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(Circulation. 1995;92:875-880.)
© 1995 American Heart Association, Inc.


Articles

Effect of Increased Drive-train Stimulus Intensity on Dispersion of Ventricular Refractoriness

Jeffrey J. Goldberger, MD; Jeffrey R. Smith, MD; You-Ho Kim, MD; Roger S. Damle, MD; Alan H. Kadish, MD

From the Division of Cardiology and the Department of Medicine, Northwestern University Medical School, Chicago, Ill.


*    Abstract
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*Abstract
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down arrowResults
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Background Most studies evaluating the effects of high-intensity drive-train (S1) stimulation on the measurement of the ventricular effective refractory period (VERP) demonstrated a shortening of the VERP. Because this effect may be due to the local release of catecholamines, VERP shortening would be expected to occur only near the site of stimulation. Local shortening in the VERP should then result in an increased dispersion of refractoriness during high-intensity drive-train stimulation. Thus, this study evaluated the spatial distribution of the VERP shortening resulting from high-intensity S1 stimulation and its effect on dispersion of refractoriness.

Methods and Results Three groups of patients were studied. In group 1, 10 subjects without structural heart disease had VERP determinations performed at the right ventricular apex (RVA) and outflow tract (RVOT) while the S1 site was changed to evaluate the effects of low-intensity S1 stimulation on the measured VERP. In group 2, the effect of high-intensity S1 stimulation on the VERP was studied 0, 7, 14, and 21 mm away from the S1 site to measure the spatial distribution of VERP shortening and the effect on dispersion of refractoriness; 10 additional subjects without structural heart disease made up group 2. Because increased dispersion of refractoriness may be deleterious in certain clinical situations, the effect of high-intensity S1 stimulation was studied in group 3, which comprised 10 subjects with chronically implanted transvenous defibrillators; noninvasive measurements of the VERP through the chronic lead were made while the S1 stimulus intensity was varied from low to high intensity. All VERP determinations were performed during continuous pacing by use of an incremental method and a low stimulus intensity for the extrastimulus. In group 1, the RVA VERPs were 218±9 and 214±10 ms when the S1 site was the RVA and RVOT, respectively (P=NS). The RVOT VERPs were also unchanged when the S1 site was changed from the RVOT to the RVA. In group 2, high-intensity S1 changed the VERP from 224±8 (at twice the threshold) to 203±10 ms (P<.01), 220±11 to 209±12 ms (P<.01), 222±12 to 221±12 ms, and 220±11 to 221±11 ms at 0, 7, 14, and 21 mm away from the S1 site, respectively. High-intensity S1 stimulation led to an increase in the dispersion of refractoriness from 13±4 to 22±9 ms (P=.006). In group 3, high-intensity S1 stimulation shortened the VERP from 309±23 to 285±30 ms (P=.0003).

Conclusions Low-intensity S1 stimulation has no significant effect on the VERP. High-intensity S1 stimulation shortens the refractory period maximally at the site of stimulation; the VERP shortening dissipates between 7 and 14 mm away from the site of S1 stimulation, resulting in an increased dispersion of refractoriness. The local VERP shortening with high-intensity stimulation is noted in patients with chronically implanted defibrillator leads, which may have implications for the mechanism of proarrhythmia during high-intensity stimulation.


Key Words: electrophysiology • pacing • ventricles • electric stimulation • refractory period


*    Introduction
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up arrowAbstract
*Introduction
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The ventricular effective refractory period is typically measured after a basic drive train.1 Several studies evaluated the effects of various properties of this drive train such as rate, duration, and stimulus intensity on the determinations of the refractory period. When the refractory period is measured at a particular test site, it is customary to apply the basic drive train at the same site. However, the basic drive train may be applied from other sites. In this manner, a number of studies2 3 4 5 evaluated whether the refractory period measured at the test site changes when the basic drive train is moved to a site remote from the test site (with a stimulus output 1.5 to 2 times the late diastolic threshold) and yielded conflicting results. Thus, some investigators reported that drive-train stimulation at the test site shortens the refractory period,2 3 4 while others reported that it lengthens the refractory period.5 In the present study, the effect of low-intensity drive-train stimulation at the site of refractory period determination (versus a site remote from the site of refractory period determination) on the measured refractory period was reevaluated.

