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Research Article Free access | 10.1172/JCI106322

Hypoxic ventilatory drive in normal man

John V. Weil, Edward Byrne-Quinn, Ingvar E. Sodal, W. Otto Friesen, Brian Underhill, Giles F. Filley, and Robert F. Grover

Department of Medicine and Webb Waring Institute, University of Colorado Medical Center, Denver, Colorado 80220

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Department of Medicine and Webb Waring Institute, University of Colorado Medical Center, Denver, Colorado 80220

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Department of Medicine and Webb Waring Institute, University of Colorado Medical Center, Denver, Colorado 80220

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Department of Medicine and Webb Waring Institute, University of Colorado Medical Center, Denver, Colorado 80220

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Department of Medicine and Webb Waring Institute, University of Colorado Medical Center, Denver, Colorado 80220

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Department of Medicine and Webb Waring Institute, University of Colorado Medical Center, Denver, Colorado 80220

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Department of Medicine and Webb Waring Institute, University of Colorado Medical Center, Denver, Colorado 80220

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Published June 1, 1970 - More info

Published in Volume 49, Issue 6 on June 1, 1970
J Clin Invest. 1970;49(6):1061–1072. https://doi.org/10.1172/JCI106322.
© 1970 The American Society for Clinical Investigation
Published June 1, 1970 - Version history
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Abstract

A technique is described which permits the inscription of the ventilatory response to isocapnic hypoxia in man as a continuous curve relating alveolar oxygen tension and minute ventilation. The adjustment of ventilation to changes in alveolar oxygen tension is complete in 18-23 sec and this is sufficiently rapid to justify the use of a non-steady-state method. Changes in alveolar carbon dioxide tension are prevented by addition of carbon dioxide to the inspired gas. The resulting [unk]VE-PAo2 curves are hyperbolic such that falling PAo2 produces only slight rises in [unk]VE until a critical PAo2 range of 50-60 mm Hg is reached. With further fall in PAo2, [unk]VE increases steeply and the slope of the curve approaches infinity at a tension of 30-40 mm Hg. For purposes of quantitation these curves are approximated by a simple hyperbolic function, the parameters of which are evaluated by a least squares fit of the data. The parameter A denotes curve shape such that the higher the value of A. the greater the increase in ventilation for a given decrease in PAo2 and hence the greater the hypoxic drive. Curves are highly reproducible for each subject and curves from different subjects are similar. In 10 normal subjects at resting PACo2, A = 180.2 ±14.5 (SEM). When PACo2 is adjusted to levels 5 mm Hg above and below control in six subjects A = 453.4 ±103 and 30.2 ±6.8 respectively. These latter values differed significantly from control (P < 0.05). These changes in curve shape provide a clear graphic description of interaction between hypercapnic and hypoxic ventilatory stimuli. At normal PACo2 the [unk]VE-PAo2 curve has an inflection zone located over the same Po2 range as the inflection in the oxygen-hemoglobin dissociation curve. This indicated that ventilation might be a linear function of arterial oxygen saturation or content. Studies in four subjects have demonstrated that ventilation is indeed related to arterial oxygen content in a linear fashion. These data suggest, but do not prove, that oxygen tension in chemoreceptor tissue as in part determined by circulatory oxygen delivery may be an important factor in controlling the ventilatory response to hypoxia.

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