(Circulation. 1995;92:1179-1187.)
© 1995 American Heart Association, Inc.
Articles |
From the Division of Cardiology and Program in Human Molecular Biology and Genetics (M.C.S.), Eccles Institute of Human Genetics, University of Utah, Salt Lake City.
Correspondence to Dr Michael C. Sanguinetti, Program in Human Molecular Biology and Genetics, Eccles Institute of Human Genetics, Bldg 533, Room 4220, University of Utah, Salt Lake City, UT 84112.
| Abstract |
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Methods and Results Subendocardial tissues were obtained during routine biopsies of the right interventricular septum of seven heart transplant recipients. Subepicardial tissues were obtained from five patients with normal LV function during open heart surgery. IK1 amplitude was the same in myocytes isolated from both regions. Delayed rectifier K+ currents were small or absent in these cells. Ito1 was only slightly larger in LV subepicardial versus RV septal subendocardial myocytes. For example, at +60 mV, Ito1 was 7.2±0.4 pA/pF (n=33) in subepicardial cells compared with 6.0±0.5 pA/pF (n=36) in subendocardial cells. All characteristics of Ito1 examined, including the voltage dependence of activation and inactivation, rate of inactivation, and percent decline of peak current during repetitive pulsing, were similar in myocytes isolated from both regions. These findings are in contrast to previous studies that demonstrated that Ito1 of subendocardial myocytes isolated from the LV free wall of human hearts was smaller and that recovery from inactivation of this current was much slower compared with that observed in subepicardial myocytes.
Conclusions We conclude that the major repolarizing K+ currents in normal human ventricular myocytes are IK1 and Ito1 and that the properties of Ito1 of subendocardial cells isolated from the right interventricular septum are more similar to subepicardial cells than to subendocardial cells of the LV free wall. The similar electric properties shared by myocytes from these two regions may be functionally important inasmuch as the right side of the interventricular septum functions as an extension of the subepicardium of the left ventricle during the contractile cycle.
Key Words: electrophysiology myocardium potassium
| Introduction |
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Because of the relative unavailability of normal human cardiac tissue for research purposes, initial studies characterized currents in myocytes dissociated from diseased human hearts.1 2 3 However, the properties of currents recorded from cells isolated from diseased tissue may differ from those found in normal tissue. For example, the delayed rectifier K+ current (IK) was reported to be smaller and the inward rectifier K+ current (IK1) was reported to be larger in feline ventricular myocytes dissociated from hypertrophied tissue compared with normal tissue.4 In humans, the magnitude of IK1 and the transient outward K+ current (Ito1) were reported to be reduced in myocytes obtained from hearts of patients with terminal heart failure.1 These differences may reflect adaptations to different loading or activation conditions rather than primary pathological changes. The extent to which transmembrane currents adapt to pathophysiological conditions has not been explored adequately in human myocytes. Thus, there is a need to characterize and compare repolarizing K+ currents from a larger number of nonfailing human cardiac myocytes obtained from functionally and anatomically diverse sites. Such information could serve as reference data with which to compare similar voltage clamp measurements with myocytes obtained from diseased hearts.
