The burbot (Lota lota) is a cold stenothermic fish species whose heart is adapted to function in the cold. In this study we use whole-cell voltage-clamp techniques to characterize the electrophysiological properties of burbot ventricular myocytes and to test the hypothesis that changes in membrane currents and intracellular Ca2+ cycling associated cold-acclimation in other fish species are routine for stenothermic cold-adapted species. Experiments were performed at 4°C, which is the body temperature of burbot for most of the year, and after myocytes were acutely warmed to 11°C, which is in the upper range of temperatures experienced by burbot in nature. Results on K+ channels support our hypothesis as the relative density of K-channel conductances in the burbot heart are similar to those found for cold-acclimated cold-active fish species. IK1 conductance was small (39.2±5.4 pS pF-1 at 4°C and 71.4±1.7 pS pF-1 at 11°C)and IKr was large (199±27 pS pF-1 at 4°C and 320.3±8 pS pF-1 at 11°C) in burbot ventricular myocytes. We found high Na+-Ca2+ exchange(NCX) activity (35.9±6.3 pS pF-1 at 4°C and 58.6±8.4 pS pF-1 at 11°C between -40 and 20 mV),suggesting that it may be the primary pathway for sarcolemmal (SL)Ca2+ influx in this species. In contrast, the density(ICa, 0.81±0.13 pA pF-1 at 4°C, and 1.35±0.18 pA pF-1 at 11°C) and the charge(QCa, 0.24±0.043 pC pF-1 at 4°C and 0.21±0.034 pC pF-1 at 11°C) carried by the l-type Ca2+ current was small. Our results on sarcolemmal ion currents in burbot ventricular myocytes suggest that cold stenothermy and compensative cold-acclimation involve many of the same subcellular adaptations that culminate in enhanced excitability in the cold.

Ectotherms are able to acclimatize to different temperatures, adjusting physiological and biochemical processes to meet the demands of their environment. Acclimatization of the heart is especially important as cardiac output must match the changes in activity level, metabolic rate and blood viscosity that occur with changes in temperature. The effects of temperature acclimation on cardiac contractility in ectotherms are well documented(Keen et al., 1994; Shiels and Farrell, 1997; Aho and Vornanen, 1999) (for a review, see Driedzic and Gesser,1994). More recent work has focused on elucidating adaptations in cardiac myocyte excitability (Vornanen et al., 2002a; Paajanen and Vornanen, 2004), cellular Ca2+ cycling(Hove-Madsen and Tort, 1998; Hove-Madsen et al., 1998; Harwood et al., 2000, Shiels et al., 2000; Shiels et al., 2002a; Shiels et al., 2002b; Hove-Madsen et al., 2003) and protein structure (Yang et al.,2000; Gillis et al.,2000; Gillis et al.,2003) associated with maintained cardiac viability in the cold(for reviews, see Vornanen et al.,2002b; Gillis and Tibbits,2002). Although some ectotherms cope with cold temperatures via cold-torpor and resultant reductions in metabolic rate and heart rate, there are several compensative changes often associated with ectotherms that remain active in the cold. These include an increase in relative ventricular mass, possibly to offset increased blood viscosity(Goolish, 1987; Graham and Farrell, 1989), a proliferation of the sarcoplasmic reticulum (SR)(Bowler and Tirri, 1990)suggesting increased reliance on intracellular Ca2+ cycling during excitation-contraction coupling (Keen et al., 1994; Shiels and Farrell,1997; Aho and Vornanen,1999; Tiitu and Vornanen,2002b) and changes in K+ channel conductances that decrease action potential duration (APD) ensuring myocyte excitability in the cold (Vornanen et al., 2002a; Paajanen and Vornanen,2004).

