Spectral Doppler interrogation is a cornerstone of echocardiographic evaluation of a patent ductus arteriosus (PDA). Beyond simply confirming ductal patency with two-dimensional and color Doppler imaging, spectral Doppler allows detailed assessment of shunt direction, velocity, and hemodynamic significance. Using pulsed-wave (PW) or continuous-wave (CW) Doppler aligned with ductal flow, clinicians can characterize shunt physiology and gain insight into the instantaneous pressure relationships between the systemic and pulmonary circulations. A restrictive PDA is one in which the effective ductal diameter is sufficiently small that flow and pressure transmission are limited by the ductal narrowing itself. In this setting, shunt magnitude is constrained by ductal resistance, and high velocities reflect a large pressure gradient across a narrow conduit. In contrast, an unrestrictive PDA is large enough that intrinsic ductal resistance is negligible, and shunt volume is determined primarily by the instantaneous systemic–pulmonary pressure gradient, as well as by the relative impedance and compliance of the two vascular beds. Importantly, the concept of ductal “restrictiveness” is not binary. Ductal shunting is governed by continuous variables—effective diameter, length, geometry, and dynamic smooth muscle tone—interacting with continuously changing systemic and pulmonary vascular resistance, impedance, and compliance. As these determinants evolve over the cardiac cycle and over postnatal time, the PDA transitions progressively from an unrestrictive to a restrictive conduit. Restrictive and unrestrictive PDAs therefore represent points along a physiologic continuum rather than discrete states. The ductus arteriosus provides a dynamic window into the interaction between the pulmonary artery and aorta throughout the cardiac cycle. During systole, when ventricular ejection raises pressures in both great arteries, ductal flow reflects the relative timing and magnitude of pressure rise, ventricular–vascular coupling, and the balance between left and right ventricular output. During diastole, differences in pressure decay dominate ductal flow behavior: pressure falls more slowly in the stiffer systemic circulation and more rapidly in the typically more compliant pulmonary vascular bed, often shaping late-diastolic and presystolic shunt velocity profiles. Because the ductus is a passive conduit, it does not generate flow but faithfully transmits moment-to-moment hydraulic relationships between the two circulations. As such, the PDA acts as a real-time integrator of ventriculo-arterial interaction, vascular compliance, impedance, and transitional physiology rather than a static anatomic lesion. The ductus itself may change caliber from beat to beat, and even within a single cardiac cycle, with a tendency toward larger diameter during systole and relative narrowing during diastole or during phases when pulmonary and systemic pressures approach equilibrium. Consequently, velocity and pressure gradients across the ductus reflect a continuously evolving balance between aortic and pulmonary arterial pressures and vascular properties, underscoring why PDA spectral Doppler patterns must be interpreted dynamically across the entire cardiac cycle rather than at a single time point.
1. Doppler Measures an Instantaneous Gradient, Not Pressure
Doppler interrogation of a patent ductus arteriosus does not measure pressure directly. Instead, it provides an instantaneous velocity that can be converted using the Bernoulli relationship into an instantaneous pressure gradient between the aorta and the pulmonary artery at that specific moment in the cardiac cycle. This gradient represents only the pressure difference between the two vascular beds at that instant and should not be equated with systolic aortic pressure, systolic pulmonary arterial pressure, or mean pressure unless strict timing assumptions are met.
2. Aortic and Pulmonary Artery Pressure Curves Are Not Synchronous
The aortic and pulmonary artery pressure waveforms have different shapes and timing characteristics. Aortic pressure rises rapidly and reaches a higher peak, while pulmonary artery pressure has a slower upstroke, a lower systolic peak, peak tend to occur relatively earlier after QRS and has a more rapid diastolic decay due to higher compliance. As a result, the maximal separation between the two curves, which determines ductal flow velocity, does not necessarily occur at peak systole. The highest PDA velocity may occur before, at, or after peak aortic or pulmonary artery pressure.
3. Electrical Systole Does Not Define Mechanical Systole
Mechanical ventricular systole does not extend to the end of the T wave. Peak ventricular pressure and peak arterial pressure typically occur during the early phase of ventricular repolarization, rather than at the apex of the T wave. Because PDA Doppler velocities are often referenced to the ECG, there is a risk of mislabeling velocities as “systolic” when they do not coincide with true peak mechanical systole or maximal arterial pressures.