Ito1 is the most prominent outward current in canine and human atrial5 and ventricular3 6 cardiac myocytes. Antzelevitch and colleagues7 8 9 showed that the marked regional variation in the configuration of canine ventricular action potentials can be attributed primarily to a variable magnitude of Ito1. The initial repolarization phase of action potentials recorded from subepicardial and midmyocardial myocytes is characterized by a prominent notch. This notch is virtually absent in subendocardial myocytes because of a much reduced Ito1. Ito1 is also much larger in epicardial than in endocardial ventricular tissue of the cat10 and rat.11 Lukas and Antzelevitch12 proposed that such transmural heterogeneity in channel density and gating properties may be important in normal dispersion of refractoriness, arrhythmogenesis, and responsiveness to drugs and ischemia. Recently, Wettwer et al6 reported that a marked transmural gradient in the magnitude of Ito1 also exists across the left ventricular (LV) free wall in nonfailing and failing human myocardium. Ito1 was found to be about two times larger in subepicardial relative to subendocardial myocytes dissociated from the LV free wall. The gating of Ito1 channels also exhibited regional variability. The rate of Ito1 recovery from inactivation was much slower in subendocardial than in subepicardial myocytes.6
In this study, we have characterized the major K+ currents in human ventricular myocytes isolated from biopsy samples taken from the right interventricular septum of heart transplant recipients and the LV subepicardium of patients undergoing coronary artery bypass graft surgery. The tissue obtained by biopsies of these patients is composed of relatively normal myocytes, at least compared with those obtained from explanted failing hearts. We found that the average magnitude and recovery kinetics of Ito1 were not markedly different between these two regions of the human heart in contrast to the transmural gradient reported for LV free wall. This similarity may reflect the functional similarity of tissues that form the outer surface of the LV chamber.
| Methods |
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Myocyte Isolation
The method used to enzymatically dissociate
human
ventricular biopsy samples was described previously in
detail.15 Biopsy specimens were immediately transported to
the laboratory in ice-cold, oxygenated HEPES-buffered/2,3
butanedione monoxime (BDM) saline (composition described below). The
addition of BDM to this solution minimizes cutting and
reoxygenation injury of isolated
myocytes.16 After a 30-minute equilibration at room
temperature in this transport solution, the tissue sample was placed in
Ca2+-free HEPES-buffered/BDM saline and sliced into
400-µm pieces with a mechanical vibratome. The slices were then
incubated at 37°C with protease and collagenase while the
solution was constantly bubbled with 100% oxygen. Slices were
transferred to a solution containing fresh enzyme every 10 to 15
minutes for a total of 90 minutes. The enzyme solution containing
dissociated cells was diluted with an equal volume of recovery medium
and centrifuged at 100g for 5 minutes. The resulting
pellets were then resuspended in recovery media and kept at room
temperature.
Voltage Clamp Data Acquisition and Analysis
The suction
microelectrode voltage clamp technique described by
Giles and Shibata17 was used to record currents in
single ventricular myocytes. Pipettes were fabricated from
1-mm-OD square-bore borosilicate glass (Frederick & Dimmock) and had
resistances of 3 to 6 M
when filled with an intracellular solution
that consisted of 0.5 mol/L potassium gluconate and 25 mmol/L KCl (pH
7.3). Series resistance was compensated by at least 80%. The
limitations (high series resistance, loading of cells with
K+ during prolonged recordings) and advantages (no
immediate alteration of intracellular contents, ease of seal formation)
of using these electrodes and filling solutions were described
previously.18 19 Command voltage pulses were
generated by
use of PCLAMP software, a Digidata 1200 interface (Axon
Instruments) connected to a 486DX, 50-MHz desktop computer, and an
Axopatch 200 amplifier (Axon Instruments). Currents were
low-passfiltered with a cutoff frequency (-3 dB) of 1 or 2 kHz.
Currents are usually expressed relative to total cell capacitance to
facilitate comparison between cells of various sizes.
In most
experiments, cells were bathed in a nominally
Ca2+-free "extracellular solution" (room
temperature) containing 1 mmol/L CoCl2 to block
Ca2+ currents and prevent cell contraction. Unless
indicated otherwise, currents were elicited with stepped pulses from a
holding potential of -60 mV. At -60 mV, a small
Na+
current (INa) remained available for activation on
depolarization. Therefore, each test pulse was preceded by a 20-ms
pulse to -30 mV, which served to inactivate any remaining
INa. To determine the current-voltage relation for
Ito1, pulses were applied every 8 seconds in 10-mV
increments to test potentials ranging from -30 to +70 mV. This
pulsing
rate was sufficiently slow to allow recovery of Ito1 from
inactivation at -60 mV between successive test pulses. The time course
of Ito1 inactivation was fit with a single exponential
relation:
Ito1(t)=A0+A1e(-t/
)
with a Chebyshev noniterative fitting technique (PCLAMP,
Axon Instruments). A nonlinear least-squares fitting routine
(KALEIDAGRAPH, Abelback Software) was used to fit
normalized data describing the voltage dependence of Ito1
activation and inactivation to a Boltzmann distribution. The voltage
dependence of Ito1 activation was determined from the
amplitude of tail currents after 20-ms pulses to potentials
(Vt) ranging from -40 to +20 mV. Tail currents were
normalized to the maximum value (Ito1max) determined
by fits of data from an individual experiment. Cumulative data were
then averaged and fit with a Boltzmann relation,
Ito1/Ito1max=1/{1+exp[(V1/2-Vt)/k]},
to estimate the average half-point (V1/2) and slope factor
(k) for this relation.