Some ectothermic animals do not tolerate large seasonal increases in temperature, and therefore inhabit a cold stenothermic environment. Fish species such as the burbot Lota lota, are cold stenotherms spending most of their life at temperatures between 1°C and 7°C, and are rarely found in waters above 13°C (Carl,1995). Burbot are benthic, and are sluggish swimmers but are cold-active, spawning in winter under ice-covered lakes(Pääkkönen and Marjomäki, 2000). Examination of burbot heart morphology and contractility suggests that the changes normally associated with cold-acclimation in active species such as rainbow trout (Oncorhynchus mykiss), may be routine for cold-adapted species. The relative ventricular mass of the burbot (∼0.15% body mass) is elevated in comparison with most eurythermal species (∼0.08% body mass)(Tiitu and Vornanen, 2002a). Both atrial and ventricular muscle isolated from burbot heart exhibit increased ryanodine-sensitivity of contraction, suggesting that the SR may be routinely involved in delivering Ca2+ to the myofilaments during force development (Tiitu and Vornanen,2002b). Furthermore, [3H]ryanodine binding to cardiac preparations from burbot and rat show similar Ca2+-dependent activation of the SR Ca2+ release channel, suggesting that Ca2+-induced Ca2+-release (CICR) may operate during excitation-contraction coupling in this species(Vornanen, 2006). Collectively, these results suggest that many of the subcellular changes that are required to maintain cardiac function during cold acclimation may also play a role in long-term cold adaptation. However, at present no studies have examined excitation-contraction coupling at the level of the myocyte in the burbot or any cold stenothermic species.

In this study, we investigated the electrophysiological properties of burbot ventricular myocytes at 4°C, which is the typical habitat temperature of this species for most of the year. We also examined electrophysiological parameters after acutely warming the myocytes to 11°C because we were interested in how excitation-contraction coupling in the stenothermic heart is modulated during acute temperature change and because 11°C is approaching the upper temperature at which this species is found(Carl, 1995; Pääkkönen and Marjomäki, 2000). We first set out to measure APs and the major sarcolemmal (SL) ion currents involved in regulating myocyte excitability and maintaining electrical stability in the cold. Next, to investigate possible changes in cellular Ca2+ dynamics in a cold-adapted species we examined SR Ca2+ accumulation and release using caffeine. We assumed that if the changes found in rainbow trout and other active teleosts under cold-acclimation were adaptive, then, through evolutionary processes, similar changes may be permanent in the genome of cold stenothermic fish. First, we hypothesized that reorganisation of K+currents would occur with a shift from the dominance of the inward rectifier K current (IK1) in favour of the delayed rectifier K+ current (IKr)(Vornanen et al., 2002a). Second, we expected that intracellular Ca2+ stores of the SR would make a significant contribution to excitation-contraction coupling(Tiitu and Vornanen, 2002b)and appear as accelerated decay of the l-type Ca2+current (ICa) (Shiels et al., 2002b). In agreement with the first hypothesis, IK1 was small and IKr large in ventricular myocytes of the burbot heart. However, we did not find evidence of increased SR Ca2+ involvement in our measurements of ICa inactivation. Rather, we report an increase in SL Na+-Ca2+ exchange (NCX) activity, which we suggest is the primary pathway for SL Ca2+ influx in this species.

Fish origin and care

Sexually mature burbot Lota lota L. (body mass 224.6±12.7 g, N=22) of both sexes were caught during spawning time from Lake Orivesi (62°30′N) in Finland. In the laboratory fish were held in 500 liter stainless steel tanks at 4°C with continuous circulation(approximately 0.5 l min-1) of aerated groundwater. Fish were fed with dead vendace (Coregonus albula) three times a week. Photoperiod was 15 h:9 h dark:light.

Myocyte isolation

All procedures were in accordance with local animal handling protocols. A detailed description of myocyte preparation has been previously published for other fish species (Vornanen,1997; Shiels et al.,2000). Briefly, fish were stunned with a blow to the head, the spine was cut just behind the brain and the heart was excised. The heart was then perfused first with an isolating solution for 8-10 min, and then with a proteolytic enzyme solution for 15 min at ∼15°C. After enzymatic treatment, the ventricle was placed in isolating solution, cut into small pieces with scissors and then triturated through the opening of a Pasteur pipette to free individual myocytes. The myocytes were stored in fresh isolating solution at 4°C and used within 8 h.

Solutions

The isolating solution contained (mmol l-1): NaCl 100, KCl 10,KH2PO4 1.2, MgSO4 4, taurine 50, glucose 20,and Hepes 10, adjusted to pH 6.9 with KOH. For enzymatic digestion,collagenase (Type IA from Sigma, St Louis, MI, USA; 0.75 mg ml-1),trypsin (Type IX from Sigma; 0.5 mg ml-1) and fatty acid-free bovine serum albumin (BSA, from Sigma; 0.75 mg ml-1) were added to this solution.

