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1 Department of Medicine, University of Liverpool, Liverpool L69 3GA, United Kingdom; and 2 Department of Physiology and Pharmacology, Tel-Aviv University, Ramat-Aviv 69978, Israel
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ABSTRACT |
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Cardiac hypertrophy was
induced in rats by daily injection of isoproterenol (5 mg/kg ip) for 7 days. Membrane voltage and currents were recorded using the whole cell
patch-clamp technique in left ventricular myocytes from control and
hypertrophied hearts. Ryanodine-sensitive delayed afterdepolarizations
(DADs) and transient inward current (Iti)
appeared in hypertrophied cells more often and were of larger amplitude
than in control cells. DADs and Iti are carried
principally by Na/Ca exchange with smaller contributions from a
nonselective cation channel and from a Cl
channel. The
latter is expressed only in hypertrophied myocytes. In hypertrophy, the
density of caffeine-induced Na/Ca exchange current
(INa/Ca) was increased by 26%, sarcoplasmic
reticulum (SR) Ca2+ content as assessed from the integral
of INa/Ca was increased by 30%, the density of
Na-pump current (Ipump) was reduced by 40%, and
the intracellular Na+ content, measured by
Na+-selective microelectrodes was increased by 55%. The
results indicate that DADs and Iti are generated
by spontaneous Ca2+ release from an overloaded SR caused by
a downregulated Na pump and an upregulated Na/Ca exchange. These
findings may explain the propensity for arrhythmias seen in this model
of hypertrophy.
transient inward current; sodium/calcium exchange current; chloride current; nonselective cation current; sodium-pump current; arrhythmia
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INTRODUCTION |
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VENTRICULAR ARRHYTHMIAS are common in cardiac hypertrophy and may contribute to sudden death in patients with this condition (28). Although cardiac hypertrophy is strongly associated with arrhythmias and mortality, cellular mechanisms for triggered arrhythmias have not been extensively investigated in hypertrophied hearts. Delayed afterdepolarizations (DADs) that are responsible for some forms of triggered arrhythmias have been demonstrated in hypertrophied myocardium from rats with renal hypertension (2), in diseased myocardium from rats with streptozotocin-induced diabetes (36), and in postmyocardial infarction remodeled hearts (41). Furthermore, augmented after-contractions have been observed in papillary muscles isolated from rats with cardiac hypertrophy (20). We have observed DADs in left ventricular trabeculae (34) in a model of cardiac hypertrophy induced in the rat by repeated administration of isoproterenol (34, 44). It has been known for a long time that the mechanism underlying DADs is the transient inward current (Iti) (23). Although it has also been well demonstrated that intracellular Ca2+ concentration ([Ca2+]i) overload must be present for the generation of Iti, its ionic mechanism is still a subject of debate and is undocumented in diseased cardiac myocytes. [Ca2+]i elevation can be induced by an increased intracellular Na+ level as a result of Na pump inhibition, which makes the Na/Ca exchange operate in reverse mode (2, 15, 23, 31). The elevated [Ca2+]i causes overloading of the sarcoplasmic reticulum (SR) with Ca2+ and induces spontaneous oscillatory release of Ca2+ from the SR after depolarization or an action potential (4, 23, 32). In nonhypertrophied tissue, Iti has been shown to depend in part on Na/Ca exchange (31). Na/Ca exchange current (INa/Ca) and protein expression are increased in hypertrophied myocytes (17, 19, 45, 51), but DADs have not previously been reported in hypertrophied cardiac myocytes. The aims of the present study were therefore to establish the mechanisms and properties of Iti and to characterize the ionic basis for this current in catecholamine-induced cardiac hypertrophy in the rat.
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MATERIALS AND METHODS |
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Induction of cardiac hypertrophy. Cardiac hypertrophy was induced in male Wistar rats weighing 200-250 g by intraperitoneal injection of 5 mg/kg isoprenaline once daily for 7 days (34, 44). Age-matched control rats received the same volume of 0.9% NaCl solution. The animals were used for experiments 24 h after the last injection. The degree of hypertrophy was estimated by measuring blotted wet heart weight and the body weight and calculating heart weight-to-body weight ratio. These experiments were done on 10 pairs of animals. The investigation conforms with the Guidance on the Operation of the Animals (Scientific Procedures) Act 1986 (Her Majesty's Stationery Office, United Kingdom).
