Highsmith S, Eden D
Biochemistry. 1987 May 19;26(10):2747-50. doi: 10.1021/bi00384a014.
The effects of limited trypsinolysis of myosin subfragment 1 (S1) on its structural dynamics were investigated by using the method of transient electric birefringence. Conversion of S1 by trypsin to produce S1 (T) did not change the specific Kerr constant [(8.1 +/- 0.3) X 10(-7) and (8.0 +/- 0.3) X 10(-7) cm2/statvolt2 for S1(T) and S1, respectively] or the degree of alignment in a weak electric field, suggesting that the size of S1 and its permanent electric dipole moment are not modified by trypsin. On the other hand, the relaxation time for the field-free rotation, after achieving a steady-state birefringence signal, was reduced from 316 ns for S1 to 269 ns for S1(T), at 3.7 degrees C, suggesting that trypsinolysis increases the flexibility of the connections between S1 segments or introduces additional segmental motions. For both S1 and S1(T), the rate of decay for a steady-state signal was independent of the field strength, between 3.34 and 20.3 statvolt/cm. Shortening the duration of the weak electric field pulses to 0.35 microseconds, so that steady-state signals were not achieved, decreased the relaxation times for S1 and S1(T) to 240 and 210 ns, respectively, which is consistent with the segmented flexible S1 structure proposed earlier [Highsmith, S., & Eden, D. (1986) Biochemistry 25, 2237]. When the strength of the electric field was increased to above 10 statvolt/cm, in order to make the interaction energy for the S1(T) electric dipole moment in the electric field greater than the thermal energy, the relaxation time after a 0.35-microseconds pulse decreased from 210 to 170 ns as the field was increased from 7 to 20 statvolt/cm. (ABSTRACT TRUNCATED AT 250 WORDS)
采用瞬态电双折射方法研究了肌球蛋白亚片段1(S1)有限胰蛋白酶解对其结构动力学的影响。胰蛋白酶将S1转化为S1(T),并未改变比克尔常数[S1(T)和S1分别为(8.1±0.3)×10⁻⁷和(8.0±0.3)×10⁻⁷ cm²/statvolt²]或在弱电场中的排列程度,这表明胰蛋白酶不会改变S1的大小及其永久电偶极矩。另一方面,在3.7℃下,达到稳态双折射信号后,无场旋转弛豫时间从S1的316 ns降至S1(T)的269 ns,这表明胰蛋白酶解增加了S1各片段间连接的灵活性或引入了额外的片段运动。对于S1和S1(T),在3.34至20.3 statvolt/cm之间,稳态信号的衰减速率与场强无关。将弱电场脉冲持续时间缩短至0.35微秒,使得未达到稳态信号,S1和S1(T)的弛豫时间分别降至240和210 ns,这与之前提出的S1分段柔性结构一致[Highsmith, S., & Eden, D. (1986) Biochemistry 25, 2237]。当电场强度增加到10 statvolt/cm以上,以使电场中S1(T)电偶极矩的相互作用能大于热能时,0.35微秒脉冲后的弛豫时间随着场强从7 statvolt/cm增加到20 statvolt/cm而从210 ns降至170 ns。(摘要截断于250字)