The external solution used for measuring ventricular action potentials (AP)contained (mmol l-1): NaCl 150, KCl 3, MgSO4 1.2,NaH2PO4 1.2, CaCl21.8, glucose 10 and Hepes 10, adjusted to pH 7.6 with NaOH. The external solution used for measuring K+ currents contained (mmol l-1): NaCl 150, KCl 5.4,CaCl2 1.8, MgCl2 1.2, glucose 10 and Hepes 10, adjusted to pH 7.6 with NaOH at 20°C. Specific inhibition of the rapid component of the delayed rectifier K+ current (IKr) was accomplished with E-4031 (1 μmol l-1; Alomone Labs Ltd,Jerusalem, Israel). The external solution used for measuring Na+-Ca2+ exchange current (INCX) and l-type Ca2+ current (ICa) contained(mmol l-1): NaCl 150, CsCl 5.4, MgSO4 1.5,NaH2PO4 0.4, CaCl2 1.8, glucose 10 and Hepes 10, adjusted to pH 7.6 with CsOH. Unless otherwise stated, 0.5 μmol l-1 TTX (Tocris Cookson, Bristol, UK), 10 μmol l-1nifedipine and 100 μmol l-1 ouabain (both from Sigma) were included to block Na+ channels, l-type Ca2+channels and Na+/K+ ATPase, respectively, when recording INCX. Nifedipine and ouabain were omitted when recording ICa.

The pipette solution used during K+ current experiments contained (mmol l-1): KCl 140, MgATP 4, MgCl2 1, EGTA 5 and Hepes 10, adjusted to pH 7.2 with KOH. Pipette solutions for measurement of INCX contained (mmol l-1): CsCl 140,MgCl2 1, CaCl2 9, BAPTA 20, Na2ATP 5,Na2GTP 0.03 and Hepes 10, adjusted to pH 7.2 with CsOH at 20°C. The free intracellular Ca2+ concentration of this solution was calculated (MaxChelator) to be 179.5 and 186.6 nmol l-1 at 4°and 11°C, respectively. Under these conditions, intracellular calcium is buffered to a diastolic level. In some experiments, we investigated the effect of using a lower level of Ca2+ buffering on INCX by replacing BAPTA with 0.025 mmol l-1EGTA. ICa was initially characterised with pipettes containing (mmol l-1): CsCl 130, MgATP 5, tetraethylammonium chloride (TEA) 15, MgCl2 1, oxaloacetate 5, EGTA 5,Na2GTP 0.03 and Hepes 10 adjusted to pH 7.2 with CsOH. In latter experiments ICa and SR Ca2+ loading were assessed using the same pipette solution except that EGTA concentration was decreased from 5 mmol l-1 to 0.025 mmol l-1 to better mimic in vivo cytosol Ca2+ buffering(Hove-Madsen and Tort, 1998). Steady-state kinetics parameters of ICa were obtained by fitting activation and inactivation data to Boltzman functions to determine the half-activating, half-inactivating potentials (Vh) and the slope (k) of activation and inactivation, as previously described(Vornanen, 1998).

Experimental procedures

Intracellular APs were measured from spontaneously beating whole-heart preparations at 4°C and 11°C as described previously(Vornanen, 1996). Briefly, the excised ventricle was medially opened, spread and secured on the bottom of a 10 ml tissue chamber filled with oxygenated saline. Ventricular APs were recorded using high-resistance microelectrodes (30-60 MΩ when filled with 3 mol l-1 KCl) fabricated from borosilicate glass (World Precision Instruments, 1BBL, Sarasota, FL, USA) with a two-stage horizontal puller (Campden Instruments Ltd, UK). Microelectrode signals were recorded using a high-impedance amplifier (KS-700, WPI, Sarasota, FL, USA), digitized(DigiData 1200, Axon Instruments, Foster City, CA, USA) and stored to a computer using Axotape 2.2 acquisition software and then analysed offline(Clampfit, Axon Instruments). The time course of contraction was recorded simultaneously with APs by attaching one corner of the ventricle to a force transducer (FT03 Grass Instruments, West Warwick, RI, USA) by a small metal hook and braided silk thread. Muscle was slightly tensioned and the force signal was amplified by a Grass 7D polygraph amplifier and fed through the digitizer to the computer for later off-line analysis.

