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Am J Physiol Heart Circ Physiol 283: H1370-H1378, 2002. First published May 23, 2002; doi:10.1152/ajpheart.00051.2002
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Vol. 283, Issue 4, H1370-H1378, October 2002

Quantification of interventricular asynchrony during LBBB and ventricular pacing

Xander A. A. M. Verbeek, Kevin Vernooy, Maaike Peschar, Theo Van der Nagel, Arne Van Hunnik, and Frits W. Prinzen

Department of Physiology, Cardiovascular Research Institute Maastricht, Maastricht University, 6200 MD Maastricht, The Netherlands


    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

The quantification of mechanical interventricular asynchrony (IVA) was investigated. In 12 dogs left bundle branch block (LBBB) was induced by radio frequency ablation. Left ventricular (LV) and right ventricular (RV) pressures were recorded before and after induction of LBBB and during LBBB + LV apex pacing at different atrioventricular (AV) delays. Four IVA measures were validated using computer simulations on experimentally obtained pressure signals. The most robust measure for IVA was the time delay between the upslope of the LV and RV pressure signals (Delta Tup), estimated by cross correlation. The induction of experimental LBBB decreased Delta Tup from -6.9 ± 7.0 ms (RV before LV) to -33.9 ± 7.6 ms (P < 0.05) in combination with a significant decrease of LV maximal first derivative of pressure development over time (dP/dtmax). During LV apex pacing, Delta Tup increased with decreasing AV delay up to +20.9 ± 14.6 ms (P < 0.05). Interventricular resynchronization (Delta Tup = 0 ms) significantly improved LV dP/dtmax by 15.1 ± 5.9%. QRS duration increased significantly after induction of LBBB but did not change during LV apex pacing. In conclusion, Delta Tup is a reliable measure of mechanical IVA, which adds valuable information concerning the nature of asynchronous activation of the ventricles.

left bundle branch block; resynchronization


    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

DURING LEFT BUNDLE BRANCH BLOCK (LBBB), cardiac function is impaired most likely due to a disturbed synchrony of cardiac contraction (7). In patients with heart failure and LBBB, left ventricular (LV) or biventricular pacing therapy endeavors to improve cardiac function by restoring contractile synchrony (3, 4, 6). Indeed, in these patients, pacing therapy can produce a more synchronous pattern of contraction (9, 16) and improves cardiac function (2, 8, 9).

In general, ventricular asynchrony can be divided into intraventricular and interventricular asynchrony (IVA) (3, 9). Ventricular pacing may restore either intraventricular synchrony, interventricular synchrony, or both. Some studies (7, 9, 12) suggest the functional significance of IVA.

The duration of the QRS complex on the surface ECG is often used as a measure for total ventricular asynchrony. More detailed quantitative information about electrical asynchrony is obtained using endocardial electrical mapping techniques (17). For detailed quantification of mechanical asynchrony, MRI tagging (13) or phase imaging based on radionuclide scintography (nuclear phase imaging) (5, 7, 9, 16) has been applied. Also, echocardiography and Doppler myocardial imaging have been used to study ventricular asynchrony (7, 14). Most of these techniques provide information of intraventricular asynchrony. Only the nuclear and echocardiographic techniques have been applied to study IVA (5, 7, 9, 14, 16). More recently, assessment of IVA from LV and right ventricular (RV) pressure signals has been suggested (18, 19).

The present study was undertaken to investigate the feasibility to reliably assess IVA from simultaneously acquired LV and RV pressure signals. These pressure signals represent the combined mechanical behavior of the ventricles and expose an asynchronous time course during pacing and LBBB (11, 12). In the present study, four measures that potentially quantify mechanical IVA were derived from the pressure signals. The measures were compared and validated by computer simulations based on real pressure signals and evaluated by animal experiments during experimental LBBB and LV pacing. A reliable measure for IVA will be an important tool for future studies on elucidation of the mechanism of the influence of asynchronous activation on cardiac function.


    METHODS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Animal experiments. Animal handling was performed according to the Dutch Law on Animal Experimentation and The European Directive for the Protection of Vertebrate Animals used for Experimental and other Scientific Purposes (86/609/EU). The protocol was approved by the Experimental Animal Committee of the Maastricht University.

