Akerman B, Jonsson M, Nordén B, Lalande M
Biopolymers. 1989 Sep;28(9):1541-71. doi: 10.1002/bip.360280906.
The understanding, on a molecular level, of the mechanisms responsible for the improved separation in DNA gel electrophoresis when using modulated electric fields requires detailed information about conformational distribution and dynamics in the DNA/gel system. The orientational order due to electrophoretic migration ("electrophoretic orientation") is an interesting piece of information in this context that can be obtained through linear dichroism spectroscopy [M. Jonsson, B. Akerman, and B. Nordén, (1988) Biopolymers 27, 381-414]. The technique permits measurement of the orientation factor S of DNA (S = 1 corresponds to perfect orientation) within an electrophoretic zone in the gel during the electrophoresis. It is reported that the degree of orientation of T2 DNA [170 kilo base pairs (kpb)] is considerable (S = 0.17 in 1% agarose at 10 V/cm) compared to relatively modest orientations of short fragments found earlier (for 23-kbp DNA, S = 0.03 in 1% agarose at 10 V/cm), showing that large DNA coils are substantially deformed during the migration. Growth and relaxation dynamics of the orientational order of the T2 DNA are also reported, as functions of gel concentration (0.3-2%), electric field strength (0-40 V/cm), and pulse characteristics. The rise profile of the DNA orientation, when applying a constant field, is a nonmonotonic function that displays a pronounced overshoot, followed by a minor undershoot, before it reaches steady-state orientation (after 12 s in 1% agarose, 9 V/cm). The orientational relaxation in absence of field shows a multiexponential decay in a time region of some 10 s, when most of the DNA anisotropy has disappeared. A surprising phenomenon is a memory over minutes of the DNA/gel system to previous pulses: with two consecutive rectangular pulses (of the same polarity), the orientational overshoot and undershoot as a response to the second pulse are significantly reduced compared to the first pulse. The time required to recover 90% of their amplitudes is typically 1200 s (1% agarose, 9 V/cm), which may be compared to the time required to relax 90% of the DNA orientation, which is only 6 s. The major part of the over- and undershoot recovery is thus a reorganization of a system in which DNA is already randomly oriented. The different response amplitudes and relaxation times, including the amplitude and recovery time of the overshoot, of the orientational order of DNA in the electrophoretic gel have been studied as functions of gel concentration and field strength. The results are discussed against relevant theories of polymer dynamics.
要从分子层面理解在使用调制电场时DNA凝胶电泳中分离效果改善的机制,需要详细了解DNA/凝胶系统中的构象分布和动力学信息。在这种情况下,由于电泳迁移导致的取向有序性(“电泳取向”)是一个有趣的信息,可以通过线性二色光谱法获得[M. 琼森、B. 阿克曼和B. 诺登,(1988年)《生物聚合物》27卷,381 - 414页]。该技术能够在电泳过程中测量凝胶中电泳区域内DNA的取向因子S(S = 1表示完美取向)。据报道,与早期发现的短片段相对较小的取向相比,T2 DNA[170千碱基对(kpb)]的取向程度相当可观(在1%琼脂糖中,10 V/cm时S = 0.17)(对于23 - kbp DNA,在1%琼脂糖中,10 V/cm时S = 0.03),这表明大的DNA线圈在迁移过程中会发生显著变形。还报道了T2 DNA取向有序性的增长和弛豫动力学,作为凝胶浓度(0.3 - 2%)、电场强度(0 - 40 V/cm)和脉冲特性的函数。当施加恒定电场时,DNA取向的上升曲线是一个非单调函数,在达到稳态取向之前(在1%琼脂糖中,9 V/cm时12秒后)会出现明显的过冲,随后有一个小的下冲。在无电场时的取向弛豫在大约10秒的时间区域内呈现多指数衰减,此时大部分DNA各向异性已经消失。一个令人惊讶的现象是DNA/凝胶系统对先前脉冲有长达数分钟的记忆:对于两个连续的矩形脉冲(相同极性),与第一个脉冲相比,作为对第二个脉冲的响应,取向过冲和下冲会显著减小。恢复其幅度的90%所需的时间通常为1200秒(1%琼脂糖,9 V/cm),这可以与使DNA取向弛豫90%所需的时间(仅6秒)进行比较。因此,过冲和下冲恢复的主要部分是一个DNA已经随机取向的系统的重组。已经研究了电泳凝胶中DNA取向有序性的不同响应幅度和弛豫时间,包括过冲的幅度和恢复时间,作为凝胶浓度和场强的函数。根据聚合物动力学的相关理论对结果进行了讨论。