Cell isolation. Single left ventricular myocytes used for these electrophysiological experiments were isolated from six pairs of animals. Cells were obtained from control and hypertrophied hearts according to the method described previously (45). Briefly, the animals received 500 units heparin intraperitoneally 20 min before death by cervical dislocation. The heart was removed and perfused retrogradely with a nominally Ca2+-free Tyrode solution at 35°C for 4 min and then perfused for 12 min with a Tyrode solution containing 1 mg/ml collagenase and 0.1 mg/ml protease. The heart was removed from the column, and the left ventricle and septum were dissected free, roughly chopped, suspended in the enzyme solution (but without protease), and stirred slowly on a heated plate. Fractions were removed at 5- to 10-min intervals and the cells were washed twice after centrifugation in a normal Tyrode solution containing 5 mg/ml bovine serum albumin. The cells were stored at room temperature in Dulbecco's modified Eagle's medium with 2 mg/ml Ultraser G (GIBCO-BRL, Paisley, UK). Cells were left for 1 h before use and were used within 8 h.
Electrophysiological protocols. Myocytes were layered on a glass coverslip that formed the base of a perfusion chamber. This was mounted on the stage of an inverted microscope situated on an isolation table. The flow rate of perfusion fluid was 2-3 ml/min. Temperature of the bath was maintained at 35 ± 1°C by a heating block surrounding the input line, which was controlled by a feedback circuit using a sensing thermocouple positioned in the chamber. The level of solution in the bath was controlled using a feedback circuit, the sensor for which was a piece of photographic film positioned on the meniscus and connected by a stainless steel rod to an Akers transducer (SensoNor; Horten, Norway). For experimentation, only those myocytes were used that showed rod shape, clear cross striations, no blebs on the surface, and no spontaneous contractions.
The whole cell voltage-clamp technique was used to record membrane currents using an Axopatch-200 amplifier (Axon Instruments; Burlingame, CA). Electrical compensation was made for whole cell capacitance and series resistance. Cell capacitance was measured directly from the Axopatch-200 after correction for series resistance. Patch pipettes were pulled from filamented borosilicate capillary glass (Clark Electromedical Instruments; Pangbourne, UK) on a microprocessor-based three-stage puller (Mecanex BB-CH-PC; Basel, Switzerland). The pipettes had resistances of 2-5 M
after filling with the appropriate
internal solution. The resistance of the seals between the pipette tip
and the myocytes was 5-10 G
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To record DADs and Iti, micropipettes were
filled with a solution containing (in mM) 140 KCl, 2 MgCl2,
5 Mg-ATP, 5 Na2-phosphocreatine, 10 HEPES (at pH 7.2, adjusted with KOH). Cells were superfused with an external solution
containing (in mM) 134 NaCl, 5.4 KCl, 2.5 CaCl2, 1 MgCl2, 10 glucose, 10 HEPES (at pH 7.4, adjusted with
NaOH). Action potentials were initiated by depolarizing current pulses
(2-5 ms duration) at a frequency of 0.3 Hz under whole cell
current clamp conditions. Iti was induced by
applying depolarizing voltage pulses from a holding potential of
40
mV at a frequency of 0.3 Hz under whole cell voltage-clamp conditions.
The caffeine-dependent INa/Ca was induced at a
holding potential of
80 mV by short application of 20 mM of caffeine
onto the whole cell voltage-clamped myocyte after a 1-min rest period following a train of stimulation to ensure that the SR was consistently loaded with Ca2+ (54). Rapid solution changes
were evoked through a system of solenoids. In these experiments, the
external solution contained 1 mM CaCl2, to which 5 mM
4-aminopyridine and 0.1 mM BaCl2 were added to block
potassium currents, and 10 µM
4,4'-diisothiocyanostilbene-2,2'-disulfonic acid (DIDS) were added
to block chloride current. All of the other components of the external
and internal solutions were the same as described above. To assess SR
Ca2+ content, INa/Ca was integrated
and converted to total Ca2+ fluxes (53, 54).
Considering that INa/Ca is generated mostly by
Na/Ca exchange but is 1) contaminated by other
[Ca2+]i-activated currents, and 2)
caffeine-released Ca2+ can also be removed from the cell by
mechanisms other than Na/Ca exchange, INa/Ca was
first corrected for these mechanisms by multiplying using a factor of
1.5 (53, 54). Cell volume was calculated from the membrane
surface area obtained from the membrane capacitance assuming a
capacitance-to-volume ratio of 6.76 pF/pl for rats (47, 53,
54).
To study the Na-pump current (Ipump),
micropipettes were filled with a solution containing (in mM) 86 CsCl, 2 MgCl2, 10 Mg-ATP, 5 Na2-phosphocreatine, 20 tetraethylammonium-chloride, 5 EGTA, and 5 HEPES (at pH 7.2, adjusted with CsOH). Cells were superfused with an external solution
containing (in mM) 143 NaCl, 5.4 KCl, 1 MgCl2, 5.5 glucose,
2 BaCl2, 2 CoCl2, and 5 HEPES (at pH 7.4, adjusted with NaOH). Temperature was 35 ± 1°C.
Ipump was activated on returning to 5.4 mM
external K+ after 2 min in K+-free solution at
a holding potential of
40 mV (10).