Stimulation, acquisition and analysis of ventricular myocyte whole-cell voltage and current signals was achieved using established methods(Vornanen, 1997; Shiels et al., 2000; Paajanen and Vornanen, 2002)on either an Axopatch 1D amplifier in conjunction with pClamp 8.2 and Clampfit software, or on an EPC-9 amplifier in conjunction with Pulse 6.3 and Pulsefit software (Heka, Lambrecht, Germany). Myocytes (capacitance 23.7±0.5 pF, N=179 cells) were placed in the recording chamber (RCP-10T, Dagan,Maryland, MI, USA, volume 500 μl or RC-26, Warner Instruments Corp. Brunswick, Handen, CT, USA, volume 150 μl) and were superfused continuously with external saline at the rate of 1.5-2 ml min-1. The temperature of the saline was regulated at either 4±1°C or 11±1°C by circulating water baths or a Peltier device. Bath temperature was continuously monitored by thermocouples positioned no less than 5 mm from the cell under investigation. Patch electrodes were pulled from borosilicate glass (Garner F-78045, Claremont, CA, USA) with a two-stage vertical puller (L/M-3P-A, List Medical, Darmstadt, Germany). The resistance of the electrodes was 2-4 MΩ when filled with pipette solutions. Pipette and whole cell capacitances were routinely compensated, and access resistance was recorded but not compensated. Currents were filtered at 2.0 kHz using either a 4-pole or a 8-pole Bessel filter.

During SR Ca2+ loading and release experiments, rapid (∼50 ms) application of caffeine and/or channel inhibitors was achieved by switching between temperature controlled barrels of a rapid solution changer(RS200, Biologic, Claix, France). CdCl2 (100 μmol l-1) or a combination of CdCl2 (30 μmol l-1) and verapamil (10 μmol l-1) was used to rapidly block ICa.. NiCl2 (10 mmol l-1) was used to inhibit the NCX. SR Ca2+ content was assessed by the application of caffeine (10 mmol l-1), which induces the release of Ca2+ from the SR. This Ca2+ is then extruded from the cell via the NCX generating an inward current (see Results), which is directly proportional to the Ca2+ released from the SR(Varro et al., 1993). The time integral of this caffeine-induced INCX current was used to calculate the SR Ca2+ content (in pC) at the time of caffeine application. This value was expressed per unit capacitance (pC pF-1). SR Ca2+ content was also expressed in μmol Ca2+ l-1 non-myofibrillar cell volume [40% as determined previously (Vornanen, 1998)]. Cell volume was calculated from cell surface area, obtained by measurements of cell capacitance (pF) and assuming a specific membrane capacitance of 1.59μF cm-2, and a surface-to-volume ratio of 1.15.

Details of the voltage clamp waveforms and protocols used to study the electrophysiological properties of whole-cell currents are provided in the results and the figures. When values are presented as means, the number of observations (N) and statistical significance are provided in the text or appropriate figure legend.

Action potential characteristics in burbot ventricular myocytes

At 4°C the beating frequency of the burbot heart was 17.98±0.36 contractions min-1 (N=10) (0.3 Hz). The duration of contraction and AP closely matched and were slightly less than 2 s at 4°C(Fig. 1). The close match between AP duration (APD) and the duration of contraction suggest that the activation and relaxation of cardiac twitch are governed by membrane potential. Peak ventricular force occurred when the AP had repolarised to about -20 mV. The resting membrane potential (RMP) and AP overshoot were-70.4±1.1 mV and 14.4±0.7 mV, respectively (N=10). AP duration at plateau (0 mV), and at 50, 90 and 100% repolarisation was 292±48, 1108±28, 1544±29 and 1830±46 ms,respectively (N=10). At 11°C, RMP and AP overshoot were-75.0±1.8 and 15.8±1.2 mV, respectively, whereas corresponding values of AP duration were 250±44, 771±39, 1159±61 and 1313±72 ms at 0 mV, and at 50, 90 and 100% repolarisation, respectively(N=12). The APD was significantly shorter at 11°C than 4°C with APD at 90% repolarization (APD90) values of 1091±179 and 1594±16 ms, respectively (P<0.0002). Absolute force decreases with increasing temperature (Fig. 1). This was a regular finding and has been quantitatively reported previously (see Tiitu and Vornanen, 2002b).

