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Pacemaker potential
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In the pacemaking cells of the heart (e.g., the sinoatrial node), the pacemaker potential (also called the pacemaker current) is the slow, positive increase in voltage across the cell's membrane, that occurs between the end of one action potential and the beginning of the next. It is responsible for the self-generated rhythmic firing (automaticity) of pacemaker cells.
Background
[edit]The cardiac pacemaker is the heart's natural rhythm generator. It employs pacemaker cells that generate electrical impulses, known as cardiac action potentials. These potentials cause the cardiac muscle to contract, and the rate of which these muscles contract determines the heart rate.
As with any other cells, pacemaker cells have an electrical charge on their membranes. This electrical charge is called the membrane potential. After the firing of an action potential, the pacemaking cell's membrane repolarizes (decreases in voltage) to its resting potential of -60 mV. From here, the membrane gradually depolarizes (increases in voltage) to the threshold potential of -40 mV,[1] upon which the cell would go on to fire the next action potential. The rate of depolarization is the slope: the faster voltage increases, the steeper the slopes are in graphs. The slope determines the time taken to reach the threshold potential, and thus the timing of the next action potential.[2]
In a healthy sinoatrial node (SAN, a complex tissue within the right atrium containing pacemaker cells that normally determine the intrinsic firing rate for the entire heart[3][4]), the pacemaker potential is the main determinant of the heart rate. Because the pacemaker potential represents the non-contracting time between heart beats (diastole), it is also called the diastolic depolarization. The amount of net inward current required to move the cell membrane potential during the pacemaker phase is extremely small, in the order of few pAs, but this net flux arises from time to time changing contribution of several currents that flow with different voltage and time dependence. Evidence in support of the active presence of K+, Ca2+, Na+ channels and Na+/K+ exchanger during the pacemaker phase have been variously reported in the literature, but several indications point to the “funny”(If) current as one of the most important.[5] (see funny current). There is now substantial evidence that also sarcoplasmic reticulum (SR) Ca2+-transients participate to the generation of the diastolic depolarization via a process involving the Na–Ca exchanger.
The rhythmic activity of some neurons like the pre-Bötzinger complex is modulated by neurotransmitters and neuropeptides, and such modulatory connectivity gives to the neurons the necessary plasticity to generating distinctive, state-dependent rhythmic patterns that depend on pacemaker potentials.[6]
Pacemakers
[edit]
The heart has several pacemakers, each which fires at its own intrinsic rate:
- SA node: 60–100 bpm
- Atrioventricular node(AVN): 40–60 bpm
- Purkinje fibres: 20–40 bpm
The potentials will normally travel in order
SA node → Atrioventricular node → Purkinje fibres
Normally, all the foci will end up firing at the SA node rate, not their intrinsic rate in a phenomenon known as overdrive-suppression. Thus, in the normal, healthy heart, only the SA node intrinsic rate is observable.
Pathology
[edit]However, in pathological conditions, the intrinsic rate becomes apparent. Consider a heart attack which damages the region of the heart between the SA node and the AV node.
SA node → |block| AV node → Purkinje fibres
The other foci will not see the SA node firing; however, they will see the atrial foci. The heart will now beat at the intrinsic rate of the AV node.
Induction
[edit]The firing of the pacemaker cells is induced electrically by reaching the threshold potential of the cell membrane. The threshold potential is the potential an excitable cell membrane, such as a myocyte, must reach in order to induce an action potential.[7] This depolarization is caused by very small net inward currents of calcium ions across the cell membrane, which gives rise to the action potential.[8][9]
Bio-pacemakers
[edit]Bio-pacemakers are the outcome of a rapidly emerging field of research into a replacement for the electronic pacemaker. The bio-pacemaker turns quiescent myocardial cells (e.g. atrial cells) into pacemaker cells. This is achieved by making the cells express a gene which creates a pacemaker current.[10]
See also
[edit]References
[edit]- ^ Wei, Xingyu; Yohannan, Sandesh; Richards, John R. (2025). "Physiology, Cardiac Repolarization Dispersion and Reserve". StatPearls. StatPearls Publishing. PMID 30725879.
[Depolarization] starts when the membrane potential reaches -40 mV, the threshold potential for pacemaker cells. [...This] results in an upstroke in membrane potential from -40 mV to +10mV. [... Repolarization involves a] rapid decrease of membrane potential from +10 mV to -60 mV.
- ^ Sokolov, E.N.; Grechenko, T.N. (1981). "Pacemaker Plasticity in Isolated Neuron". Brain and Behaviour. pp. 7–12. doi:10.1016/B978-0-08-027338-9.50007-4. ISBN 978-0-08-027338-9.