The experiments were performed on 12 adult mongrel dogs (28 ± 4 kg wt) of either gender. The dogs were premedicated with acepromazine (0.2 mg/kg), atropine (0.1 mg/kg), and oxycodone (2 mg/kg im). Anesthesia was induced with thiopental sodium (15 mg/kg iv) and maintained by ventilation with halothane (0.8 to 1.0%) in a 1:2 mixture of O2 and N2O. A thermal mattress was used to maintain adequate body temperature. Surface ECG was derived from limb leads. LV and RV pressures were recorded simultaneously with two catheter tip manometers (Sentron) introduced through the carotid artery and jugular vein, respectively. Pressure and ECG signals were digitized at a 200-Hz sampling rate and stored on a disk for offline analysis. After the thorax was opened, temporary myocardial pacing leads (model 6500, Medtronic) were implanted at the epicardium of the LV apex and the right atrium. These leads were connected with an external pacemaker (model 5311B AV pacing System Analyzer, Medtronic). LBBB was induced by radio frequency ablation with the use of an ablation catheter (MarinR, Medtronic) and a radio frequency power generator (Atakr, Medtronic). LBBB was characterized by a broad (±100 ms) QRS complex, which, in the dogs, was positive in lead II.

Measurements were performed during sinus rhythm before induction of LBBB, after induction of LBBB, and during LBBB in combination with pacing of the LV apex. Pacing was performed in the VDD mode (atrial sensing and ventricular pacing) with AV intervals increasing from 30 ms to a maximum of 140 ms, with 10-ms steps (n = 6). Pacing at each AV delay was maintained for two to four respiratory cycles, followed by at least four respiration cycles without pacing.

Signal processing and analysis. Before offline analysis of the pressure signals, a second-order Butterworth low-pass filter with a 40-Hz cut-off frequency was used to remove high-frequency artefacts/noise. To avoid phase shifts in each of the signals, the low-pass filter was applied once in forward and once in a backward direction.

Signal processing theory states that a signal is described unambiguously when the sample frequency is at least twice the maximum signal frequency. This demand is fulfilled at the 200-Hz frequency and allows for measurement of time differences more accurately than the duration of the sampling interval (1).

QRS durations and PQ times were acquired by manual offline analysis of the ECG recorded in lead II. The effective paced AV delay (AVe delay) was determined as the time between the onset of the P wave and the pace spike. The AVe delay was used instead of the paced AV delay to correct for differences in position of the atrial sensing lead between the animals. Parameters were calculated for all heart beats within one complete ventilation cycle, of which mean values and standard deviations are reported. The first five beats after the onset of pacing or return to baseline were excluded from the analysis.

The relative timing between the onset of electrical activation of the ventricles was calculated as the difference between the PQ time during LBBB and the AVe delay. During LBBB the PQ time represents the time between the onset of atrial activation to onset of electrical activation of the RV, whereas during LV pacing the AVe delay represents the time between the onset of atrial activation and onset of LV activation. Consequently, the difference between these parameters (PQ timeLBBB - AVe delay) provides the RV-LV excitation time difference.

Quantification of IVA. In Fig. 1, typical examples of LV and RV pressure curves, acquired before induction of LBBB, during LBBB and during LBBB + LV apex pacing with a short AV delay, are presented. The curves were normalized to their full amplitude range to accentuate timing differences. By visual inspection, it is recognized that before induction of LBBB both ventricles contracted approximately synchronously (Fig. 1A), whereas during LBBB, the entire systole of the LV is delayed with respect to that of the RV (Fig. 1B). In contrast, during LV pacing with short AV delay (Fig. 1C), an earlier LV than RV contraction is observed.


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Fig. 1.   Typical examples of left ventricular (LV) and right ventricular (RV) pressure curves acquired before induction of left bundle branch block (LBBB) (A), during LBBB (B), and during LBBB + LV apex pacing (C) with a short atrioventricular (AV) delay (25 ms). Pressures are normalized to their full amplitude range to emphasize timing differences.

