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J Physiol Volume 521, Number 2, 351-361, December 1, 1999
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The Journal of Physiology (1999), 521.2, pp. 351-361
© Copyright 1999 The Physiological Society

Constitutive beta2-adrenergic signalling enhances sarcoplasmic reticulum Ca2+ cycling to augment contraction in mouse heart

Ying-Ying Zhou, Long-Sheng Song, Edward G. Lakatta, Rui-Ping Xiao and Heping Cheng

Laboratory of Cardiovascular Science, Gerontology Research Center, National Institute on Aging, National Institutes of Health, Baltimore, MD 21224, USA

MS 9779 Received 25 June 1999; accepted after revision 9 September 1999.
  ABSTRACT
Top
Abstract
Introduction
Methods
Results
Discussion
References

  1. Transgenic overexpression of the beta2-adrenergic receptor (beta2AR) in mouse heart augments baseline cardiac function in a ligand-independent manner, due to the presence of spontaneously active beta2AR (beta2AR*). This study aims to elucidate the mechanism of beta2AR*-mediated modulation of cardiac excitation-contraction (EC) coupling.

  2. Confocal imaging was used to analyse Ca2+ sparks and spatially resolve Ca2+ transients in single ventricular myocytes from transgenic (TG4) and non-transgenic (NTG) littermates. Whole-cell voltage- and current-clamp techniques were used to record L-type Ca2+ currents (ICa) and action potentials, respectively.

  3. In the absence of any beta2AR ligand, TG4 myocytes had greater contraction amplitudes, larger Ca2+ transients and faster relaxation times than did NTG cells.

  4. The action potentials of TG4 and NTG myocytes were similar, except for a prolonged end-stage repolarization in TG4 cells; the ICa density and kinetics were nearly identical. The relationship between peak Ca2+ and contraction, which reflects myofilament Ca2+ sensitivity, was similar.

  5. In TG4 cells, the frequency of Ca2+ sparks (spontaneous or evoked at -40 mV) was 2-7 times greater, despite the absence of change in the resting Ca2+, sarcoplasmic reticulum (SR) Ca2+ content, and ICa. Individual sparks were brighter, broader and lasted longer, leading to a 2·3-fold greater signal mass. Thus, changes in both spark frequency and size underlie the greater Ca2+ transient in TG4 cells.

  6. The inverse agonist ICI 118,551 (ICI, 5 × 10-7 M), which blocks spontaneous beta2AR activation, reversed the aforementioned beta2AR* effects on cardiac EC coupling without affecting the sarcolemmal ICa. However, ICI failed to detect significant constitutive beta2AR activity in NTG cells.

  7. We conclude that beta2AR*-mediated signalling enhances SR release channel activity and Ca2+-induced Ca2+ release in TG4 cardiac myocytes, and that beta2AR* enhances EC coupling by reinforcing SR Ca2+ cycling (release and reuptake), but bypassing the sarcolemmal ICa.
  INTRODUCTION
Top
Abstract
Introduction
Methods
Results
Discussion
References

Excitation-Ca2+ release coupling is a pivotal event in cardiac function. During membrane depolarization, sarcolemmal Ca2+ influx through the voltage-operated L-type Ca2+ channels triggers the sarcoplasmic reticulum (SR) to release Ca2+ via the Ca2+-induced Ca2+ release (CICR) mechanism (Fabiato, 1983). The resultant cytosolic Ca2+ transient activates myofilament proteins and initiates contraction. Cardiac relaxation ensues when the elevated cytoplasmic Ca2+ is resequestered by the SR Ca2+ pump, or, to a lesser extent, extruded via the sarcolemmal Na+-Ca2+ exchanger. In order to meet the body's variable circulatory demands, cardiac excitation-contraction (EC) coupling is constantly modulated by an array of physiological mechanisms. Driven by sympathetic neurotransmitters and adrenal hormones, beta-adrenergic receptor (betaAR) signalling interacts with virtually all constituents of the EC coupling cascade, including the L-type Ca2+ channel current (ICa) (Tsien et al. 1986; Xiao & Lakatta, 1993), SR Ca2+ release channels/ryanodine receptors (RyRs) (Yoshida et al. 1992; Valdivia et al. 1995), phospholamban (PLB) (Lindemann et al. 1983; Kuschel et al. 1999a), and contractile myofilaments (Rapundalo et al. 1989; Kuschel et al. 1999b). Additionally, beta-adrenergic stimulation may modulate other sarcolemmal ionic currents, such as K+ currents (Scamps, 1996), and electrogenic transporters, such as Na+-Ca2+ exchanger (in non-mammalian species) (Shuba et al. 1998), to alter the action potential configuration, and subsequently, the Ca2+ fluxes during a cardiac cycle.

Although both beta1AR and beta2AR stimulation enhance cardiac contractility, recent studies have revealed several features unique to beta2AR subtype signal transduction. Specifically, while beta1AR couples exclusively to stimulatory G protein (Gs), agonist-occupied beta2AR in several species dually couples to Gs and inhibitory G protein (Gi), generating cross-talk between the two signalling pathways through a single receptor (Xiao et al. 1995, 1999; Kuschel et al. 1999a). As a result, beta2AR signalling is uncoupled from phosphorylation of cytoplasmic and SR proteins (in rat and dog), and induces a less potent relaxant effect (in rat) (Xiao et al. 1994; Altschuld et al. 1995; Kuschel et al. 1999a,b). The contractile response to beta2AR signalling depends largely, if not exclusively, on an augmentation of ICa (Xiao & Lakatta, 1993; Zhou et al. 1997). In an extreme case, potent beta2AR-Gi signalling in the mouse heart fully negates the concurrent beta2AR-Gs signalling in most mouse ventricular myocytes, such that a contractile response is unmasked only if the Gi function is inhibited (Xiao et al. 1999).

