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Molecular dynamics simulation of Kv channel voltage sensor helix in a lipid membrane with applied electric field.

机译:施加电场的脂质膜中Kv通道电压传感器螺旋的分子动力学模拟。

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In this article, we present the results of the molecular dynamics simulations of amphiphilic helix peptides of 13 amino-acid residues, placed at the lipid-water interface of dipalmitoylphosphatidylcholine bilayers. The peptides are identical with, or are derivatives of, the N-terminal segment of the S4 helix of voltage-dependent K channel KvAP, containing four voltage-sensing arginine residues (R1-R4). Upon changing the direction of the externally applied electric field, the tilt angle of the wild-type peptide changes relative to the lipid-water interface, with the N-terminus heading up with an outward electric field. These movements were not observed using an octane membrane in place of the dipalmitoylphosphatidylcholine membrane, and were markedly suppressed by 1), substituting Phe located one residue before the first arginine (R1) with a hydrophilic residue (Ser, Thr); or 2), changing the periodicity rule of Rs from at-every-third to at-every-fourth position; or 3), replacing R1 with a lysine residue (K). These and other findings suggest that the voltage-dependent movement requires deep positioning of Rs when the resting (inward) electric field is present. Later, we performed simulations of the voltage sensor domain (S1-S4) of Kv1.2 channel. In simulations with a strong electric field (0.1 Vm or above) and positional restraints on the S1 and S2 helices, S4 movement was observed consisting of displacement along the S4 helix axis and a screwlike axial rotation. Gating-charge-carrying Rs were observed to make serial interactions with E183 in S1 and E226 in S2, in the outer water crevice. A 30-ns-backward simulation started from the open-state model gave rise to a structure similar to the recent resting-state model, with S4 moving vertically approximately 6.7 A. The energy landscape around the movement of S4 appears very ragged due to salt bridges formed between gating-charge-carrying residues and negatively charged residues of S1, S2, and S3 helices. Overall, features of S3 and S4 movements are consistent with the recent helical-screw model. Both forward and backward simulations show the presence of at least two stable intermediate structures in which R2 and R3 form salt bridges with E183 or E226, respectively. These structures are the candidates for the states postulated in previous gating kinetic models, such as the Zagotta-Hoshi-Aldrich model, to account for more than one transition step per subunit for activation.
机译:在本文中,我们介绍了13个氨基酸残基的两亲性螺旋肽的分子动力学模拟结果,该肽位于二棕榈酰磷脂酰胆碱双层的脂质-水界面。这些肽与电压依赖性K通道KvAP的S4螺旋的N末端区段相同或为其衍生物,其中包含四个电压感应精氨酸残基(R1-R4)。在改变外部施加的电场的方向时,野生型肽的倾斜角相对于脂质-水界面而改变,其中N端朝向向外的电场。用辛烷膜代替二棕榈酰磷脂酰胆碱膜未观察到这些运动,并被1)显着抑制,用位于亲水性残基(Ser,Thr)的第一个精氨酸(R1)之前的一个残基取代Phe;或2),将Rs的周期性规则从第三位置更改为第四位置;或者或3),将R1替换为赖氨酸残基(K)。这些和其他发现表明,当存在静止(向内)电场时,电压相关运动需要对Rs进行深度定位。之后,我们对Kv1.2通道的电压传感器域(S1-S4)进行了仿真。在具有强电场(0.1 V / nm或更高)并且在S1和S2螺旋上有位置限制的模拟中,观察到S4运动包括沿S4螺旋轴的位移和螺旋状的轴向旋转。观察到携带电荷的Rs与外部水缝中的S1中的E183和S2中的E226发生系列相互作用。从开放状态模型开始的向后30 ns模拟产生了类似于最近的静止状态模型的结构,其中S4垂直移动约6.7A。由于盐的作用,S4周围的能量状况显得非常参差不齐在S1,S2和S3螺旋的带门电荷的残基和带负电荷的残基之间形成桥。总体而言,S3和S4机芯的功能与最近的螺旋螺杆模型一致。向前和向后的模拟都表明存在至少两个稳定的中间结构,其中R2和R3分别与E183或E226形成盐桥。这些结构是先前门控动力学模型(例如Zagotta-Hoshi-Aldrich模型)中假定的状态的候选者,以说明每个亚基激活所需的一个以上过渡步骤。

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