For quantification mechanical IVA four measures were derived from the LV and RV pressure signals. The first measure estimates the delay between these signals (Delta Tfull) by shifting them in time until the cross-correlation coefficient (xcc) between the signals reaches its maximal value
xcc<IT>=</IT><FR><NU><LIM><OP>∑</OP><LL><IT>i=</IT>1</LL><UL><IT>N</IT></UL></LIM> (PLV<SUB><IT>i</IT></SUB><IT>−</IT><OVL>PLV</OVL>)<IT>·</IT>(PRV<SUB><IT>i</IT></SUB><IT>−</IT><OVL>PRV</OVL>)</NU><DE><RAD><RCD><LIM><OP>∑</OP><LL><IT>i=</IT>1</LL><UL><IT>N</IT></UL></LIM> (PLV<SUB><IT>i</IT></SUB><IT>−</IT><OVL>PLV</OVL>)<SUP>2</SUP><IT>·</IT><LIM><OP>∑</OP><LL><IT>i=</IT>1</LL><UL><IT>N</IT></UL></LIM> (PRV<SUB><IT>i</IT></SUB><IT>−</IT><OVL>PRV</OVL>)<SUP>2</SUP></RCD></RAD></DE></FR> (1)
where PLVi and PRVi represent the samples of the LV and RV pressure signals, respectively, and <OVL>PLV</OVL> and <OVL>PRV</OVL> represent the mean LV and RV pressure, respectively. By restricting cross-correlation analysis to the upslope of the two pressure curves, a second measure was obtained, now providing an estimate for timing differences between the LV and RV contraction phases (Delta Tup). By definition the timing difference Delta Tup is positive for an earlier LV than RV upslope. Figure 2A shows the cross-correlation function for the examples of LV and RV pressure signals presented in Fig. 1. In this example, cross-correlation analysis was restricted to the upslopes. The estimated time delay between the signals upslopes, determined by the peak of the cross-correlation function, was close to zero before LBBB, negative during LBBB, and positive during pacing. In all cases, the maximal cross-correlation coefficient was close to 1 (>0.99), indicating a high shape similarity of the pressure wave upslopes.


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Fig. 2.   Methods to quantify mechanical interventricular asynchrony (IVA) illustrated using the examples presented in Fig. 1. A: temporal lag resulting in the maximal cross-correlation coefficient (xcc) between the upslope of the LV and RV pressure signals determines the delay (Delta Tup, marked for LBBB). B: the area of the normalized LV-RV pressure loop (PLVn). C: the synchrony index (SI) principle (example for LBBB pressures signals only). dP/dt, first derivative of pressure development over time; LVA25, LV apex pacing at an AV delay of 25 ms; Pn, normalized pressure.

The third measure for IVA is the area of the normalized LV-RV pressure diagram (Fig. 2B). This measure is based on the principle that when plotting any two arbitrary but identical shaped signals against each other, the corresponding loop area equals zero if the signals are completely synchronous, whereas the loop area increases to a maximum area of one with increasing asynchrony. The normalized loop area (APP) was calculated as
A<SUB>PP</SUB><IT>=</IT><LIM><OP>∑</OP><LL><IT>i=</IT>1</LL><UL><IT>N−</IT>1</UL></LIM> (PLVn<SUB><IT>i</IT></SUB><IT>−</IT>PLVn<SUB><IT>i+</IT>1</SUB>)<IT>·</IT>½ (PRVn<SUB><IT>i</IT></SUB><IT>+</IT>PRVn<SUB><IT>i+</IT>1</SUB>) (2)
with PLVni and PRVni samples of the normalized LV and RV pressure signals, respectively. APP has been reported before in preliminary studies (18, 19) but without mentioning directional information. In the present study, APP is positive, by definition, for a clockwise loop direction, i.e., an earlier LV than RV pressure rise and fall, and negative for the counter clockwise direction. An intrinsic property of this measure is that it expresses asynchrony based on the pressures during the complete cardiac cycle, rather than during the contraction phase only. In Fig. 2B, the loops are shown for the three earlier mentioned situations. Before induction of LBBB, the loop has a small negative area, whereas during LBBB the loop is larger. During LV pacing with a short AV delay, the loop is also larger than before LBBB but with a reversed course.