Current theories predict that, in addition to agonist-induced activation, receptors can undergo spontaneous conformational changes, resulting in ligand-independent activity. Since these spontaneously activated receptors are scarce (see Samama et al. 1993 for constitutively active mutants), their functional manifestation and significance have not been appreciated until recently. In TG4 transgenic mice, which have 200-fold overexpression of wild-type human beta2ARs, the existence of ligand-independent, spontaneously activated beta2AR (beta2AR*) has been convincingly documented in the intact animal, in isolated atria, and in single myocytes (Milano et al. 1994; Bond et al. 1995; Du et al. 1996; Xiao et al. 1999). In retrospect, the observation that beta2AR* induces a robust inotropic effect is rather surprising, because our recent report illustrated that ligand-occupied beta2AR is usually quiescent in both TG4 and non-transgenic (NTG) littermates due to the Gi coupling (Xiao et al. 1999). These results indicate that, unlike liganded beta2AR, beta2AR* modulates EC coupling in a distinctly different fashion.

The present study aims to elucidate the cellular mechanism(s) that underlies beta2AR*-mediated contractile responses. We systematically characterized the major components of EC coupling, including action potential, ICa, SR Ca2+ content, the elementary SR Ca2+ release events (Ca2+ sparks), Ca2+ transients and cell contraction in ventricular myocytes from TG4 and NTG mice. The present findings reveal profound modulatory effects of beta2AR* on both CICR sensitivity and SR Ca2+ reuptake, in contrast to the lack of effect on ICa. These results suggest a novel mode of cardiac inotropic regulation: an enhanced SR Ca2+ cycling mediates the positive inotropic effect, while the sarcolemmal ICa and myofilament Ca2+ sensitivity remain unchanged.

  METHODS
Top
Abstract
Introduction
Methods
Results
Discussion
References

Cell isolation

This investigation conforms to NIH guidelines on the care and use of animals. Transgenic mice with beta2AR 200-fold overexpression (TG4) and their non-transgenic littermates (NTG) were generously provided by Drs Walter J. Koch and Robert J. Lefkowitz (Duke University Medical Center, Durham, NC, USA). Single murine cardiac myocytes were isolated from the hearts of 2- to 3-month-old mice using a standard enzymatic technique (Korzick et al. 1997). Briefly, mice were anaesthetized by intraperitoneal injection with 100 mg kg-1 sodium pentobarbitone. After all reflex activity had ceased, the chest was opened and the heart quickly removed and retrogradely perfused with collagenase B and protease using the Langendorff method. Cells were then shaken loose from the minced heart and suspended in Hepes-buffered solution consisting of (mM): CaCl2 1, NaCl 137, KCl 5·4, dextrose 15, MgSO4 1·3, NaH2PO4 1·2, Hepes 20; pH 7·4 adjusted with NaOH.

Confocal microscopy

Cells were placed on the stage of a Zeiss LSM-410 inverted confocal microscope (Carl Zeiss, Inc., Germany) and excited by the 488 nm line of an argon laser. In whole-cell patch-clamp experiments, cells were dialysed with 100 µM fluo-3 pentapotassium salt (Molecular Probes) via a patch pipette. In experiments using field electrical stimulation, fluo-3 loading was achieved by a 10 min incubation of the myocytes in Hepes buffer containing 10 µM of the acetoxymethyl ester form fluo-3 AM (Molecular Probes), dissolved in DMSO, followed by a 15 min wash in fresh Hepes buffer (Cheng et al. 1993).

All images were taken in line-scan mode, with the scan line usually oriented along the long axis of the myocyte, avoiding the nucleus or nuclei of the cell. Each image consisted of 512 line-scan images 2·09-4·38 ms apart, and each line consisted of 512 pixels spaced at 0·10-0·25 µm intervals. The microscope was equipped with a Zeiss Plan-Neofluar × 40 oil immersion objective lens (NA, 1·3). The confocal pinhole was set to render spatial resolutions of 1·0 µm (axial) and 0·4 µm (perpendicular to the optical axis). Image processing, data analysis and presentation were performed with IDL software (Research Systems, Boulder, CO, USA).

Spark detection and measurement

To detect and characterize Ca2+ sparks objectively, we used a modified version of the automated spark detector recently described (Cheng et al. 1999). The basic steps in the algorithm include: (1) locating tentative spark regions as pixels/regions that are 2 × standard deviation (S.D.) above the mean fluorescence intensity; (2) excising these provisional sparks from the image, and recomputing the statistics of the remaining regions (presumed to have no spark); (3) determining final spark regions by their excessive deviation (3·8 S.D.) from the background. However, some sparks were clustered and overlapped in space and time, usually with a 'seeder' spark at the beginning of the cluster. To measure the rate of occurrence of sparks spontaneously activated at rest, we considered each cluster as a primary event; secondary sparks usually reflect a local regeneration driven by the seeder. Therefore, a primary event was defined as a connected area that exceeded a weak threshold condition (2·0 S.D.), while containing at least one pixel that exceeded a stronger (i.e. 3·8 S.D.) threshold. An event so detected was then compared with a reference image formed by high-pass filtering and thresholding the raw image, to determine spark clustering. Solitary sparks were those whose non-zero pixels in the reference image were all connected in a single islet. Otherwise, it was deemed as a spark cluster. All parametric measurements were performed on solitary Ca2+ sparks.

In voltage-clamped TG4 cells held at -40 mV, evoked sparks were too numerous to be counted by the automated spark detector. In this case, we estimated the spark number by the 'signal mass'. The signal mass is defined as the integral of the change in the normalized fluorescence (DeltaF/F0 = F/F0 - 1, where F0 refers to the background fluorescence intensity) over space-time (xt) in the line-scan image. Specifically, we first calculated the total signal mass (M):

eq01

The number of sparks that collectively produced the signal M was then estimated by dividing M by the signal mass of the averaged spontaneous solitary Ca2+ spark from TG4 myocytes. This algorithm can be justified on the bases that (1) in the most parsimonious model, all cardiac SR Ca2+ release consists of Ca2+ sparks (Cannell et al. 1995; Lopez-Lopez et al. 1995; see Shirokova et al. 1999 for a recent review); (2) unitary properties of Ca2+ sparks are relatively independent of trigger Ca2+ or voltage (when release intensity is low) (Cannell et al. 1995; Lopez-Lopez et al. 1995; Collier et al. 1999); (3) when Ca2+ sparks overlap each other, a linear approximation for summation of the fluo-3 fluorescence signal can be validated from model simulation (Cheng et al. 1999; Shirokova et al. 1999). However, it should be noted that the spark rate may be underestimated by this method when the release is large, as the unitary Ca2+ spark signal decreases when the SR Ca2+ is partially depleted (Song et al. 1997).