[When the pacemaker potential] reaches threshold (approximately –40mV in nodal cells) it triggers an action potential, which sparks off the next heart beat. The slope of the pacemaker potential determines the time taken to reach the threshold value, so the slope governs heart rate; the steeper the slope the sooner threshold is reached and the shorter the time between beats. Since the pacemaker slope is steeper in SA node cells than elsewhere in the electrical system, the SA node has the fastest intrinsic firing rate and initiates each heart beat.
- ^ Verkerk AO, van Boren MM, Peters RJ, Broekhuis E, Lam K, Coronel R, de Bakker JM, Tan HR (7 September 2007). "Pacemaker current (If) in the human sinoatrial node". European Heart Journal. 28 (20): 2472–2478. doi:10.1093/eurheartj/ehm339. PMID 17823213.
- ^ Boron, Walter. F; Emile Boulpaep (2003). Medical Physiology. Elsevier Saunders. p. 489. ISBN 978-0-7216-0076-5.
- ^ DiFrancesco D (May 2006). "Funny channels in the control of cardiac rhythm and mode of action of selective blockers". Pharmacol. Res. 53 (5): 399–406. doi:10.1016/j.phrs.2006.03.006. PMID 16638640.
- ^ Morgado-Valle, Consuelo; Beltran-Parrazal, Luis (2017). "Respiratory Rhythm Generation: The Whole is Greater Than the Sum of the Parts". The Plastic Brain. Advances in Experimental Medicine and Biology. Vol. 1015. pp. 147–161. doi:10.1007/978-3-319-62817-2_9. ISBN 978-3-319-62815-8. ISSN 0065-2598. PMID 29080026.
- ^ Campbell, Neil. A (1996). Biology. Benjamin Cummings. p. G–21. ISBN 978-0-07-366175-9.
- ^ Verkerk, Arie O.; van Ginneken, Antoni C.G.; Wilders, Ronald (March 2009). "Pacemaker activity of the human sinoatrial node: Role of the hyperpolarization-activated current, If". International Journal of Cardiology. 132 (3): 318–336. doi:10.1016/j.ijcard.2008.12.196. PMID 19181406.
- ^ Boron, Walter. F; Emile Boulpaep (2003). Medical Physiology. Elsevier Saunders. p. 487. ISBN 978-0-7216-0076-5.
- ^ Verkerk AO, Zegers JG, Van Ginneken AC, Wilders R (2008). "Dynamic action potential clamp as a powerful tool in the development of a gene-based bio-pacemaker". 2008 30th Annual International Conference of the IEEE Engineering in Medicine and Biology Society. Vol. 1. pp. 133–6. doi:10.1109/IEMBS.2008.4649108. ISBN 978-1-4244-1814-5. PMID 19162611.
Pacemaker potential
View on GrokipediaPhysiological Fundamentals
Definition and Overview
The pacemaker potential refers to the gradual, spontaneous depolarization of the membrane potential in specialized cardiac cells, starting from the maximum diastolic potential (typically around -60 mV) and progressing to the threshold for action potential initiation (approximately -40 to -30 mV), which underlies the heart's automaticity.[5] This process enables these cells to generate rhythmic electrical impulses without external stimulation, distinguishing them from other cardiac tissues.[6] The concept of a cardiac pacemaker originated in the early 20th century with the anatomical identification of the sinoatrial node by Arthur Keith and Martin Flack in 1907, who described it as a distinct structure in the right atrium responsible for initiating heartbeats in mammals.[3] This discovery built on earlier physiological observations, such as those by Walter Gaskell in the 1880s, and marked a foundational step in understanding the heart's intrinsic rhythm generation, though the electrophysiological details of the pacemaker potential were elucidated later through voltage-clamp techniques in the mid-20th century.[3] In the cardiac cycle, the pacemaker potential drives the primary rhythm of the heartbeat by producing regular action potentials that propagate through the conduction system to coordinate atrial and ventricular contractions.[5] Unlike contractile myocytes, which maintain a stable resting membrane potential during diastole, pacemaker cells exhibit this ongoing depolarization, ensuring continuous impulse generation at a rate of about 60-100 beats per minute under normal conditions.[6] Primarily located in the sinoatrial node, this mechanism provides the heart with its autonomous pacing capability.[3] The waveform of the pacemaker potential is characterized by a slow, nonlinear upward slope during phase 4 of the action potential, contrasting sharply with the rapid, steep depolarization seen in the fast action potentials of the working myocardium.[5] This gradual curve reflects the integrated balance of ionic fluxes that progressively reduce hyperpolarization, culminating in threshold crossing and the onset of the next heartbeat.[6]Phases and Characteristics
