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Transcript
Europace (2001) 3, 275–277
doi:10.1053/eupc.2001.0195, available online at http://www.idealibrary.com on
Editorial
Is there an optimal capacitance for defibrillation?
All implantable cardioverter-defibrillators (ICDs)
contain a capacitor, which is an electronic component
that can store electric charge. While capacitors come
in many sizes and shapes and are constructed of
different materials, essentially they all consist of two
conductors separated by an insulator. When a capacitor is connected to a battery, electrons flow to the
conductor in the capacitor attached to the cathode of
the battery. The anode of the battery attracts electrons away from the other conductor in the capacitor.
Thus, the first conductor acquires a net negative
charge while the second conductor acquires a net
positive charge of equal magnitude. When the battery
is disconnected, these electrical charges of opposite
polarity, separated by the insulator, are stored until
the conductor is connected by a conducting path.
After the connection is made, electrons pass from the
negatively charged conductor through the conductive
pathway to the positively charged conductor.
The energy required to defibrillate is much greater
than can be delivered directly from ICD batteries
during the few milliseconds of a shock. By connecting
an ICD battery to a capacitor for several seconds, the
capacitor can be charged to a high energy level and
then rapidly deliver the charge as a shock. The
rapidity with which the capacitor delivers its charge
to a patient depends on the capacitance (C) and the
resistance (R). Capacitance is a measure of the
amount of charge that the capacitor can store for a
given voltage, while resistance is a measure of the
impedance to current flow in the discharge circuit,
which consists primarily of the ICD leads and the
patient’s body. The time for the capacitor to discharge increases with increases in either R or C. This
time is quantified by the time constant (), the
amount of time required for the capacitor to discharge sufficiently to decrease the voltage across it
by 63%, which is equal to the product of R and C.
When C is expressed in farads (the capacitance of a
capacitor which stores one coulomb of charge
[6·241018 electrons] with a 1 volt difference across
the capacitor) and R is given in ohms (1 ohm []
causes a current of 1 amp [1 coulomb per s] when 1
volt is applied across the resistance), will be in
seconds. As the capacitor discharges through a fixed
1099–5129/01/040275+03 $35.00/0
resistance, the voltage across the capacitor decreases
exponentially with time.
In addition to , there are several other variables
associated with the ICD capacitor or the waveform it
generates that have clinical significance, since they
influence the likelihood that the shock will succeed in
halting fibrillation. Some of these variables are the
stored voltage across the capacitor, the stored energy
in the capacitor, and the delivered energy to the
patient when the capacitor is discharged during the
shock. The delivered energy is less than the stored
energy, because the capacitor is not allowed to discharge fully during the shock. Rather, the shock
waveform is truncated by switching off the capacitor
before it is fully discharged. The tilt of the shock
waveform is defined as the difference between the
shock voltage when the shock is turned on (the
leading-edge voltage) and when the shock is turned
off (the trailing-edge voltage) divided by the leadingedge voltage. For example, the tilt of a waveform
whose duration is equal to is 63%. In addition to
tilt, other important variables affecting defibrillation
efficacy are the number of phases of the waveform
and the duration of each phase of the waveform. All
of these variables are not independent. The stored
energy can be calculated from the capacitance and the
stored voltage (V): E=1/2CV2. Waveform tilt can be
calculated from and the waveform duration (d):
tilt=1e d/t, where e=2·72.
What is the optimal capacitance for the ICD? The
answer to this question depends upon which quantity
is chosen to be optimized. There are at least five
quantities that can be optimized by finding the
capacitance for which the quantities are a minimum:
(1) the voltage required for defibrillation, (2) the
energy required for defibrillation, (3) detrimental
effects caused by the shock[1], (4) the size of the ICD,
and (5) the amount of time necessary to charge the
capacitor[2]. In presently available ICDs this last
variable, which partially determines the duration of
fibrillation before the shock is given, is directly related to the stored energy independent of the capacitance, since constant power charge circuits are used.