Ipump was measured either as a constant holding
current or during ramp pulse protocols. A quasi-steady-state
current-voltage relationship was determined by applying slow voltage
ramp (53 mV/s) between +40 and
120 mV from a holding potential of
40 mV (49). The negative ramp was used to prevent
activating the voltage-gated sodium channel.
Intracellular Na+ concentration
([Na+]i) was measured in control and
hypertrophied ventricular myocytes using voltage-sensitive and
Na+-sensitive microelectrodes. The latter were made with
the Na+ ionophore I (ETH-227, Fluka; Buchs, Switzerland)
and filled with 150 mM NaCl as described by Rodrigo and Chapman
(43). [Na+]i was obtained by
interpolating on the Na+-electrode calibration curve the
difference between potentials measured by the Na+-sensitive
and voltage-sensitive electrodes.
The cyclic hexapeptide FRCRCFa (828 mol wt) was obtained as a powder,
made up as a 1 mM stock solution in distilled water, and kept in the
freezer. FRCRCFa was applied in the pipette solution to inhibit Na/Ca
exchange from the cytoplasmic side.
Chemicals. dl-Isoprenaline hydrochloride (Saventrine Intravenous, Pharmax; Bexley, Kent, UK), collagenase type IV (Worthington Biochemical), Ultraser G (GIBCO-BRL), and FRCRCFa were synthesized by D. Khanashvili (25). All of the other chemicals were obtained from Sigma (St. Louis, MO).
Data analysis. Commercial software (pCLAMP 5.5.1 and 6.02, Axon Instruments) was used for generating voltage pulses, data acquisition, and analysis of digitized whole cell currents. The current signals were filtered with an eight-pole Bessel filter (5-kHz cutoff frequency) and sampled at 3-10 kHz. All values are presented as means ± SE. Unpaired Student's t-tests were used to evaluate the statistical significance of differences between means. Values of P < 0.05 were considered to indicate significance.
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RESULTS |
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Characteristics of hypertrophy. At day 7 after the start of isoproterenol injections, this model demonstrated compensated, moderate left ventricular hypertrophy without heart failure. At this stage, rats did not exhibit fatigue nor hyperpnea. When the body cavity was opened to remove the heart, pulmonary edema, pleural effusion, ascites, and hepatomegaly were never observed in any treated animal. The heart weight gradually increased throughout. The body weight of the animals increased similarly in control and treated animals. The heart weight-to-body weight ratio, as an indicator of the degree of hypertrophy, was increased from 3.21 ± 0.05 mg/g (control) to 4.16 ± 0.07 mg/g (hypertrophy) (n = 10, P < 0.05). The lung weight-to-body weight ratio was unchanged at 5.04 ± 0.15 mg/g (control) and 5.12 ± 0.11 (hypertrophy) (n = 10, not significant), as was the liver weight-to-body weight ratio at 41.8 ± 1.9 mg/g (control) and 42.2 ± 1.4 mg/g (hypertrophy) (n = 10, not significant). No serous cavity effusions were observed.
Changes in the action potential.
The resting potential recorded from 29 hypertrophied left ventricular
myocytes was depolarized compared with 23 control myocytes (
76.8 ± 1.1 mV, control;
71.2 ± 0.9 mV, hypertrophy,
P < 0.05, n = 3 pairs of animals). The
amplitude of the overshoot was unchanged in hypertrophy. Action
potential duration was prolonged in the hypertrophied myocytes (Fig.
1). Action potential duration at 25%
repolarization was 290% of the control value (8.1 ± 0.9 ms, control; 23.5 ± 2.7 ms, hypertrophy, P < 0.01),
and action potential duration at 95% repolarization
(APD95) was 155% of the control value (99.4 ± 3.6 ms, control; 152.7 ± 5.4 ms, hypertrophy, P < 0.01).
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Occurrence and ionic properties of DADs. Spontaneous DADs were frequently observed in the hypertrophied myocytes after completion of a prolonged action potential, but they were rarely seen in control myocytes (Fig. 1). The incidence of DADs was 9 of 32 in control and 23 of 31 in hypertrophied myocytes. The amplitude of DADs averaged 2.9 ± 0.4 mV in control, and 12.4 ± 1.3 mV in hypertrophied myocytes (P < 0.05). In five pairs of hypertrophied ventricular myocytes, we studied the pharmacological properties of DADs. In the group of myocytes in which DADs were recorded without FRCRCFa (a specific blocker of Na/Ca exchange) in the pipette, the amplitude of DADs was 13.2 ± 1.6 mV. After inclusion of 10 µM FRCRCFa in the pipette, the amplitude of DADs was 2.8 ± 0.3 mV (P < 0.05). Application of 10 µM DIDS into the superfusing solution reduced the DADs amplitude further to 1.7 ± 0.3 mV (P < 0.05).