The voltage dependence of Ito1 inactivation was determined by use of 5-second conditioning test pulses. Each conditioning pulse was applied to a potential ranging from -70 to -5 mV and was followed by a pulse to -30 mV (to inactivate any INa present) and then to +50 mV to monitor the extent of Ito1 inactivation. The currents were normalized to the largest current for each experiment; then cumulative normalized data were fit in a manner similar to that described for the activation curve.
To determine the current-voltage relation for IK1, 140-ms pulses were applied every 4 seconds from a holding potential of -60 mV. Test pulses were applied in -10-mV increments to potentials ranging from -40 to -170 mV. The amplitude of IK1 at each potential was determined by measuring peak current relative to the zero current level.
Solutions
The HEPES-buffered/BDM solution used for transport
of tissue
specimens contained (in mmol/L) NaCl 120, KCl 5.4, MgSO4
0.5, CaCl2 0.25, sodium pyruvate 5, glucose 20, taurine 20,
BDM 30, and HEPES 10; pH was adjusted to 7.0 with NaOH. The enzyme
solution was prepared by adding 0.1 mg/mL protease type XXIV (Sigma
Chemical Co) and 1 mg/mL collagenase type 2 (Worthington)
to HEPES-buffered/BDM solution in which the CaCl2
concentration was reduced to 50 µmol/L. The recovery medium was the
same as the HEPES-buffered/BDM solution, except that it also contained
1% BSA and the pH was adjusted to 7.2.
The extracellular solution bathing the cells during the voltage clamp experiments contained (in mmol/L) NaCl 132, KCl 4, MgCl2 1.2, HEPES 10, glucose 10, and CoCl2 1; pH was adjusted to 7.4 with NaOH.
Statistics
All cumulative data are expressed as
mean±SEM. Comparisons were
performed by a two-way ANOVA where appropriate followed by a
multiple-comparisons test (Tukey-Kramer) to test for differences
between unpaired data (eg, currents recorded from subepicardial and
subendocardial cells at a given test potential). Differences between
values were considered statistically significant when
P<.05.
| Results |
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Inward Rectifier K Current
The magnitude of IK1
was similar in LV subepicardial
and right ventricular (RV) septal subendocardial myocytes
throughout the voltage range examined (-60 to -170 mV). At the
test
potential of -140 mV, IK1 averaged -18.2±1.4
pA/pF
(range, -10.4 to -27.8 pA/pF) for LV subepicardial cells
(n=15, two
hearts) and -18.7±1.0 pA/pF (range, -9.1 to -33.1
pA/pF) for RV
septal subendocardial cells (n=35, six hearts). Outward current
recorded at -60 mV was small: 0.076±0.046 pA/pF in subendocardial
cells and 0.097±0.042 pA/pF in subepicardial cells. IK1
exhibited marked time-dependent inactivation at very negative
potentials. For example, at -170 mV, current measured at the end of a
140-ms test pulse decayed to about half its initial value (Fig
1
). The time course of IK1 inactivation was
best fit with a single exponential relation. The time constants for
inactivation were significantly slower in the LV subepicardial than in
the RV septal myocytes at all potentials (Fig 1C
). The
biological
significance of this difference is uncertain because of the limited
sample size (IK1 was recorded in myocytes isolated from
only two RV septal biopsies).