The pacemaker potential in cardiac pacemaker cells, particularly those of the sinoatrial node, is characterized by a distinctive waveform that lacks a stable resting phase, instead featuring continuous spontaneous depolarization. The primary phase is phase 4, known as diastolic depolarization, which drives automaticity. This phase begins at the maximum diastolic potential (MDP) of approximately -60 mV and progresses nonlinearly toward the threshold potential of about -40 mV.[2][7] Phase 4 can be divided into an early slow rise, where the membrane potential depolarizes gradually from the MDP at a relatively constant rate, followed by late acceleration as the slope steepens, culminating in threshold crossing that triggers the action potential. The early phase involves contributions from hyperpolarization-activated cyclic nucleotide-gated (HCN) channels, which initiate the slow depolarization.[2] This nonlinear slope reflects the progressive activation of voltage-dependent currents, enabling the cell to reach threshold without external stimuli. Phase 0 follows, consisting of a rapid upstroke driven by calcium influx through L-type Ca²⁺ channels, reaching a peak overshoot potential of around +20 mV; unlike ventricular action potentials, this upstroke is slower and Ca²⁺-dependent rather than Na⁺-mediated.[2][7] Key biophysical properties include a typical cycle length of 800–1000 ms in humans, corresponding to a resting heart rate of 60–75 beats per minute, with the rate modulated by autonomic tone—sympathetic stimulation accelerates the slope of phase 4, while parasympathetic input slows it. Unlike ventricular myocytes, which exhibit a stable phase 3 repolarization plateau and resting potential near -90 mV, pacemaker potentials show no such plateau, maintaining a more depolarized MDP around -60 mV and emphasizing their role in rhythmic impulse generation within the sinoatrial node.[2][7] These characteristics are sensitive to temperature, with elevations increasing the rate of diastolic depolarization and thus heart rate, as observed in physiological ranges. Additionally, pacemaker automaticity exhibits metabolic dependence, relying on ATP-driven ion pumps to sustain the ionic gradients necessary for the depolarization cycle.[8][2]Cellular and Ionic Mechanisms
Key Ion Channels and Currents
The pacemaker potential in cardiac sinoatrial node cells is primarily driven by a series of inward currents that progressively depolarize the membrane during the diastolic phase. The funny current (I_f), mediated by hyperpolarization-activated cyclic nucleotide-gated (HCN) channels, plays a central role in initiating this depolarization. HCN channels, predominantly HCN4 in the sinoatrial node, conduct a mixed Na⁺/K⁺ influx with a reversal potential of approximately -20 to -30 mV, activating upon hyperpolarization to potentials below -40 to -50 mV following repolarization. This inward current contributes significantly to the early phase of diastolic depolarization, with its degree of activation determining the slope of the pacemaker potential and thus the firing rate.[9][10] The T-type Ca²⁺ current (I_{Ca,T}), carried mainly by Cav3.1 channels, activates at more negative potentials (around -60 to -40 mV) and supports the middle phase of depolarization by providing additional inward Ca²⁺ flux, bridging the transition from I_f dominance to later currents. In sinoatrial node cells, I_{Ca,T} contributes modestly to pacemaking, as its blockade reduces but does not abolish spontaneous activity. The L-type Ca²⁺ current (I_{Ca,L}), primarily through Cav1.3 channels, activates at higher voltages (around -40 to -10 mV) and drives the late upstroke of the pacemaker potential, culminating in the action potential threshold. This current is essential for the final depolarization phase, with its abolition markedly slowing or disrupting pacemaker rhythm.[11][12] The sodium-calcium exchanger (NCX) current (I_NCX), operating in forward mode, provides an additional inward current during late diastole. Triggered by spontaneous Ca²⁺ releases from the sarcoplasmic reticulum, NCX extrudes Ca²⁺ in exchange for Na⁺ influx, contributing to the final acceleration of depolarization toward the threshold. This current is integral to the coupled clock system and supports rhythmic pacemaking.[13][14] Repolarizing influences are subdued in pacemaker cells to permit spontaneous depolarization. The inward rectifier K⁺ current (I_{K1}) is minimal or absent in sinoatrial node cells, lacking the strong stabilizing effect seen in ventricular myocytes and thereby facilitating the unstable diastolic potential necessary for pacemaking. Delayed rectifier K⁺ currents (I_K), including rapid (I_{Kr}) and slow (I_{Ks}) components, provide partial repolarization during the action potential upstroke and early diastole, counterbalancing inward currents to reset the membrane potential. These outward K⁺ fluxes activate during depolarization and decay slowly, contributing to the oscillatory balance.