Measurement of cell shortening

Free-load cell shortening was measured in both indicator-loaded and non-loaded cells. Cells were placed on the stage of an inverted fluorescence microscope (Zeiss IM-35) and illuminated with red (650-750 nm) light through the normal bright-field path of the microscope. The change in cell length following field stimulation (4 ms pulses delivered at 0·5 Hz) was monitored from the bright-field image by an optical edge tracking method using a photodiode array (Model 1024 SAQ, Reticon) with a 3 ms time resolution (Xiao & Lakatta, 1993). In fluo-3 loaded cells, the time course of shortening was extracted off-line by tracing the cell ends in the line-scan images. tpeak was measured as the time from stimulation to peak shortening; t50 and t90 were measured as the time from the peak to 50 % and 90 % relaxation, respectively.

Electrophysiological measurements

Myocytes were either voltage or current clamped using the standard whole-cell patch-clamp technique with an Axopatch 200B patch-clamp amplifier (Axon Instruments, Inc.). Low resistance (1-2 MOmega) patch pipettes were made using a micropipette puller (Model P-97, Sutter Instrument Co.). Action potentials were evoked and recorded in current-clamp mode by injecting 4 ms current pulses with a 1·5 × threshold amplitude. The pipette solution for action potential recording consisted of (mM): KCl 140, NaCl 10, Hepes 10, MgATP 5; pH 7·2 adjusted with KOH. The superfusion solution was the Hepes buffer solution described in 'Cell isolation'.

To activate ICa selectively, membrane potential was ramped from -70 to -40 mV in 1 s and was then held at -40 mV for 100 ms to inactivate the Na+ and T-type Ca2+ channels. Potassium currents were inhibited by appropriate blockers in the pipette solution containing (mM): CsCl 100, NaCl 10, TEACl 20, Hepes 10, MgATP 5; pH 7·2 adjusted with CsOH. The extracellular solution contained the Hepes buffer solution with 0·01 mM tetrodotoxin. In a subset of experiments when the Ca2+ signal was not recorded, 10 mM EGTA was included in the pipette and the extracellular K+ was replaced by equimolar Cs+. The ICa was elicited by a depolarization from -40 to 0 mV for 300 ms and continuously followed to monitor drug effects. The amplitude of ICa was measured as the difference between the currents at the peak and at the end of the pulse. pCLAMP 6.0 software was used for bi-exponential fitting of ICa. The voltage pulses were synchronized with confocal image acquisition by a 2 ms flash from a light emitting diode on the transmission image channel.

Experimental protocols

All experiments were carried out at room temperature (22-24°C). The bathing solutions containing designated drugs were delivered locally to the target cell by gravity at a rate of 200 µl min-1 so that each solution switch occurred within 2 s. Background perfusion was maintained at a rate of 2 ml min-1 to prevent the accumulation of locally applied drugs. In addition, a subset of cells was pre-incubated with or without ICI 118,551 (ICI, 5 × 10-7 M), for 1 h at 37°C. To determine the SR Ca2+ load, 10 mM caffeine was rapidly applied via pressure injection onto the designated cell at rest, or during electrical pacing at 0·5 Hz.

Materials

Tetrodotoxin and isoproterenol hydrochloride were purchased from Sigma (St Louis, MO, USA). Ryanodine and thapsigargin were purchased from Calbiochem (La Jolla, CA, USA). ICI 118,551 was kindly supplied by Imperial Chemical Industry (UK).

Statistical analysis

Data are reported as means ± S.E.M. Student's t test was used to test for differences between TG4 and NTG groups. A paired t test was used for assessing the significance of drug effects. Analysis of variance (ANOVA) was chosen to appraise differences among NTG, TG4 and ICI-treated TG4 groups. Values of P < 0·05 were considered to be statistically significant.

  RESULTS
Top
Abstract
Introduction
Methods
Results
Discussion
References

beta2AR*-mediated positive inotropic and lusitropic effects

In the absence of any agonist, the amplitude of unloaded shortening of ventricular myocytes was greater in TG4 cells (4·97 ± 0·30 % of resting cell length, 56 cells from 18 hearts) than in NTG cells (3·02 ± 0·28 % of resting cell length, 39 cells from 15 hearts, P < 0·01) (Fig. 1A and B). This enhanced baseline contractility is beta2AR* dependent, because it was completely reversed by incubation of these cells with ICI (Fig. 1B), an inverse beta2AR agonist (also known as a negative agonist, it preferentially binds to the inactive conformation R of the receptor, shifting the equilibrium between R and R* towards R) (Bond et al. 1995). These observations are in good agreement with previous reports (Milano et al. 1994; Bond et al. 1995; Du et al. 1996; Xiao et al. 1999) and substantiate the idea that ligand-free beta2ARs possess constitutive activity, which is amplified in TG4 due to the vast overexpression of beta2ARs.

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    Figure 1. Transgenic overexpression of beta2AR induces positive inotropic and lusitropic effects in the absence of beta2AR agonist

    A, typical traces of cell shortening in ventricular myocytes isolated from non-transgenic (NTG) and transgenic (TG4) mouse hearts. The resting cell lengths were 107·8 and 126·5 µm for NTG and TG4 cells, respectively. B, mean contraction amplitudes of NTG and TG4 cells, and TG4 cells treated with ICI 118,551 (TG4-ICI). The mean resting cell lengths were 127·9 ± 3·9 µm (NTG, n = 39) and 139·1 ± 3·7 µm (TG4, n = 56). C-E, rise time (tpeak, C), half-relaxation time (t50, D) and 90 % relaxation time (t90, E) for NTG, TG4 and TG4-ICI cells. Data were obtained from 39 cells of 15 NTG hearts, 56 cells of 18 TG4 hearts, and 23 TG4-ICI cells of 9 TG4 hearts, under steady-state stimulation at 0·5 Hz. Data are presented as means ± S.E.M. *P < 0·01 vs. NTG and TG4-ICI groups, daggerP < 0·05 vs. NTG group.