Finally, a synchrony index (SI) was derived from the two pressure curves. The SI has been reported (15) as a measure of the synchrony of volume changes between ventricular segments with the conductance catheter technique. This index provides a measure for the time that the two signals change in the same direction, relative to the duration of the cardiac cycle. In the present study, SI was calculated by considering only that part of the cardiac cycle during which the product of the first derivative of the LV and RV pressure signal is >0. To increase the stability of the SI, both the LV and RV pressures were required to exceed the LV and RV end diastolic pressure, respectively, and only simultaneous positive pressure changes were considered, thus restricting calculation of the SI to the contraction phases (Fig. 2C).

Simulations/validation of measures of IVA. To validate the four proposed measures, computer simulations were performed with the use of pressure signals obtained from the experiments. To study how each measure responds to a timing difference, the LV and RV pressure curves were shifted in time with respect to each other approximating gradual changes in timing, similar to those presented in Fig. 1. To enable shifting the pressure curves with respect to each other with 1-ms steps during simulations, the signals were reinterpolated at 1 KHz. For each temporal lag Delta Tfull, Delta Tup, APP, and SI were determined. For the loop area method, the APP as a function of the temporal lag was also calculated without taking into account the directional information. Simulations were performed using pressure curves acquired during sinus rhythm before induction of LBBB, after induction of LBBB, and during LBBB + LV apex pacing at short AV delay, to demonstrate the effect of different initial pressure curve shapes.

To study the influence of shape changes of the pressure signals in more detail, gradual changes in rate of pressure rise and width of the pressure signals were simulated. LV maximal first derivative of pressure development over time (dP/dtmax) was changed by application of a low-pass filter, whereas the RV pressure curve was not changed. The cutoff frequency of the filter was decreased until a desired change in dP/dtmax was attained. The width of the LV pressure signal was changed by reinterpolating the LV pressure signals followed by setting the time resolution to 1 ms.

The frequency at which reinterpolation was performed was varied until a desired change in curve width is attained, characterized by its full width at half maximum (FWHM). Again, the RV pressure curve was not changed. For each of the initial LV pressure waves, the width was changed in a range from -20 to 20 ms. To ensure that the curve upslope (dP/dtmax) was not affected, only the part of the curve after instance of the peak pressure was reinterpolated.


    RESULTS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Simulation results. Figure 3 depicts how the simulated temporal lag between in vivo recorded LV and RV pressure signals influences the four proposed measures of IVA. A linear relation was found between the applied temporal lag and estimated Delta Tfull and Delta Tup (Fig. 3, A and B). The offset in Delta T between the pre-LBBB, LBBB, and LBBB + pacing results can, among others, be attributed to timing differences in LV and RV pressure signals between the different experimental conditions.


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Fig. 3.   Simulation results for evaluation of IVA measures. Experimentally obtained LV and RV pressure signals were shifted in time with respect to each other with temporal lags ranging from -100 to 100 ms. Simulations were repeated for pressure signals acquired before induction of LBBB (pre-LBBB), during LBBB, and during LBBB + LV apex pacing at a 25-ms AV delay. Presented are the estimates for the time delay between the full LV and RV pressure signals (Delta Tfull) (A), the time delay between the upslopes of the LV and RV pressure signals (Delta Tup) (B), the normalized pressure loop area APP (C), and SI (D). Also shown in C is the APP calculated without taking into account the loop direction (see *).

The relation between APP and the imposed temporal lag was nonlinear and shows a different behavior for each of the three experimental conditions (Fig. 3C). Neglecting the loop direction results in a measure for IVA without an indication of which ventricle is activated first (always positive values).

By definition also the SI was always positive and therefore did not include directional information. Comparison of the three experimental conditions showed different maximum values for each experimental situation (Fig. 3D). The plateau around the maximum originated from differences in duration of the LV and RV contraction phases, the shorter phase coinciding with the longer phase for a range of subsequent temporal lags.

