Palmer Bradley M, Wang Yuan, Miller Mark S
Department of Molecular Physiology and Biophysics, University of Vermont, 122 HSRF, Beaumont Avenue, Burlington, VT 05405, USA.
J Biomed Biotechnol. 2011;2011:592343. doi: 10.1155/2011/592343. Epub 2011 Nov 17.
We demonstrate that viscoelastic mechanics of striated muscle, measured as elastic and viscous moduli, emerge directly from the myosin crossbridge attachment time, t(att), also called time-on. The distribution of t(att) was modeled using a gamma distribution with shape parameter, p, and scale parameter, β. At 5 mM MgATP, β was similar between mouse α-MyHC (16.0 ± 3.7 ms) and β-MyHC (17.9 ± 2.0 ms), and p was higher (P < 0.05) for β-MyHC (5.6 ± 0.4 no units) compared to α-MyHC (3.2 ± 0.9). At 1 mM MgATP, p approached a value of 10 in both isoforms, but β rose only in the β-MyHC (34.8 ± 5.8 ms). The estimated mean t(att) (i.e., pβ product) was longer in the β-MyHC compared to α-MyHC, and became prolonged in both isoforms as MgATP was reduced as expected. The application of our viscoelastic model to these isoforms and varying MgATP conditions suggest that t(att) is better modeled as a gamma distribution due to its representing multiple temporal events occurring within t(att) compared to a single exponential distribution which assumes only one temporal event within t(att).
我们证明,横纹肌的粘弹性力学,以弹性模量和粘性模量来衡量,直接源自肌球蛋白横桥附着时间t(att),也称为作用时间。t(att)的分布采用形状参数为p、尺度参数为β的伽马分布进行建模。在5 mM MgATP条件下,小鼠α - 肌球蛋白重链(α - MyHC,16.0 ± 3.7 ms)和β - 肌球蛋白重链(β - MyHC,17.9 ± 2.0 ms)之间的β相似,而与α - MyHC(3.2 ± 0.9)相比,β - MyHC的p更高(P < 0.05)(5.6 ± 0.4,无单位)。在1 mM MgATP条件下,两种同工型的p均接近10,但β仅在β - MyHC中升高(34.8 ± 5.8 ms)。与α - MyHC相比,β - MyHC中估计的平均t(att)(即pβ乘积)更长,并且正如预期的那样,随着MgATP减少,两种同工型的t(att)都延长。将我们的粘弹性模型应用于这些同工型和不同的MgATP条件表明,t(att)更适合用伽马分布建模,因为与仅假设t(att)内有一个时间事件的单指数分布相比,它代表了t(att)内发生的多个时间事件。