Benedetti Fabrizio, Gazizova Yulia, Kulik Andrzej J, Marszalek Piotr E, Klinov Dmitry V, Dietler Giovanni, Sekatskii Sergey K
Laboratoire de Physique de la Matière Vivante, IPHYS, BSP, École Polytechnique Fédérale de Lausanne, Lausanne, Switzerland.
Laboratoire de Physique de la Matière Vivante, IPHYS, BSP, École Polytechnique Fédérale de Lausanne, Lausanne, Switzerland; Russian Institute of Physical-Chemical Medicine, Moscow, Russia; Department of Biological and Medical Physics, Moscow Institute of Physics and Technology, Moscow, Russia.
Biophys J. 2016 Sep 20;111(6):1163-1172. doi: 10.1016/j.bpj.2016.08.018.
We performed dynamic force spectroscopy of single dextran and titin I27 molecules using small-amplitude and low-frequency (40-240 Hz) dithering of an atomic force microscope tip excited by a sine wave voltage fed onto the tip-carrying piezo. We show that for such low-frequency dithering experiments, recorded phase information can be unambiguously interpreted within the framework of a transparent theoretical model that starts from a well-known partial differential equation to describe the dithering of an atomic force microscope cantilever and a single molecule attached to its end system, uses an appropriate set of initial and boundary conditions, and does not exploit any implicit suggestions. We conclude that the observed phase (dissipation) signal is due completely to the dissipation related to the dithering of the cantilever itself (i.e., to the change of boundary conditions in the course of stretching). For both cases, only the upper bound of the dissipation of a single molecule has been established as not exceeding 3⋅10(-7)kg/s. We compare our results with previously reported measurements of the viscoelastic properties of single molecules, and we emphasize that extreme caution must be taken in distinguishing between the dissipation related to the stretched molecule and the dissipation that originates from the viscous damping of the dithered cantilever. We also present the results of an amplitude channel data analysis, which reveal that the typical values of the spring constant of a I27 molecule at the moment of module unfolding are equal to 4±1.5mN/m, and the typical values of the spring constant of dextran at the moment of chair-boat transition are equal to 30-50mN/m.
我们使用由施加在承载探针的压电体上的正弦波电压激发的原子力显微镜探针进行小振幅和低频(40 - 240 Hz)抖动,对单个葡聚糖和肌联蛋白I27分子进行了动态力谱分析。我们表明,对于此类低频抖动实验,记录的相位信息可以在一个透明的理论模型框架内得到明确解释,该模型从一个众所周知的偏微分方程开始,以描述原子力显微镜悬臂及其末端附着的单个分子的抖动,使用一组适当的初始和边界条件,且不利用任何隐含假设。我们得出结论,观察到的相位(耗散)信号完全归因于与悬臂自身抖动相关的耗散(即拉伸过程中边界条件的变化)。对于这两种情况,仅确定单个分子耗散的上限不超过3×10⁻⁷ kg/s。我们将我们的结果与先前报道的单分子粘弹性性质的测量结果进行比较,并强调在区分与拉伸分子相关的耗散和源于抖动悬臂粘性阻尼的耗散时必须极其谨慎。我们还展示了幅度通道数据分析的结果,该结果表明I27分子在模块展开时刻的弹簧常数典型值等于4±1.5 mN/m,葡聚糖在椅式 - 船式转变时刻的弹簧常数典型值等于30 - 50 mN/m。