Silencing of glycolysis in muscle: experimental observation and numerical analysis - PubMed
Silencing of glycolysis in muscle: experimental observation and numerical analysis
Joep P J Schmitz et al. Exp Physiol. 2010 Feb.
Abstract
The longstanding problem of rapid inactivation of the glycolytic pathway in skeletal muscle after contraction was investigated using (31)P NMR spectroscopy and computational modelling. Accumulation of phosphorylated glycolytic intermediates (hexose monophosphates) during cyclic contraction and subsequent turnover during metabolic recovery was measured in vivo in human quadriceps muscle using dynamic (31)P NMR spectroscopy. The concentration of hexose monophosphates in muscle peaked 40 s into metabolic recovery from maximal contractile work at 6.9 +/- 1.3 mm (mean +/- s.d.; n = 8) and subsequently declined at a rate of 0.009 +/- 0.001 mm s(1). It was next tested whether the current knowledge of the kinetic controls in the glycolytic pathway in muscle integrated in the Lambeth and Kushmerick computational model of skeletal muscle glycolysis explained the experimental data. It was found that the model underestimated the magnitude of deactivation of the glycolytic pathway in resting muscle, resulting in depletion of glycolytic intermediates and substrate for oxidative ATP synthesis. Numerical analysis of the model identified phosphofructokinase and pyruvate kinase as the kinetic control sites involved in deactivation of the glycolytic pathway. Ancillary 100-fold inhibition of both phosphofructokinase and pyruvate kinase was found necessary to predict glycolytic intermediate and ADP concentrations correctly in resting human muscle. Incorporation of this information into the model resulted in highly improved agreement between predicted and measured in vivo dynamics of hexose monophosphates in muscle following contraction. We concluded that silencing of the glycolytic pathway in muscle following contraction is most likely to be mediated by phosphofructokinase and pyruvate kinase inactivation on a time scale of seconds and minutes, respectively, and is necessary to prevent depletion of vital cellular substrates.
Figures

Recovery condition model (A), original Lambeth and Kushmerick model (B), resting condition model (C).

The spectrum at rest (A), end of exercise (B), 40s into recovery (C) and 240s into recovery (D) are shown. Spectra were apodized with a 10Hz lorentzian function. Signal intensity is expressed in arbitrary units.

The vertical solid black lines separate the data points of the three different workloads and recovery period. The error bars indicate the standard deviation (n=8). The [PCr] • and [Pi] □ (A), [PME] Δ (B), [ATP] ○ and [total phosphate pool] ▪ (C), pH ♦ (D), are shown. The part of the data analyzed with the computational model is indicated by a black bar.

The solution space is indicated by the mean ± SD of the 5000 simulations that were run in a Monte Carlo approach.

Model predictions of HMP dynamics were calculated by summation of G1P, G6P and F6P dynamics. The solution space is indicated by the mean ± SD of the 5000 simulations that were run in a Monte Carlo approach. Experimental data represent the pooled results of all eight subjects, error bars indicate standard deviation (n=8).

Inhibition of the enzyme activity was modeled by setting Vmax values to 5%. The predictions of the original model are shown as a darker bar. The shaded area represents the physiological range and the horizontal solid black line indicates the mean value, as listed in table 2.

The solution space is indicated by the mean ± SD of the 5000 simulations that were run in a Monte Carlo approach.

The solution space is indicated by the mean ± SD deviation of the 5000 simulations that were run in a Monte Carlo approach.

Model predictions of HMP dynamics were calculated by summation of G1P, G6P and F6P dynamics. The solution space is indicated by the mean ± SD of the 5000 simulations that were run in a Monte Carlo approach. Experimental data (▲) represent the pooled results of all eight subjects (n=8), error bars were omitted for clarity of presentation. The value of the steady state G6P, F-1,6P2 and ADP relative to literature values were calculated by dividing steady state model predictions by the mean value reported in literature as listed in table 2.
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