School of Biomedical Sciences, Faculty of Biological Sciences, University of Leeds, Leeds, UK.
J Physiol. 2013 Feb 1;591(3):731-44. doi: 10.1113/jphysiol.2012.241992. Epub 2012 Nov 19.
The mechanisms controlling skeletal muscle oxygen consumption (V(o)₂) during exercise are not well understood. We determined whether first-order control could explain V(o)₂kinetics at contractions onset (V(o)₂(on)) and cessation (V(o)₂off)) in single skeletal muscle fibres differing in oxdidative capacity, and across stimulation intensities up to V(o)₂(max). Xenopus laevis fibres (n = 21) were suspended in a sealed chamber with a fast response P(o)₂ electrode to measure V(o)₂ every second before, during and after stimulated isometric contractions. A first-order model did not well characterize on-transient V(o)₂ kinetics. Including a time delay (TD) in the model provided a significantly improved characterization than a first-order fit without TD (F-ratio; P < 0.05), and revealed separate 'activation' and 'exponential' phases in 15/21 fibres contracting at V(o)₂(max) (mean ± SD TD: 14 ± 3s). On-transient kinetics (τV(o)₂(on)) was weakly and linearly related to V(o)₂(max) (R² = 0.271, P = 0.015). Off-transient kinetics, however, were first-order, and τV(o)₂(off) was greater in low-oxidative (V(o)₂max < 0.05 nmol mm⁻³s⁻¹ than high-oxidative fibres (V(o)₂(max > 0.10 nmol mm ⁻³ s⁻¹; 170 ± 70 vs. 29 ± 6 s, P < 0.001). 1/ τV(o)₂(off) was proportional to V(o)₂(max) (R² = 0.727, P < 0.001), unlike in the on-transient. The calculated oxygen deficit was larger (P < 0.05) than the post-contraction volume of consumed oxygen at all intensities except V(o)₂(max). These data show a clear dissociation between the kinetic control of V(o)₂at the onset and cessation of contractions and across stimulation intensities. More complex models are therefore required to understand the activation of mitochondrial respiration in skeletal muscle at the start of exercise.
运动时控制骨骼肌耗氧量(V(o)₂)的机制尚不清楚。我们确定了一级控制是否可以解释在不同氧化能力的单个骨骼肌纤维和刺激强度高达 V(o)₂(max)的情况下,收缩起始(V(o)₂(on))和终止(V(o)₂off)时的 V(o)₂动力学。使用快速响应 P(o)₂电极,将非洲爪蟾纤维(n = 21)悬挂在密封室中,在刺激等长收缩之前、期间和之后每秒测量一次 V(o)₂。一阶模型不能很好地描述瞬变 V(o)₂动力学。在模型中包含时间延迟(TD)比不包含 TD 的一阶拟合提供了更好的特征描述(F 比;P < 0.05),并且在 15/21 条在 V(o)₂(max)下收缩的纤维中揭示了单独的“激活”和“指数”阶段(平均 ± SD TD:14 ± 3s)。瞬变动力学(τV(o)₂(on))与 V(o)₂(max)呈弱线性关系(R² = 0.271,P = 0.015)。然而,瞬变动力学是一阶的,并且 τV(o)₂(off)在低氧化(V(o)₂max < 0.05 nmol mm⁻³s⁻¹)纤维中大于高氧化纤维(V(o)₂(max > 0.10 nmol mm ⁻³ s⁻¹;170 ± 70 比 29 ± 6 s,P < 0.001)。1/τV(o)₂(off)与 V(o)₂(max)成比例(R² = 0.727,P < 0.001),与瞬变相反。除了 V(o)₂(max)之外,在所有强度下,计算出的氧亏大于收缩后消耗的氧的体积(P < 0.05)。这些数据表明,在收缩起始和终止时以及在不同刺激强度下,V(o)₂的动力学控制之间存在明显的分离。因此,需要更复杂的模型来了解运动开始时骨骼肌线粒体呼吸的激活。