In intact TG4 mice, the decline of left ventricle pressure (-dP/dt) is faster than in NTG mice, and this relaxant effect is accompanied by an approximately 50 % (Rockman et al. 1996) reduction in the abundance of PLB, which in its dephosphorylated state, inhibits the SR Ca2+ ATPase (Lindemann et al. 1983). Similarly, we found that in single TG4 myocytes, contractile relaxation was also accelerated (Fig. 1A). On average, the half-relaxation time (t50) and the 90 % relaxation time (t90) were reduced by 38 and 36 %, respectively (Fig. 1D and E), whereas no significant difference was observed in the rise time (tpeak) (Fig. 1C). For comparison, NTG myocytes have a similar maximal 30-40 % reduction in t50 after beta1AR stimulation (Korzick et al. 1997). In TG4 cells pretreated with ICI, t50 and t90 were largely restored, although t50 was still significantly briefer than that in NTG (Fig. 1D and E). These results suggest that the enhanced myocardial relaxation is attributable not only to the downregulation of PLB as proposed previously (Rockman et al. 1996), but also to acute beta2AR* signalling, presumably by protein kinase A (PKA)-dependent PLB phosphorylation. The fact that beta2AR* induces a maximal relaxation effect is somewhat surprising, because ligand-activated beta2AR signalling is dissociated from phosphorylation of PLB (Xiao et al. 1994; Altschuld et al. 1995; Kuschel et al. 1999a), and in some species, manifests only a minor relaxant effect (Xiao & Lakatta, 1993; Xiao et al. 1994; Kuschel et al. 1999a).

Enhanced Ca2+ transients in TG4 myocytes

In principle, the greater contractility of TG4 myocytes could arise from an enhanced excitation-Ca2+ release coupling that gives rise to a greater Ca2+ transient, or from an enhanced myofilament sensitivity to Ca2+, as is the case with alpha-adrenergic stimulation (Gambassi et al. 1998). To discriminate between these possibilities, we examined Ca2+ transients and contraction in cells loaded with the Ca2+ indicator fluo-3. As shown in Fig. 2B, the beta2AR*-mediated contractile effect was accompanied by an increase in the amplitude of the Ca2+ transients (indexed by peak F/F0 of fluo-3 signal). The maximal rising rate of F/F0, which roughly reflects the peak SR release flux (Sipido & Wier, 1991), was also enhanced in TG4. The background fluo-3 signal (F0) was, however, very similar in TG4 (24·9 ± 0·86, n = 38 cells) and NTG cells (25·6 ± 0·64, n = 24), suggesting similar diastolic Ca2+ concentrations in the two groups. In fluo-3-loaded cells, contractile relaxation was considerably slowed (compare Fig. 2 with Fig. 1), probably due to the Ca2+ buffering effect of the indicator. Nevertheless, the pattern remained unchanged: TG4 cells relengthened more rapidly (t50, 256 ± 13 ms; n = 15) than NTG cells (t50, 312 ± 19 ms; n = 9) (P < 0·05). A similar result was observed for the Ca2+ transient decay in these cells (t50, 146 ± 12 and 239 ± 27 ms in TG4 and NTG, respectively; P < 0·05).

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    Figure 2. Cell contraction and Ca2+ transients in cardiac myocytes loaded with fluo-3

    A, representative traces of Ca2+ transients (upper trace), represented by fluo-3 fluorescence intensity, and cell contraction (lower trace) after stimulation of a TG4 mouse myocyte after a 1 min rest. Note the negative staircase for both contraction and Ca2+ transients. B, peak amplitudes of cell contraction (left), Ca2+ transient (middle), and the maximal rising rate of the normalized fluorescence, d(F/F0)/dt (right), under steady-state conditions. NTG, n = 9 cells; TG4, n = 15. *P < 0·05 vs. NTG group. C, peak contraction amplitude (expressed as a percentage of resting cell length) plotted as a function of the peak amplitude of the Ca2+ transient (F/F0). Data were obtained from 12 NTG cells and 18 TG4 cells during the negative staircase following stimulation from rest. Slopes of the regression lines are 3·38 ± 0·18 (continuous line) and 3·23 ± 0·38 (dashed line) for TG4 and NTG, respectively.

To determine the possible effect of beta2AR* on myofilaments, we plotted the contraction amplitude as a function of the peak Ca2+ transient during the negative staircase that followed stimulation of cells from rest (Fig. 2A and C). Linear regression revealed that the slope for TG4 (3·38 ± 0·18) was not significantly different from that for NTG (3·23 ± 0·38) (Fig. 2C), suggesting that the myofilament-Ca2+ interaction is probably not altered in TG4 myocytes. Thus, beta2AR* signalling must interact with the EC coupling cascade at steps upstream of the Ca2+ transient.

Action potential and ICa

To understand Ca2+ handling in TG4 cells, we explored possibilities in two categories: the mechanisms affecting sarcolemmal Ca2+ cycling and those related to SR Ca2+ cycling. In addition to contributing directly to cytosolic Ca2+, ICa dictates SR Ca2+ release via the CICR mechanism (Fabiato, 1983), and affects the SR Ca2+ load in a more complex manner (Eisner et al. 1998). Unexpectedly, our recent study showed that the L-type channel, the key effector of agonist-elicited beta2AR signalling, is untouched by beta2AR* (Zhou et al. 1999). In agreement, we found that the ICa amplitudes were nearly identical in TG4 and NTG (806 ± 82·5 pA, n = 14 and 764 ± 63·0 pA, n = 13, respectively, at 0 mV in the presence of EGTA). The ICa kinetics were not significantly different (TG4 vs. NTG: tau1, 15·09 ± 1·12 vs. 17·74 ± 1·67 ms; tau2, 56·98 ± 2·98 vs. 61·68 ± 4·94 ms) (see also Zhou et al. 1999). While favouring the interpretation that beta2AR* signalling bypasses the ICa to augment cardiac contractility, these data do not exclude the involvement of ICa in the field-stimulated cells, because the trigger ICa may vary if the action potential configuration differs. Therefore, we recorded action potentials in TG4 and NTG cells (Fig. 3). The mean parameters in Table 1 show that TG4 and NTG cells have similar resting membrane potentials (Vrest), action potential (AP) amplitude, and time to 50 % repolarization (t50). The time to 90 % repolarization (t90) was prolonged in TG4 cells. None of these parameters, nor the entire trace of the action potentials was sensitive to ICI. Since the ICa should be deactivated at the end-stage repolarization, and since the prolonged t90 in TG4 cells was unaltered by ICI, the prolongation of t90, which might reflect long-term electrophysiological remodelling, has little relevance to altered EC coupling in TG4 cells. The exact cause, however, was not further explored in the present study.