A number of studies2 6 7 also evaluated the effects of high-intensity stimulation during only the conditioning drive on the measurement of the refractory period. Most studies show a decrease in the ventricular effective refractory period when a high stimulus intensity is used for the conditioning drive. Langberg et al6 demonstrated that increasing the drive-train stimulus intensity in humans shortens ventricular refractoriness at the site of stimulation. In that study, autonomic blockade blunted the effect of increased drive-train stimulus intensity on the ventricular effective refractory period, suggesting that a local release of norepinephrine may be the mechanism for this effect. In support of this, other studies8 9 10 suggested that high-intensity electric stimulation of myocardium may result in the release of catecholamines.

Because local release of catecholamines would be expected to have only a regional effect on the refractory period, the present study was designed to evaluate the spatial distribution of the shortening of ventricular refractoriness resulting from high-intensity stimulation. Specifically, we postulated that the shortening of ventricular refractoriness observed with increased drive-train stimulus intensity would be most prominent at the site of drive-train stimulation and would decrease progressively as one moved away from the site of stimulation. This local shortening in the ventricular effective refractory period should then result in an increased dispersion of refractoriness during high-intensity drive-train stimulation. To isolate the effect of high-intensity stimulation, the effect of low-intensity stimulation was first characterized. Finally, the effect of high-intensity drive-train stimulation was evaluated in a group of patients with chronically implanted transvenous defibrillators, a group in whom increased dispersion of refractoriness might be deleterious.


*    Methods
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up arrowAbstract
up arrowIntroduction
*Methods
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Patient Population
Three groups of subjects were evaluated in this study. Group 1 comprised 10 subjects without structural heart disease who were undergoing electrophysiology studies in the drug-free state for the evaluation and/or treatment of paroxysmal supraventricular tachycardia (n=9) or syncope (n=1). There were 8 men and 2 women with a mean age of 33.5±9.9 years. The effect of moving the site of drive-train (S1) stimulation (using a low stimulus intensity) relative to the test (S2) site on the ventricular effective refractory period was evaluated in this group.

Group 2 comprised 10 subjects without structural heart disease who were undergoing electrophysiology studies in the drug-free state for the evaluation and/or treatment of paroxysmal supraventricular tachycardia (n=10). There were 4 men and 6 women with a mean age of 44.2±12.1 years. The effects of high-intensity drive-train stimulation on the ventricular effective refractory period at the site of drive-train stimulation and at selected distances from this site were evaluated in this group.

Group 3 comprised 10 subjects who had transvenous implantable cardioverter-defibrillators (ICDs) at least 1 month before evaluation. All systems consisted of the Cadence ICD (Ventritex) and the Endotak C0064 series (Cardiac Pacemakers Inc) lead system. There were 9 men and 1 woman with a mean age of 71.2±8.0 years. Indications for ICD implantation were either cardiac arrest (n=3) or ventricular tachycardia (n=7). Three patients were receiving amiodarone therapy at the time of evaluation. Eight patients had coronary artery disease; the other 2 had noncoronary cardiomyopathies. Three had anterior myocardial infarctions, 3 had inferior myocardial infarctions, and 1 had both inferior and anterior myocardial infarctions. Seven patients had ejection fractions <30% (mean ejection fraction, 35±19%; range, 20% to 68%). The effect of high-intensity drive-train stimulation on the ventricular effective refractory period at the site of drive-train stimulation was evaluated in this group.

All patients provided written, informed consent for this study, which was approved by the Institutional Review Board of Northwestern University.