|
Transient Outward K Current
The current-voltage relation for
Ito1 was determined
from a holding potential of -60 mV. The small INa that
remained available for activation was further inactivated
during a 20-ms prepulse to -30 mV (Fig 2A
). The
amplitude of Ito1 was estimated by measurement of the
time-dependent component from its peak outward value to its
steady-state value at the end of 500-ms test pulses. The sustained
current remaining at the end of these test pulses is referred to as
Isus. The transient outward current activated by
this protocol is assumed to be the voltage-dependent component
(Ito1) because Ca2+-dependent transient
outward current (Ito2) requires entry of
Ca2+ through Ca2+ channels for
its activation.5 20 Further evidence that only
Ito1 was present under these experimental conditions
was the finding that inactivation of the current was usually best fit
with a single exponential function. However, because the cell interior
was not perfused and the recording pipette did not contain a
Ca2+ buffering agent such as EGTA, we cannot exclude
the presence of a small Ito2 component. The average
amplitudes of Ito1 and Isus were only slightly
larger in subepicardial than in subendocardial myocytes at all test
potentials (Figs 2
and 3
). For example,
Ito1
was 1.8±0.1 pA/pF (range, 0.1 to 3.2 pA/pF) at 0 mV and 7.2±0.4
pA/pF
(range, 3.2 to 11.3 pA/pF) at +60 mV in subepicardial cells (n=33
cells, five hearts). In RV septal subendocardial myocytes,
Ito1 was 1.3±0.1 pA/pF (range, 0.2 to 2.8 pA/pF) at 0 mV
and 6.0±0.5 pA/pF (range, 1.3 to 12.9 pA/pF) at +60 mV
(n=36 cells,
seven hearts). Ito1 was significantly (P<.05)
larger in subepicardial than in subendocardial myocytes only at test
potentials ranging from -10 to +20 mV (Fig 2B
).
There was considerable
variation in the magnitude of peak Ito1 recorded in
myocytes isolated from a single preparation. For example, at the test
potential of +60 mV, Ito1 varied from 4.6 to 10.9 pA/pF
(n=13) in cells dissociated from one subepicardial specimen and from
1.5 to 12.9 pA/pF (n=12) from one subendocardial specimen. There was no
significant correlation (correlation coefficient, .05) between the
current densities of Ito1 and IK1 within a
given cell. With the assumption that IK1 and
Ito1 are subject to the same detrimental effects of
metabolic or other imbalances, this suggests but does not
prove that the variation in the magnitude of Ito1 does not
simply reflect the overall condition of a given myocyte.
|
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Isus exhibited outward rectification at test potentials
>0
mV (Fig 3
). At test potentials of 0 and +60 mV,
Isus was
0.22±0.03 and 1.50±0.13 pA/pF in LV subepicardial cells
(n=30 cells,
five hearts) and 0.11±0.02 and 1.31±0.12 pA/pF in RV septal
subendocardial cells (n=30 cells, seven hearts), respectively. The
channel type underlying Isus is not known. It is probably
not a K+ current because it was not blocked by 5 mmol/L
4-aminopyridine or 2 mmol/L BaCl2 (data not
shown).
The time course of Ito1 inactivation was determined
by
fitting the decay phase of currents recorded during 500-ms pulses
to potentials ranging from -10 to +70 mV with either one or two
exponential functions. In a few cells, inactivation of Ito1
was best fit with two exponentials at potentials
+30 mV. However, the
currents at all potentials for the majority of cells were best fit with
a single exponential function. The time constants for Ito1
inactivation showed only a slight voltage dependence, ranging from 60
to 80 ms for both subepicardial and subendocardial cells (Fig
2C
).