Table 1. Mean data for action potential parameters from NTG and TG4 cells, and TG4 cells in the presence of ICI (TG4-ICI)

  Vrest
(mV)
AP amplitude
(mV)
t50
(ms)
t90
(ms)
n
NTG -70·6 ± 0·9 112 ± 4·3 8·5 ± 3·1 48·3 ± 9·1 11
TG4 -69·6 ± 0·9 123 ± 3·1 8·9 ± 1·8 104 ± 12 * 12
TG4-ICI -68·0 ± 0·7 121 ± 3·8 9·6 ± 1·9 105 ± 13 * 7
Vrest, resting membrane potential; AP, action potential; t50 and t90, time from stimulation to 50 and 90 % repolarization, respectively. Note that APs in TG4 cells have a prolonged t90 that is not altered by ICI. *P < 0·01 vs. NTG.

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    Figure 3. Effect of ICI 118,551 on properties of the action potential in TG4 myocytes

    Representative traces were recorded by whole-cell current clamping a TG4 cardiomyocyte before (control) and 10 min after exposure to ICI (5 × 10-7 M).

Having not found relevant changes in the trigger ICa and action potentials, we next focused on various aspects of SR Ca2+ regulation.

SR Ca2+ filling status

The aforementioned results on hastened Ca2+ and contractile relaxation suggest that SR Ca2+ resequestration is enhanced in TG4 cells. As pointed out by Eisner and his colleagues (Trafford et al. 1998; Eisner et al. 1998), increases in SR Ca2+ pump function would induce a delayed but sustained augmentation on the Ca2+ transient or contractility, due to the subsequent increase in SR Ca2+ filling. SR Ca2+ content is known to be an important determinant for the amplitude of elementary Ca2+ release events or 'Ca2+ sparks' (Cheng et al. 1996; Song et al. 1997; Satoh et al. 1997), the fraction of SR Ca2+ released (Spencer & Berlin, 1997; Schlotthauer et al. 1998) and possibly CICR sensitivity (Lukyanenko et al. 1996; Spencer & Berlin, 1997). To determine whether SR Ca2+ load is altered in TG4, a high concentration of caffeine (10 mM) was applied to empty the SR Ca2+ store rapidly (Fig. 4A). SR Ca2+ content, defined as the amplitude of the caffeine-elicited Ca2+ transient, was comparable in TG4 and NTG, both at rest and during steady-state field stimulation at 0·5 Hz (Fig. 4B). In both TG4 and NTG groups, the SR Ca2+ filling was slightly lower in the paced cells, consistent with another report (Li et al. 1997). The absence of alterations in SR Ca2+ content in TG4 myocytes indicates that additional changes in SR Ca2+ handling must be involved to sustain the chronic inotropic effect of beta2AR* signalling and at the same time maintain the SR loading against an enhanced SR pump function.

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    Figure 4. Measurement of SR Ca2+ content in TG4 and NTG cardiomyocytes

    A, a caffeine-elicited Ca2+ transient in a TG4 myocyte. SR filling status was determined by emptying the SR via rapid pressure injection (400 ms, bar) of 10 mM caffeine onto the cell. The peak F/F0 of the ensuing Ca2+ transient was used as an index of SR Ca2+ load. B, mean SR Ca2+ load at rest or under steady-state field stimulation (0·5 Hz) in NTG (n = 19) and TG4 (n = 12) cells.

Properties of Ca2+ sparks

In cardiac myocytes, global Ca2+ transients result from the summation of discrete elementary events, namely Ca2+ sparks originating from RyRs in the SR (Cheng et al. 1993). Characterization of Ca2+ spark properties may reveal the mechanisms responsible for altered EC coupling. Using confocal microscopy in conjunction with an automated spark detector (Cheng et al. 1999, also see Methods), we examined both spontaneous and evoked Ca2+ sparks in TG4 and NTG myocytes (Fig. 5). In resting cells, the rates of occurrence of spontaneous sparks were 7·60 ± 1·58 (n = 16) and 3·74 ± 0·90 sparks s-1 (100 µm)-1 (n = 10, P < 0·05) for TG4 and NTG, respectively. Ca2+ sparks in TG4 cells sometimes (133 out of 782 events, or 17 %) ignited neighbouring release sites, creating spatially and temporally clustered events (Fig. 5); spark clusters were less frequent in NTG cells (25 out of 280; 9 %). Regardless of beta2AR density, all Ca2+ sparks were completely abolished within 5 to 10 min of exposure of the cells to ryanodine (10 µM) plus thapsigargin (5 µM), an SR Ca2+ pump inhibitor (data not shown).

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    Figure 5. Comparison of properties of unitary Ca2+ sparks in NTG and TG4 myocytes

    A, representative confocal line-scan images of Ca2+ sparks. As indicated by the black arrows, time runs horizontally, and spatial information is displayed vertically. The white arrow in the right panel image indicates a 'seeder' event which initiates a spark cluster. Such clustered events were excluded from the measurement of unitary spark properties. Each cluster was counted as one primary event when measuring the rate of spontaneous spark occurrence (see Methods). B-E, histograms of spark amplitude (F/F0, B), full width (FWHM, C) and duration (FDHM, D) at half-maximum, and signal mass (E). A total of 280 and 782 sparks were detected from 10 NTG and 16 TG4 cells, respectively. Events with amplitudes larger than 2·5 or durations longer than 130 ms or signal masses greater than 125 µm ms are omitted in the related plots.