Refractory Period Determinations
All subjects were studied while in the mildly sedated, fasting state. For groups 1 and 2, multiple electrode catheters were positioned, as clinically indicated, in the high right atrium, His bundle region, and right ventricle through sheaths placed in the femoral vein. Surface ECG leads I, II, III, V1, and V6 and intracardiac electrograms (groups 1 and 2) were displayed on an oscilloscope and recorded at a paper speed of 25 to 200 mm/s, as needed. Intracardiac electrograms were filtered from 40 to 400 Hz. For groups 1 and 2, pacing was performed with a programmable stimulator (Bloom Associates) with one or two stimulus isolation units, as needed, using 2-ms rectangular pulses. For group 3, pacing was performed noninvasively with the Cadence programmer.

All refractory period determinations were performed during continuous ventricular overdrive pacing (S1 cycle lengths, 500 ms for groups 1 and 2 and 670 ms for group 3). After a 2-minute conditioning period, an extrastimulus (S2) was initially introduced at a coupling interval less than the refractory period and was incremented by 2 ms every fifth beat until capture was noted. In group 3, the minimum increment available was 10 ms. The incremental method was shown to result in more accurate refractory period determinations.11 The S2 stimulus strength was set at two times the late diastolic threshold for all determinations. When the S1 and S2 sites were the same, the ventricular effective refractory period was defined as the longest S1S2 interval that failed to evoke a ventricular depolarization. If the S1 and S2 stimulation sites differed, the conduction time from the S1 to the S2 site during continuous pacing was measured (stimulus to first rapid deflection of the electrogram recorded at the test site; Fig 1Down). The ventricular effective refractory period at the test site was defined as the longest S1S2 interval that failed to evoke a ventricular depolarization minus the conduction time from the S1 site to the S2 site.



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Figure 1. Simultaneous recordings of surface ECG leads I, II, and V1 and intracardiac recordings from the proximal three pairs of electrodes. S1 stimulation is performed from the distal pair of electrodes. The conduction times to the three successively more proximal pairs of electrodes (RV2, RV3, and RV4—most proximal) are 10, 20, and 30 ms. When the refractory periods at these proximal sites are measured while S1 stimulation is performed from the distal pair of electrodes, these conduction times are subtracted from the longest S1S2 interval that failed to evoke a ventricular depolarization to obtain the true refractory period at that site.

Effect of Low-Intensity Drive-train Stimulation on Ventricular Refractoriness
To evaluate the effect of low-intensity S1 stimulation on ventricular refractoriness, the S1 stimulation intensity was kept fixed while the S1 stimulation site varied relative to the S2 stimulation site. Thus, in group 1, quadripolar catheters with 2-mm interelectrode spacing within each pair of electrodes and 5-mm spacing between each pair (2-5-2 configuration) were positioned in the right ventricular apex and right ventricular outflow tract. A capture threshold <1.0 mA was required at both sites. The refractory period was measured at the right ventricular apex by use of S1 drive trains from both the right ventricular apex and outflow tract. The refractory period was also measured at the right ventricular outflow tract by use of S1 drive trains from both the right ventricular apex and outflow tract. Thus, four refractory period determinations were made in random sequence. The stimulus intensity was twice the diastolic threshold for both the S1 drive and the extrastimulus.

Spatial Effect of High-Intensity Drive-train Stimulation on Ventricular Refractoriness
In group 2, the effect of the distance from the S1 stimulation site on the shortening of ventricular refractoriness resulting from high-intensity S1 stimulation was evaluated. Thus, the S1 stimulation site was fixed, but the S1 stimulus intensity was varied, as was the S2 stimulation site (with a fixed low stimulus intensity). A custom-designed octapolar 7F catheter (Mansfield) was positioned in the right ventricular apex. The four pairs of electrodes had 2-mm spacing within each pair of electrodes and 5-mm spacing between each pair (2-5-2-5-2-5-2 configuration). Thus, the spacing between electrode pairs was 7 mm. The catheter was positioned with the tip in the right ventricular apex and the more proximal electrodes against the ventricular septum. If a capture threshold <1.0 mA could not be achieved at all four sites, the catheter was repositioned so that all four sites had capture thresholds <1 mA (5 of 15 subjects initially screened were excluded because of an inability to achieve a stable threshold <1 mA at all four sites).