Many experimental studies in animals and humans
have been performed to answer these questions. In
2001 The European Society of Cardiology
276
Editorial
most of these studies the efficacies of the different
waveforms have been ranked based on their ability to
minimize the delivered energy. From these experimental results, investigators have derived relatively
simple equations to predict the efficacy of different
waveforms and of different capacitances[3–7]. These
models predict that a capacitance of 90 F or even
less should be superior to the 140–150 F capacitance
that is standard in ICDs because they should require
less energy when a short duration waveform is used.
While a smaller capacitance (60 F) does not defibrillate with lower energy than a 120 F capacitance
when the lead resistance is low (c40 ), it requires
less energy to defibrillate when the lead resistance is
high (>60 )[8]. However, defibrillation with smaller
capacitance requires significantly more voltage,
even though the energy is the same or moderately
decreased, since according to the equation given
above a smaller C requires a larger V for the capacitor to contain the same amount of energy. Since some
evidence suggests that detrimental effects of shock,
such as electroporation, are more closely related to
peak shock voltage than shock energy[9,10], these
shocks from ICDs with a smaller capacitance may be
more likely to cause damage, even though they are
the same or slightly lower energy than shocks from
ICDs with a standard size capacitance.
Other investigators have taken the opposite approach and have experimentally evaluated larger
capacitors of 336–500 F[11,12], which models indicate
should decrease the voltage required for defibrillation. The most recent of these studies is that by
Brugada et al. in this issue of Europace[13]. These
studies found that, while the larger capacitors markedly reduced the voltage required for defibrillation,
they either did not significantly change or only
slightly increased the energy required for defibrillation. In the study by Brugada et al.[13], a biphasic
waveform delivered from a 336 F capacitor with a
total tilt of 60%, in which the first phase was 60% of
the total waveform duration, required significantly
lower energy for defibrillation than did an 80% tilt
biphasic waveform delivered from a 140 F capacitor
with the first phase 60% of the total waveform
duration.
A 336 F capacitor was used in the study by
Brugada et al. because it consisted of only a single
physical capacitor. The standard 140 F capacitor, as
well as the smaller capacitors discussed above, physically consist of two or more capacitors connected in
series. Standard capacitors used in ICDs cannot be
charged to voltages greater than approximately 390
volts, which is not enough energy to defibrillate for a
capacitance of 140 F or less. Since the total voltage
output of capacitors in series is equal to the sum of
Europace, Vol. 3, October 2001
the voltages of each of the capacitors, it is necessary
to connect two or more capacitors in series to provide
sufficient voltage and energy for defibrillation. A
voltage of 390 V across a 336 F capacitor stores 26 J
which, in the study by Brugada et al., was sufficient to
provide a 10 J safety margin for all patients, since no
patient had a defibrillation threshold higher than 15 J
with the 60% tilt waveform delivered from the 336 F
capacitor.
According to Brugada et al.[13], use of a single
336 F capacitor instead of the two capacitors in
series to create the 140 F net capacitance in standard
ICDs would save approximately 7 cc of space, which
would allow the defibrillator to be smaller. However,
newer types of capacitors have recently become available that occupy less space even when several are
connected in series. In addition, before unequivocally
accepting the results of this study and its implications
for the optimal capacitance in ICDs, several limitations of the study must be considered, some of which
are acknowledged by the authors.
One, the study was stopped early. Based on a
power calculation performed before the beginning of
the studies, each study was to have enrolled 41
patients. Yet, the first study was terminated after
enroling 33 patients and the second study after enroling 21 patients, because significant differences between the two waveforms were already present.
Statistically evaluating the tested variables several
times during a study will increase the probability that
a significant difference will be found by chance. While
there are statistical techniques to compensate for
analysing the data multiple times during the course of
a study[14], there is no indication in the manuscript
that the authors employed such techniques.
Two, the patients in the two studies appear to have
been different. As can be seen in Fig. 2 of the paper by
Brugada et al.[13], the mean reference defibrillation
threshold for the shock from the 140 F capacitor
was different in the two studies. In fact, the defibrillation threshold for the 140 F shock in the second
group of patients was lower than the defibrillation
threshold for the 336 F shocks in the first group
of patients, which was significantly lower than
the defibrillation threshold for this same 140 F
capacitor shock in the first group of patients.