Similarly, when membrane potential was held at -40 mV after a ramp from -70 mV, the evoked Ca2+ sparks occurred at a 3-fold higher frequency in TG4 (36·4 ± 9·1 sparks (100 ms)-1 (100 µm)-1, 12 images from 3 cells; estimated from the signal mass; see Methods) than in NTG cells (12·8 ± 2·1 sparks (100 ms)-1 (100 µm)-1, 12 images from 3 cells; P < 0·05 vs. TG4). ICI treatment to inactivate beta2AR* reduced the evoked spark frequency nearly 7-fold to 5·22 ± 1·9 sparks (100 ms)-1 (100 µm)-1 (P < 0·01 vs. control) (see Fig. 6). Since ICa and the resting Ca2+ were similar in TG4 and NTG, these results suggest that CICR sensitivity, operationally defined as the number of sparks activated by a given amount of trigger Ca2+, was augmented 2- to 7-fold in TG4 cells.

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    Figure 6. Simultaneous recordings of ICa, intracellular Ca2+ and cell length in a representative TG4 ventricular myocyte

    From top to bottom: confocal line-scan image of fluo-3 fluorescence, voltage-clamp protocol, spatially averaged fluo-3 fluorescence transient (F/F0), shortening of cell length and ICa. Data were recorded immediately before (left), or 5 min after (middle) application of the beta2AR inverse agonist ICI 118,551, and 5 min after washout of ICI (wash). Note that ICI markedly and reversibly inhibits the contraction and the Ca2+ transient with a profound reduction in Ca2+ spark frequency, but has no effect on the simultaneously recorded ICa. Similar results were obtained from 3 cells.

Figure 5B-E shows histogram distributions of properties of unitary Ca2+ sparks. Compared with those in NTG cells, Ca2+ sparks in TG4 were enlarged in all dimensions, including amplitude (mean F/F0, 1·61 vs. 1·43), spatial width (FWHM, 1·81 vs. 1·52 µm), and duration (FDHM, 45·9 vs. 25·8 ms). As a result, the integral of DeltaF/F0 in space-time or signal mass was increased from 15·8 µm ms in NTG to 36·4 µm ms in TG4. Interestingly, a long tail was evident in the F/F0, FDHM and signal mass plots for TG4, but was absent in NTG plots. This suggests that TG4 cells have a novel population of events: those with F/F0 > 1·80 (84 events; 13 %), or FDHM > 70 ms (98 events; 15 %), or signal mass > 65 µm ms (100 events; 15 %). These large events account for 50 % of the increases in unitary spark parameters, and suggest that beta2AR* signalling may increase local release flux. These local increases in Ca2+ flux could be the result of recruiting more RyRs within the release unit, longer RyR openings, or an increase in local CICR endurance. Thus, increases in both spark size and frequency contribute to the greater Ca2+ transients in TG4.

Simultaneous recordings of ICa, Ca2+ sparks, Ca2+ transients and contraction

To monitor simultaneously the main events of EC coupling in the same cell, we employed confocal imaging combined with whole-cell voltage clamping. Representative results from a TG4 cell are shown in Fig. 6, displaying, from top to bottom, line-scan images of intracellular Ca2+, membrane potential, spatially averaged Ca2+ transients, cell shortening and whole-cell ICa. ICI markedly and reversibly suppressed the cell-wide Ca2+ transient (F/F0 from 5·46 ± 0·18 to 2·44 ± 0·1, n = 3, P < 0·05), contraction (from 12·6 ± 2·3 to 2·45 ± 0·68 % of resting length, n = 3, P < 0·01), and Ca2+ sparks prior to the transients. Notably, the kinetics of both the Ca2+ transient and contraction slowed in the presence of ICI (Fig. 6). In contrast, the amplitude of ICa recorded simultaneously in the same cells was unaffected by ICI (from -616 ± 18 to -675 ± 88 pA, n = 3, P > 0·05), although there was a slight slowing in the fast inactivation time constant of ICa (tau1) (from 12·67 ± 1·24 to 16·14 ± 1·91 ms, n = 3, P < 0·05). The slowing of tau1 by ICI, which reduced SR Ca2+ release, is consistent with the Ca2+-dependent inactivation of the L-type channel reported previously (Sham, 1997). Control experiments performed in NTG cells using the same protocol revealed only minor effects of ICI on basal contractility, Ca2+ transient, ICa amplitude, and Ca2+ spark frequency at -40 mV (93·8 ± 6·2 %, 91·9 ± 2·2 %, 97·8 ± 1·2 % and 91·4 ± 4·9 %, respectively, n = 3), consistent with previous observations (Xiao et al. 1999; Zhou et al. 1999). Taken together, these data strongly support the notion that beta2AR*-mediated signalling does not regulate ICa; instead, it reinforces excitation-Ca2+ release coupling and promotes SR Ca2+ reuptake.

  DISCUSSION
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Abstract
Introduction
Methods
Results
Discussion
References

A novel cellular mechanism regulating cardiac EC coupling

Ligand-independent, spontaneous activation of beta2AR overexpressed in mouse cardiomyocytes produces positive inotropic and lusitropic effects, even in the absence of any related changes in action potential, ICa, SR Ca2+ content, or myofilament Ca2+ sensitivity. In contrast, Ca2+ spark frequency and solitary signal mass are grossly increased, resulting in enhanced SR release and greater global Ca2+ transients in TG4 myocytes. The efficiency of SR Ca2+ recycling, as reflected by the kinetics of the Ca2+ transient and contraction, is enhanced concomitantly in the presence of beta2AR*. Based on these findings, we propose a simple mechanistic model to explain beta2AR*-mediated modulation of cardiac EC coupling (Fig. 7). In this model, beta2AR* reinforces the CICR and the ability of the SR to recycle the released Ca2+, while not necessarily affecting the sarcolemmal Ca2+ influx and efflux. The resultant Ca2+ transient and contraction are both characterized by increased amplitudes, but a compressed relaxation time course. Since beta2AR* activates adenylyl cyclase (Milano et al. 1994) and increases cAMP production (Zhou et al. 1999) in an ICI-sensitive manner, and since the blockade of the PKA activation (by inhibitory cAMP analogues) mimics the effect of ICI to reverse beta2AR*-induced augmentation in cell contraction (Zhou et al. 1999), the beta2AR* signalling is most probably mediated by a cAMP/PKA-dependent protein phosphorylation, as is the case with ligand-elicited betaAR stimulation.