These results indicate that in the hypertrophied ventricular cells, DADs are carried principally but not exclusively by Na/Ca exchange. Minor components are carried by a [Ca2+]i-activated nonselective cation current and by [Ca2+]i-activated Cl
current. The relative contributions of these components to the overall
amplitude of DADs are ~80% Na/Ca exchange, 7% Cl
current, and 13% nonselective cation current.
Induction of Iti.
To elucidate the membrane currents underlying the hypertrophy-induced
arrhythmias, cells were voltage-clamped using the whole cell
configuration. Figure 2A shows
representative currents induced by depolarizing voltage pulses of
different amplitudes (0, +30, and +60 mV for 2 s) from a holding
potential of
40 mV in a control cell (middle) and in a
hypertrophied cell (bottom). Iti of
very small amplitude could be seen in 12 of 30 control cells. However, this oscillatory current was seen in 23 of 31 hypertrophied cells at
the termination of the long depolarizing pulses (Fig. 2A,
bottom) at each of the potentials shown. The pattern of
Iti appears to be different, i.e., in some cells
it is single, and in other cases it is oscillatory. Furthermore, in
some cases, the Iti is superimposed on a slowly
decaying inward current, which appears to be carried by Na/Ca exchange.
Similar patterns have also been reported by others in control cells in
which Iti was induced by reoxygenation (4) or oxidative stress (32). The amplitude
of Iti increased after depolarizing to more
positive potentials. Only the first oscillatory current component was
used for evaluation, the amplitude of which was measured as the
difference current between the maximum inward peak and a baseline level
constructed from the tangent joining the two neighboring nadirs as
described by Benndorf et al. (4). The mean amplitude of
Iti induced by +60 mV depolarization was
32 ± 6 pA in 12 control cells and
225 ± 11 pA in 23 hypertrophied cells (P < 0.001).
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0.28 ± 0.05 pA/pF (n = 12) in control cells and
1.39 ± 0.12 pA/pF in hypertrophy
(n = 23, P < 0.001). Figure
2C shows that increasing the amplitude of a depolarizing
voltage pulse reduces the time to peak current.
It is generally accepted that oscillatory release of Ca2+
from the SR associated with intracellular Ca2+ overload is
involved in the generation of Iti (5,
23). In five ventricular myocytes taken from three hypertrophied
hearts, we have therefore studied the effect of ryanodine, which
interferes with the SR Ca2+-release channel
(33) and blocks the
[Ca2+]i-activated Iti
(6), consequently abolishing DADs (14, 31). Figure 3 shows an example of the results
obtained after 2-min exposure to 10 µM ryanodine, which would be
expected to abolish any SR contribution to current generation. Figure
3A illustrates Iti on repolarization
after a 2-s pulse to +60 mV in a hypertrophied cell. This large
oscillatory current component is completely abolished by ryanodine
(Fig. 3B). In addition, ryanodine also inhibits current oscillations, which may be seen during the long depolarizing voltage pulse.
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Ionic basis of Iti.
Current-voltage relationships for Iti density
were constructed by applying a double-pulse protocol (16,
32) illustrated in Fig. 4A,
top. A prepulse to +60 mV of 2-s duration was applied from a
holding potential of
40 mV. The membrane was then repolarized to
different test potentials for 2 s before being returned to the
holding potential. Figure 4A shows representative current traces from a hypertrophied cell. The amplitude of
Iti varies markedly with repolarization voltage,
the largest current being seen at
40 mV. The mean current
density-voltage relationship obtained from nine hypertrophied myocytes
is shown in Fig. 5A (curve a). Iti values recorded during
the test pulses are plotted against the corresponding test voltage.
Iti amplitude reached a peak of
1.49 ± 0.08 pA/pF at
40 mV and decreased on either side of this voltage. The
current remained inward over the voltage range tested (
60 mV to +60
mV) with no apparent reversal potential.
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40 to 0 mV
for 1 min. We have proved that this allowed sufficient time for the
peptide to dialyze into the cell (results not shown). The pulse
protocol was then changed to the protocol used above. Figure
4B shows that under these conditions,
Iti amplitude is markedly reduced. Inward
current oscillations are present only at negative potentials. At
positive potentials, outward current oscillations can be observed both during the depolarizing prepulse and on repolarization. At 0 mV no
current oscillation can be seen. The mean current
density-voltage relationship constructed from data obtained in 12 hypertrophied ventricular myocytes is shown in Fig. 5A
(curve b). This curve represents the small proportion of
Iti carried by mechanisms other than Na/Ca
exchange. The current density-voltage relation reverses at +2.5 ± 2.0 mV.
