Research interests of V. Kumaran

Flow in flexible tubes:

Introduction

The flow of a fluid in flexible tubes and channels is encountered in many biological systems, such as the flow of blood in arteries and veins. Many reaction and separation processes in biotechnological industries also involve this type of flow. A salient feature of parallel flows is the transition from laminar to turbulent flow at a critical Reynolds number, because the characteristics of the laminar and turbulent states are very different. For example, the mass and heat transfer coefficient of the turbulent flow is three orders of magnitude greater than that of the laminar flow. An accurate knowledge of the transition point is of importance for the design of these systems. In a rigid tube, the transition takes place at a Reynolds number of about 2300, but in flexible tubes the wall flexibility could influence the transition.

Objectives

The objective of this project is to determine the effect of the wall flexibility on the transition in rigid tubes and channels, and to study the flow structure in the turbulent regime.

Results

The stability of the flow is a function of the Reynolds number, which is the ratio of inertial and viscous forces, and an additional parameter which gives the ratio of the viscous forces in the fluid and the elastic forces in the wall.
  1. The stability of the flow in the low Reynolds number limit has been studied using asymptotic analysis. In this limit the viscous forces are neglected and it is found that the flow becomes unstable when the velocity is increased beyond a critical value.
  2. Asymptotic analysis was used to study the stability of axisymmetric modes in the high Reynolds limit. In this, there are two types of modes -- {\em inviscid modes} and {\em wall modes}. The asymptotic analysis revealed that both these types of modes are stable.
  3. Numerical calculations of the variation in the critical velocity over five orders of magnitude was undertaken. These computations reveal that there is indeed an instability at high Reynolds number, and the most unstable mode is the wall mode modified by the inertia of the flexible wall of the tube.
  4. The possibility of unstable non - axisymmetric modes has been analysed. For plane surfaces, the Squire's theorem states that two dimensional perturbations are always unstable than three dimensional perturbations. No such theorem exists for flows in cylindrical tubes. The equivalents of the Rayleigh theorem have been derived for the flow in a flexible tube, and it is found that the axisymmetric modes are always stable for a parabolic mean flow, but non - axisymmetric modes could become unstable.
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