Fig. 1.

Representative recordings of ventricular action potentials and associated contractions of the burbot ventricle at 4°C and 11°C. Scale bars are for recordings at both temperatures. Force of contraction is in arbitrary units.

Fig. 1.

Representative recordings of ventricular action potentials and associated contractions of the burbot ventricle at 4°C and 11°C. Scale bars are for recordings at both temperatures. Force of contraction is in arbitrary units.

K+ currents in burbot ventricular myocytes

The two main K+ currents in burbot ventricular myocytes are the background inward rectifier (IK1) and the rapid component of the delayed rectifier current (IKr). The conductance of IK1, which is the major K+ current in ventricular myocytes of most vertebrate species, was surprisingly low in burbot myocytes (39.2±5.4 pS pF-1 at 4°C; Fig. 2A). Even at 11°C, IK1 conductance of the burbot ventricular myocyte was only 71.4±1.7 pS pF-1. In contrast, the size of IKr was large. At 4°C, the maximum density of the E4031-sensitive (1 μmol l-1) tail current was 2.9±0.3 pA pF-1 (Fig. 2B). When temperature was increased to 11°C, current density increased to 3.8±1.1 pA pF-1 (P=0.04) and caused a 15 mV shift(P=0.04) of the current-voltage relation to hyperpolarising voltages. The slope conductance of IKr was 199±27 and 320±8 pS pF-1 at 4°C and 11°C, respectively, i.e. 4.5-5 times that of the IK1.

Fig. 2.

The two major K+ currents in burbot ventricular myocytes. (A)Background inward rectifier K+ current, IK1. Values are means ± s.e.m. from 6-8 cells at 4°C (black circles) and 11°C (white circles) measured at the beginning of 500 ms square wave pulses that were elicited from the holding potential of -80 mV to voltages between -120 and 40 mV in 20 mV steps (inset). (B) Delayed rectifier K+ current, IKr, measured as an outward tail current at -40 mV after 5 s depolarising pulses between -80 and 80 mV (inset). Representative recordings at 4°C and mean values (± s.e.m.) from 5-10 cells at 4°C (black circles) and 11°C (white circles). *Density of IKr is increased significantly by acute warming to 11°C (Student's t-test, P<0.005).

Fig. 2.

The two major K+ currents in burbot ventricular myocytes. (A)Background inward rectifier K+ current, IK1. Values are means ± s.e.m. from 6-8 cells at 4°C (black circles) and 11°C (white circles) measured at the beginning of 500 ms square wave pulses that were elicited from the holding potential of -80 mV to voltages between -120 and 40 mV in 20 mV steps (inset). (B) Delayed rectifier K+ current, IKr, measured as an outward tail current at -40 mV after 5 s depolarising pulses between -80 and 80 mV (inset). Representative recordings at 4°C and mean values (± s.e.m.) from 5-10 cells at 4°C (black circles) and 11°C (white circles). *Density of IKr is increased significantly by acute warming to 11°C (Student's t-test, P<0.005).

INCX in burbot ventricular myocytes

We investigated the efficacy of the NCX at two different levels of intracellular Ca2+ buffering. In the first series of experiments(Fig. 3A) we measured the NCX under conditions that held intracellular Ca2+ at diastolic levels(see Materials and methods). INCX was elicited at 4 s intervals from the calculated reversal potential of the exchanger (-26.5 mV)by ramp pulses (Fig. 3A,inset). INCX was measured as the Ni2+-sensitive current during the hyperpolarizing phase of the ramp. At 4°C, the conductance of INCX was 35.9±6.3 pS pF-1between -40 and 20 mV and it increased with a Q10 of 2.49±0.29 to 58.6±8.4 pS pF-1 when temperature was increased to 11°C (Fig. 3A). The measured reversal potential of INCXwas -23.5±0.1 and -23.7±0.8 mV at 4°C and 11°C,respectively, which is close to theoretical equilibrium potential. Neither 2μmol l-1 isoprenaline nor 10 mmol l-1 caffeine had any effect on burbot INCX (not shown). Isoprenaline (10μmol l-1) caused a small but non-significant (P=0.142, N=5) increase in INCX (not shown).