4. Ductal Flow Is Impedance-Driven, Not Valve-Driven
Flow through the ductus arteriosus is governed by impedance rather than by valvular mechanics. The PDA is not a fixed orifice and does not fully satisfy the assumptions required for strict Bernoulli application. Ductal flow reflects the interaction of instantaneous pressure differences, ductal size and geometry, pulmonary vascular impedance, and the compliance of both arterial systems. The estimation of Right Ventricular Systolic Pressure (RVSP) via a PDA-derived gradient can result in both underestimation and overestimation.
5. PDA-Based sPAP Estimates Tend to Underestimate True RVSP, but can also Overestimate
When PDA peak velocity is used to estimate systolic pulmonary artery pressure by subtracting the Doppler-derived gradient from systolic blood pressure, the result often underestimates true right ventricular systolic pressure. This occurs because the peak PDA velocity is frequently measured at a time when aortic pressure has not yet reached its maximum or when pulmonary artery pressure has already begun to fall. The gradient therefore reflects a submaximal pressure difference rather than true peak systolic separation. Overestimation of RVSP occurs if the PDA gradient is underestimated. The most common cause is Doppler beam misalignment; if the ultrasound beam is not perfectly parallel to the blood flow, the recorded velocity will be lower than reality. A lower velocity produces a smaller gradient, which, when subtracted from the SBP, leaves a falsely high (overestimated) RVSP. Similarly, if the systemic blood pressure used in the calculation is measured at a different time than the echocardiogram and is falsely elevated, the resulting RVSP will be overestimated.
6. Directional Flow Changes Reflect Instantaneous Dominance
Bidirectional or transient right-to-left components of PDA flow reflect instantaneous pressure dominance rather than mean or sustained pressure relationships. Early systolic right-to-left flow may occur when pulmonary vascular resistance briefly exceeds systemic resistance, even without suprasystemic pulmonary pressures at peak systole. As systole and diastole progress, left-to-right flow typically dominates as aortic pressure remains higher while pulmonary artery pressure decays more rapidly. Net shunt direction over the cardiac cycle does not capture these instantaneous dynamics.
7. Peak Velocity Does Not Equal Peak Pressure Difference
The maximal Doppler velocity across the ductus does not necessarily correspond to the maximal physiologic pressure difference between the aorta and pulmonary artery (as the peak pressure difference may occur at different moment of the cardiac cycle). Indeed, the peak pulmonar Larger gradients may occur early in systole when pressure curves diverge rapidly, while smaller gradients may be present at the time of true peak arterial pressures. End-diastolic gradients reflect diastolic pressure separation and should not be interpreted as systolic load. Timing, rather than magnitude alone, determines physiologic meaning.
8. Limitations of Bernoulli-Based Pressure Reconstruction
Attempts to reconstruct pressure curves from PDA Doppler velocities assume stable geometry, negligible energy loss, and complete applicability of Bernoulli principles, assumptions that are rarely satisfied in neonatal ductal physiology. Turbulence, changing ductal caliber, pulsatile impedance, and compliance effects all introduce error. As a result, pressure curves extrapolated from PDA velocities should be considered conceptual aids rather than precise physiologic measurements.
9. Clinical Integration and the Role of Complementary Measures
These concepts emphasize that PDA Doppler is best interpreted as a dynamic physiologic signal rather than a static pressure estimator. While it provides valuable insight into timing, impedance, and shunt behavior, it should not be used in isolation to quantify systolic pulmonary artery pressure. Integration with tricuspid regurgitation velocity, systemic blood pressure, septal configuration, ventricular performance, and the overall clinical context remains essential for accurate hemodynamic interpretation.
In this left-to-right, restrictive patent ductus arteriosus, the peak systolic velocity corresponds to a pressure gradient of 16.6 mmHg (2.04 m/s) to 19.3 mmHg. When aligned with the ECG, a transient reduction in left-to-right ductal velocity is observed immediately following the QRS complex with a velocity in early systole at 0.89 m/s to 1 m/s (corresponding to 3.2 mmHg - 4 mmHg). Of note, the assumptions underlying the modified Bernoulli equation are not fully met in the setting of a patent ductus arteriosus. As a result, converting ductal flow velocities into pressure gradients represents an approximation, and these estimates should be interpreted with an understanding of the limitations inherent to this simplified application of the equation. This indicates that during very early systole, the instantaneous pressure gradient between the aorta and the pulmonary artery briefly decreases, resulting in reduced ductal flow velocity. Shortly thereafter, ductal flow accelerates and reaches a plateau that is maintained through the remainder of systole (peak systolic velocity) and into diastole, until the subsequent QRS complex. This early systolic phenomenon can be explained by the onset of right ventricular ejection while the left ventricle is still in isovolumic contraction. During this brief phase, pulmonary artery pressure rises before aortic pressure has fully increased, temporarily narrowing the aorto-pulmonary pressure gradient and reducing left-to-right ductal flow.