The voltage dependence of Ito1
activation was determined by
tail current analysis as described in the "Methods"
section (Fig 4
). The half-points for activation of
Ito1 were -8.9±0.19 and -7.8±0.2 mV for
subepicardial
(n=15 cells, four hearts) and subendocardial cells (n=20, six
hearts),
respectively. The slope factors of the activation curves were 6.2±0.2
and 5.7±0.2 mV for subepicardial and subendocardial cells,
respectively. Activation curves were also constructed from peak values
of outward Ito1 (data from Fig 2B
) after correction
for
changes in driving force for K+ and with the assumption of
a reversal potential of -80 mV. The V1/2 and slope factor
determined by this method were more positive than that determined by
tail current analysis; however, these data were not well fit
with a single Boltzmann distribution.
|
The voltage dependence of
Ito1 inactivation was assessed
with 5-second conditioning prepulses (Fig 5
). The
half-points of this relation were -36.3±0.4 mV for subepicardial
myocytes (n=23, four hearts) and -33.0±0.4 mV for
subendocardial
myocytes (n=25, six hearts). The slope factors for the inactivation
curves were -5.6±0.2 and -5.2±0.2 mV for
subepicardial and
subendocardial myocytes, respectively. There was only a slight overlap
between the voltage dependence of activation and inactivation,
delineating the range of potentials over which Ito1 could
activate but not inactivate. The resulting
"window current" would occur between -35 and -5 mV and
represent
5% of peak current amplitude at potentials from
-20 to -5 mV (Fig 5C
).
|
The recovery from
inactivation of Ito1 is known to depend
on voltage.6 20 As an indirect measure of this
phenomenon,
we recorded the decrease in Ito1 magnitude during a
train of 10 pulses applied from a variable holding potential to a
common test potential of +40 mV. Test pulses of 200-ms duration were
applied at a rate of 120 pulses per minute. Cells were held for at
least 1 minute at a holding potential of -40, -50, or -60 mV
before
the train of test pulses was applied. The amplitude of Ito1
during the first pulse was dependent on holding potential (smallest at
-40 mV) as expected from the voltage dependence of inactivation
described in Fig 5
. To facilitate comparison of the data
obtained at
different holding potentials, the data are plotted relative to the
amplitude of Ito1 for the first pulse at a given holding
potential. The rate-dependent decrease in Ito1 was the same
for both left subepicardial and right septal subendocardial myocytes
(Fig 6
). This suggests that the recovery from
inactivation of the currents was the same for cells isolated from the
two regions of the ventricle.
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Delayed Rectifier K+ Current
Slowly
activating delayed rectifier K+ current
(IK) was not measurable under the conditions used in this
study. It is possible that IK was present in these
cells but that the absence of extracellular
Ca2+, the presence of 1 mmol/L
Co2+, and the recording of currents at room
temperature reduced its size. Cobalt blocks IKr in guinea
pig cardiac myocytes.21 Therefore, several myocytes were
voltage clamped while bathed in a solution containing 1.8 mmol/L
CaCl2 and at 35°C. These same conditions were used
previously to record robust IK currents in isolated
guinea pig ventricular myocytes.18 Even under
these conditions, IK was very small or absent. The average
time-dependent IK during a 3.5-second test pulse to +60 mV
in 6 subepicardial myocytes from one heart was 28±23 pA (range, 0 to
128 pA), equivalent to about 0.028 pA/pF.
| Discussion |
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The
magnitude of Ito1 reported previously from
midmyocardial myocytes was much larger than we or others have reported
for this current in subepicardial or subendocardial myocytes.
Beuckelmann et al1 reported that peak Ito1
measured at +40 mV averaged 9.2 pA/pF in nonfailing myocytes. The
average peak Ito1 at +40 mV in our cells were 4.3
(subendocardium) and 5.4 (subepicardium) pA/pF. The size of our biopsy
samples (
1.5-mm depth) was small enough to ensure that only
subendocardial and subepicardial tissues and not midmyocardial tissue
were collected. Further study is needed to confirm whether
K+ currents are indeed larger in midmyocardial than in
subepicardial or subendocardial myocytes.
