T he study of clinical electrophysiology essentially comprises examining how electric excitation develops and spreads through the millions of cells that constitute the heart. Given the enormous number of cells in a human heart, there is an extremely large number of possible ways that the heart can behave. We encounter rhythms across the spectrum from the organized and orderly behavior of sinus rhythm through repetitive continuous excitation (via reentry) in structurally defined circuits like atrial flutter and, finally, the complex, dynamic, and disorganized behavior of fibrillation. Despite these myriad possibilities, one can apply a basic understanding of the principles of propagation to predict how cardiac tissue will behave under varied circumstances and in response to various manipulations.In this article, we review the principles of propagation and how these can be used to understand reentry of all degrees of complexity. We use these principles to explain the mechanisms by which antiarrhythmic medications and ablation can terminate and prevent reentry. This article is not intended to be an exhaustive description of the physiology of cardiac propagation, rather, it is meant to capture the essence of propagation with sufficient detail to provide an intuitive feel for the interplay of the physiological features relevant to propagation.The figures and videos used in this article were created using a computational model of cardiac propagation (VisibleEP LLC, Colchester, VT). It is a hybrid between a physics-based and cellular automaton model. The model incorporates the fundamental features of propagation without modeling individual ion channels.1 The model manifests several relevant emergent properties, for example, electrotonic interactions, restitution of action potential duration, and conduction velocity as well as source-sink balance-dependent propagation.
Impulse Propagation Cell ExcitationA cell becomes excited when the balance of inward and outward currents passes a critical point after which inward currents exceed outward and an action potential ensues. When the membrane voltage of a cell rises above the activation threshold of its depolarizing currents (sodium current [I Na + ] or calcium current [I Ca ++ ]), its inward current grows. Meanwhile, as membrane voltage increases, the amplitude of outward currents decreases. Excitation (or the lack thereof) is dependent on a delicate balance between these currents.To reach threshold, the net transmembrane current must be sufficient to discharge the membrane capacitance.2 This term is not necessarily intuitive for those unfamiliar with physics or engineering but the concept is in fact fairly simple. The membrane separates charges across the space between its inner and outer surfaces, resulting in a voltage gradient. The size of the voltage gradient is determined by the number of charges separated and the distance by which they are separated. Think of the force that is required to keep these charges from wandering away from the cell surface. This force is...