Similar to the prior example, this represents a restrictive left-to-right patent ductus arteriosus. However, the ductus appears more restrictive, as suggested by the loss of pulsatility in the Doppler profile, which means that the pressure gradient across the ductus is relatively constant throughout the cardiac cycle, with diminished transmission of phasic aorto-pulmonary pressure changes and a reduced ability of systolic–diastolic pressure oscillations to modulate ductal flow. A transient reduction in the early systolic pressure gradient is observed immediately following the QRS complex, with a measured velocity of 0.93 m/s, corresponding to an estimated gradient of 3.4 mmHg between the aorta and the pulmonary artery. This brief deceleration of ductal flow during early systole likely reflects a short-lived reduction in the aorto-pulmonary pressure gradient. At this time, the right ventricle has begun ejection, leading to an early rise in pulmonary artery pressure, while the left ventricle remains in isovolumic contraction and aortic pressure continues to decay toward its diastolic nadir. As left ventricular ejection subsequently begins and aortic pressure rises, the pressure gradient across the ductus increases, resulting in re-acceleration of left-to-right ductal flow.
This PDA Doppler profile is consistent with a left-to-right patent ductus arteriosus with partial pulsatility and some degree of restriction. The ductal signal demonstrates a high peak systolic velocity, with flow velocity building up after the QRS during ventricular contraction. The peak velocity is approximately 3.56 m/s, corresponding to an estimated systolic aorto-pulmonary pressure gradient of about 51 mmHg, indicating that the PDA behaves as restrictive during systole and limits pressure transmission. This reflects a relatively preserved systolic pressure difference between the aorta and the pulmonary artery and supports some restrictive nature of the ductus. In contrast, the end-diastolic velocity is substantially lower, measured at approximately 1.31 m/s (estimated gradient ~7 mmHg). This occurs near the instantaneous nadir of the pressure difference between the pulmonary artery and the aorta. It is important to note that the nadir of diastolic aortic pressure does not necessarily occur simultaneously with the nadir of pulmonary artery pressure. The marked reduction in diastolic velocity reflects a significant decrease in the aorto-pulmonary pressure gradient during diastole, suggesting relative convergence of aortic and pulmonary artery pressures at that phase of the cardiac cycle. The waveform remains pulsatile, with prominent systolic peaks and deep troughs approaching low diastolic velocities, rather than a continuous, non-pulsatile profile. In a very restrictive PDA, resistance across the ductus is so high that systemic (aortic) pressure cannot sufficiently transmit into the pulmonary artery to equalize pressures. As a result, the aorta remains at high pressure while the pulmonary artery stays at lower pressure throughout the cardiac cycle, leading to a loss of pulsatility and a more continuous, high-velocity flow profile. In contrast, in an unrestrictive (large) PDA, aortic and pulmonary artery pressures are nearly equal. During diastole, the pressure difference becomes minimal, causing flow to slow markedly or even briefly cease, resulting in high pulsatility with a large swing between faster systolic and slower diastolic flow. In a very restrictive PDA, because pulmonary artery pressure remains much lower than aortic pressure throughout the entire cycle, a large pressure gradient persists even during diastole. This maintains high-velocity flow across the ductus at all times and leads to low pulsatility. When the end-diastolic velocity exceeds half of the peak systolic velocity (Vmax / V-end-diastole < 2), the flow is described as non-pulsatile or “filled-in.” Overall, this pattern suggests that ductal flow is predominantly driven by systolic pressure differences, while still retaining some pulsatility due to a relatively small residual pressure difference between the aorta and pulmonary artery at end diastole.