[15][16] The dynamics of these currents follow a simplified clockwork model where overlapping inward and outward fluxes create the gradual depolarization gradient. For instance, the funny current can be approximated as: where is the time- and voltage-dependent conductance, modulated by cyclic AMP (cAMP) through shifts in activation (positive shift of 10-25 mV under adrenergic stimulation), and is the reversal potential; the activation time constant ranges from approximately 100 to 1000 ms, slowing at hyperpolarized potentials. This overlap—such as the decay of I_K alongside progressive activation of I_f, I_{Ca,T}, I_{Ca,L}, and I_NCX—ensures a continuous, self-sustaining depolarization without stable resting potentials, as observed in the phenotypic phases of the pacemaker cycle.[17]Molecular Regulation
The molecular regulation of pacemaker potential involves key ion channel isoforms and transcription factors that establish and maintain automaticity in cardiac pacemaker cells. Hyperpolarization-activated cyclic nucleotide-gated (HCN) channels, particularly the HCN4 isoform, predominate in the heart and are essential for generating the funny current (I_f), which initiates diastolic depolarization. HCN4's high expression in sinoatrial node cells ensures robust pacemaker activity, with its activation threshold and kinetics finely tuned to physiological demands. Transcription factors such as Tbx3 and Shox2 play critical roles in orchestrating pacemaker-specific gene expression; Tbx3 acts as a repressor of atrial genes while promoting pacemaker identity, and Shox2 drives the differentiation of sinoatrial node progenitors by regulating downstream targets like Hcn4. These factors form a genetic cascade that confines pacemaker properties to specific cardiac regions during development. Autonomic nervous system inputs dynamically modulate pacemaker potential through biochemical signaling pathways. Sympathetic stimulation via β-adrenergic receptors activates adenylyl cyclase, elevating cyclic AMP (cAMP) levels and activating protein kinase A (PKA), which phosphorylates HCN channels to shift their activation curve and enhance I_f, while also increasing L-type calcium current (I_{Ca,L}) to accelerate depolarization. In contrast, parasympathetic (vagal) activation releases acetylcholine, which binds muscarinic receptors to decrease cAMP via Gi protein inhibition, thereby reducing I_f and I_{Ca,L} to slow the heart rate. These opposing pathways allow rapid adaptation of pacemaker rate to physiological needs, with cAMP serving as a central integrator. Intracellular signaling contributes to pacemaker automaticity through the Ca^{2+}-clock mechanism, where spontaneous calcium releases from the sarcoplasmic reticulum (SR) via ryanodine receptors trigger Na^+/Ca^{2+} exchanger (NCX) activity in forward mode, generating an inward current that sustains late diastolic depolarization. This SR-driven Ca^{2+} cycling couples with membrane ion channels to produce rhythmic action potentials, ensuring reliable pacemaking even under varying conditions. The interplay between SR Ca^{2+} release and NCX maintains the necessary temporal precision for automaticity. Genetic models highlight the importance of molecular regulation in pacemaker function, particularly mutations in the Cacna1d gene encoding the Ca_v1.3 L-type calcium channel subunit. Loss-of-function Cacna1d mutations impair channel conductance, leading to reduced I_{Ca,L} and sinoatrial node dysfunction, manifesting as bradycardia and rhythm disorders in affected individuals. These findings underscore Ca_v1.3's role in fine-tuning depolarization and its vulnerability to genetic perturbations.Pacemaker Tissues in the Heart
Sinoatrial Node as Primary Pacemaker
The sinoatrial node (SAN) is anatomically positioned at the junction between the superior vena cava and the right atrium, forming a crescent-shaped structure that extends along the crista terminalis.[18][19] This specialized tissue consists of approximately 10,000 specialized cardiomyocytes embedded within a dense network of connective tissue, which provides insulation from the surrounding atrial myocardium to prevent premature activation.[20][21] The cellular composition of the SAN is heterogeneous, comprising primarily pacemaker (P) cells in the central region and transitional cells at the periphery.[22] P cells, characterized by their pale cytoplasm and prominent expression of the hyperpolarization-activated funny current (I_f), serve as the true pacemakers responsible for initiating the pacemaker potential.[23][10] Transitional cells, in contrast, exhibit action potential shapes intermediate between those of P cells and atrial myocytes, facilitating the integration of pacemaker activity with broader atrial conduction.