A large transmural gradient in the magnitude of Ito1 has been documented for the left ventricle of diseased human hearts. In explanted diseased hearts, Ito1 was about 2.5 times larger in LV subepicardial than in subendocardial myocytes when assessed at a test potential of +40 mV.22 In another study, myocytes isolated from failing hearts differed regionally by a factor of 3.4-fold in failing hearts but by only 1.5-fold in nonfailing hearts (6.8 pA/pF, n=16, versus 4.4 pA/pF, n=5, at +60 mV in LV subepicardial and subendocardial myocytes, respectively).6 A nonuniform distribution in the magnitude of endocardial Ito1 was also reported to exist in rabbit ventricle. Ito1 of rabbit subepicardial myocytes was reported to be two times larger than in subendocardial cells isolated from papillary muscles but only 1.16-fold larger than that recorded from subendocardial cells isolated from the ventricular free wall.28 We found that Ito1 averaged 7.2 and 6.0 pA/pF at +60 mV in LV subepicardial and RV septal subendocardial myocytes, respectively (a 1.2-fold difference).
A significant transmural difference in the voltage dependence of Ito1 activation was previously reported for myocytes isolated from undiseased human LV free wall. Half-maximal activation of Ito1 was +9.7 mV in subepicardial cells compared with +23.1 mV in subendocardial cells.6 We determined the voltage dependence of Ito1 activation by tail current analysis and did not detect any significant regional difference between the LV subepicardial and RV septal subendocardial layers, either in the potential at which Ito1 was half-activated or in the slope of the activation curve. This apparent discrepancy may be related to experimental conditions. We used pipettes with very small tip diameters (to minimize cell dialysis) that were loaded with 0.5 mol/L K gluconate and 25 mmol/L KCl and bathed the cells in a nominally Ca2+-free solution containing 1 mmol/L CoCl2. Differences in pipette (internal) solution and extracellular divalent cations (Cd2+ versus Co2+ to block Ca2+ current; presence or absence of CaCl2) may explain some of these apparent differences in the voltage dependence of Ito1 activation. The voltage dependence of Ito1 determined by tail current analysis in our study was similar to that reported for rabbit atrial cells (V1/2, -12 mV; slope factor, 9.6 mV).29 The slope and V1/2 of the isochronal (5-second) inactivation curve for Ito1 determined in our study were similar to those reported previously when 2-second conditioning pulses were used in normal6 or failing ventricular myocytes.2
Our findings confirm the major findings of Wettwer et al,3 6 Nabauer et al,2 and Beuckelmann et al1 that the most prominent K+ currents of human ventricular myocytes are IK1 and Ito1. Like these previous investigators, we found that delayed rectifier K+ currents were small or absent in these cells. All these studies are complicated by the poor yield and low viability of myocytes isolated from human heart tissue and by the potential, yet unknown, effects of the many medications that patients received before biopsy. Despite these numerous complicating factors, we felt it was reasonable to compare voltage clamp data obtained from myocytes dissociated from both types of biopsy samples because all tissues were handled the same and the methods used to record currents were identical.
Regional Variability in Rate-Dependent Decrease in
Ito1
The decrease in Ito1 during a train of
pulses applied
at 120 pulses per minute was nearly identical for RV septal and LV
subepicardial myocytes, regardless of holding potential (Fig
6
). The
decrease in Ito1 during repetitive pulsing results from a
combination of the rate of current inactivation during the test pulse
and the rate of recovery from this inactivation. Because the rate of
Ito1 inactivation was essentially the same in all myocytes,
we can conclude that the rate of recovery from inactivation of
Ito1 was also the same at holding potentials of -40,
-50,
and -60 mV for myocytes isolated from both regions of the heart. Using
a similar pulse train protocol applied from a holding potential of -60
mV, Nabauer and Beuckelmann22 reported that
Ito1 was decreased by 16.3% in subepicardial cells and
85.4% in subendocardial cells isolated from explanted hearts. We found
that Ito1 decreased by about 15% in myocytes from both the
LV subepicardium and RV septal subendocardium. This is further evidence
that myocytes isolated from the right interventricular
septum are more like myocytes of the LV subepicardium than LV
subendocardium with respect to properties of Ito1. The
pulse-dependent decrease in ventricular Ito1
observed in our study is quite similar to that reported by Fermini et
al30 for human atrial myocytes. Ito1 of human
atrial cells was reduced by about 5% when paced at 2 Hz from a holding
potential of -60 mV. Thus, the previously reported findings that
Ito1 of human subendocardial myocytes is characterized by a
reduced amplitude, a more positive V1/2 for
voltage-dependent activation, and a comparatively slow recovery from
inactivation do not apply to the entire subendocardium.