The drive-train (S1) stimulation site was the distal set of electrodes for all refractory period determinations. Ventricular effective refractory period determinations were made at each of the four sets of electrodes along the catheter in random order. At each site, the ventricular effective refractory period was determined by use of a drive-train stimulus intensity of two times the late diastolic threshold (of the distal set of electrodes) and at 10 mA. The S2 stimulus strength was set at two times the late diastolic threshold for each site for determinations at both S1 stimulus intensities. Thus, eight refractory period determinations were made in random sequence (at each of the four sites using low- and high-intensity drive-train stimulation). The effect of high-intensity stimulation at each site was evaluated by examination of the difference in refractory periods between the two stimulus intensities. Dispersion of refractoriness at each stimulus intensity was defined as the longest ventricular effective refractory period measurement minus the shortest one for that stimulus intensity.

Effect of High-Intensity Drive-train Stimulation on Ventricular Refractoriness in Patients With ICDs
In group 3, the S1 stimulation site was fixed, but the stimulus intensity was varied. Continuous pacing at 90 beats per minute was initiated through the bradycardia programming function. Low-intensity S1 stimulation was either at 1 or 2 V, whichever led to consistent ventricular capture. High-intensity stimulation was achieved with a 10-V output from the bradycardia programming function. After the 2-minute conditioning period, extrastimuli were applied with the noninvasive programmed stimulation feature. The initial coupling interval was below the refractory period and was increased by 10-ms increments until capture was obtained. The stimulus intensity for S2 was set at 1 or 2V. Thus, two refractory period determinations were made in random sequence.

Data Analysis
All data are presented as mean±SD. A paired Student's t test was used to compare all paired data. In group 2, a one-factor ANOVA was used to evaluate the effects of distance from the S1 stimulation site on the difference in refractory periods between the two stimulus intensities. A value of P<.05 was considered statistically significant.


*    Results
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up arrowIntroduction
up arrowMethods
*Results
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Effect of Low-Intensity Drive-train Stimulation on Ventricular Refractoriness
The late diastolic capture threshold at the right ventricular apex was 0.38±0.10 and 0.42±0.22 mA at the right ventricular outflow tract. Ventricular effective refractory period determinations at the right ventricular apex or outflow tract did not significantly vary as the S1 stimulation site varied. Thus, the refractory periods at the right ventricular apex were 218±9 and 214±10 ms when the S1 stimulation site was the apex and the outflow tract, respectively. The refractory periods at the right ventricular outflow tract were 214±16 and 214±15 ms when the S1 stimulation site was the outflow tract and the apex, respectively. Thus, low-intensity S1 stimulation at the site of refractory period determination has no effect on the measured refractory period.

Spatial Effect of High-Intensity Drive-train Stimulation on Ventricular Refractoriness
The late diastolic capture thresholds at each of the four test sites were 0.36±0.11 mA at the distal pair of electrodes, 0.50±0.25 mA at pair 2, 0.48±0.23 mA at pair 3, and 0.59±0.29 mA at the most proximal pair (P=NS by ANOVA). When both S1 and S2 were delivered at the distal electrode, the mean ventricular effective refractory period decreased from 224±8 ms at a drive-train stimulus intensity of two times the diastolic threshold to 203±10 ms at a drive-train stimulus intensity of 10 mA (P<.01; Fig 2Down). When S2 was delivered 7 mm away from the S1 stimulation site, the ventricular effective refractory period decreased from 220±11 ms at an S1 stimulus intensity of two times the diastolic threshold to 209±12 ms at an S1 stimulus intensity of 10 mA (P<.01; Fig 2Down). When S2 was delivered 14 and 21 mm away from the S1 stimulation site, there were no significant differences between the ventricular effective refractory periods at S1 stimulus intensities of two times the diastolic threshold or at 10 mA (Fig 2Down). At an S1 stimulus intensity of two times the diastolic threshold, the ventricular effective refractory periods were 222±12 and 220±11 ms at 14 and 21 mm, respectively. At an S1 stimulus intensity of 10 mA, the ventricular effective refractory periods were 221±12 and 221±11 ms at 14 and 21 mm away from the S1 stimulation site. There were no significant differences between the ventricular effective refractory periods measured at each of the four sites when determined at an S1 stimulus intensity of two times the diastolic threshold.