[24] This heterogeneity contributes to varied action potential morphologies across SAN cell populations, enhancing the robustness of pacemaking.[25] Functionally, the SAN dominates cardiac rhythm generation with an intrinsic firing rate of 60-100 beats per minute in humans, establishing it as the primary pacemaker under normal conditions.[2] Its higher automaticity leads to overdrive suppression of latent pacemaker sites elsewhere in the heart, ensuring hierarchical control of the heartbeat. Action potentials from the SAN propagate to the atria through internodal pathways, including anterior, middle, and posterior tracts composed of specialized transitional fibers.[26] Developmentally, the SAN arises from Tbx18-expressing progenitor cells in the embryonic sinus venosus, which differentiate into pacemaker myocardium around embryonic day 9.5 in mice.[20] These progenitors contribute to the formation of the SAN head and body, establishing its positional identity at the venous pole of the heart.[27]Subsidiary Pacemaker Sites
Subsidiary pacemaker sites in the heart provide redundancy to the primary sinoatrial node (SAN) by generating spontaneous action potentials at slower rates, ensuring continued cardiac rhythm during failures of higher pacemakers. These sites include the atrioventricular (AV) node, Purkinje fibers in the ventricular conduction system, and, under conditions of stress or suppression of dominant pacemakers, latent foci within the atrial and ventricular myocardium. The AV node, situated in the triangle of Koch at the base of the interatrial septum, exhibits an intrinsic firing rate of approximately 40-60 beats per minute (bpm). Purkinje fibers, distributed throughout the subendocardium of the ventricles, display even slower intrinsic rates of 20-40 bpm. Latent pacemakers in the atrial or ventricular myocardium typically emerge only under pathological stress, such as ischemia or electrolyte imbalances, and generate rates below 30 bpm when active.[28][29][30] The properties of these subsidiary sites reflect their subordinate role, characterized by slower rates of diastolic depolarization compared to the SAN. This reduced automaticity arises from less prominent expression and density of key ion currents, including the hyperpolarization-activated funny current (I_f) and calcium currents (I_Ca,L and I_Ca,T). In the AV node, I_f is present but heterogeneous across cell types, with lower overall contribution to the depolarization slope due to slower activation kinetics and weaker coupling with intracellular calcium handling. Purkinje fibers possess I_f that activates at more negative potentials (around -90 mV maximum diastolic potential), but high inward rectifier potassium current (I_K1) hyperpolarizes the membrane, limiting the effectiveness of depolarizing currents and resulting in a higher threshold for spontaneous activity initiation. These features ensure that subsidiary sites remain suppressed under normal conditions, activating only when overdrive suppression from faster pacemakers is relieved.[31][32][31] Activation of subsidiary pacemakers primarily occurs through escape rhythms, where they assume control if conduction from the SAN or AV node is blocked, such as in sinus arrest or high-degree AV block. For instance, an AV nodal escape rhythm emerges after a pause exceeding its intrinsic cycle length, producing junctional beats with retrograde or absent P waves. Purkinje fiber escapes manifest as wide-complex idioventricular rhythms during prolonged asystole. These sites can be accelerated by catecholamines, such as norepinephrine, which enhance I_f and calcium currents via β-adrenergic stimulation, potentially increasing rates to 60-100 bpm in the AV node or 40-60 bpm in Purkinje fibers during sympathetic activation. This modulation supports adaptive responses to stress but can contribute to tachyarrhythmias if excessive.[33][28][34] A hierarchical organization governs pacemaker dominance, with the SAN's faster rate (60-100 bpm) suppressing lower sites through overdrive suppression via membrane hyperpolarization and reduced automaticity. If the SAN fails, the AV node takes precedence due to its intermediate rate, followed by Purkinje fibers as the final backup. This gradient, rooted in differences in ion channel expression and membrane properties, maintains efficient conduction under normal physiology while providing fail-safes against bradycardia.[29][32][35]| Pacemaker Site | Intrinsic Rate (bpm) | Primary Ion Currents Involved | Activation Threshold Context |
|---|---|---|---|
| AV Node | 40-60 | I_f, I_Ca,L, I_Ca,T | Intermediate; suppressed by SAN overdrive |
| Purkinje Fibers | 20-40 | I_f (limited), I_Ca,T | High (negative MDP ~ -90 mV) due to I_K1 |
| Atrial/Ventricular Myocardium (latent) | <30 | Variable, enhanced under stress | Emerges only after suppression of higher sites |