This Doppler profile is consistent with an unrestrictive left-to-right patent ductus arteriosus with minimal pressure gradient across the ductus. The measured peak velocity is low, approximately 0.58 m/s, corresponding to an estimated instantaneous systolic aorto-pulmonary pressure gradient of only ~1.4 mmHg. This indicates near-equalization of aortic and pulmonary artery pressures, a hallmark of an unrestrictive ductus. The waveform is highly pulsatile, with clear systolic acceleration after the QRS followed by marked deceleration in diastole, and velocities approaching near-zero during end diastole (before the QRS). This pattern reflects the fact that, in a large PDA, the ductus offers very little resistance to flow. As a result, systolic aortic pressure is readily transmitted into the pulmonary circulation, while during diastole the aorto-pulmonary pressure gradient diminishes substantially as pressures converge. The low velocities do not imply low shunt volume; rather, they imply pressure equalization. Of note, the low velocity throughout the cardiac cycle may also reflect that systemic vascular resistance, while still higher than pulmonary vascular resistance (given the fully left-to-right shunt), remains relatively close to pulmonary vascular resistance, thereby limiting the magnitude of the aorto-pulmonary velocity gradient across the ductus.
This pulsed-wave Doppler profile obtained across the patent ductus arteriosus demonstrates a continuous left-to-right pulsatile unrestrictive shunt with clear phasic modulation across the cardiac cycle. During systole, there is a tall, dense, higher-velocity antegrade jet from the aorta into the pulmonary artery, reflecting the higher systolic instantaneous velocity gradient between the systemic and pulmonary circulations due to the SVR/PVR relationship during peak of systole. The peak systolic velocity is around 2 m/s (pressure gradient of 8 mmHg between the pulmonary and aortic end). As ventricular systole ends and early diastole begins, forward flow persists without interruption, confirming true ductal patency rather than intermittent shunting; the velocity decreases rapidly in systole due to rapid pressure equalization with a low diastolic velocity.
Left to right unrestrictive PDA with a pulsatile pattern. There is a presystolic (late-diastolic) acceleration of left-to-right ductal flow (see box), which is explainable by differences in vascular impedance and compliance. This sharp, very brief late-diastolic acceleration occurs at the end of diastole, before ventricular depolarization, at a time when no new ventricular pressure is being generated. Instead, it reflects how pressure decays on either side of the ductus. During diastole, aortic pressure decays relatively slowly because the systemic circulation has higher impedance and lower compliance, whereas pulmonary arterial pressure decays more rapidly because the pulmonary vascular bed is highly compliant, even when pulmonary vascular resistance is elevated. As diastole progresses, this difference in pressure decay becomes maximal, and just before systole the aorto-pulmonary pressure gradient transiently widens in favor of left-to-right shunting. Because the PDA is wide and unrestrictive, even a very small pressure difference produces a brief, sharp velocity spike. This is a passive hydraulic phenomenon reflecting differential diastolic runoff rather than myocardial activity. At the onset of the QRS complex, ventricular contraction begins. RV ejection starts slightly before LV ejection, when the LV is still in isovolumetric contraction. This creates a drop in the velocity gradient between the aorta and pulmonary artery before the LV ejection occurs and there is a more pronounced gap produced between the Aortic and Pulmonary pressure. Left-to-right ductal flow rebuilds during systole, often with a lower peak velocity than in a restrictive PDA because aortic and pulmonary artery pressures remain relatively close. Overall, this pattern indicates an unrestrictive PDA with near-systemic pulmonary arterial pressure.
Legend: "Representative Doppler spectral velocity profiles of PDA flow in patients with isolated left-to-right shunting. A, Restrictive PDA with high pressure gradients. The superimposed simultaneous pressure tracing (upper panel) demonstrates a continuous pressure gradient from the aorta to the main pulmonary artery (MPA). A peak Doppler-derived gradient of 54 mmHg corresponded to a peak instantaneous pressure gradient of 53 mmHg. The minimum Doppler-derived gradient of 23 mmHg, occurring at end-diastole, corresponded to a minimum pressure gradient of 26 mmHg. The mean Doppler-derived gradient was 41 mmHg, closely matching a mean pressure gradient of 40 mmHg. B, Hypertensive PDA with low pressure gradients. The peak instantaneous systolic pressure gradient was 30 mmHg, corresponding to a maximal Doppler-derived gradient of 32 mmHg. The mean pressure gradient was 14 mmHg, with a mean Doppler-derived gradient of 12 mmHg. Flow below the zero baseline was simultaneously recorded from the descending aorta using continuous-wave Doppler. Ao = aorta; MPA = main pulmonary artery." From: Musewe, N. N., et al. "Validation of Doppler-derived pulmonary arterial pressure in patients with ductus arteriosus under different hemodynamic states." Circulation 76.5 (1987): 1081-1091.
