Institute of Membrane and Systems Biology, Faculty of Biological Sciences, Multidisciplinary Cardiovascular Research Center, University of Leeds, Leeds, United Kingdom.
Biophys J. 2012 Jan 4;102(1):30-8. doi: 10.1016/j.bpj.2011.10.036. Epub 2012 Jan 3.
Optical mapping has become an indispensible tool for studying cardiac electrical activity. However, due to the three-dimensional nature of the optical signal, the optical upstroke is significantly longer than the electrical upstroke. This raises the issue of how to accurately determine the activation time on the epicardial surface. The purpose of this study was to establish a link between the optical upstroke and exact surface activation time using computer simulations, with subsequent validation by a combination of microelectrode recordings and optical mapping experiments. To simulate wave propagation and associated optical signals, we used a hybrid electro-optical model. We found that the time of the surface electrical activation (t(E)) within the accuracy of our simulations coincided with the maximal slope of the optical upstroke (t(F)) for a broad range of optical attenuation lengths. This was not the case when the activation time was determined at 50% amplitude (t(F50)) of the optical upstroke. The validation experiments were conducted in isolated Langendorff-perfused rat hearts and coronary-perfused pig left ventricles stained with either di-4-ANEPPS or the near-infrared dye di-4-ANBDQBS. We found that t(F) was a more accurate measure of t(E) than was t(F50) in all experimental settings tested (P = 0.0002). Using t(F)* instead of t(F50) produced the most significant improvement in measurements of the conduction anisotropy and the transmural conduction time in pig ventricles.
光学标测已成为研究心脏电活动不可或缺的工具。然而,由于光学信号的三维性质,光学上升支明显长于电上升支。这就提出了如何准确确定心外膜表面激活时间的问题。本研究旨在使用计算机模拟建立光学上升支与确切表面激活时间之间的联系,随后通过微电极记录和光学标测实验的组合进行验证。为了模拟波传播和相关的光学信号,我们使用了混合电-光模型。我们发现,在我们的模拟精度范围内,表面电激活时间(t(E))与光学上升支的最大斜率(t(F)*)相吻合,对于广泛的光学衰减长度都是如此。当在光学上升支的 50%幅度(t(F50))处确定激活时间时,情况并非如此。验证实验在离体 Langendorff 灌注大鼠心脏和用 di-4-ANEPPS 或近红外染料 di-4-ANBDQBS 染色的冠状灌注猪左心室中进行。我们发现,在所有测试的实验设置中,t(F)*是 t(E)的更准确测量值,优于 t(F50)(P = 0.0002)。与使用 t(F50)相比,使用 t(F)*可显著提高猪心室的传导各向异性和跨壁传导时间的测量精度。