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A new interpolation-free procedure for breath-by-breath analysis of oxygen uptake in exercise transients

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Abstract

Introduction

Interpolation methods circumvent poor time resolution of breath-by-breath oxygen uptake (\(\dot{V}{\text{O}}_{2}\)) kinetics at exercise onset. We report an interpolation-free approach to the improvement of poor time resolution in the analysis of \(\dot{V}{\text{O}}_{2}\) kinetics.

Methods

Noiseless and noisy (10 % Gaussian noise) synthetic data were generated by Monte Carlo method from pre-selected parameters (Exact Parameters). Each data set comprised 10 (\(\dot{V}{\text{O}}_{2}\))-on transitions with noisy breath distribution within a physiological range. Transitions were superposed (no interpolation, None), then analysed by bi-exponential model. Fitted model parameters were compared with those from interpolation methods (average transition after Linear or Step 1-s interpolations), applied on the same data. Experimental data during cycling were also analysed. The 95 % confidence interval around a line of parameters’ equality was computed to analyse agreement between exact parameters and corresponding parameters of fitted functions.

Results

The line of parameters’ equality stayed within confidence intervals for noiseless synthetic parameters with None, unlike Step and Linear, indicating that None reproduced Exact Parameters. Noise addition reduced differences among pre-treatment procedures. Experimental data provided lower phase I time constants with None than with Step.

Conclusion

In conclusion, None revealed better precision and accuracy than Step and Linear, especially when phenomena characterized by time constants of <30 s are to be analysed. Therefore, we endorse the utilization of None to improve the quality of breath-by-breath \(\dot{V}{\text{O}}_{2}\) data during exercise transients, especially when a double exponential model is applied and phase I is accounted for.

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Abbreviations

a 1 :

Amplitude of response of first exponential

a 2 :

Amplitude of response of second exponential

b :

Baseline resting \(\dot{V}{\text{O}}_{2}\) value

d 1 :

Time delay of first exponential

d 2 :

Time delay of second exponential

T :

Time

s:

Second

\(\dot{V}{\text{O}}_{2}\) :

Oxygen uptake

\(\theta\) :

Heaviside function

\(\tau_{1}\) :

Time constant of first exponential

\(\tau_{2}\) :

Time constant of second exponential

\(\in\) :

Mathematical symbol meaning “is an element of”

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Acknowledgments

This study was supported by Swiss National Science Foundation Grants 32003B_127620 and 32003B_143427 to Guido Ferretti. The authors thank the volunteers for their implication in this study.

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Correspondence to Aurélien Bringard.

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Communicated by Carsten Lundby.

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Bringard, A., Adami, A., Moia, C. et al. A new interpolation-free procedure for breath-by-breath analysis of oxygen uptake in exercise transients. Eur J Appl Physiol 114, 1983–1994 (2014). https://doi.org/10.1007/s00421-014-2920-z

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  • DOI: https://doi.org/10.1007/s00421-014-2920-z

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