(Circulation. 1997;96:3732-3736.)
© 1997 American Heart Association, Inc.
Articles |
From the Section of Electrophysiology and Pacing, Department of Cardiology, The Cleveland Clinic Foundation, Cleveland, Ohio.
Correspondence to Mark J. Niebauer, MD, PhD, Desk F-15, Cleveland Clinic Foundation, 9500 Euclid Ave, Cleveland, OH 44195. E-mail niebaum{at}cesmtp.ccf.org
| Abstract |
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Methods and Results The defibrillation threshold (DFT) was
determined in 13 swine with both IROX-coated and uncoated ICD leads
paired with an uncoated "can" electrode. The leads were exchanged
through a Teflon sheath to reproduce the intracardiac position. The
delivered energy DFT of the IROX-coated lead was 15.9±5.4 J and was
significantly lower than the delivered energy DFT of the uncoated lead
(19.1±5.1 J; P<.006). The initial lead impedance was
equivalent in both leads (IROX, 41.7±5.8
; uncoated, 41.3±4.7
;
P=NS) at DFT. However, the impedance rose by 7.3±2.0
during the first phase and by 3.7±2
during the second phase with
the uncoated lead, whereas the corresponding impedance change was
1.0±0.3
during phase 1 and 1.6±0.5
during phase 2
(P<.01 each phase) when the IROX-coated lead was used.
Conclusions This study shows that an IROX coating of this lead system significantly lowers the DFT energy in the swine model. The blunting of the impedance rise by the IROX coating that is seen is consistent with a reduction in electrode polarization.
Key Words: defibrillation electrical stimulation arrhythmia fibrillation ventricles
| Introduction |
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Much of the research on electrode materials has been performed with pacemaker electrodes at pacing stimulus amplitudes. This is not surprising, given the relatively short period of time that nonthoracotomy defibrillator leads have been available compared with pacemaker leads. Studies conducted on pacing electrodes that use a coating of the low-polarization material IROX have demonstrated a reduction of electrode polarization and a reduction of pacing thresholds.9 10 A transvenous lead with an IROX-coated defibrillation electrode has been developed and is now in clinical trials. This study examines the in vivo electrode characteristics and defibrillation efficacy of the IROX-coated, transvenous defibrillation electrode placed in the right ventricle, paired to an uncoated, pectoral can electrode. The lead characteristics as well as defibrillation energy requirements (DFT) of this lead were compared with an otherwise identical system using an uncoated transvenous lead in an anesthetized swine model.
| Methods |
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Endocardial Lead Positioning and Exchange
The order in which the uncoated and IROX-coated electrodes were
tested was randomized for each experiment. The active fixation
transvenous defibrillator lead with IROX coating (model 497-20, Sulzer
Intermedics Inc) or without IROX coating (model 497-06, Sulzer
Intermedics Inc) was inserted through the right internal jugular vein,
and the active fixation tip was positioned in the right
ventricular apex under fluoroscopic guidance. The shock
electrode incorporated into this 11F lead consists of a titanium coil
(with or without IROX coating) 5 cm in length, with a surface area of
4.4 cm2 located 1 cm from the distal tip. The
defibrillation path consisted of the transvenous shock electrode coil
(±IROX coating) paired to a titanium can electrode (surface area, 92
cm2) implanted subcutaneously in the left prepectoral
fascia. Defibrillation testing of the lead was then carried out (see
description below).
Once testing with the initial endocardial lead was completed, that lead
was exchanged as follows. First, a Teflon sheath (Cook Pacemaker Corp)
was advanced over the lead, under fluoroscopic guidance, until the
sheath reached the right ventricular endocardium (Fig 1
). Then, the lead was withdrawn through
the sheath, which was left in place to maintain the endocardial
position. The second lead was immediately advanced through the sheath
and fixed to the endocardium. The sheath was then removed, leaving the
new lead in the same endocardial location as the original lead. An
equivalent amount of lead "slack" was adjusted fluoroscopically.
Defibrillation testing of the new lead was then performed. The pectoral
can electrode was not moved during the study.
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Defibrillation Testing
Testing of each lead/can combination was performed with the
endocardial coil configured as the cathode for the first phase of a
biphasic waveform and the pectoral can as the anode. The defibrillation
waveform used for both leads was generated by an experimental
defibrillator (Angeion Corp) programmed to deliver a 135-µF biphasic
waveform with fixed 65% tilt (each phase). This device sampled
delivered voltage and current at 0.1-ms intervals throughout each
phase. Delivered energy and lead impedance were calculated from these
data. Stored energy was calculated from the peak voltage and
capacitance values.
