Hostname: page-component-cd9895bd7-hc48f Total loading time: 0 Render date: 2024-12-28T04:27:26.976Z Has data issue: false hasContentIssue false

Fluid-elastic instabilities of liquid-lined flexible tubes

Published online by Cambridge University Press:  26 April 2006

D. Halpern
Affiliation:
Biomedical Engineering Department, Robert R. McCormick School of Engineering and Applied Science Northwestern University, Evanaton, IL 60208, USA and Department of Anesthesia, Northwestern University Medical School, Chicago, IL 60611. USA
J. B. Grotberg
Affiliation:
Biomedical Engineering Department, Robert R. McCormick School of Engineering and Applied Science Northwestern University, Evanaton, IL 60208, USA and Department of Anesthesia, Northwestern University Medical School, Chicago, IL 60611. USA

Abstract

The dynamics of a thin film of Newtonian fluid coating the inner surface of an elastic circular tube is analysed. This problem is motivated by an interest in the closure of small airways of the lungs either by formation of a liquid bridge, the collapse of the airway wall or a combination of both processes. Liquid bridge formation is due to the destabilization of the liquid film that coats the inner surface of airways, while wall collapse can be due to either the high surface tension of the air–liquid interface or the flexibility of the wall.

Nonlinear evolution equations for the film thickness and wall position are derived using lubrication theory, but an accurate representation of the curvatures of both the liquid and wall interfaces is employed which is valid for thick films. These approximations allow closure to be predicted. In addition, these approximations are justified by comparison with rigid-wall results obtained by solving the full Navier–Stokes equations and because fluid inertia only becomes important in the very late stages of closure. The linear stability of these equations is examined using normal-mode analysis for infinitesimal disturbances and the nonlinear stability is investigated by solving the governing equations numerically using the method of lines. Solutions show that there is a critical film thickness, strongly dependent on fluid and wall properties, above which unstable waves grow to form liquid bridges. The critical film thickness decreases with increasing surface tension or wall compliance since waves grow faster. Even for relatively stiff airways, the volume of fluid in the liquid lining required for closure can be approximately 70% of the volume for the rigid-tube case. Wall damping is an important effect only when the airway is sufficiently compliant. Airway closure occurs more rapidly with increasing unperturbed film thickness, surface tension and wall flexibility and decreasing wall damping.

Type
Research Article
Copyright
© 1992 Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Atabek, H. B. & Lew H. S. 1966 Wave propagation through a viscous incompressible fluid contained in an initially stressed elastic tube. Biophys. J. 6, 481503.Google Scholar
Crawford A. B. H., Cotton D. J., Paiva, M. & Engel L. A. 1989 Effect of airway closure on ventilation distribution. J. Appl. Physiol. 66, 25112515.Google Scholar
Dragon, C. A. & Grotberg J. B. 1991 Oscillatory flow and mass transport in a flexible tube. J. Fluid Mech. 231, 135155.Google Scholar
Elad D., Foux, A. & Kivity Y. 1988a A model for the nonlinear elastic response of large arteries. J. Biomed. Engng 110, 185189.Google Scholar
Elad D., Kamm, R. D. & Shapiro A. H. 1988b Tube law for the intrapulmonary airway. J. Appl. Physiol. 65, 713.Google Scholar
Frazer D. G., Weber, K. C. & Franz G. N. 1985 Evidence of sequential opening and closing of lung units during inflation–deflation of excised rat lungs. Resp. Physiol. 61, 277288.Google Scholar
Gauglitz, P. A. & Radke C. J. 1988 An extended evolution equation for liquid film breakup in cylindrical capillaries. Chem. Engng Sci. 43, 14571465.Google Scholar
Goldenveizer A. C. 1961 Theory of Elastic Thin Shells. Pergamon.
Goren S. L. 1962 The instability of an annular thread of fluid. J. Fluid Mech. 12, 309319.Google Scholar
Hammond P. S. 1983 Nonlinear adjustment of a thin annular film of viscous fluid surrounding a thread of another within a circular pipe. J. Fluid Mech. 137, 363384.Google Scholar
Hickox C. 1971 Instability due to a viscosity and density stratification in axisymmetric pipe flow. Phys. Fluids 14, 251262.Google Scholar
Holt M. 1984 Numerical Method in Fluid Dynamics. Springer.
Hughes J. M. B., Rosenzweig, D. Y. & Kivitz P. B. 1970 Site of airway closure in excised dog lungs: histologic demonstration. J. Appl. Physiol. 29, 340344.Google Scholar
Johnson M., Kamm R., Ho L. W., Shapiro, A. & Pedley T. J. 1991 The nonlinear growth of surface-tension-driven instabilities of a thin annular film. J. Fluid Mech. 223, 141156.Google Scholar
Kamm, R. D. & Johnson M. 1990 Airway closure at low lung volume: The role of liquid film instabilities. Appl. Mech. Rev. 43, Part 2, S92–97.Google Scholar
Kamm, R. D. & Schroter R. C. 1989 Is airway closure caused by a thin liquid instability? Respir. Physiol. 75, 141156.Google Scholar
Macklem P. T., Proctor, D. F. & Hogg J. C. 1970 The stability of peripheral airways. Respir, Physiol. 8, 191203.Google Scholar
Oron, A. & Rosenau P. 1989 Nonlinear evolution and breaking of interfacial Rayleigh–Taylor waves Phys. Fluids A 1, 11551165.Google Scholar
Otis D. R., Johnson M., Pedley, T. J. & Kamm R. D. 1990 The effect of surfactant on liquid film stability in the peripheral airways. Abstract, ASME Winter Annual Meeting.
Rayleigh Lord 1902 On the instability of cylindrical fluid surfaces. In Scientific Papers, vol. 3, pp. 594996. Cambridge University Press.
Rosenau, P. & Oron A. 1989 Evolution and breaking of liquid film flowing on a vertical cylinder Phys. Fluids A 1, 17631766.Google Scholar
Weibel E. R. 1963 Morphometry of the Human Lung. Academic.