Literature DB >> 3082848

A general dimensionless equation of gas transport by high-frequency ventilation.

J G Venegas, C A Hales, D J Strieder.   

Abstract

To identify a general relationship between eucapnic oscillatory flow (Vosc) and frequency (f) in high-frequency ventilation (HFV), we searched the literature for eucapnic HFV data in different mammalian species. We found suitable results for rat, rabbit, monkey, dog, human, and horse, which we expressed in terms of two dimensionless variables, Q = Vosc/Va and F = f/(VA/VD), with VA the alveolar ventilation and VD the volume of the conducting airways. The experimental HFV data define the linear regression equation in Q = 0.54 In F + 0.92 (R = 0.94). Krogh's equation for conventional ventilation (CV), Vosc = VA + fVD, in dimensionless terms becomes Q = 1 + F, which is valid for low F. The intersection of the CV and HFV equations at F = 5.0 defines a transition frequency, ft = 5.0 (VA/VD). At that point the alveolar ventilation per breath, VA/f, represents 20% of VD, and tidal volume (VT) equals 1.20 VD. For eucapnia ft ranges from 5.9 Hz in the rat to 0.9 Hz in the dog. The dimensional form of our HFV equation, VA = 0.13 (VT/VD)1.2 (VTf) is very similar to other empirical equations reported for dogs in noneucapnic settings. Therefore the dimensionless equation should also be valid within a species at noneucapnic settings.

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Year:  1986        PMID: 3082848     DOI: 10.1152/jappl.1986.60.3.1025

Source DB:  PubMed          Journal:  J Appl Physiol (1985)        ISSN: 0161-7567


  9 in total

1.  High frequency ventilation.

Authors:  A B Froese
Journal:  Can J Anaesth       Date:  1987-05       Impact factor: 5.063

2.  Computational Modeling of Primary Blast Lung Injury: Implications for Ventilator Management.

Authors:  Jacob Herrmann; Merryn H Tawhai; David W Kaczka
Journal:  Mil Med       Date:  2019-03-01       Impact factor: 1.437

3.  Regional gas transport in the heterogeneous lung during oscillatory ventilation.

Authors:  Jacob Herrmann; Merryn H Tawhai; David W Kaczka
Journal:  J Appl Physiol (1985)       Date:  2016-10-07

4.  Strain, strain rate, and mechanical power: An optimization comparison for oscillatory ventilation.

Authors:  Jacob Herrmann; Merryn H Tawhai; David W Kaczka
Journal:  Int J Numer Method Biomed Eng       Date:  2019-08-06       Impact factor: 2.747

5.  Total and regional lung volume changes during high-frequency oscillatory ventilation (HFOV) of the normal lung.

Authors:  R Blaine Easley; Christopher T Lancaster; Matthew K Fuld; Jason W Custer; David N Hager; David W Kaczka; Brett A Simon
Journal:  Respir Physiol Neurobiol       Date:  2008-10-18       Impact factor: 1.931

6.  Multifrequency Oscillatory Ventilation in the Premature Lung: Effects on Gas Exchange, Mechanics, and Ventilation Distribution.

Authors:  David W Kaczka; Jacob Herrmann; C Elroy Zonneveld; David G Tingay; Anna Lavizzari; Peter B Noble; J Jane Pillow
Journal:  Anesthesiology       Date:  2015-12       Impact factor: 7.892

7.  Impact of ventilation frequency and parenchymal stiffness on flow and pressure distribution in a canine lung model.

Authors:  Reza Amini; David W Kaczka
Journal:  Ann Biomed Eng       Date:  2013-07-20       Impact factor: 3.934

8.  Sphingosine 1-phosphate rescues canine LPS-induced acute lung injury and alters systemic inflammatory cytokine production in vivo.

Authors:  William S Szczepaniak; Yingze Zhang; Sarah Hagerty; Michael T Crow; Priya Kesari; Joe G N Garcia; Augustine M K Choi; Brett A Simon; Bryan J McVerry
Journal:  Transl Res       Date:  2008-10-11       Impact factor: 7.012

9.  Parenchymal strain heterogeneity during oscillatory ventilation: why two frequencies are better than one.

Authors:  Jacob Herrmann; Merryn H Tawhai; David W Kaczka
Journal:  J Appl Physiol (1985)       Date:  2017-10-19
  9 in total

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