Legend: "Bidirectional flow across the patent ductus arteriosus (PDA) in a patient from group 2. Simultaneous invasive pressure tracings (upper panels) and Doppler spectral velocity recordings are displayed. Flow directed toward the transducer (from the aorta to the main pulmonary artery) is shown above the zero baseline. Abbreviations are as defined in previous figures. All pressure and Doppler measurements were obtained while the patient was breathing room air. No pressure gradient was present between the aorta and the main pulmonary artery during either systole or diastole. The Doppler tracing demonstrates right-to-left shunting during systole and very low-velocity, variable left-to-right shunting during diastole. Pulsed-wave Doppler was used for this assessment, with the sample volume positioned at the pulmonary arterial end of the ductus." From: Musewe, N. N., et al. "Validation of Doppler-derived pulmonary arterial pressure in patients with ductus arteriosus under different hemodynamic states." Circulation 76.5 (1987): 1081-1091.
Legend - "Doppler spectral velocity display with simultaneous invasive pressure tracings from patient 8 (Table 2), who had suprasystemic systolic pulmonary arterial pressure. The presence of a right-to-left systolic pressure gradient is reflected by sustained right-to-left ductal Doppler flow, which is more prolonged than that observed in the other group 2 patients. Flow directed toward the transducer (from the descending aorta to the main pulmonary artery) is displayed above the zero baseline. Abbreviations are as defined in previous figures". From: Musewe, N. N., et al. "Validation of Doppler-derived pulmonary arterial pressure in patients with ductus arteriosus under different hemodynamic states." Circulation 76.5 (1987): 1081-1091.
In the presence of a PDA or VSD shunt - one may use velocity gradient to estimate systolic PA pressure, by evaluating the directionality and systemic systolic blood pressure at the time of echocardiography. However, the PDA is a funnel/tube - as such, all the assumptions of the Bernouilli equation are not respected. The Bernoulli equation is valid for a discrete or focal narrowing, but not for a multi-level obstruction or a gradually progressive narrowing.
R to L post-tricuspid shunt systolic velocity gradient: systolic systemic BP + gradient = estimation of systolic pulmonary arterial pressure
L to R post-tricuspid shunt systolic velocity gradient: systolic systemic BP - gradient = estimation of systolic pulmonary arterial pressure
Important to remember that using the PDA velocity gradient is a rough estimation and assumes the peak systolic velocity gradient occurs at the time of peak systolic aortic pressure and pulmonary arterial pressure (and that both of these peak pressures occur also simultaneously), which is often not true.
An instantaneous pressure gradient is the pressure difference between two locations measured at a specific moment in time during the cardiac cycle. In Doppler echocardiography, this is what is derived from velocity using the Bernoulli equation: it reflects the real-time difference in pressure across a structure (for example, across a PDA, valve, or regurgitant orifice) at the exact instant when that velocity is recorded. When we speak of a peak instantaneous pressure gradient, we mean the largest velocity of flow (and pressure) difference observed at any single moment, which corresponds to the moment of maximal velocity difference—not necessarily to maximal pressure in either chamber or vessel. A peak (or end-systolic) pressure difference, in contrast, refers to the difference between absolute pressures at their own peaks, typically near end-systole. This concept comes from invasive pressure measurements or pressure tracings, where one can identify the maximal aortic pressure and maximal pulmonary or ventricular pressure and then compare them at a defined phase of systole. It is tied to pressure peaks, not to flow velocity. These two quantities do not necessarily occur at the same time.
PDA and VSD shunts do not fully satisfy the assumptions of the simplified Bernoulli equation because the pressure–velocity relationship across these lesions is not governed by a short, fixed, purely resistive orifice under steady conditions. Shunt flow is highly pulsatile and time-dependent, with rapid acceleration and deceleration, so Doppler-derived velocity reflects an instantaneous pressure gradient rather than a stable peak pressure difference. The geometry of a PDA (finite length, curvature, variable diameter) and of many VSDs (irregular or multiple orifices, eccentric jets, partial obstruction by valve tissue) introduces viscous losses, turbulence, and energy dissipation that are not accounted for by the 4V² approximation. In addition, upstream velocity is often non-negligible, and pressure recovery and wave-reflection effects may occur. Most importantly in clinical practice, peak shunt velocity does not necessarily coincide in time with peak aortic, pulmonary arterial, or ventricular pressure; combining a Doppler-derived instantaneous gradient with a non-simultaneous systolic blood pressure can therefore under- or overestimate true chamber or arterial pressures, particularly in large, unrestrictive shunts.