To investigate whether a [Ca2+]i-activated
outward Cl
current (57) contributes to the
generation of Iti in hypertrophied rat myocytes,
we added the specific Cl
channel blocker DIDS (16,
50) to the superfusate in a concentration of 10 µM, while at
the same time including 10 µM FRCRCFa in the pipette solution. Figure
4C shows that under these conditions, outward current
oscillations during the long depolarizing prepulse and on
repolarization are markedly suppressed, but inward current oscillations
at negative potentials are only slightly reduced compared with Fig.
4B. Figure 5B shows that the mean current
density-voltage relationship (curve b) from 12 cells is
depressed and the reversal potential (+15.0 ± 4.0 mV) is shifted
toward more positive potentials, compared with the curve obtained after
block of Na/Ca exchange in the absence of DIDS. The DIDS-sensitive
component of the current (shown as a dashed line in Fig. 5B)
is an outward rectifier current with a reversal potential of
4.0 ± 3.1 mV close to the calculated Cl
equilibrium
potential of
1.8 mV. The current remaining after block of Na/Ca
exchange and Cl
current shows marked inward rectification
(Fig. 5B, curve b).
These results demonstrate that in hypertrophied ventricular myocytes,
similarly to DADs, Iti is carried principally
but not exclusively by Na/Ca exchange. Minor components are carried by a [Ca2+]i-activated nonselective cation
current and by [Ca2+]i-activated
Cl
current. The relative contributions of these
components to the overall amplitude of Iti
density at
40 mV are ~82% Na/Ca exchange, 5% Cl
current, and 13% nonselective cation current.
In five pairs of control myocytes, we studied the pharmacological
properties of Iti to determine whether
Iti has the same charge carriers in control
cells that was observed in hypertrophied cells. In the group of
myocytes in which Iti were recorded without FRCRCFa (a specific blocker of Na/Ca exchange) in the pipette, the
density of Iti was
0.32 ± 0.06 pA/pF.
After inclusion of 10 µM FRCRCFa in the pipette, the density of
Iti was
0.05 ± 0.02 pA/pF at
40 mV
(P < 0.05). Application of the Cl
channel blocker DIDS (10 µM) into the superfusate failed to exert any
further effect on the density of Iti. The result
suggests that in control ventricular myocytes,
Iti is carried principally but not exclusively
by Na/Ca exchange with a smaller contribution from a
[Ca2+]i-activated nonselective cation current
but with no contribution from a
[Ca2+]i-activated Cl
current.
This result emphasizes that Cl
current component of
Iti is expressed in hypertrophy.
Changes in Na/Ca exchange current and SR
Ca2+ content.
In a series of experiments, we wanted to study whether there is any
change in the SR Ca2+ content as a possible mechanism
underlying the appearance of arrhythmogenic DADs and
Iti in hypertrophied myocytes.
Caffeine-dependent inward INa/Ca was induced at
a holding potential of
80 mV by a short application of 20 mM caffeine
onto the myocytes after a 1-min rest period following a train of
stimulation to ensure that the SR was consistently loaded with
Ca2+ (54). The amplitude of
INa/Ca was increased in hypertrophied myocytes
from
103.5 ± 5.2 pA in control myocytes (n = 40) to
179.9 ± 6.9 pA in hypertrophied myocytes
(n = 41, P < 0.001). Examples of these
changes are shown in Fig. 6. The density
of INa/Ca was increased by 31% in hypertrophied
myocytes (control,
1.04 ± 0.02 pA/pF; hypertrophy,
1.31 ± 0.02 pA/pF; P < 0.001).
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Changes in Ipump current and intracellular
Na+ content.
In another series of experiments we investigated whether decreased
Ipump could underlie the increase in SR
Ca2+ content. Ipump was isolated
using extracellular and intrapipette solutions that suppressed channel
currents and INa/Ca (see MATERIALS AND
METHODS). The Ipump was activated on
returning to 5.4 mM extracellular K+ concentration
([K+]o) after 2 min in K+-free
solution (10, 49) in both control and hypertrophied myocytes at
40 mV holding potential (Fig.
