LEF-1高迁移率组盒采用无dna形式的残余结构

IF 2.624
T. Reid Alderson , Hermann Habacher , Benjamin Bourgeois , Tobias Madl
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引用次数: 1

摘要

内在无序区(IDRs)缺乏稳定的三级结构,而是在不同构象之间快速相互转换。这种结构可塑性使idr在细胞信号通路中发挥关键作用。转录因子在idr中丰富,其中许多在DNA或其他结合伙伴的存在下被稳定或获得三级结构。以t细胞因子/淋巴细胞增强因子结合因子1 (TCF/ lev -1)转录因子为模型系统,我们表征了缺乏DNA时高迁移基团(HMG)结构域的结构和动力学。包含在HMG结构域侧面的idr导致蛋白质的溶解度增强。次级13Cα化学位移、1H核Overhauser效应、15N自旋弛豫和1HN溶剂顺磁弛豫增强表明,HMG结构域的三个螺旋取向与蛋白质的dna结合形式相似。相比之下,侧翼的idr没有显示出结构的证据。螺旋1和螺旋3在无DNA构象中似乎不太稳定,这表明在没有DNA的情况下存在某种形式的构象交换或局部运动。鉴于TCF/LEF转录因子家族的高度序列保守性,我们的结果应该适用于该家族的其他成员。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

The LEF-1 high-mobility group box adopts residual structure in its DNA-free form

The LEF-1 high-mobility group box adopts residual structure in its DNA-free form

Intrinsically disordered regions (IDRs) lack stable tertiary structure and instead rapidly interconvert between different conformations. This structural plasticity enables IDRs to act as key players in cellular signaling pathways. Transcription factors are enriched in IDRs, many of which are stabilized by or acquire tertiary structure in the presence of DNA or other binding partners. Using the T-cell factor/lymphoid enhancer binding factor 1 (TCF/LEF-1) transcription factor as a model system, we characterized the structure and dynamics of the high-mobility group (HMG) domain in the absence of DNA. Inclusion of the IDRs that flank the HMG domain led to enhanced solubility of the protein. Secondary 13Cα chemical shifts, 1H nuclear Overhauser effects, 15N spin relaxation, and 1HN solvent paramagnetic relaxation enhancements indicate that the three helices in the HMG domain are oriented similarly to the DNA-bound form of the protein. By contrast, the flanking IDRs do not show evidence of structure. Helix 1 and helix 3 appear to be less stable in the DNA-free conformation, indicating some form of conformational exchange or local motion in the absence of DNA. Given the high degree of sequence conservation in the TCF/LEF family of transcription factors, our results should apply to other members of the family.

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CiteScore
1.90
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