Figure 4 depicts the effect of changes in LV dP/dtmax on the behavior of the four measures. The absolute errors were only 1 ms for Delta Tup (Fig. 4B) but as large as 7 ms for Delta Tfull (Fig. 4A) whereas errors introduced in APP and SI were significantly larger (Fig. 4, C and D). Figure 5 shows that changing FWHM introduced significant errors in Delta Tfull (Fig. 5A), APP, and SI (Fig. 5, C and D), whereas Delta Tup is not affected by the FWHM (Fig. 5B).


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Fig. 4.   Effect of increase in LV maximum dP/dt (dP/dtmax) on the IVA measures. Changes are applied to experimentally obtained pressure signals acquired before induction of LBBB, during LBBB, and during LBBB + LVA25. Absolute errors in Delta Tfull (A), Delta Tup (B), APP (C), and SI (D) vs. the applied change in LV dP/dtmax.



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Fig. 5.   The effect of changes in LV pressure signal width [full width at half maximum (FWHM)] on the IVA measures. Changes are applied to real pressure signals acquired before induction of LBBB, during LBBB, and during LBBB + LV apex pacing at an AV delay of 25 ms (dotted lines). Absolute errors in Delta Tfull (A), Delta Tup (B), APP (C), and SI (D) vs. the applied change in FWHM.

Experimental results. Table 1 presents the values of Delta Tfull, Delta Tup, APP, SI, and hemodynamic values measured before and directly after induction of LBBB. After the induction of LBBB, Delta Tfull, Delta Tup, and APP decreased significantly compared with pre-LBBB values. Induction of LBBB significantly increased QRS duration and decreased LV dP/dtmax but did not change heart rate and RV and LV systolic and end-diastolic pressures.

                              
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Table 1.   Changes in interventricular asynchrony, QRS duration, and hemodynamics due to induction of LBBB

In Fig. 6, the relation between Delta Tup and the paced AV delay is presented, showing a large variation between the animals. This variation completely disappeared when the AV delay was standardized with the use of the RV-LV excitation time difference (Fig. 7B).


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Fig. 6.   Estimated Delta Tup vs. the paced AV delay for 8 different dogs, showing a large variation between the animals at each AV delay.



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Fig. 7.   Estimated Delta Tfull (A), Delta Tup (B), APP (C), and SI (D) vs. electrical RV- LV excitation time difference (= PQ timeLBBB - AVe delay) for 8 different dogs. Also displayed are values during LBBB without pacing. PQ times during LBBB for the different dogs ranged from 80 to 144 ms. AVe, effective AV delay (see METHODS).

Figure 7 depicts the relation between the four IVA measures during LV apex pacing with different AV delays as a function of the RV-LV excitation time difference (PQ timeLBBB - AVe delay, see METHODS). For Delta Tfull, Delta Tup, and APP, a sigmoid relation was found with the lowest values during pacing with the longest AV delays and the highest values during pacing with the shortest AV interval (25-30 ms). For Delta Tup, an excellent match of the results from the various dogs was found. Delta Tup increased in an almost linear fashion from approximately -35 to 35 ms when the RV-LV excitation time difference increased from 0 to 80 ms. Linear regression provided an r2 = 0.95, a slope = 0.7, and an intercept with the horizontal axis of 29 ms. A similar sigmoid shape for Delta Tfull and APP was found, but with more variation between animals. The data for SI were very noisy, caused by both beat-to-beat and interanimal differences (Fig. 5D).

In Fig. 8 the relation between QRS duration and Delta Tup is presented for measurements before and after induction of LBBB and during LBBB + LV apex pacing for all AV delays. A good correlation was found for the combined before and after LBBB measurements (r = 0.81) but a poor and completely different correlation was present during LBBB + LV apex pacing (r = 0.63).


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Fig. 8.   Relation between QRS duration and Delta Tup for measurements before and after induction of LBBB and during LBBB + LV apex pacing for all AV delays. Also shown are regression lines for the combined measurements before and after LBBB and during LBBB + LV apex pacing for all AV delays.