8, A and
B). On reducing [K+]o to 0 mM, holding current shifted inward by about 20 pA in control and 15 pA
in hypertrophied myocyte. Restoration of
[K+]o to 5.4 mM after 2 min in
K+-free solution transiently stimulated the Na pump to
extrude Na+ that had accumulated intracellularly. The peak
of the outwardly directed holding current reached about 130 pA in
control and 100 pA in hypertrophied cells. This
[K+]o-activated transient outward
Ipump was completely prevented by adding 300 µM ouabain into the superfusate (Fig. 8, C and
D) and was reactivated after ouabain has been washed out in
both control and hypertrophied myocytes (Fig. 8, E and
F). These results indicate that the
[K+]o-activated Ipump
is a ouabain-sensitive current and generated fully by the Na pump.
Figure 9 illustrates current-voltage
relationships for Ipump obtained by ramp pulses
superimposed on the constant holding current as shown in Fig. 8.
Current traces taken in 0 mM [K+]o show no
change in the background current in hypertrophied myocytes compared
with the control ones. In both control and hypertrophy, the current
trace crosses the voltage axis at 0 mV. The current traces, taken in
5.4 mM [K+]o were shifted toward higher
Ipump values. Averaged data show that
Ipump, at 0 mV membrane potential, was
136.5 ± 6.6 pA in control cells (n = 36) and
117.3 ± 6.4 pA in hypertrophied cells (n = 33, P < 0.05) (Fig. 9, A and B).
Figure 9C demonstrates the current density-voltage
relationships of the difference currents obtained by subtracting
current traces in 0 mM [K+]o from current
traces in 5.4 mM [K+]o and normalized for
cell capacitance in control and hypertrophied myocytes. These current
density-voltage relationships for the [K+]o-activated Ipump
increase gradually between
120 and
40 mV and saturate between
40
and +40 mV. Ipump density is substantially reduced in hypertrophied myocytes at 0 mV (control, 1.31 ± 0.05 pA/pF; hypertrophy, 0.79 ± 0.04 pA/pF, P < 0.001). The zero-current potential estimated by linear extrapolation
averaged
158 ± 15 mV in control and
153 ± 18 mV in
hypertrophied cells, in agreement with data reported by others
(13).
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DISCUSSION |
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This study shows for the first time that at the cellular level,
both the incidence and magnitude of Iti is
greatly increased in compensated left ventricular hypertrophy. The
major charge carrier for this current is the electrogenic Na/Ca
exchange with smaller contributions from a nonselective cation channel
and from a Cl
channel. We suggest that the mechanism
underlying Iti is spontaneous Ca2+
release from the SR, which is overloaded with Ca2+ as a
consequence of Na-pump downregulation and Na/Ca exchange upregulation.
Iti can account for triggered activity based on DADs, which leads to arrhythmias often observed in hypertrophied ventricular myocardium (2, 20, 34).
It could be postulated that effects seen in this model could be the direct response of the elevated level of circulating isoproterenol at the time of the experiments. However, it has been shown that catecholamine clearance kinetics in humans have two phases with half times of 2 and 34 min (11). In congestive heart failure, clearance is reduced to 67% of control (18), but it would still be expected that catecholamines would be completely cleared after ~4 h (5 half times). Catecholamine clearance levels in the rat are not available, but if it is assumed that the clearance rates are of the same order as those reported for humans, and because these animals were used for experimentation 24 h after the last injection of the catecholamine, any changes observed are unlikely to be due to a direct effect of the isoproterenol used to induce the hypertrophy, but rather to the effects of the hypertrophy itself.
Charge carriers for Iti. In different preparations cyclic release of Ca2+ from the SR can activate different charge-carrier mechanisms such as 1) [Ca2+]i-activated nonselective cation current (8, 16, 23), 2) [Ca2+]i-activated chloride current (16, 55), and/or 3) the electrogenic Na/Ca exchange (4, 12, 32), and thus induces Iti. Our data demonstrate that the major charge carrier for the Iti recorded in hypertrophy is Na/Ca exchange, and the current-voltage relation for this current shows no reversal potential because of the change in the reversal potential of the Na/Ca exchange (ENa/Ca) (4, 12, 16, 32). However, it has been reported that Iti may be comprised of more than one current mechanism in a given myocyte (16). Therefore, we wanted to investigate whether the Iti seen in this model of hypertrophy has more components than the Na/Ca exchange current. To exclude the exchanger we added a specific and selective exchange inhibitor, the cyclic hexapeptide FRCRCFa (21, 25), into the pipette solution, because the specific receptor sites for this peptide are on the intracellular side of the Na/Ca exchange molecule. This peptide gives us the possibility of inhibiting the exchanger in the presence of physiological concentrations of Na+ and Ca2+ on both sides of the sarcolemma. With FRCRCFa in the pipette, the current-voltage relationship for the remaining current component shows a reversal potential at +2.5 mV, thus indicating that Iti is carried not only by the Na/Ca exchange but also by one or more channels. Further proof for this view is provided by the fact that this remaining current component shows different voltage sensitivity from that which was recorded without FRCRCFa.
