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On the role of thermal backbone fluctuations in myoglobin ligand gate dynamics

机译:关于热骨架波动在肌红蛋白配体门动力学中的作用

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We construct an energy function that describes the crystallographic structure of sperm whale myoglobin backbone. As a model in our construction, we use the Protein Data Bank entry 1ABS that has been measured at liquid helium temperature. Consequently, the thermal B-factor fluctuations are very small, which is an advantage in our construction. The energy function that we utilize resembles that of the discrete nonlinear Schr?dinger equation. Likewise, ours supports topological solitons as local minimum energy configurations. We describe the 1ABS backbone in terms of topological solitons with a precision that deviates from 1ABS by an average root-mean-square distance, which is less than the experimentally observed Debye-Waller B-factor fluctuation distance. We then subject the topological multi-soliton solution to extensive numerical heating and cooling experiments, over a very wide range of temperatures. We concentrate in particular to temperatures above 300 K and below the Θ-point unfolding temperature, which is around 348 K. We confirm that the behavior of the topological multi-soliton is fully consistent with Anfinsens thermodynamic principle, up to very high temperatures. We observe that the structure responds to an increase of temperature consistently in a very similar manner. This enables us to characterize the onset of thermally induced conformational changes in terms of three distinct backbone ligand gates. One of the gates is made of the helix F and the helix E. The two other gates are chosen similarly, when open they provide a direct access route for a ligand to reach the heme. We find that out of the three gates we investigate, the one which is formed by helices B and G is the most sensitive to thermally induced conformational changes. Our approach provides a novel perspective to the important problem of ligand entry and exit.
机译:我们构建了一个能量函数,该函数描述了抹香鲸肌红蛋白骨架的晶体结构。作为构建模型,我们使用在液氦温度下测量的Protein Data Bank条目1ABS。因此,热B因子波动非常小,这对我们的结构是有利的。我们利用的能量函数类似于离散非线性Schrdinger方程的能量函数。同样,我们支持拓扑孤子作为局部最小能量配置。我们以拓扑孤子来描述1ABS骨干,其精度与1ABS的偏差为平均均方根距离,该均方根距离小于实验观察到的Debye-Waller B因子波动距离。然后,我们在非常宽的温度范围内对拓扑多孤子解决方案进行广泛的数值加热和冷却实验。我们特别关注的温度是高于300 K且低于θ点展开温度(约348 K)。我们确认拓扑多孤子的行为在非常高的温度下完全符合Anfinsens热力学原理。我们观察到该结构以非常相似的方式一致地响应温度的升高。这使我们能够根据三个不同的骨架配体门表征热诱导的构象变化的开始。其中一个门由螺旋F和螺旋E制成。另外两个门的选择类似,当打开时,它们为配体到达血红素提供了直接通道。我们发现,在我们研究的三个闸门中,由螺旋B和G形成的闸门对热诱导的构象变化最敏感。我们的方法为配体进入和退出的重要问题提供了新颖的视角。

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