscillations of coated bubbles accounting for buckling and rupture. J Acoust Soc Am 118(6):3499–3505

    Article  Google Scholar 

  43. Timoshenko S, Woinowsky-Krieger S (1959) Theory of Plates and Shells. McGraw-Hill, Singapore

    MATH  Google Scholar 

  44. Tsiglifis K, Pelekasis N (2008) Nonlinear radial oscillations of encapsulated microbubbles subject to ultrasound: the effect of membrane constitutive law. J Acoust Soc Am 123(6):4059–4070

    Article  Google Scholar 

  45. Tsiglifis K, Pelekasis N (2011) Parametric stability and dynamic buckling of encapsulated microbubble subject to acoustic disturbances. Phys Fluids 23:012102

    Article  Google Scholar 

  46. Vlachomitrou M, Pelekasis N (2017) Dynamic simulation of a coated microbubble in an unbounded flow: response to a step change in pressure. J Fluid Mech 822:717–761

    Article  MathSciNet  MATH  Google Scholar 

  47. Dimakopoulos Y, Tsamopoulos J (2003) A quasi-elliptic transformation for moving boundary problems with large anisotropic deformations. J Comput Phys 192(2):494–522

    Article  MATH  Google Scholar 

  48. Timoshenko S (1947) Strength of materials Part II: advanced theory & problems. D. van Nostrand, New York

  49. Dupont C, Le Tallec P, Barthes-Biesel D, Vidrascu M, Salsac AV (2015) Dynamics of a spherical capsule in a planar hyperbolic flow: influence of bending resistance. Procedia IUTAM 16:70–79

    Article  Google Scholar 

  50. Chu TX, Salsac AV, Barthes-Biesel D, Griscom L, Edwards-Levy F, Leclerc E (2013) Fabrication and in-situ characterization of microcapsules in a microfluidic system. Microfluid Nanofluid 14:309–317

    Article  Google Scholar 

Download references

Acknowledgements

This research is co-funded by Greece and the European Union (European Social Fund—ESF) by the Operational Programme ‘Human Resources Development, Education and Lifelong Learning 2014-2030’ in the context of the project ‘Numerical and theoretical study of the production process of encapsulated microbubbles with lipid surfactant coating with the use of flow focused microfluidic device’ (MIS 5048922).

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to N. Pelekasis.

Additional information

Publisher's Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Rights and permissions

Reprints and permissions

About this article

Check for updates. Verify currency and authenticity via CrossMark

Cite this article

Vlachomitrou, M., Lytra, A. & Pelekasis, N. Dynamic simulations of an encapsulated microbubble translating in a tube at low capillary and Reynolds numbers. J Eng Math 129, 8 (2021). https://doi.org/10.1007/s10665-021-10144-0

Download citation

  • Received:

  • Accepted:

  • Published:

  • DOI: https://doi.org/10.1007/s10665-021-10144-0

Keywords

Navigation