Figure 9 shows the changes in LV and RV curve width difference (Delta FWHMLR = FWHMLV - FWHMRV) as a function of the RV-LV excitation time difference. In most cases, the LV curve was clearly wider than the RV curve but pacing significantly affected Delta FWHMLR. Moreover, RV-LV curve width differences and its changes during pacing varied considerably between experiments.


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Fig. 9.   Changes in LV and RV curve width difference (Delta FWHMLR) as a function of the RV-LV excitation time (= PQ timeLBBB - AVe delay). Also displayed are LBBB values.

Finally, Table 2 shows the changes in heart rate and QRS duration and hemodynamic parameters measured during LBBB + LV apex pacing at the AV delays at which Delta Tup = 0. LV dP/dtmax increased significantly by 15.1 ± 5.9%. There was a good correlation between Delta Tup and improvement in LV dP/dtmax (r = 0.86 ± 0.10). QRS duration, heart rate, and other hemodynamic parameters showed no significant changes, except for a slight decrease of RV systolic pressure.

                              
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Table 2.   Changes in QRS duration, heart rate, and hemodynamic values measured during interventricular resynchronization


    DISCUSSION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

The present study shows that IVA can be reliably assessed from simultaneously acquired LV and RV pressure signals. The time difference between the upslope of the pressure signals estimated by cross correlation proves to be the most reliable measure because it is virtually insensitive to changes in the shape of the curves, the experimental results show an excellent reproducibility of Delta Tup changes between the animals, there is a linear relation between Delta Tup and the applied RV-LV excitation time difference, and it provides a beat-to-beat measure for asynchrony in milliseconds, which can be easily interpreted.

The simulations on in vivo recorded pressure signals revealed a linear relation between the applied temporal lag and the estimated time delay both for Delta Tfull as for Delta Tup, but this finding is trivial based on pure mathematical considerations. However, experimentally a similar relation was found between Delta Tup and a major part of the range of RV-LV excitation time differences (Fig. 7B). The intercept of the estimated mechanical IVA with the horizontal axis is probably due to the electromechanical delay. The observed intercept value of 29 ms is within the range of values of the interval between the Q wave and LV pressure rise in intact dog hearts (21 ± 5 to 33 ± 14 ms) (10). The slope between Delta Tup and the RV-LV excitation time difference was <1. This may be explained by different fusion patterns and timing of the merging wave fronts coming from the LV (pacing) and RV (right bundle branch). With decreasing or increasing RV-LV excitation time difference during LBBB + pacing, one ventricle will eventually be completely activated via the other one through transseptal conduction. Therefore, more extreme values of the RV-LV excitation time difference will cause no further change in IVA, which explains the sigmoid shape of the relation between applied RV-LV excitation time difference and mechanical IVA. Variations in Delta Tup values during LBBB between the animals can be attributed to differences in trans septal conduction time.

The results from Figs. 6 and 7 indicate the importance of standardizing the AV delay by introduction of the RV-LV excitation time difference. An alternative method for standardizing the AV delay was introduced by Auricchio et al. (2), who normalized AV delay on PR interval. For the present study, where absolute differences in timing between the LV and RV are relevant, the RV-LV excitation time difference is preferred.

The two IVA measures, which are based on analysis of the pressure curves during the full cycle (Delta Tfull and APP), performed less that Delta Tup. The simulations show that both measures are sensitive to shape changes in the pressure curves. Shape changes similar to those produced by simulations also occur during experimental variation of the mode of activation and are therefore a plausible explanation the lower reproducibility of Delta Tfull and APP. The experiments reveal that changes in shape occur gradually with increasing AV delay (Fig. 9), thus explaining the still smooth, instead of noisy, behavior of the experimental results for Delta Tfull and APP for each separate animal (Fig. 7, A and C).

An additional problem of APP, exposed by the simulations, is the nonlinear relation with the imposed timing differences between the LV and RV pressure waves. Within the range of timing differences in the present study, however, the relation with APP is approximately linear. The similarity between the experimental results for APP and Delta Tfull illustrates that the reliability of an IVA estimate is not determined by the method of assessing it (RV-LV pressure loop vs. cross correlation) but rather by restricting the analysis to the upslope of the pressure curves. Time domain restriction to the contraction phase is not possible for the loop method because the loop method is essentially a frequency domain measurement. The SI is clearly the worst-performing measure of IVA, due to a high sensitivity to curve shape. Also, the range of the SI values in the experiments is small and the SI does not contain directional information.

