1993
DOI: 10.1152/jappl.1993.75.5.2028
|View full text |Cite
|
Sign up to set email alerts
|

Spreading of exogenous surfactant in an airway

Abstract: Using a theoretical model, we studied spreading of a bolus of insoluble surfactant deposited on a thin liquid layer of a model airway. Applications include instillation of exogenous surfactant as a treatment for neonatal respiratory distress syndrome, the use of surfactant carriers to deliver drugs via the lung, and the movement of liquid along the airway tree due to naturally occurring gradients of surface tension. The time-dependent governing equations were solved numerically for longitudinal axisymmetric su… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

6
75
1

Year Published

1997
1997
2012
2012

Publication Types

Select...
9
1

Relationship

0
10

Authors

Journals

citations
Cited by 76 publications
(82 citation statements)
references
References 0 publications
6
75
1
Order By: Relevance
“…Surface active material instilled into the airways has the capacity to rapidly spread and distribute to the periphery of the lung [147][148][149]. Spreading from the central airways towards the alveoli is promoted by surface tension gradients that drive transport from regions of high surfactant concentration to regions of lower surfactant concentration.…”
Section: Delivery Methods and Dosages For Exogenous Surfactant Therapmentioning
confidence: 99%
“…Surface active material instilled into the airways has the capacity to rapidly spread and distribute to the periphery of the lung [147][148][149]. Spreading from the central airways towards the alveoli is promoted by surface tension gradients that drive transport from regions of high surfactant concentration to regions of lower surfactant concentration.…”
Section: Delivery Methods and Dosages For Exogenous Surfactant Therapmentioning
confidence: 99%
“…Since Marangoni driven spreading is rather rapid, it is computationally more efficient to introduce a stretched horizontal coordinate, , whose overall length is determined by the leading edge of the surfactant monolayer. For a finite amount of insoluble surfactant spreading in a one-dimensional geometry, a simple scaling analysis 5,28 shows that the leading edge advances in time as L(t)ϭt 1/3 . The following transformations therefore describe the spreading process in stretched coordinates:…”
Section: Base Statementioning
confidence: 99%
“…10,11,16,17 The case ␥ϭ1/2 yields the spreading behavior R(t)ϳt 1/2 , whose base flow solutions 18 and stability characteristics 9 have frequently been discussed in the literature. Equations ͑19͒ and ͑20͒, which describe the film thickness and surface concentration profiles, cannot be integrated exactly for arbitrary values of 1 and 2 .…”
Section: ͑23͒mentioning
confidence: 99%