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Figure 2. Line graph showing mean±SD of the ventricular effective refractory period (VERP) at each site when the S1 stimulus intensity was twice the threshold and 10 mA. The most marked shortening in VERP is noted at the S1 stimulation site. A significant shortening in the VERP is noted 7 mm away from the S1 stimulation site. At 14 and 21 mm away, there is no significant change in the VERP. *P<.01.

Because low-intensity S1 stimulation was shown to have no significant effect on the measurement of the ventricular effective refractory period, the change in refractory period at each site when the S1 stimulus intensity was increased from twice the threshold to 10 mA represents the effect of the increased S1 stimulus intensity at that distance from the S1 site. Increasing the drive-train stimulus intensity from twice the diastolic threshold to 10 mA resulted in significant shortening of the refractory period (P<.0001; Fig 2Up). At the site of stimulation, there was a 21±9-ms shortening (P<.05 versus 7 mm away and P<.0001 versus 14 and 21 mm away). There was an 11±7-ms shortening 7 mm away from the site of stimulation (P<.05 versus 14 mm and P<.005 versus 21 mm away). At 14 and 21 mm away from the site of drive-train stimulation, there was no significant shortening of the refractory period with an increase in the drive-train stimulus intensity (1±3 and -1±2 ms, respectively).

Dispersion of refractoriness at the four tested sites at an S1 stimulus intensity of two times the diastolic threshold was 13±4 ms. At an S1 stimulus intensity of 10 mA, the dispersion of refractoriness increased to 22±9 ms (P=.006). Fig 3Down shows the individual changes in the dispersion of refractoriness. Of the 10 patients, 8 had an increase in the dispersion of refractoriness at 10 mA versus that at twice the threshold. Overall, the mean increase in dispersion of refractoriness was 9±10 ms (range, -5 to 22 ms).



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Figure 3. Line graph showing changes in dispersion of ventricular refractoriness for each of the 10 subjects ({circ}) noted at an S1 stimulus intensity of twice the threshold and at 10 mA. {blacksquare} indicates the mean±SD for the two groups. *P=.006.

Effect of High-Intensity Drive-train Stimulation on Ventricular Refractoriness in Patients With ICDs
Interrogation of the ICD revealed that the R-wave amplitude at the site of stimulation was >10 mV (at an autogain setting of 0) in 9 patients and 6 mV (at an autogain setting of 1) in 1 patient. In 6 patients, low-intensity S1 and S2 stimulation was performed at an output of 1 V; in the other 4, an output of 2 V was required. The mean ventricular effective refractory period decreased from 309±23 ms at a low drive-train stimulus intensity to 285±30 ms at a drive-train stimulus intensity of 10 V (P=.0003). Thus, high-intensity stimulation resulted in a mean shortening of the ventricular effective refractory period of 24±15 ms. All subjects had a shorter refractory period with high-intensity S1 stimulation (range, 10 to 50 ms). There was no correlation between the shortening of the ventricular effective refractory period and either age or ejection fraction. Similarly, the patients who were taking amiodarone had a similar shortening of the ventricular effective refractory period with high-intensity S1 stimulation compared with those not taking antiarrhythmic drugs (27 versus 23 ms).