In the second series of experiments we reduced intracellular Ca2+ buffering to a more physiological level by replacing 20 mmol l-1 BAPTA with 0.025 mmol l-1 EGTA. Repolarising ramps from 30 to -100 mV were applied at every 4th second from a holding potential of -80 mV (see inset Fig. 3B). These experiments were preformed at 4°C only. The outward NCX current is significantly smaller in the weakly buffered pipette solution than in the heavily buffered solution given in Fig. 3A, with a mean conductance of 13.8±2.3 pS pF-1at 10 mV. The mean reversal potential of the NCX current was -8.88±1.6 mV (N=9).

Fig. 3.

Na+-Ca2+ exchange current (INCX)measured as the Ni2+-sensitive current during the hyperpolarising phase of the ramp pulse in ventricular myocytes from the burbot heart. (A)Values are means ± s.e.m. from 8 cells at 4°C and 11°C when the intracellular solution contained 20 mmol l-1 BAPTA. *Density of INCX is increased significantly by acute warming to 11°C (Student's t-test, P<0.005).(B) Mean values (± s.e.m.) from 9 cells at 4°C only. The pipette solution contained a lower level of Ca2+ buffering (0.025 mmol l-1 EGTA). Insets show voltage ramp protocols.

Fig. 3.

Na+-Ca2+ exchange current (INCX)measured as the Ni2+-sensitive current during the hyperpolarising phase of the ramp pulse in ventricular myocytes from the burbot heart. (A)Values are means ± s.e.m. from 8 cells at 4°C and 11°C when the intracellular solution contained 20 mmol l-1 BAPTA. *Density of INCX is increased significantly by acute warming to 11°C (Student's t-test, P<0.005).(B) Mean values (± s.e.m.) from 9 cells at 4°C only. The pipette solution contained a lower level of Ca2+ buffering (0.025 mmol l-1 EGTA). Insets show voltage ramp protocols.

ICa in burbot ventricular myocytesI

Ca was elicited from a holding potential of -80 mV to voltages between -70 and +60 mV for 1 s, in the absence and presence of a saturating concentration of isoprenaline (10 μmol l-1)(Fig. 4). The density of ICa measured using 5 mmol l-1 EGTA, which will augment current amplitude, was only 0.81±0.13 pA pF-1 at 4°C, and increased to 1.35±0.18 pA pF-1 at 11°C(Q10=2.08; P=0.01). The charge density(QCa) of ICa was 0.24±0.043 pC pF-1 and 0.21±0.034 pC pF-1 at 4°C and 11°C, respectively. Temperature does not affect charge density(P=0.6), primarily due to the slowing of current decay at the colder temperature. Single exponential equations fit to the decay of the ICa under physiological buffering conditions (i.e. 25μmol l-1 EGTA, Fig. 6C) provide a time constant (τ) of 211.9±12.9 ms and 155.8±19.7 ms, at 4°C and 11°C, respectively(P<0.001).

Fig. 4.

l-type Ca2+ current in burbot ventricular myocytes measured with 5 mmol l-1 EGTA in the pipette solution. (A)Representative recording at 11°C with and without stimulation by isoprenaline (10 μmol l-1). Values are means ± s.e.m. from 6-12 cells at 4°C (B) and 11°C (C) under control conditions and in the presence of 10 μmol l-1 isoprenaline (Iso). *Density of ICa is increased significantly by 10 μmol l-1 isoprenaline (Student's t-test, P<0.01). (D) Steady-state activation and inactivation relationships ICa at 4°C only. (E) The ICa window current (product of activation and inactivation curves in D) at 4°C.

Fig. 4.

l-type Ca2+ current in burbot ventricular myocytes measured with 5 mmol l-1 EGTA in the pipette solution. (A)Representative recording at 11°C with and without stimulation by isoprenaline (10 μmol l-1). Values are means ± s.e.m. from 6-12 cells at 4°C (B) and 11°C (C) under control conditions and in the presence of 10 μmol l-1 isoprenaline (Iso). *Density of ICa is increased significantly by 10 μmol l-1 isoprenaline (Student's t-test, P<0.01). (D) Steady-state activation and inactivation relationships ICa at 4°C only. (E) The ICa window current (product of activation and inactivation curves in D) at 4°C.