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    Figure 7. A simplified model of beta2AR*-mediated modulation of cardiac EC coupling

    beta2AR* enhances SR Ca2+ release without altering the action potential (AP) and the sarcolemmal Ca2+ fluxes. At the same time, the SR Ca2+ recycling is similarly enhanced, to balance the SR efflux. The resulting Ca2+ transient has a greater amplitude but a compressed time course. The overall Ca2+ extrusion during a complete cardiac cycle is also unchanged, in balance with the sarcolemmal Ca2+ influx. The beta2AR inverse agonist ICI 118,551 blocks the effects of beta2AR* by stabilizing the receptor in an inactive conformational state.

Eisner and his colleagues (Trafford et al. 1997, 1998; Eisner et al. 1998) demonstrated that targeting RyRs to alter CICR is insufficient to evoke a substantial long-lasting Ca2+ or inotropic response. For instance, an increase in SR Ca2+ release by low dose caffeine leads only to a brief increase in Ca2+ transients because cardiac Ca2+ autoregulation can compensate for the primary change by depleting SR Ca2+ load. In contrast, a single perturbation of the sarcolemmal Ca2+ influx or efflux may permanently alter Ca2+ and contractile performances. Theoretical analysis suggested that the sustained effect is linked to an altered SR Ca2+ load (Eisner et al. 1998). To this end, our finding in TG4 ventricular myocytes illustrates a previously unidentified scenario: synchronous increases in SR release and reuptake, when acting in concert, can support a marked, chronic positive inotropic effect. Neither an increase in the ICa nor an alteration in the SR Ca2+ load is obligatory to the enhanced contractility (Fig. 7).

The aforementioned results in this transgenic model suggest that SR Ca2+ recycling, independent of sarcolemmal Ca2+ fluxes, constitutes an important determinant of cardiac contractility. In this regard, it is noteworthy that alterations of SR Ca2+ recycling in TG4 myocytes appear to mirror those in the failing heart, in which a depressed Ca2+ transient and contractility are accompanied by a decreased ICa to Ca2+ spark coupling efficiency (Gómez et al. 1997), reduced SR Ca2+ ATPase expression (e.g. Arai et al. 1993), slowed Ca2+ transient and contraction (e.g. Gómez et al. 1997), but without evident change in ICa density (e.g. Gómez et al. 1997).

beta2AR* modulates RyR channel activity in situ

RyR, the SR Ca2+ release channel, is phosphorylated by PKA during beta-adrenergic stimulation (Yoshida et al. 1992; Hohenegger & Suko, 1993). Phosphorylation of RyR increases the probability of channel opening and promotes Ca2+ release from the SR (Hain et al. 1995; Lokuta et al. 1995). In agreement with these reports, we found that beta2AR* signalling exerts a profound effect on RyR activity and thereby on CICR sensitivity in situ. In TG4 cells, Ca2+ sparks are larger and occur more frequently than those in NTG myocytes, despite the fact that the resting cytosolic Ca2+, the SR Ca2+ load, and the triggering ICa are unaltered. These data suggest that beta2AR*-mediated cAMP/PKA signalling directly modulates the RyR channel molecules to alter their Ca2+ sensitivity or release-linked inactivation (Sham et al. 1998). We therefore conclude that RyR, in addition to the L-type channel, PLB and contractile myofilaments, constitutes an important target protein for betaAR signalling in intact cardiac myocytes. This conclusion is consistent with previous observations that the non-selective betaAR agonist isoproterenol promotes spontaneous Ca2+ sparks in rat ventricular myocytes (Tanaka et al. 1997).

Fidelity of coupling between the L-type channel and RyR

On the molecular level, EC coupling is essentially a tale of two molecules, the L-type channel and RyR, communicating over the nanometre space of the T-tubule-SR junction. L-type channels open and close stochastically, and trigger the associated RyRs in an all-or-none manner to generate Ca2+ sparks. The 'digital' coupling fidelity, delta, is here defined as the ratio of the number of L-type channel openings to the number of Ca2+ sparks activated. To accommodate the 7-fold reduction in the frequency of evoked sparks at -40 mV by the beta2AR* blockade, delta must be far greater than 1:1 under normal conditions. That is, in contrast to the numerical results of Cannell & Soeller (1997), L-type channel opening is not always followed by RyR activation, i.e. only one in several openings triggers an SR release event.

This point may be better appreciated by examining the macro- and microscopic properties of the ICa and SR Ca2+ release. Let iL, tauL, iS and tauS stand for unitary flux and mean duration of L-type channel opening and elementary SR release, respectively. The ratio of mean unitary fluxes of L-type channel and of Ca2+ spark (rho), which reflects the gain of microscopic coupling if delta = 1:1, is then given by:

eq02

Assuming iS = 3 pA, tauS = 10 ms (Cheng et al. 1993), iL = 260 fA (at -40 mV, scaling factor of 2 for 10 vs. 1 mM Ca2+ as the charge carrier) or 130 fA (at 0 mV), and tauL = 0·3 ms (Rose et al. 1992; Sham et al. 1998), the value of rho would be as low as 1:385 (at -40 mV) or 1:770 at (0 mV). Previous studies on the gain of macroscopic EC coupling (g = rhodelta) have established that g equv 60 at -40 mV and g equv 15 at 0 mV (Wier et al. 1994; Song et al. 1998). Combined with the microscopic measurements described above, this translates into a value of delta to the order of 6·4:1 (at -40 mV) to 51:1 (at 0 mV), though the latter might be overestimated because of a significant (1/3) SR depletion at 0 mV (Sham et al. 1998). The higher fidelity (i.e. smaller delta ratio) at -40 mV associated with the larger unitary current (iL) at this voltage is consistent with the 'local control' theory (Wier et al. 1994; Santana et al. 1996) and the non-linear dependence of the occurrence of evoked Ca2+ sparks on the triggered Ca2+ (Santana et al. 1996).