Defibrillation efficacy was established with a down-up, down-up protocol that has been described in previous studies and shown to approximate the probabilistic method of determining the ED50.11 This protocol has been detailed elsewhere and consists of a series of fibrillation-defibrillation episodes (steps) in which the test shock intensity is decremented (down) or incremented (up) by 1 J. This protocol was followed for both uncoated and IROX-coated leads. At each step, ventricular fibrillation is induced with a 4-second alternating current burst of 10 to 20 V delivered through the high-energy electrodes. Once ventricular fibrillation was confirmed by ECG and loss of arterial pressure pulses and a total duration of 10 seconds had elapsed (including ventricular fibrillation induction time), a test shock was delivered. Success or failure of the test shock was judged by the ECG and by the return of arterial pressure pulsation. If the test shock failed, a second monophasic shock of 40- to 50-J intensity was delivered through the electrodes. This second rescue shock succeeded in all animals. A 3- to 5-minute stabilization period was observed between each step. Subsequent test shocks were either decremented by 1-J intensity after a successful test shock or incremented by 1 J after a failed test shock. All shock parameters (energy, voltage, current, and impedance) were averaged, beginning with the last successful shock during the initial down sequence and up to and including the final shock observed during the second up series. The average values for each parameter were defined as the DFT values.
In Vivo Lead Performance
To compare the impedance characteristics of the two transvenous
leads, the energy, current, and impedance values obtained for shocks of
similar intensity (peak voltage of 575±50 V) were compared, regardless
of defibrillation success or failure. A least-squares regression of
impedance versus time (
/ms) was obtained in each pig for both leads
to obtain the rate of impedance rise (slope). This slope was used to
quantify the polarization effect present in both electrodes.
Statistical Analysis
The distributions of all DFT values were found to have similar
variances. Comparison of these values and those for the in vivo
comparison of lead impedance for both noncoated and IROX-coated leads
was performed with the paired t test. Analysis of
the lead voltage, current, and impedance values and slopes of the
impedance regression lines during the in vivo lead performance
testing were analyzed by the nonparametric
Wilcoxon signed-rank test because of the unequal variance seen.
A value of P<.05 was required to denote statistical
significance of endocardial lead characteristics between groups.
| Results |
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Interestingly, the duration of the second phase was longer when the uncoated lead was used (8.4±1.1 versus 6.4±1.4 ms, P<.01) compared with the IROX-coated lead. The biphasic waveform used in this study was of variable duration because of the requirement for a fixed 65% tilt. The first phase duration, although slightly longer when the uncoated electrode was used compared with the IROX-coated electrode, was not significantly different.
In Vivo Lead Performance
At DFT intensity, the impedance changes (ie, initial and final)
during each phase were obtained, and the results of both leads were
compared (Table 1
). The initial impedance of the uncoated titanium coil
and titanium can combination (41.3±4.7
) was equivalent to the
initial impedance of the IROX-coated lead system (41.7±5.8
).
However, the impedance rises during the two phases were significantly
greater during shocks delivered through the uncoated lead (7.3±2.0 and
3.7±2.0
, phases 1 and 2, respectively) than during shocks
delivered through the IROX-coated lead (1.0±0.3 and 1.6±0.5
,
respectively; P<.01 both phases).
Because of concern that the impedance rise may be voltage dependent,
the rates of impedance rise of both leads (ie, slopes of impedance
versus pulse duration) during phase 1 were compared at equivalent peak
voltage shocks (
575 V; range, 523 to 616 V). Fig 2
shows the lead impedance measurements
throughout both phases obtained from one experimental preparation for
shocks delivered through the noncoated and the IROX-coated leads. As
can be seen, the impedance rose more slowly when the IROX-coated
electrode was used compared with the uncoated lead. The mean slope of
the regression line for the impedance-versus-time curve obtained for
the uncoated lead during phase 1 (1.0±0.3
/ms) was significantly
greater than that obtained for shocks delivered through the IROX-coated
lead (0.4±0.3
/ms, P<.005; Table 2
).
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| Discussion |
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Polarization is an electrochemical process that occurs at the stimulating electrode/electrolyte interface during a stimulation impulse. It is manifested by an impedance rise during the delivery of the energy pulse and as a transient afterpotential (of opposite polarity) that appears immediately after the delivered pulse.13 The polarization effect of defibrillator electrodes has been recognized in a previous study by Alt et al14 in which the effectiveness of a carbon-braid electrode (a low-polarization material) was compared with two clinically available leads: the CPI 0062 Endotak and the Medtronic 6966 Transvene. The carbon-braid electrode exhibited significantly lower DFTs compared with the clinical leads.