The current recorded with FRCRCFa in the pipette reverses close to the expected reversal potential of Cl
current
(ECl) and consists mainly of an
outwardly rectifying, Ca2+-activated Cl
current (57) and an inwardly rectifying
Ca2+-activated nonselective cation current
(8). The outward current oscillations, which may be
visible during the depolarizing pulse and on repolarization to positive
potentials, are markedly reduced after superfusion with 10 µM DIDS, a
specific Cl
channel blocker (16, 50), thus
proving that this outward component of the Iti
depends on an outward Cl
current. The pure
Cl
current component of the Iti
was calculated by subtracting the DIDS-insensitive current from the
total current. This difference current (Fig. 5B,
dashed line) shows a reversal potential at
3 mV that is
very close to the calculated ECl (
2 mV).
However, the reversal potential of the small current that remains after block of both Na/Ca exchange and the Cl
current, is
shifted to more positive potentials (+15 mV), suggesting a contribution
for Na+ entry. It appears to be an inwardly rectifying
Ca2+-activated nonselective cation current that can be
carried by both Na+ and K+ (16).
Our present results indicate that in hypertrophied myocytes,
Iti can be the underlying mechanism of DADs,
because they are carried by the same charge carrier mechanisms both
qualitatively and quantitatively. However, our results also suggest
that Itis are not similar in control and
hypertrophied cells because in control cells,
Iti has no DIDS-sensitive component. These
findings are in good agreement with those showing that control
ventricular myocytes do not have Cl
current
(27), but hypertrophied myocytes express it
(3).
Mechanisms of induction of Iti. It is generally accepted that Iti is generated by an oscillatory release of Ca2+ from an overloaded SR that occurs when [Ca2+]i is elevated after a long depolarizing pulse or a prolonged action potential in myocytes having altered Ca2+ and/or Na+ handling capability (5, 23, 31). Our experimental data to support this idea are that increasing the amplitude or the duration of the voltage pulse, conditions which favor increased SR Ca2+ loading, cause an increase in the density of Iti and reduce the time to the peak of the first oscillatory component. The other supporting fact is that ryanodine, a Ca2+-release channel blocker at the SR (33), abolishes DADs and Iti, which is in common with previous reports (6, 14, 31, 34). Moreover, we could not elicit Iti after inclusion of EGTA in the patch pipette (data not shown). These experiments confirm that the Iti we have observed in hypertrophied myocytes depends on elevated [Ca2+]i causing oscillatory Ca2+ release from the SR, such as in normal tissue under conditions such as glycoside toxicity (23), reoxygenation (4), or oxidative stress (32).
In this study, we demonstrate an increased SR Ca2+ content in hypertrophied myocytes in which Iti density is elevated. This finding is consistent with the view that increased SR Ca2+ content can give rise to greater release of Ca2+ after a given rise in [Ca2+]i and, therefore, to a larger Iti in the hypertrophied myocyte. Upregulation of the SR functions, including increased uptake and release of Ca2+ associated with increased contractile force, have been reported in the early stage of both pressure overload-induced cardiac hypertrophy (29, 37) and catecholamine-induced hypertrophy (52). In addition, the SR Ca-pump activity has been reported to show no change in compensated hypertrophy (38). The SR Ca2+-release channel activity was found to be upregulated as reflected by an increased density of the ryanodine receptors in cardiomyopathic hamster hearts early in the development of the disease (46) and in pressure overloaded hypertrophy in the rat (42) in which the Ca2+-ATPase and ryanodine receptor mRNA levels are also increased (1). What mechanisms can cause the SR to overload with Ca2+ in hypertrophied ventricular myocytes? Our data show that hypertrophy-induced reduction of Na-pump activity increases [Na+]i. In accordance with other reports (48), this increased [Na+]i reduces transmembrane [Na+] gradient, which then shifts the reversal potential of the ENa/Ca to more negative potentials closer to the resting membrane potential (Vm). This condition makes the Na/Ca exchange less able to extrude Ca2+ from the cell and eventually results in a net Ca2+ gain during diastole. If [Na+]i increases further, ENa/Ca can be shifted to potentials even more negative than Vm at which Na/Ca exchange works in reverse mode and now brings Ca2+ into the cell and causes a more elevated [Ca2+]i. A high [Ca2+]i can then overload the SR with Ca2+ (4, 23, 32). This Ca2+ loading can be increased further if the Na/Ca exchange is upregulated, i.e., its density is increased, as has been reported to occur in cardiac hypertrophy (24, 51). Under such circumstances, if a spontaneous Ca2+ release from the SR takes place, ENa/Ca is shifted to potentials less negative than Vm and Na/Ca exchange works in forward mode, takes the Ca2+ out of the cell, and generates a large Iti. Thus a downregulated Na pump could be one of the most likely candidates initially responsible for the appearance of Iti in hypertrophied myocytes. What causes the Na pump to downregulate? Our findings of a reduced Ipump activity and an elevated [Na+]i in hypertrophied myocytes confirm that downregulation of the Na pump plays a crucial role in Iti generation. Although hypertrophy-induced Na+-K+-ATPase inhibition (26, 34, 35, 38) and [Na+]i elevation (22, 39) are not new, the present data show for the first time that hypertrophy decreases Ipump, a current generated by the Na-pump enzyme. Reduced Ipump activity can also be due to altered isoform expression of the
subunit of the
Na+-K+-ATPase, as it has been demonstrated by
Kim et al. (26) in a similar catecholamine model in which
hypertrophy was induced by chronic norepinephrine infusion. These
authors found that in hypertrophy the myocardial ouabain-binding sites
are reduced and the
3-isoform protein of the
Na+-K+-ATPase is decreased, but there is no
significant change in the
1-isoform protein. Similar
results were reported by Charlemagne et al. (7) who
observed an isoform shift in another hypertrophy model induced by
aortic constriction in the rat, in which myocardial ouabain binding
characteristics and Na+-K+-ATPase activity
changed to those resembling neonatal form.
