Stein L A, Schwarz R P, Chock P B, Eisenberg E
Biochemistry. 1979 Sep 4;18(18):3895-909. doi: 10.1021/bi00585a009.
We have investigated the steps in the actomyosin ATPase cycle that determine the maximum ATPase rate (Vmax) and the binding between myosin subfragment one (S-1) and actin which occurs when the ATPase activity is close to Vmax. We find that the forward rate constant of the initial ATP hydrolysis (initial Pi burst) is about 5 times faster than the maximum turnover rate of the actin S-1 ATPase. Thus, another step in the cycle must be considerably slower than the forward rate of the initial Pi burst. If this slower step occurs only when S-1 is complexed with actin, as originally predicted by the Lymn-Taylor model, the ATPase activity and the fraction of S-1 bound to actin in the steady state should increase almost in parallel as the actin concentration is increased. As measured by turbidity determined in the stopped-flow apparatus, the fraction of S-1 bound to actin, like the ATPase activity, shows a hyperbolic dependence on actin concentration, approaching 100% asymptotically. However, the actin concentration required so that 50% of the S-1 is bound to actin is about 4 times greater than the actin concentration required for half-maximal ATPase activity. Thus, as previously found at 0 degrees C, at 15 degrees C much of the S-1 is dissociated from actin when the ATPase is close to Vmax, showing that a slow first-order transition which follows the initial Pi burst (the transition from the refractory to the nonrefractory state) must be the slowest step in the ATPase cycle. Stopped-flow studies also reveal that the steady-state turbidity level is reached almost instantaneously after the S-1, actin, and ATP are mixed, regardless of the order of mixing. Thus, the binding between S-1 and actin which is observed in the steady state is due to a rapid equilibrium between S-1--ATP and acto--S-1--ATP which is shifted toward acto-S-1--ATP at high actin concentration. Furthermore, both S-1--ATP and S-1--ADP.Pi (the state occurring immediately after the initial Pi burst) appear to have the same binding constant to actin. Thus, at high actin concentration both S-1--ATP and S-1--ADP.Pi are in rapid equilibrium with their respective actin complexes. Although at very high actin concentration almost complete binding of S-1--ATP and S-1--ADP.Pi to actin occurs, there is no inhibition of the ATPase activity at high actin concentration. This strongly suggests that both the initial Pi burst and the slow rate-limiting transition which follows (the transition from the refractory to the nonrefractory state) occur at about the same rates whether the S-1 is bound to or dissociated from actin. We, therefore, conclude that S-1 does not have to dissociate from actin each time an ATP molecule is hydrolyzed.
我们研究了肌动球蛋白ATP酶循环中决定最大ATP酶速率(Vmax)以及肌球蛋白亚片段1(S-1)与肌动蛋白之间结合的步骤,这种结合发生在ATP酶活性接近Vmax时。我们发现初始ATP水解的正向速率常数(初始Pi爆发)比肌动蛋白S-1 ATP酶的最大周转速率快约5倍。因此,循环中的另一步必定比初始Pi爆发的正向速率慢得多。如果这个较慢的步骤仅在S-1与肌动蛋白形成复合物时发生,正如Lymn-Taylor模型最初所预测的那样,那么随着肌动蛋白浓度增加,稳态下的ATP酶活性和与肌动蛋白结合的S-1比例应几乎平行增加。通过停流装置中测定的浊度来衡量,与肌动蛋白结合的S-1比例,如同ATP酶活性一样,对肌动蛋白浓度呈双曲线依赖关系,渐近地接近100%。然而,使50%的S-1与肌动蛋白结合所需的肌动蛋白浓度大约是半最大ATP酶活性所需肌动蛋白浓度的4倍。因此,正如之前在0℃时所发现的,在15℃下当ATP酶接近Vmax时,许多S-1会从肌动蛋白上解离,这表明在初始Pi爆发之后的一个缓慢的一级转变(从不应期到非不应期的转变)必定是ATP酶循环中最慢的步骤。停流研究还表明,在S-1、肌动蛋白和ATP混合后,几乎瞬间就达到了稳态浊度水平,而与混合顺序无关。因此,在稳态下观察到的S-1与肌动蛋白之间的结合是由于S-1-ATP和肌动蛋白-S-1-ATP之间的快速平衡,在高肌动蛋白浓度下该平衡向肌动蛋白-S-1-ATP方向移动。此外,S-1-ATP和S-1-ADP·Pi(初始Pi爆发后立即出现的状态)似乎与肌动蛋白具有相同的结合常数。因此,在高肌动蛋白浓度下,S-1-ATP和S-1-ADP·Pi都与其各自的肌动蛋白复合物处于快速平衡状态。尽管在非常高的肌动蛋白浓度下,S-1-ATP和S-1-ADP·Pi几乎完全与肌动蛋白结合,但在高肌动蛋白浓度下ATP酶活性并未受到抑制。这有力地表明,无论S-1与肌动蛋白结合还是解离,初始Pi爆发以及随后的缓慢限速转变(从不应期到非不应期的转变)都以大致相同的速率发生。因此,我们得出结论,每次ATP分子水解时,S-1并不一定必须从肌动蛋白上解离。