*    Discussion
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up arrowAbstract
up arrowIntroduction
up arrowMethods
up arrowResults
*Discussion
down arrowReferences
 
This study showed that low-intensity drive-train stimulation has no significant effect on the ventricular effective refractory period because the refractory period was similar whether the S1 stimulation site was at or remote from the S2 stimulation site. Furthermore, we have confirmed that high-intensity (10-mA) drive-train stimulation results in approximately a 10% decrease in the ventricular effective refractory period at the site of stimulation. We have established that this is a local effect, observable only near the site of S1 stimulation. Specifically, shortening of ventricular refractoriness is noted 7 mm away from the S1 stimulation site and is no longer noted 14 mm away from the S1 stimulation site. Because the ventricular effective refractory period is shortened locally by high-intensity drive-train stimulation, there is an increase in dispersion of ventricular refractoriness associated with high current stimulation versus stimulation at twice the diastolic threshold. Finally, the shortening of the ventricular effective refractory period resulting from high-intensity drive-train stimulation is observable in patients with cardiac disease, specifically those with chronically implanted transvenous ICDs.

Effect of Low-Intensity Drive-train Stimulation on Ventricular Refractoriness
The effect of drive-train stimuli at 1.5 to 2 times the threshold on the measured ventricular refractory periods has been studied. Several canine studies2 3 demonstrated a shortening of the epicardial effective refractory period when the drive-train stimulation is performed at rather than remote from the site of refractory period determination. Of note, Avitall et al2 noted a difference of {approx}20 ms that dissipated when the S1 and S2 sites were separated by between 10 and 15 mm. In contrast, Toyoshima and Burgess5 showed that the refractory period lengthens when the S1 stimulation site and test site are the same versus remote (40 to 60 mm) from each other; the magnitude of this effect was 4.4 to 13.4 ms. In humans, with stimulation at 1.5 to 2 times the diastolic threshold, the endocardial effective refractory period was shown to shorten when the S1 stimulation site and test site are the same versus remote from each other.4 In that study, when the S1 stimulation site was switched from the right ventricular apex to the right ventricular outflow tract, the apex refractory period changed by 60 to 100 ms. A similar change in refractory period was noted at the outflow tract when the S1 stimulation site was moved from the outflow tract to the apex. In the present study, there was no effect of changing the pacing site from the apex to outflow tract (or vice versa) on the refractory period measured at the apex. Several possible explanations exist for the disparity of these findings. Aside from the potential differences between human and canine physiologies, the studies in dogs were done with epicardial stimulation, while the studies in humans were done with endocardial stimulation. Given that the efferent sympathetic nerves are located in the superficial subepicardium,12 it is possible that low-intensity stimulation of the epicardium may produce local catecholamine release, thereby affecting the local refractory period. In contrast, low-intensity stimulation of the endocardium may not produce these effects. Although Guss et al4 reported profound changes in the refractory period when the S1 and S2 sites were remote from each other, those differences may reflect the conduction times from one site to the other that were not taken into account in reporting on the refractory periods.

Spatial Effect of High-Intensity Drive-train Stimulation on Ventricular Refractoriness
Previous studies in dogs2 and humans6 demonstrated a 10% to 15% shortening in ventricular refractoriness when only the S1 stimulus intensity was increased from a relatively low level to high intensity. Although one study in humans7 demonstrated no significant change in ventricular refractoriness when the S1 stimulus intensity was increased from twice the threshold to 10 mA, several methodological differences between that study and that of Langberg et al6 and the current study may explain the differences. Avitall et al2 noted that S1 stimulation at 10 times the late diastolic threshold shortened the ventricular effective refractory period by 15.3% at the site of stimulation and by only 8.1% at 15 mm away from the S1 stimulation site. In the present study in humans, high-intensity S1 stimulation shortened the refractory period at the site of stimulation and 7 mm away but had no effect 14 mm away from the S1 stimulation site. While the quantitative effects of high-intensity S1 stimulation among these studies may differ, the qualitative findings are similar. Specifically, high-intensity S1 stimulation has the greatest effect on ventricular refractoriness at the site of stimulation and progressively decreases as one moves away from the S1 stimulation site.