Isus and IK
The sustained outward
current remaining after inactivation of
Ito1 in isolated human atrial myocytes represents
an ultrarapidly activating delayed rectifier K+ current
(IKur) that is half-blocked by 0.05 mol/L
4-aminopyridine (4-AP).31 32 The outward current
(Isus) remaining at the end of 500-ms pulses was not
blocked by 4-AP or BaCl2. This is in agreement with an
earlier report2 that 5 mmol/L 4-AP had no effect on
sustained current after complete inactivation of Ito1 in
ventricular myocytes isolated from failing human hearts.
The lack of effect of 4-AP indicates the absence of IKur in
these cells. The nonlinear current-voltage relation of Isus
indicates that this current is not merely a leak current. We did not
determine the ionic selectivity of this conductance. It is possible
that Isus is an undescribed nonselective cation current, a
Cl- current, or some combination of these and other small
currents.
IK is extremely small or absent in nonfailing human ventricular myocytes. Beuckelmann et al1 also reported that IK was absent in cells isolated from nonfailing human hearts. These findings are somewhat puzzling because several drugs known to specifically block one type of IK (IKr) have been reported to lengthen action potential duration of isolated human papillary muscles in vitro33 and prolong QT in patients, and both types of IK (IKr and IKs) have been recorded from human atrial myocytes.34 IK was observed in human atrial myocytes even in the presence of 2 mmol/L CoCl2 and 2 mmol/L 4-AP, used to block Ca2+ current and Ito2.31 However, a significant number of atrial myocytes (28% of total) were found to have a large Ito but no IK. These myocytes were called type 3 cells to distinguish them from those that had large Ito and IK (type 1 cells) or large IK and no Ito1 (type 2 cells). With regard to the major types of repolarizing K+ currents, human ventricular myocytes are most like type 3 atrial cells characterized by Wang et al.31 As discussed previously,15 our myocyte isolation technique results in a relatively poor yield compared with the more commonly used retrograde perfusion of entire animal hearts. The most obvious potential explanation for the findings that IK was not observed in isolated cells and yet drugs such as E-4031 prolong the action potential duration of cells recorded from intact human muscle is that IK channels were somehow altered during tissue dissociation with protease. However, IK is still present in guinea pig ventricular myocytes isolated from strips of tissue with the same procedures we used to dissociate cells from human tissue.15 Another unexplored possibility is that E-4031 and related methanesulfonanilide compounds lengthen cardiac action potentials by affecting a repolarizing current other than IKr. This is an unlikely possibility because these drugs were shown to block IKr specifically and have no effect on Ito1 or IK1 in isolated human atrial myocytes.34
Conclusions
We found only small or no differences in the
magnitude and
properties of IK1 and Ito1 in LV subepicardial
myocytes compared with cells isolated from the right
interventricular septum. Previous studies clearly
demonstrated that Ito1 of human LV subendocardial myocytes
is significantly smaller than and is characterized by gating properties
that are distinctly different from LV subepicardial myocytes. Future
studies are needed to determine whether the right
interventricular septum shares other electric
properties with the LV subepicardium and whether such properties are
important in the functional coupling between these two anatomic
regions.
| Acknowledgments |
|---|
Received January 9, 1995; revision received March 9, 1995; accepted March 17, 1995.
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