Palmer Bradley M, Suzuki Takeki, Wang Yuan, Barnes William D, Miller Mark S, Maughan David W
Department of Molecular Physiology and Biophysics, University of Vermont, Burlington, Vermont, USA.
Biophys J. 2007 Aug 1;93(3):760-9. doi: 10.1529/biophysj.106.101626. Epub 2007 May 11.
The force response of activated striated muscle to length perturbations includes the so-called C-process, which has been considered the frequency domain representation of the fast single-exponential force decay after a length step (phases 1 and 2). The underlying molecular mechanisms of this phenomenon, however, are still the subject of various hypotheses. In this study, we derived analytical expressions and created a corresponding computer model to describe the consequences of independent acto-myosin cross-bridges characterized solely by 1), intermittent periods of attachment (t(att)) and detachment (t(det)), whose values are stochastically governed by independent probability density functions; and 2), a finite Hookian stiffness (k(stiff)) effective only during periods of attachment. The computer-simulated force response of 20,000 (N) cross-bridges making up a half-sarcomere (F(hs)(t)) to sinusoidal length perturbations (L(hs)(t)) was predicted by the analytical expression in the frequency domain, (F(hs)(omega)/L(hs)(omega))=(t(att)/t(cycle))Nk(stiff)(iomega/(t(att)(-1)+iomega)), where t(att) = mean value of t(att), t(cycle) = mean value of t(att) + t(det), k(stiff) = mean stiffness, and omega = 2pi x frequency of perturbation. The simulated force response due to a length step (L(hs)) was furthermore predicted by the analytical expression in the time domain, F(hs)(t)=(t(att)/t(cycle))Nk(stiff)L(hs)e(-t/t(att)). The forms of these analytically derived expressions are consistent with expressions historically used to describe these specific characteristics of a force response and suggest that the cycling of acto-myosin cross-bridges and their associated stiffnesses are responsible for the C-process and for phases 1 and 2. The rate constant 2pic, i.e., the frequency parameter of the historically defined C-process, is shown here to be equal to t(att)(-1). Experimental results from activated cardiac muscle examined at different temperatures and containing predominately alpha- or beta-myosin heavy chain isoforms were found to be consistent with the above interpretation.
活化横纹肌对长度扰动的力响应包括所谓的C过程,该过程被认为是长度阶跃后快速单指数力衰减(阶段1和阶段2)的频域表示。然而,这一现象的潜在分子机制仍然是各种假说的主题。在本研究中,我们推导了解析表达式并创建了相应的计算机模型,以描述仅由以下特征表征的独立肌动球蛋白横桥的结果:1)附着(t(att))和脱离(t(det))的间歇期,其值由独立概率密度函数随机控制;2)仅在附着期有效的有限胡克刚度(k(stiff))。由20,000个(N)构成半个肌节的横桥(F(hs)(t))对正弦长度扰动(L(hs)(t))的计算机模拟力响应,通过频域解析表达式预测,(F(hs)(omega)/L(hs)(omega))=(t(att)/t(cycle))Nk(stiff)(iomega/(t(att)(-1)+iomega)),其中t(att) = t(att)的平均值,t(cycle) = t(att) + t(det)的平均值,k(stiff) = 平均刚度,omega = 2π×扰动频率。此外,由长度阶跃(L(hs))引起的模拟力响应通过时域解析表达式预测,F(hs)(t)=(t(att)/t(cycle))Nk(stiff)L(hs)e(-t/t(att))。这些解析推导表达式的形式与历史上用于描述力响应这些特定特征的表达式一致,并表明肌动球蛋白横桥的循环及其相关刚度是C过程以及阶段1和阶段2的原因。这里显示历史定义的C过程的频率参数速率常数2πc等于t(att)(-1)。在不同温度下检查的、主要含有α或β肌球蛋白重链同工型的活化心肌的实验结果与上述解释一致。