Although the superiority of the carbon-braid electrode was demonstrated, the mechanism underlying the differences seen was not elucidated. There are several differences between this study and that of the carbon-braid electrode study. Positioning of the three electrodes in the study by Alt et al was visually approximated with fluoroscopy, whereas the electrodes used in our study were carefully exchanged to maintain a constant endocardial position. Our concern over the electrode exchange is due to the results of prior studies that have shown that small differences in endocardial lead positioning produce significant differences in defibrillation efficacy.6 7 We believe that the sheath exchange method closely reproduces the endocardial position between electrodes and reduces this source of variance. In addition, the subcutaneous can electrode position was constant throughout our study, and this type of electrode is more clinically relevant to present ICD systems than the subcutaneous array electrode used in the study by Alt et al. Another difference between these studies is that DFTs in the Alt study were obtained by a modified step-down technique, in which the lowest-intensity successful shock in a decremental series of shocks is defined as the DFT. The DFT method in the present study is an average based on a minimum of five shocks, and the reproducibility of this technique, as well as its correlation to the probabilistic model of defibrillation efficacy, has been documented previously.11
The leads used in this study are identical except for the IROX coating, in that the coil length and conductor materials were exactly alike. The three electrodes compared in the carbon electrode study, however, were of various lengths and constructions.15 Such differences may have affected current distribution and consequently, defibrillation efficacy. Therefore, the differences in DFT seen among the three leads used in the Alt study cannot be attributed entirely to the carbon-braid material and its nonpolarizing properties.
The results of the present study indicate a small difference
between the defibrillating waveforms delivered through the IROX-coated
and uncoated leads. Specifically, the mean duration of the second
phase, delivered through the uncoated lead, was
2 ms longer than the
first phase, whereas shocks delivered through the IROX-coated lead
yielded a mean second phase only 0.5 ms longer than the first phase
(not statistically different). This difference is due to the nature of
the defibrillating waveform used in this study and the impedance
changes related to the respective leads, noted above. The biphasic
waveform used in this study is a clinically available, biphasic
truncated exponential waveform with a fixed tilt (65%) for both
phases. Because only the tilt was used to determine the waveform,
duration would vary to fulfill the tilt criterion. The impedance
differences shown between the two leads used in this study are the most
likely explanation for the differences in phase duration.
Previous authors had reported that certain biphasic waveforms with longer second phases produced higher DFT energies than waveforms with second phases less than or equal to the first phase.16 17 However, those earlier studies were performed in dogs with epicardial patches, and the DFT energies reported were <10% of the DFT energies seen in the present study. A more recent study using a swine model and endocardial electrodes, similar to the present study, had somewhat different results.18
In this recent study, the DFT of a biphasic waveform similar to that produced in the present experiment (first phase, 6 ms) was tested with various second-phase durations.18 There was no significant effect on DFT, measured as energy or peak voltage, for a longer second phase of up to 10-ms duration, when the polarity of the first phase was negative (cathodal), as in our study. This finding supports our conclusion that the IROX coating is responsible for the reduction in DFT seen in our results.
Limitations of the Study
The present study was performed over a relatively narrow range
of shock intensity in each animal, so that the in vivo lead
performance was not assessed over the entire range of
clinically relevant peak voltages. For example, it is possible that the
magnitude of the polarization effect may differ at lower shock
intensities, such as those used for cardioversion of
ventricular tachy-cardia. In addition, a fixed
65% tilt biphasic waveform was used in this study. Other shock
waveforms may exhibit different effects on DFT when delivered through
an electrode coated with IROX. The experimental design also did not
allow for measurement of a polarization-induced afterpotential, which
may have effects on defibrillation, postshock dysrhythmias, and
possibly postshock sensing.
In summary, this study demonstrates that a transvenous defibrillation electrode coated with IROX significantly reduces defibrillation energy requirements compared with an otherwise identical, uncoated electrode. The major difference seen between the electrodes was the reduction in the time-dependent rise in impedance seen during the shock pulse, theoretically due to electrode polarization. As a result, current was reduced as the impedance rose, necessitating a higher peak voltage and consequently, a higher delivered energy to achieve defibrillation. It is noteworthy that the magnitude of the reduction in energy requirement afforded by the IROX coating approaches the difference seen between biphasic and monophasic waveforms. The inclusion of an IROX-coated electrode with present ICD technology, which incorporates a biphasic waveform and an active pectoral can electrode, may further reduce clinical DFTs. This combination could allow for additional ICD size and energy output reduction.
| Selected Abbreviations and Acronyms |
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| Acknowledgments |
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Received April 14, 1997; revision received June 20, 1997; accepted July 15, 1997.
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