Three, the means and standard deviations of the
resistance in the two groups, 435 and 465 ,
suggests that there were few patients with a high
resistance (>70 ). It is in patients with such high
resistances that the high voltage shocks from a small
capacitor would be most advantageous vs the lower
voltage shocks from a large capacitor.
Finally, the left ventricular ejection fractions in the
two groups, 4415% and 4715%, are considerably
Editorial
higher than that in many earlier studies of patients
with ICDs[15]. The facts that the ejection fractions
were high in the patients and few of the patients had
high resistances may be responsible for the absence of
any patient with a defibrillation threshold higher than
15 J in the study. Although no patients in this study
had a defibrillation threshold higher than 15 J, it is
likely that there will be patients who have a defibrillation threshold higher than 15 J for shocks delivered
from the 336 F capacitor. If so, and if a safety factor
of at least 10 J is required, then an ICD with a 336 F
capacitor should not be used in these patients.
The quest for a tiny ICD is a laudable goal.
However, the need for ICDs to be effective is paramount. Whether or not bigger or smaller is better
depends on the entity being quantitated. Only if a
bigger capacitor is equally or more effective than the
currently used capacitor technology should it be
incorporated into ICDs. On the other hand, if capacitors are less consistently effective, a smaller ICD size
is not a service to patients.
Partially supported by NHLBI grants HL-42760 and HL-63795.
Dr Ideker’s laboratory receives research funding from Guidant
Corporation and Medtronic/Physio-Control. Drs Ideker and
Walcott are consultants and Dr Epstein is an investigator for
Guidant Corporation.
R. E. IDEKER,
A. E. EPSTEIN,
G. P. WALCOTT
Departments of Medicine, Physiology, and
Biomedical Engineering
of the University of Alabama at Birmingham,
Birmingham, Alabama, U.S.A.
277
[2] Windecker S, Ideker RE, Plumb VJ, et al. The influence of
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pulse. Pacing and Clin Electrophysiol 1993; 16: 769–77.
[4] Kroll MW. A minimal model of the single capacitor biphasic
defibrillation waveform. Pacing and Clin Electrophysiol 1994;
17: 1782–92.
[5] Walcott GP, Walker RG, Cates AW, et al. Choosing the
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[6] Irnich W. Optimal truncation of defibrillation pulses. Pacing
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[7] Cleland BG. A conceptual basis for defibrillation waveforms.
Pacing and Clin Electrophysiol 1996; 19: 1186–95.
[8] Swerdlow CD, Kass RM, Chen P-S, et al. Effect of capacitor
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[9] Al-Khadra A, Nikolski V, Efimov IR. The role of electroporation in defibrillation. Circulation Res 2000; 87: 797–804.
[10] Tung L. Electroporation of cardiac cells. Methods Mol Biol
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[11] Hahn SJ, Heil JE, Lang DJ. Large capacitor defibrillation
waveform reduces peak voltages without increasing energies.
Pacing and Clin Electrophysiol 1995; 18: 203–7.
[12] Block M, Hammel D, Böcker D, et al. Biphasic defibrillation
using a single capacitor with large capacitance: Reduction of
peak voltages and ICD device size. Pacing and Clin Electrophysiol 1996; 19: 207–14.
[13] Brugada J, Herse B, Sandstedt B, et al. Clinical evaluation of
defibrillation efficacy with a new single-capacitor implantable
cardioverter defibrillator. Europace 2001; 3: 278–84.
[14] O’Brien PC, Fleming TR. A multiple testing procedure for
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[15] Domanski MJ, Saksena S, Epstein AE, et al. Relative effectiveness of the implantable cardioverter-defibrillator and antiarrhythmic drugs in patients with varying degrees of left
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References
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pathological changes associated with non-thoracotomy implantable defibrillator leads. Circulation 1998; 98: 1517–24.
Europace, Vol. 3, October 2001