# Difference between revisions of "Hydrodynamical models for the chaotic dripping faucet"

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== Soft Matter == | == Soft Matter == | ||

− | Before examining chaotic dripping, the authors first model a static drop and investigate the possible stable shapes. A small flow rate is assumed thus the drop will not detach form the facet unless its volume exceeds a critical volume (<math>V < | + | Before examining chaotic dripping, the authors first model a static drop and investigate the possible stable shapes. A small flow rate is assumed thus the drop will not detach form the facet unless its volume exceeds a critical volume (<math>V < V_{c}</math>) and under this condition it will also be axisymmetric. The shape of the drop (see Figure 1(a)) is determined by the minimization of the gravitational energy and surface energy. This can be written in terms of when the forces perpendicular to the interface balance (nondimensionalized forms): |

− | math | + | <math>\frac{d\theta}{ds} - \frac{cos(\theta)}{r} = -z</math> |

− | + | The interfaces (r and z) can be written as: | |

− | math | + | <math>\frac{dz}{ds} = -cos(\theta)</math> |

− | The boundary conditions are | + | <math>\frac{dr}{ds} = sin(\theta)</math> |

+ | |||

+ | The boundary conditions at the bottom of the drop are: | ||

+ | |||

+ | <math>r(0) = 0</math> | ||

+ | |||

+ | <math>\theta(0) = \pi/2</math> | ||

+ | |||

+ | <math>z(0) = \frac{P_{b}}{\rho g}</math> | ||

+ | |||

+ | where <math>P_{b}</math> is the hydrostatic pressure - this unknown is the main determinant to the different family of solutions. As shown in Figure 1(b), up to <math>V\_{c}</math> the capillary forces are able to support the weight of the drop, after which the drop will be pinched-off. | ||

currently writing... | currently writing... |

## Revision as of 19:22, 27 September 2009

Original Entry by Michelle Borkin, AP225 Fall 2009

## Contents

## Overview

"Hydrodynamical models for the chaotic dripping faucet."

P. Coullet, L. Mahadevan and C. Riera, Journal of Fluid Mechanics, 526, 1-17, 2005.

## Keywords

surface tension, capillary force, chaos, hydrodynamics

## Summary

This paper presents a series of mathematical models describing the chaotic dripping of a facet. First, a static droplet of water hanging at the end of a facet is discussed, then time dependence is examined with a lubrication model, chaotic behavior is investigated using a proper orthogonal decomposition (POD) resulting in a simplified model, and finally a mechanical description encompassing the main features of these detailed fluid models is presented. The mathematical models presented importantly include and explain features of the dripping faucet such as the time between drips, chaotic dripping (i.e. drip-drop behavior), and the critical point between dripping and jetting.

## Soft Matter

Before examining chaotic dripping, the authors first model a static drop and investigate the possible stable shapes. A small flow rate is assumed thus the drop will not detach form the facet unless its volume exceeds a critical volume (<math>V < V_{c}</math>) and under this condition it will also be axisymmetric. The shape of the drop (see Figure 1(a)) is determined by the minimization of the gravitational energy and surface energy. This can be written in terms of when the forces perpendicular to the interface balance (nondimensionalized forms):

<math>\frac{d\theta}{ds} - \frac{cos(\theta)}{r} = -z</math>

The interfaces (r and z) can be written as:

<math>\frac{dz}{ds} = -cos(\theta)</math>

<math>\frac{dr}{ds} = sin(\theta)</math>

The boundary conditions at the bottom of the drop are:

<math>r(0) = 0</math>

<math>\theta(0) = \pi/2</math>

<math>z(0) = \frac{P_{b}}{\rho g}</math>

where <math>P_{b}</math> is the hydrostatic pressure - this unknown is the main determinant to the different family of solutions. As shown in Figure 1(b), up to <math>V\_{c}</math> the capillary forces are able to support the weight of the drop, after which the drop will be pinched-off.

currently writing...