The mechanism for the effect of high-intensity S1 stimulation on the shortening of the ventricular refractory period was not addressed in the present study. In the study of Avitall et al,2 although no data are presented, local adrenergic stimulation was not felt to be responsible because ablation of the stellate ganglion and adrenalectomy in dogs receiving reserpine did not influence this phenomenon. However, a number of studies8 9 13 supported the concept that electric stimulation of myocardium results in release of catecholamines. Also, stellate ganglion stimulation in dogs was shown14 to shorten the ventricular effective refractory period, although the magnitude of the effect was considerably less than that observed with high-intensity S1 stimulation. In addition, Langberg et al6 showed that autonomic blockade blunts but does not completely eliminate the shortening of ventricular refractoriness noted with high-current S1 stimulation. Because ß-blockade with propranolol is due to competitive inhibition of the ß-receptors, it is possible that high-current S1 stimulation could result in very high local levels of catecholamines, which could overcome the competitive inhibition of propranolol and nevertheless yield a mild shortening of the ventricular effective refractory period. The current study is consistent with the hypothesis that local release of catecholamines, which would affect tissue near the S1 stimulation site and not more distant tissues, is the mechanism for shortening of the refractory period. However, other local effects such as tissue heating and electrotonic effects resulting from high-current stimulation may also lead to these regional effects.

High-intensity S1 stimulation resulted in an increase in the dispersion of ventricular refractoriness. As Fig 3Up indicates, dispersion did not increase in all subjects. Two main observations account for this effect. Because there is some baseline dispersion in refractoriness, some subjects had longer refractory periods at the distal site compared with the other sites. In these subjects, when high-intensity stimulation shortens the refractory period at the distal site, it may decrease the dispersion relative to the other sites that had (and continue to have) shorter refractory periods. Conversely, subjects whose baseline refractory period at the distal site was shorter than at the other sites may develop a marked increase in dispersion when high-intensity S1 stimulation further shortens the refractory period at that site. The distribution of refractory periods with low-intensity stimulation at the distal site versus the proximal sites was random because there were no significant differences in the mean refractory periods among all sites. Thus, on average, high-intensity S1 stimulation increases the dispersion of refractoriness. The second effect is related to the magnitude of the refractory period shortening with high-intensity stimulation. Those subjects who had larger changes in refractory period with high-intensity stimulation tended to have a greater increase in the dispersion of refractoriness.

Limitations
Many factors affect the refractory period determination. In groups 1 and 2, subjects without structural heart disease were studied to evaluate the physiological effects of low- and high-intensity S1 stimulation on the refractory period and dispersion of refractoriness. The methodology used in these groups (constant pacing, incremental method, 2-ms steps for S2) was specifically chosen to provide the most accurate determinations.11 In group 3, however, the subjects were older and had a range of severity of heart disease, and some were treated with amiodarone. Given the nature of their cardiac diseases, there may also have been different degrees of right ventricular involvement. Furthermore, the methodology used for refractory period determination in this group had to be modified to match the programmable capabilities of the ICD (longer drive-train cycle length, 10-ms steps for S2). These methodological alterations may lead to quantitative differences in the results. Nevertheless, qualitatively similar physiology was demonstrated in this group; all 10 subjects had a shortening of the refractory period with high-intensity S1 stimulation. Although many of the patient characteristics were heterogeneous, this group is fairly typical of patients with serious ventricular arrhythmias requiring an ICD, and these differences did not appear to be related to the degree of shortening of the refractory period with high-intensity S1 stimulation. Thus, we could demonstrate the local shortening of the refractory period in a clinically defined population in whom the effects of increased dispersion of refractoriness could potentially have deleterious consequences.

Potential Clinical Implications of Refractory Period Effects of High-Intensity Stimulation
Dispersion of ventricular refractoriness is considered to be an arrhythmogenic entity.15 16 17 As the present study demonstrates, high-current S1 stimulation may result in an increase in the dispersion of refractoriness and may therefore be arrhythmogenic in a variety of settings. Furthermore, we demonstrated that the effect of high-current S1 stimulation is demonstrable in patients with heart disease, specifically those with serious ventricular tachyarrhythmias that required an ICD. This is an important observation because Langberg et al6 studied primarily patients with normal ejection fractions. The extrapolation of these findings to patients with significant heart disease may explain a variety of clinical phenomena.

