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. Author manuscript; available in PMC: 2017 Jan 1.
Published in final edited form as: Eur J Appl Physiol. 2015 Aug 23;116(1):97–113. doi: 10.1007/s00421-015-3228-3

Figure 6. Illustration of the effective numerical inversion of our improved SHbO2 and SHbCO2 equations under varying physiological conditions.

Figure 6

In plots (A–D), the simulations of PO2 as a function of SHbO2 are shown, while in plots (E–H), the simulations of PCO2 as a function of SHbCO2 are shown. In each scenario, three variables are fixed at their standard physiological levels, while the fourth one is allowed to increase by predetermined increments over a large range, as described in detail in the legend to Fig. 4. The inversion computations were carried out using a variant of the Newton-Raphson method (i.e. quasi-Newton-Raphson method) with appropriate initial guesses that guaranteed convergence. These plots are the mirror-images of the corresponding plots in Fig. 4 (but with different scales), illustrating the accuracy of the numerical inversion schemes.