The instantaneous pressure gradient peaks when the difference between the two pressure curves is greatest, which may occur early, mid, or late in systole—or even in late diastole—depending on the shape and timing of the pressure waveforms. Peak or end-systolic pressures, on the other hand, occur when each individual pressure reaches its maximum, which may happen later in systole and not simultaneously between the two vascular beds.
In a normal heart, the peak aortic pressure and the peak pulmonary artery pressure occur at roughly the same phase of systole, but the right ventricle reaches its peak and relaxes slightly earlier, so pulmonary artery systolic pressure typically peaks a bit earlier and falls sooner than aortic pressure. This difference in timing may becoming more or less marked in disease states or in the context of presence of shunts or congenital heart defects. In sinus rhythm with normal valves, both ventricles start ejecting shortly after the QRS, and aortic and pulmonary artery pressures rise together during early systole. The right ventricular outflow and pulmonary artery pressure waves tend to have a shorter acceleration and slightly earlier peak than the left ventricular outflow and aortic pressure wave, so pulmonary artery systolic pressure may reach its maximum a bit before the aortic systolic peak and then decline earlier in late systole.
The ventricles initiate mechanical contraction shortly after the QRS (depolarization of the ventricles). The ventricle is still in mechanical systole during the beginning of the T wave. Mechanical relaxation (the start of diastole) typically begins around the peak of the T wave and is completed by the time the T wave ends. While we often think of the T wave simply as "relaxation," there is a slight lag between the electrical signal (repolarization) and the physical movement of the muscle.
In short, Doppler measures a time-specific pressure difference (instantaneous gradient), whereas peak or end-systolic pressure differences compare absolute pressure maxima. Because pressure and velocity are time-dependent and not temporally locked, these two measures often occur at different moments in the cardiac cycle.
In sinus rhythm with normal valves, both ventricles start ejecting shortly after the QRS, and aortic and pulmonary artery pressures rise together during early systole. The right ventricular outflow and pulmonary artery pressure waves tend to have a shorter acceleration and slightly earlier peak than the left ventricular outflow and aortic pressure wave, so pulmonary artery systolic pressure may reach its maximum a bit before the aortic systolic peak and then decline earlier in late systole.
In summary, doppler interrogation of a PDA provides an estimate of the instantaneous pressure gradient (using instantaneous velocity gradient) between the aorta and the pulmonary artery at specific moments in time, derived from velocity using the Bernoulli relationship, and this gradient does not represent absolute pressure nor does it necessarily occur at peak systolic pressure in either vessel. The moment at which peak PDA velocity occurs corresponds to the time when the difference between aortic and pulmonary arterial pressures is greatest, which may occur early, mid, or late in systole, or even in late diastole, and does not have to coincide with peak aortic pressure, peak pulmonary arterial pressure, or end-systole. Importantly, peak aortic pressure and peak pulmonary arterial pressure themselves may not occur simultaneously. As systole progresses, both pressures may rise in parallel, reducing the instantaneous gradient and therefore reducing velocity, such that the velocity gradient at peak pressures can be smaller than the peak velocity observed earlier or later in the cardiac cycle. In contrast, the tricuspid regurgitation jet reflects peak right ventricular systolic pressure, which typically occurs near end-systole and therefore captures the true maximal RV pressure rather than an early or intermediate systolic value. As a result, estimates of pulmonary arterial pressure derived from PDA velocity and from TR velocity are not interchangeable, because they are sampling different physiologic moments. Using peak PDA velocity in combination with a non-simultaneous systolic blood pressure mixes time-mismatched data and can lead to systematic under- or overestimation of true pulmonary arterial systolic pressure, most commonly underestimation when peak PDA velocity occurs early in systole. The central teaching point is that PDA Doppler measures instantaneous pressure gradients rather than absolute pressures, peak velocity is not equivalent to peak pressure, timing within the cardiac cycle is critical, and combining peak values that do not occur simultaneously introduces predictable physiologic error.
This refers to the physiological process by which electrical activation (depolarization and repolarization) leads to mechanical events (contraction, pressure rise, ejection, relaxation). Normal cardiac function depends on intact electromechanical coupling between electrical activation and mechanical contraction.
Atrial Coupling (The P-Wave): The cycle begins with the P-wave, representing atrial depolarization.
