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琼脂糖凝胶的瞬态电双折射。II. 反向电场及与其他聚合物凝胶的比较。

Transient electric birefringence of agarose gels. II. Reversing electric fields and comparison with other polymer gels.

作者信息

Stellwagen J, Stellwagen N C

机构信息

Department of Biochemistry, University of Iowa, Iowa City 52242.

出版信息

Biopolymers. 1994 Sep;34(9):1259-73. doi: 10.1002/bip.360340914.

Abstract

The transient electric birefringence of low electroendosmosis (LE) agarose gels oriented by pulsed unidirectional electric fields was described in detail in Part I [J. Stellwagen and N. C. Stellwagen (1994), Biopolymers, Vol. 34, p. 187]. Here, the birefringence of LE agarose gels in rapidly reversing electric fields, similar in amplitude and duration to those used for field inversion gel electrophoresis, is reported. Symmetric reversing electric fields cause the sign of the birefringence of LE agarose gels, and hence the direction of orientation of the agarose fibers, to oscillate in phase with the applied electric field. Because of long-lasting memory effects, the alternating sign of the birefringence appears to be due to metastable changes in gel structure induced by the electric field. If the reversing field pulses are equal in amplitude but different in duration, the orientation behavior depends critically on the applied voltage. If E < 7 V/cm, the amplitude of the birefringence gradually decreases with increasing pulse number and becomes unmeasurably small. However, if E > 7 V/cm, the amplitude of the birefringence increases more than 10-fold after approximately 20 pulses have been applied to the gel, suggesting that a cooperative change in gel structure has occurred. Because there is no concomitant change in the relaxation times of the orienting particles, the large increase in the amplitude of the birefringence must be due to an increase in the number of agarose fibers and/or fiber bundles orienting in the electric field, which in turn indicates a cooperative breakdown of the noncovalent "junction zones" that cross-link the fibers into the gel matrix. The sign of the birefringence of LE agarose gels is always positive after extensive junction zone breakdown, indicating that the agarose fibers and fiber bundles preferentially orient parallel to the electric field when they are freed from the constraints of the gel matrix. Three other gel-forming polymers, high electroendosmosis (HEEO) agarose (a more highly charged agarose), beta-carrageenan (a stereoisomer of agarose), and polyacrylamide (a chemically cross-linked polymer) were also studied in unidirectional and rapidly reversing electric fields. The birefringence of HEEO agarose gels in reversing fields is very similar to that of LE agarose gels, suggesting that the orientation anomalies are not due to the occasional charged residues on the agarose backbone chain. The beta-carrageenan gels exhibit variable orientation behavior in reversing electric fields, suggesting that its internal gel structure is not as tightly interconnected as that of agarose gels.(ABSTRACT TRUNCATED AT 400 WORDS)

摘要

第一部分[J. 斯特尔瓦根和N. C. 斯特尔瓦根(1994年),《生物聚合物》,第34卷,第187页]详细描述了由脉冲单向电场取向的低电渗(LE)琼脂糖凝胶的瞬态电双折射。本文报道了LE琼脂糖凝胶在快速反向电场中的双折射情况,该电场的幅度和持续时间与用于场反转凝胶电泳的电场相似。对称的反向电场会使LE琼脂糖凝胶双折射的符号,进而使琼脂糖纤维的取向方向,与施加的电场同相振荡。由于存在持久的记忆效应,双折射交替出现的符号似乎是由电场引起的凝胶结构的亚稳态变化所致。如果反向场脉冲的幅度相等但持续时间不同,取向行为将严重依赖于所施加的电压。如果E < 7 V/cm,双折射的幅度会随着脉冲数的增加而逐渐减小,直至变得小到无法测量。然而,如果E > 7 V/cm,在向凝胶施加大约20个脉冲后,双折射的幅度会增加10倍以上,这表明凝胶结构发生了协同变化。由于取向颗粒的弛豫时间没有伴随变化,双折射幅度的大幅增加必定是由于在电场中取向的琼脂糖纤维和/或纤维束数量增加,这反过来表明将纤维交联到凝胶基质中的非共价“连接区”发生了协同破坏。在广泛的连接区破坏之后,LE琼脂糖凝胶双折射的符号始终为正,这表明当琼脂糖纤维和纤维束从凝胶基质的限制中解放出来时,它们优先平行于电场取向。还对另外三种凝胶形成聚合物进行了研究,即高电渗(HEEO)琼脂糖(一种电荷更高的琼脂糖)、β-角叉菜胶(琼脂糖的一种立体异构体)和聚丙烯酰胺(一种化学交联聚合物),研究了它们在单向和快速反向电场中的情况。HEEO琼脂糖凝胶在反向电场中的双折射与LE琼脂糖凝胶非常相似,这表明取向异常并非由于琼脂糖主链上偶尔出现的带电残基。β-角叉菜胶凝胶在反向电场中表现出可变的取向行为,这表明其内部凝胶结构不像琼脂糖凝胶那样紧密相连。(摘要截选至400字)

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