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通过荧光共振能量转移观察到的肌动蛋白中的结构域运动。

Domain motion in actin observed by fluorescence resonance energy transfer.

作者信息

Miki M, Kouyama T

机构信息

Department of Applied Chemistry and BioTechnology, Fukui University, Japan.

出版信息

Biochemistry. 1994 Aug 23;33(33):10171-7. doi: 10.1021/bi00199a045.

DOI:10.1021/bi00199a045
PMID:8060983
Abstract

Actin is composed of two well-separated globular domains which are further subdivided into two subdomains [Kabsch, W., Mannherz, H. G., Suck, D., Pai, E. F., & Holmes, K. C. (1990) Nature 347, 37-44]. Subdomains 1 and 2 constitute the small domain, and subdomains 3 and 4 comprise the large domain. In order to test a hinge bending domain motion in actin such as observed in many kinases, fluorescence resonance energy transfer between two probes attached to each of the two domains was measured by steady-state and time-resolved fluorometers. The adenine base is bound in a hydrophobic pocket between subdomains 3 and 4, and Tyr-69 is located at subdomain 2. In the present study, the adenine moiety was labeled with a fluorescence donor, epsilon ATP, and tyrosine-69 was labeled with the energy acceptor, dansyl chloride. Assuming the random orientation factor k2 = 2/3, the distance between epsilon-adenine moiety and dansyl chloride attached to Tyr-69 in G-actin was determined to be 2.46 nm from steady-state fluorescence measurements. The addition of DNase I did not appreciably change the distance (less than 0.1 nm). The distance decreased to 2.27 nm during polymerization by the addition of phalloidin under physiological salt conditions. On the other hand, time-resolved fluorescence energy transfer measurements have been used to investigate a distribution of distances for a donor-acceptor pair. In G-actin, the mean distance between probes was 2.79 nm with a full width at half-maximum of 3.91 nm, indicating a large number of conformational substates in solution.(ABSTRACT TRUNCATED AT 250 WORDS)

摘要

肌动蛋白由两个相距较远的球状结构域组成,这两个结构域又进一步细分为两个亚结构域[卡布斯,W.,曼赫茨,H. G.,萨克,D.,派,E. F.,& 霍姆斯,K. C.(1990年)《自然》347卷,37 - 44页]。亚结构域1和2构成小结构域,亚结构域3和4组成大结构域。为了测试肌动蛋白中是否存在如在许多激酶中观察到的铰链弯曲结构域运动,通过稳态和时间分辨荧光计测量了连接到两个结构域各自的两个探针之间的荧光共振能量转移。腺嘌呤碱基结合在亚结构域3和4之间的疏水口袋中,而酪氨酸 - 69位于亚结构域2。在本研究中,腺嘌呤部分用荧光供体ε - ATP标记,酪氨酸 - 69用能量受体丹磺酰氯标记。假设随机取向因子k₂ = 2/3,通过稳态荧光测量确定G - 肌动蛋白中ε - 腺嘌呤部分与连接到酪氨酸 - 69的丹磺酰氯之间的距离为2.46纳米。添加脱氧核糖核酸酶I并没有明显改变该距离(小于0.1纳米)。在生理盐条件下添加鬼笔环肽进行聚合时,距离减小到2.27纳米。另一方面,时间分辨荧光能量转移测量已用于研究供体 - 受体对的距离分布。在G - 肌动蛋白中,探针之间的平均距离为2.79纳米,半高宽为3.91纳米,表明溶液中存在大量构象亚态。(摘要截短于250字)

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