Electrical Event: The SA node fires, and the impulse spreads across the atria.
Mechanical Event (Atrial Systole): After a slight "electromechanical delay", the atria contract.
Flow Effect (The "Atrial Kick"): This contraction provides the final 20–30% of ventricular filling (the "A-wave" on a pressure tracing). This is crucial for "priming" the ventricles and increasing preload just before they contract.
The PR Interval: The PR interval reflects the electrical conduction from the atria through the AV node.
Significance: This pause is vital. It allows the mechanical contraction of the atria to finish pushing blood into the ventricles before the ventricles begin their own contraction.
Flow Effect: Without this delay, the atria and ventricles would contract simultaneously, causing the AV valves to slam shut before the "atrial kick" is complete, significantly reducing the Stroke Volume (SV).
Ventricular Coupling (QRS to T-Wave): Following the PR interval, the QRS complex triggers ventricular depolarization.
Isovolumetric Contraction: As the QRS peaks, the ventricles begin to contract. Pressure rises sharply, closing the Mitral and Tricuspid valves (S1 sound), but it is not yet high enough to open the outflow valves. No blood moves during this split second.
Ventricular Ejection: Once ventricular pressure exceeds aortic/pulmonary pressure, the semilunar valves fly open.
Rapid Ejection: Corresponds to the ST segment. This is where the bulk of the blood flow occurs.
Reduced Ejection: Corresponds to the T-wave. As the heart begins to repolarize electrically, the mechanical force starts to wane, and the flow of blood into the great arteries slows down.
The ventricles are still in mechanical systole during the beginning of the T wave. Mechanical relaxation (the start of diastole) typically begins around the peak of the T wave and is completed by the time the T wave ends. While we often think of the T wave simply as "relaxation," there is a slight lag between the electrical signal (repolarization) and the physical movement of the muscle.
The Return to the P-Wave: Mechanical systole ends near the end of the T-wave, followed by isovolumetric relaxation.
Early Diastole: The ventricles relax, and the Mitral/Tricuspid valves open, allowing for a "Rapid Filling Phase."
Diastasis: A period of slow, passive filling where atrial and ventricular pressures nearly equalize.
The Next P-Wave: The electrical P-wave arrives again to trigger the final "top-off" of the ventricles, matching the electrical rhythm to the mechanical needs of the body.
Mechanical synchrony / dyssynchrony Refers to the timing of contraction between different myocardial regions, not electrical–mechanical coupling per se.
Electrical synchrony / dyssynchrony Refers to conduction timing (e.g., bundle branch block, myocardial / coronary ischemia - fibrosis)
Electromechanical dissociation Electrical activity without effective mechanical contraction (now often called pulseless electrical activity, but still used conceptually)..
The aortic pressure waveform rises sharply after ventricular ejection begins, reaches peak in mid‑systole, then falls with a clear dicrotic notch marking aortic valve closure, followed by a higher diastolic level than the pulmonary artery. The pulmonary artery pressure waveform also rises in early systole but peaks slightly earlier, has a lower absolute amplitude, and its diastolic pressure is much lower than the aortic diastolic pressure, with a smaller dicrotic notch from pulmonic valve closure. The atrial pressure waveform is characterized by three positive deflections—the a, c, and v waves—and two negative deflections, the x and y descents (Fig. 7.1). Atrial contraction generates the a wave, which occurs shortly after the P wave on the ECG. This is followed by the x descent, reflecting atrial relaxation and the downward displacement of the tricuspid annulus during right ventricular contraction. The x descent is briefly interrupted by the c wave, a small transient rise in atrial pressure caused by bulging of the closed tricuspid valve into the right atrium during early ventricular systole. Both the a wave and the x descent are absent in atrial fibrillation. As ventricular systole progresses, passive atrial filling ends the x descent and produces the v wave, which peaks near the end of right ventricular systole and represents the maximum atrial pressure. When the tricuspid valve opens, blood flows from the right atrium into the right ventricle, leading to a rapid fall in atrial pressure and the final negative deflection, the y descent. The overall waveform morphology is similar in the left and right atria, although mean pressures are slightly higher in the left atrium, where the v wave is typically more prominent.
From: Pepine C, Hill J.A, Lambert C.R (eds): Diagnostic and Therapeutic Cardiac Catheterization, 3rd ed 1998. Williams & Wilkins , Baltimore - Link
Timing of the ECG relative to the Aortic and Pulmonary Artery pressure curves.