What causes the Na/Ca exchange to upregulate? We have found that
INa/Ca is increased in this model of hypertrophy
in line with several studies showing that Na/Ca exchange is upregulated in compensated cardiac hypertrophy on the membrane current level (19, 30, 40, 45), the mRNA expression level
(24), and the protein expression level (51).
Regression analysis of the Ipump and
INa/Ca data plotted against cell membrane
capacitance indicates a reciprocal regulation for these two currents,
insofar as the regression line fitted to the
Ipump data points is shifted to lower current
values, whereas the regression line fitted to the
INa/Ca data points is shifted to higher current
values in hypertrophied myocytes (see Figs. 7 and 10). These
observations lead us to postulate that first in the order of the events
induced by hypertrophy is a reduced Na-pump activity and an increased [Na+]i, which then upregulate the Na/Ca
exchange to take excess Na+ out of the cell at the expense
of bringing Ca2+ in. This adaptational mechanism, however,
may facilitate SR Ca2+ overload and the appearance of DADs
and Iti. Actually, DADs or Iti can be regarded as a "protective"
mechanism that removes Ca2+ from the diseased myocyte at
the expense of generating arrhythmias (9).
Clinical implications. Cellular mechanisms for cardiac arrhythmias are receiving increasing prominence in the literature as the membrane current changes underlying early and DADs that give rise to triggered activity are being evaluated in a number of different arrhythmia substrates (17). Iti has been shown to underlie clinically important arrhythmias, based on DADs resulting from cardiac glycoside toxicity (23), reoxygenation (4), and conditions of oxidative stress (32). DADs are more easily induced in cardiac hypertrophy secondary to renal hypertension (2) after myocardial infarction (41), in diabetic cardiomyopathy (36), and in failing rabbit ventricular trabecula (56). Our finding of substantially increased Iti in hypertrophied myocytes provides a cellular basis for DADs and triggered arrhythmias in cardiac hypertrophy.
The results indicate for the first time at the cellular level that Ipump is decreased, INa/Ca is increased, SR Ca2+ content is increased, and, consequently, Iti is greatly increased in myocytes from a rat model of catecholamine-induced compensated cardiac hypertrophy. Our findings also show that Iti, which can be the underlying mechanism of DADs, depends principally on the electrogenic Na/Ca exchange with smaller contributions from a Ca2+-activated nonselective cation current and a Ca2+-activated Cl
current. The latter is only expressed in hypertrophied myocytes. The
crucial factor for the generation of Iti is an
increased [Na+]i, which then causes an
intracellular Ca2+ overload through a reverse Na/Ca
exchange and oscillatory release of Ca2+ from the
overloaded SR. These findings, if confirmed in other models and humans,
may explain the propensity of hypertrophied hearts to triggered
arrhythmias based on DADs.
| |
ACKNOWLEDGEMENTS |
|---|
The authors thank Jeremy J. Coutinho, Joanna K. Lawton, and Timothy Grocott for skilled and valued technical assistance.
| |
FOOTNOTES |
|---|
This work was supported by the British Heart Foundation.
Address for reprint requests and other correspondence: J. Mészáros, Dept. of Medicine, University of Liverpool, Duncan Bldg., Daulby St., Liverpool L69 3GA, UK.
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.
Received 30 November 2000; accepted in final form 24 April 2001.
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