Clinically, high-current S1 stimulation is most likely to be used for arrhythmia induction in the electrophysiology laboratory or for antitachycardia pacing during sustained ventricular tachycardia. Prior studies showed that high-current stimulation during electrophysiology studies may result in a lower specificity owing to induction of nonclinical arrhythmias.18 Brugada et al,19 evaluating the mechanisms of acceleration of ventricular tachycardia during programmed stimulation, noted that one possible mechanism was conversion of ventricular tachycardia caused by reentry around an anatomic substrate to a circuit with a functional obstacle. In that study, stimulation during tachycardia was performed at four times the diastolic threshold. It is possible that stimulation at this output resulted in an increased dispersion of refractoriness, resulting in development of ventricular tachycardia with a functionally determined tachycardia circuit. Clinical studies of antitachycardia pacing during ventricular tachycardia in patients with ICDs demonstrated an incidence of acceleration of ventricular tachycardia ranging from 1.1% to 4.3% of all episodes20 21 22 in {approx}20% of patients.21 22 The stimulation intensity used during these studies is not known. However, in a study comparing antitachycardia pacing modalities in the electrophysiology laboratory,23 there were 7 cases of acceleration out of 110 induced ventricular tachycardias (6.4%) in 27 patients. A stimulus amplitude of 7 mA and a duration of 2 ms were used in this study. Further studies are required to establish whether low-intensity stimulation during ventricular tachycardia can reduce the risk of ventricular tachycardia acceleration while maintaining adequate capture to result in termination of the tachycardia.


*    Footnotes
 
Reprint requests to Jeffrey Goldberger, MD, Northwestern Memorial Hospital, 250 E Superior St, Ste 520, Chicago, IL 60611.

Received December 19, 1994; revision received February 14, 1995; accepted February 20, 1995.


*    References
up arrowTop
up arrowAbstract
up arrowIntroduction
up arrowMethods
up arrowResults
up arrowDiscussion
*References
 
1. Josephson ME. Electrophysiologic investigation: general concepts. In: Josephson ME, ed. Clinical Cardiac Electrophysiology. Malvern, Pa: Lea & Febiger; 1993:22-70.

2. Avitall B, Levine H, Maimi S, Donahue R, Pauker S, Adam D. Local effects of electrical and mechanical stimulation on the recovery properties of the canine ventricle. Am J Cardiol. 1982;50:263-270. [Medline] [Order article via Infotrieve]

3. Han J, deJalon G, Moe G. Fibrillation threshold of premature ventricular responses. Circ Res. 1966;18:18-25. [Abstract/Free Full Text]

4. Guss S, Kastor J, Josephson M, Scharf D. Human ventricular refractoriness: effects of cycle length, pacing site, and atropine. Circulation. 1976;53:450-455. [Abstract/Free Full Text]

5. Toyoshima H, Burgess M. Electrotonic interaction during canine ventricular repolarization. Circ Res. 1978;43:348-356. [Abstract/Free Full Text]

6. Langberg J, Calkins H, Sousa J, El-Atassi R, Morady F. Effects of drive train stimulus intensity on ventricular refractoriness in humans. Circulation. 1991;84:181-187. [Abstract/Free Full Text]

7. Tchou P, Al-Bitar I, Mahmud R, Denker S, Jazayeri M, Akhtar M. Contribution of current strengths of S1 and S2 to the measured ventricular effective refractory period in the human heart. J Electrophysiol. 1988;2:141-146.

8. Brady A, Abbott B, Mommaerts W. Inotropic effects of trains of impulses applied during the contraction of cardiac muscle. J Gen Physiol. 1960;44:415-432. [Abstract/Free Full Text]

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J. J. Sims, A. W. Miller, and M. R. Ujhelyi
Disparate effects of biphasic and monophasic shocks on postshock refractory period dispersion
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