Oscillations in the concentration of free cytosolic Ca 2+ 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 2+ 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 2+ oscillation period can be controlled by modulation of the rate of activation by Ca 2+ 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. ) are a ubiquitous signaling mechanism, occurring in many cell types and controlling a wide array of cellular functions (1-6). In many cases, the signal is carried by the oscillation frequency; for example, Ca 2+ oscillation frequency is known to control contraction of pulmonary and arteriole smooth muscle (7,8), as well as gene expression and differentiation (9-11). Although there are cell types where the frequency of Ca 2+ oscillation appears to be less important than the mean [Ca 2+ ] (12), an understanding of how Ca 2+ oscillation frequency is controlled remains critical to our understanding of many important cellular processes. Interestingly, it appears that the signal may not be carried by the absolute oscillation frequency but rather by a change in frequency (13), leading to a signaling system that is robust to intercellular variability, even within the same cell type. A concept similar to that of the Ca 2+ toolbox is important in the mathematical modeling of Ca 2+ dynamics. Models try to extract fundamental mechanisms, omitting less important details so that the basic skeleton-the basic toolbox components-can become clear. In the construction of such skeleton models, the concept of dynamical structure becomes important. The behavior of a model can be qualitatively described by a set of bifurcations and attracting or repelling sets, and this description is essentially independent of the exact model equations and parameters used to realize the underlying dynamical structure (in that there can be many different equations and parameters that have the same dynamical structure).One important question is how cells can generate Ca 2+ oscillations of widely differing periods, even though they appear to be using the same elements o...