A similar time course for spark generation and L-type Ca2+ channel openings has been observed in wild-type rat and guinea-pig ventricular myocytes, under the conditions when SR Ca2+ release is small (Cannell et al. 1995; Lopez-Lopez et al. 1995; Santana et al. 1996; Collier et al. 1999) and the release-linked RyR inactivation (Sham et al. 1998) is negligible. Thus, spark probability at a given voltage can be described by a power function of ICa with a power of unity, supporting the idea that an individual Ca2+ spark is triggered by a single L-type Ca2+ channel opening (Cannell et al. 1995; Lopez-Lopez et al. 1995; Santana et al. 1996; Collier et al. 1999). Since the ratio delta would affect only the coefficient of the power function, the close temporal relationship described above does not contradict our conclusion that the coupling fidelity is far from 1:1 under normal conditions. Rather, it suggests that delta is essentially time independent during a voltage pulse.

This low digital coupling fidelity indicates that a large reserve capacity resides in the coupling between L-type channels and RyRs. As shown in TG4 mice, facilitation of 'cross-talk' between the L-type channels and RyRs can substantially augment cardiac inotropy, an effect beneficial during stress and excise. However, it should be pointed out that an extremely high CICR sensitivity could be detrimental, because it would create a lot of RyR-RyR 'side-talk' (spark clusters), which would put the system at risk of falling into a regime of instability (generation of Ca2+ waves, all-or-none Ca2+ transients, etc.).

Intracellular sorting of receptor signalling

The present report provides new evidence for the precision of intracellular sorting of receptor-mediated transmembrane signalling. In adult TG4 myocytes, beta2AR* signalling regulates proteins in the SR (i.e. RyR and PLB) but is diverted from the L-type Ca2+ channel in the sarcolemma (Fig. 6 and Zhou et al. 1999). Conversely, ligand-elicited beta2AR signalling, which has no known effector in the cytoplasm, appears to be strictly localized to sarcolemmal microdomains in several mammalian species (Xiao et al. 1994; Altschuld et al. 1995; Zhou et al. 1997; Kuschel et al. 1999a,b). Moreover, in cultured embryonic/neonatal TG4 cells, beta2AR* specifically increases ICa, but not cAMP-sensitive K+ currents (An et al. 1999). A common thread among these observations is that receptor-mediated signalling is highly compartmentalized and target-protein specific, depending on the conformational state of the receptor or even the developmental status of the cell. This compartmentalization of receptor signalling may help to explain a general enigma in receptor physiology: how do vast numbers of G-protein-coupled receptors converge on a limited portfolio of intracellular messenger molecules (e.g. cAMP, inositol 1,4,5-triphosphate, Ca2+), but at the same time, retain a high degree of signalling diversity and specificity? Future studies are required to elucidate the specific mechanisms underlying the precise sorting of receptor signals.

Regarding the interaction between betaAR and its effector proteins, Muth et al. (1999) recently showed that cardiac specific overexpression of the alpha1 subunit of L-type Ca2+ channels curtails isoproterenol-induced contractile and ICa responses, without altering betaAR receptor density. Complementary to this finding, beta2AR*, while bolstering contractility, fails to modulate ICa (Zhou et al. 1999 and this study), indicating that the usual signalling routed toward the L-type channel is non-existent or disrupted when the receptor is overexpressed. These results suggest a novel bi-directional regulation between the receptor and its effector, which merits further investigation.

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Discussion
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Acknowledgements

The authors wish to thank Drs Walter J. Koch and Robert J. Lefkowitz for their generous supply of the transgenic mice; Dr Harold Spurgeon, Dr Sheng-Jun Zhang and Mr Bruce Ziman for their excellent technical support.

Corresponding author

H. Cheng: Laboratory of Cardiovascular Science, Gerontology Research Center, National Institute on Aging, National Institutes of Health, 5600 Nathan Shock Drive, Baltimore, MD 21224, USA.

Email: chengp{at}grc.nia.nih.gov




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C. G. Tocchetti, W. Wang, J. P. Froehlich, S. Huke, M. A. Aon, G. M. Wilson, G. Di Benedetto, B. O'Rourke, W. D. Gao, D. A. Wink, et al.
Nitroxyl Improves Cellular Heart Function by Directly Enhancing Cardiac Sarcoplasmic Reticulum Ca2+ Cycling
Circ. Res., January 5, 2007; 100(1): 96 - 104.
[Abstract] [Full Text] [PDF]


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Am. J. Physiol. Heart Circ. Physiol.Home page
S. A. Grandy and S. E. Howlett
Cardiac excitation-contraction coupling is altered in myocytes from aged male mice but not in cells from aged female mice
Am J Physiol Heart Circ Physiol, November 1, 2006; 291(5): H2362 - H2370.
[Abstract] [Full Text] [PDF]


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Circ. Res.Home page
F. Zhang, J. Cheng, G. Lam, D. K. Jin, L. Vincent, N. R. Hackett, S. Wang, L. M. Young, B. Hempstead, R. G. Crystal, et al.
Adenovirus Vector E4 Gene Regulates Connexin 40 and 43 Expression in Endothelial Cells via PKA and PI3K Signal Pathways
Circ. Res., May 13, 2005; 96(9): 950 - 957.
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Am. J. Physiol. Heart Circ. Physiol.Home page
A. M. Gomez, I. Schuster, J. Fauconnier, J. Prestle, G. Hasenfuss, and S. Richard
FKBP12.6 overexpression decreases Ca2+ spark amplitude but enhances [Ca2+]i transient in rat cardiac myocytes
Am J Physiol Heart Circ Physiol, November 1, 2004; 287(5): H1987 - H1993.
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Am. J. Physiol. Heart Circ. Physiol.Home page
S. A. Grandy, E. M. Denovan-Wright, G. R. Ferrier, and S. E. Howlett
Overexpression of human {beta}2-adrenergic receptors increases gain of excitation-contraction coupling in mouse ventricular myocytes
Am J Physiol Heart Circ Physiol, September 1, 2004; 287(3): H1029 - H1038.
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Cardiovasc ResHome page
L. Barki-Harrington, C. Perrino, and H. A Rockman
Network integration of the adrenergic system in cardiac hypertrophy
Cardiovasc Res, August 15, 2004; 63(3): 391 - 402.
[Abstract] [Full Text] [PDF]