Suhling Klaus, Levitt James A, Chung Pei-Hua, Kuimova Marina K, Yahioglu Gokhan
Department of Physics, King's College London.
J Vis Exp. 2012 Feb 9(60):2925. doi: 10.3791/2925.
Diffusion is often an important rate-determining step in chemical reactions or biological processes and plays a role in a wide range of intracellular events. Viscosity is one of the key parameters affecting the diffusion of molecules and proteins, and changes in viscosity have been linked to disease and malfunction at the cellular level. While methods to measure the bulk viscosity are well developed, imaging microviscosity remains a challenge. Viscosity maps of microscopic objects, such as single cells, have until recently been hard to obtain. Mapping viscosity with fluorescence techniques is advantageous because, similar to other optical techniques, it is minimally invasive, non-destructive and can be applied to living cells and tissues. Fluorescent molecular rotors exhibit fluorescence lifetimes and quantum yields which are a function of the viscosity of their microenvironment. Intramolecular twisting or rotation leads to non-radiative decay from the excited state back to the ground state. A viscous environment slows this rotation or twisting, restricting access to this non-radiative decay pathway. This leads to an increase in the fluorescence quantum yield and the fluorescence lifetime. Fluorescence Lifetime Imaging (FLIM) of modified hydrophobic BODIPY dyes that act as fluorescent molecular rotors show that the fluorescence lifetime of these probes is a function of the microviscosity of their environment. A logarithmic plot of the fluorescence lifetime versus the solvent viscosity yields a straight line that obeys the Förster Hoffman equation. This plot also serves as a calibration graph to convert fluorescence lifetime into viscosity. Following incubation of living cells with the modified BODIPY fluorescent molecular rotor, a punctate dye distribution is observed in the fluorescence images. The viscosity value obtained in the puncta in live cells is around 100 times higher than that of water and of cellular cytoplasm. Time-resolved fluorescence anisotropy measurements yield rotational correlation times in agreement with these large microviscosity values. Mapping the fluorescence lifetime is independent of the fluorescence intensity, and thus allows the separation of probe concentration and viscosity effects. In summary, we have developed a practical and versatile approach to map the microviscosity in cells based on FLIM of fluorescent molecular rotors.
扩散在化学反应或生物过程中通常是一个重要的速率决定步骤,并且在广泛的细胞内事件中发挥作用。粘度是影响分子和蛋白质扩散的关键参数之一,粘度变化与细胞水平的疾病和功能障碍有关。虽然测量体相粘度的方法已经很成熟,但成像微粘度仍然是一个挑战。直到最近,诸如单细胞等微观物体的粘度图仍难以获得。用荧光技术绘制粘度图具有优势,因为与其他光学技术类似,它具有微创、非破坏性的特点,并且可以应用于活细胞和组织。荧光分子转子表现出荧光寿命和量子产率,它们是其微环境粘度的函数。分子内的扭曲或旋转会导致从激发态回到基态的非辐射衰变。粘性环境会减缓这种旋转或扭曲,限制进入这种非辐射衰变途径。这导致荧光量子产率和荧光寿命增加。作为荧光分子转子的改性疏水BODIPY染料的荧光寿命成像(FLIM)表明,这些探针的荧光寿命是其环境微粘度的函数。荧光寿命与溶剂粘度的对数图产生一条符合福斯特 - 霍夫曼方程的直线。该图还用作校准图,将荧光寿命转换为粘度。用改性BODIPY荧光分子转子孵育活细胞后,在荧光图像中观察到点状染料分布。活细胞中点状区域获得的粘度值比水和细胞质的粘度值高约100倍。时间分辨荧光各向异性测量产生的旋转相关时间与这些大的微粘度值一致。绘制荧光寿命与荧光强度无关,因此可以分离探针浓度和粘度效应。总之,我们基于荧光分子转子的FLIM开发了一种实用且通用的方法来绘制细胞中的微粘度图。