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论钙振荡的动力学结构

On the dynamical structure of calcium oscillations.

作者信息

Sneyd James, Han Jung Min, Wang Liwei, Chen Jun, Yang Xueshan, Tanimura Akihiko, Sanderson Michael J, Kirk Vivien, Yule David I

机构信息

Department of Mathematics, University of Auckland, Auckland 1142, New Zealand;

Department of Mathematics, University of Auckland, Auckland 1142, New Zealand.

出版信息

Proc Natl Acad Sci U S A. 2017 Feb 14;114(7):1456-1461. doi: 10.1073/pnas.1614613114. Epub 2017 Feb 1.

Abstract

Oscillations in the concentration of free cytosolic Ca are an important and ubiquitous control mechanism in many cell types. It is thus correspondingly important to understand the mechanisms that underlie the control of these oscillations and how their period is determined. We show that Class I Ca oscillations (i.e., oscillations that can occur at a constant concentration of inositol trisphosphate) have a common dynamical structure, irrespective of the oscillation period. This commonality allows the construction of a simple canonical model that incorporates this underlying dynamical behavior. Predictions from the model are tested, and confirmed, in three different cell types, with oscillation periods ranging over an order of magnitude. The model also predicts that Ca oscillation period can be controlled by modulation of the rate of activation by Ca of the inositol trisphosphate receptor. Preliminary experimental evidence consistent with this hypothesis is presented. Our canonical model has a structure similar to, but not identical to, the classic FitzHugh-Nagumo model. The characterization of variables by speed of evolution, as either fast or slow variables, changes over the course of a typical oscillation, leading to a model without globally defined fast and slow variables.

摘要

游离胞质钙离子浓度的振荡是许多细胞类型中一种重要且普遍存在的控制机制。因此,相应地了解这些振荡控制的潜在机制以及它们的周期是如何确定的就显得尤为重要。我们表明,I类钙振荡(即可以在恒定浓度的三磷酸肌醇下发生的振荡)具有共同的动力学结构,而与振荡周期无关。这种共性使得能够构建一个包含这种潜在动力学行为的简单规范模型。该模型的预测在三种不同的细胞类型中得到了测试和证实,其振荡周期范围跨越一个数量级。该模型还预测,钙振荡周期可以通过调节三磷酸肌醇受体受钙离子激活的速率来控制。文中给出了与该假设一致的初步实验证据。我们的规范模型具有与经典菲茨休 - 纳古莫模型相似但不完全相同的结构。通过演化速度将变量表征为快变量或慢变量,在典型振荡过程中会发生变化,从而导致一个没有全局定义的快变量和慢变量的模型。

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