Inositol trisphosphate and calcium oscillations

2007 ◽  
Vol 74 (1) ◽  
pp. 1 ◽  
Author(s):  
Michael J. Berridge
Physiology ◽  
2000 ◽  
Vol 15 (1) ◽  
pp. 50-55 ◽  
Author(s):  
Jean-Pierre Savineau ◽  
Roger Marthan

In a variety of smooth muscle cells, agonists activating membrane receptors induce oscillations in the cytoplasmic Ca2+ concentration via an inositol trisphosphate-activated mechanism. Ca2+ oscillations participate in the control of cell membrane potential and the tone of smooth muscle. There is evidence that alterations in Ca2+ oscillations modulate smooth muscle responsiveness.


2006 ◽  
Vol 103 (6) ◽  
pp. 1675-1680 ◽  
Author(s):  
J. Sneyd ◽  
K. Tsaneva-Atanasova ◽  
V. Reznikov ◽  
Y. Bai ◽  
M. J. Sanderson ◽  
...  

1995 ◽  
Vol 53 (4) ◽  
pp. 766-774 ◽  
Author(s):  
Rafael A. Fissore ◽  
Clara Pinto-Correia ◽  
James M. Robl

2017 ◽  
Vol 114 (7) ◽  
pp. 1456-1461 ◽  
Author(s):  
James Sneyd ◽  
Jung Min Han ◽  
Liwei Wang ◽  
Jun Chen ◽  
Xueshan Yang ◽  
...  

Oscillations in the concentration of free cytosolic Ca2+ 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 Ca2+ 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 Ca2+ oscillation period can be controlled by modulation of the rate of activation by Ca2+ 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.


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