The good correlation between QRS duration and IVA in the canine hearts before and during LBBB is in agreement with the data presented by Rouleau et al. (14) for patients with dilated cardiomyopathy and a large range of QRS durations. However, the present study shows that during LBBB + LV apex pacing the correlation between QRS duration and IVA is lower and completely different. This is in agreement with a nuclear phase imaging study in LBBB patients during biventricular pacing therapy (9). Moreover, it indicates that IVA adds valuable information concerning the nature of asynchronous activation of the ventricles.

In patients with dilated cardiomyopathy and QRS durations >150 ms, IVA values determined with echocardiography ranged between -77 ± 15 and -88 ± 26 ms (14). Similar values (-85 ± 31 ms) were found with nuclear phase imaging for patients with isolated LBBB (7). The smaller IVA values for dogs found in the present study (-33.9 ± 7.6 ms) are not surprising because the QRS duration is also smaller in dogs (123.7 ± 20.2 ms) than in patients.

Although the decrease in LV dP/dtmax after induction of LBBB is associated with an increase in IVA (more negative Delta Tup) and QRS duration (Table 1), the increase in LV dP/dtmax due to interventricular resynchronization (Table 2) leaves the QRS duration unaltered. This finding, together with the good correlation between IVA and improvement in LV dP/dtmax, supports the idea that IVA contains important information. Further studies, including indexes of intraventricular asynchrony and IVA and the use of other pacing sites, are required to fully elucidate the importance of the various aspects of asynchronous activation for ventricular function.

A disadvantage of the currently presented method is its invasive nature requiring biventricular catheterization. Noninvasive alternatives may be provided by echocardiography or tissue Doppler imaging. MRI tagging can only provide IVA if the RV tags can also be analyzed. This has not been reported yet. In the echocardiography and tissue Doppler imaging study (14) mentioned earler, IVA was assessed as the timing difference between the opening of the pulmonary and aortic valves and the timing difference between onset of the positive waves recorded at the lateral corners of the tricuspid and mitral annulus. In nuclear phase imaging studies, timing differences are derived from a user defined region of interest in a cross section of the ventricles excluding the septum (7, 9).

An important advantage of the cross-correlation method, however, is that it incorporates the full contraction phase of the ventricles and that the pressure curves represent the true average of the contraction of the entire ventricles. Consequently, this method is more sensitive to timing differences and less sensitive to noise than a single point measurement in time, such as the opening of valves. Other advantages of the currently presented technique to assess IVA from LV and RV pressure curves are the accuracy and the relatively plain techniques. Moreover, this IVA measure provides beat-to-beat values and does not require the injection of radioisotopes.

In conclusion, mechanical IVA can be quantified reliably as the Delta Tup of the LV and RV pressure waves with the use of cross correlation. Induction of LBBB increases both QRS duration and Delta Tup significantly, but LV pacing during LBBB increases Delta Tup at unchanged QRS duration. Delta Tup relates linearly with the applied electrical delay between the ventricles during LV apex pacing at different AV delays. Interventricular resynchronization is associated with an improvement of LV dP/dtmax. Therefore, Delta Tup provides important information about the asynchronous contraction between the LV and RV during LBBB with our without ventricular pacing.


    FOOTNOTES

Address for reprint requests and other correspondence: X. A. A. M. Verbeek, Dept. of Physiology, Cardiovascular Research Institute Maastricht, Maastricht Univ., PO Box 616, 6200 MD Maastricht, The Netherlands (E-mail: x.verbeek{at}fys.unimaas.nl).

The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.

May 23, 2002;10.1152/ajpheart.00051.2002

Received 25 February 2002; accepted in final form 16 May 2002.


    REFERENCES
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

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Am J Physiol Heart Circ Physiol 283(4):H1370-H1378
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