Fig. 5.

SR Ca2+ content in burbot ventricular myocytes. Representative recordings of inward Na+-Ca2+ exchange currents(INCX) in response to caffeine (10 mmol l-1,designated by the white bar) in burbot ventricular myocytes at 4°C (A) and 11°C (B). The insets show the corresponding time integral of INCX at each temperature. (C) Mean values ± s.e.m.; N=119 myocytes at 4°C and 20 myocytes at 11°C, respectively. NS, values were not significantly different (Student's t-test, P>0.05). SR Ca2+ content is expressed as the charge carried by the integral (pC) normalized to cell capacitance (pF). In the text,values for charge (pC) are converted into μmol Ca2+ (see Materials and methods) to facilitate comparisons with literature values.

Fig. 5.

SR Ca2+ content in burbot ventricular myocytes. Representative recordings of inward Na+-Ca2+ exchange currents(INCX) in response to caffeine (10 mmol l-1,designated by the white bar) in burbot ventricular myocytes at 4°C (A) and 11°C (B). The insets show the corresponding time integral of INCX at each temperature. (C) Mean values ± s.e.m.; N=119 myocytes at 4°C and 20 myocytes at 11°C, respectively. NS, values were not significantly different (Student's t-test, P>0.05). SR Ca2+ content is expressed as the charge carried by the integral (pC) normalized to cell capacitance (pF). In the text,values for charge (pC) are converted into μmol Ca2+ (see Materials and methods) to facilitate comparisons with literature values.

ICa was blocked by both CdCl2 (100 μmol l-1) and a combination of CdCl2 (30 μmol l-1) and verapamil (10 μmol l-1) (see below). Isoprenaline increased peak ICa in the burbot ventricular myocytes by 65% and 95% at 4°C and 11°C, respectively(Fig. 4B,C).

The slow inactivation time constants and the long AP duration, especially at 4°C, suggest a prominent role for the ICa window current in this species. Steady-state activation and inactivation(Fig. 4D) and the ICa window current(Fig. 4E) was measured in burbot myocytes at 4°C using 5 mmol l-1 EGTA in the pipette. The voltage at which inactivation was halfmaximal (Vh) and slope (k) that describes the Boltzman fit to inactivation are-11.95±1.37 mV and -11.14±0.89 (mean ± s.e.m., N=9), respectively. Corresponding values for steady-state activation are -10.89±1.20 mV and 10.40±1.43 mV, respectively. These results indicate slow transition between activation and inactivation at 4°C and result in the large window current given in Fig. 4E.

SR Ca2+ cycling in burbot ventricular myocytes

The Ca2+ stores of the burbot SR were first released with caffeine so that all myocytes started with a negligible SR Ca2+content. SR Ca2+ was then replenished with a series of stimulus pulses which, under control conditions, consisted of 25 square pulses from -80 to +10 mV for 600 ms at a frequency of 0.2 Hz. SR Ca2+ accumulation was assessed by recording the NCX current generated upon the re-application of caffeine and calculating its time integral. Representative recordings of INCX and its time integral at 4°C and 11°C are given in Fig. 5A,B. The mean values for SR Ca2+ content in burbot myocytes at 4°C and 11°C are given in Fig. 5Cand are expressed as charge (pC) normalized to myocyte capacitance (pF). The ability to load Ca2+ into the SR is not significantly affected by acute warming with Ca2+ content being 124±23 μmol l-1 at 4°C and 165±33 μmol l-1 at 11°C. This small steady-state SR Ca2+ content in burbot cells was not the result of incomplete Ca2+ release during the 3 s caffeine pulse as longer single caffeine applications of up to 10 s did not result in a greater SR Ca2+ release, nor did repeated shorter duration single caffeine applications (not shown).

Stimulating burbot myocytes with long square depolarizing pulses (1-4 s) to high voltages (+50 mV) did not significantly increase SR Ca2+content compared with that obtained under the control loading conditions given in Fig. 5C. Furthermore,applying loading pulses (25-75 pulses, to either +10 or +50 mV, for either 1 s or 4 s) in bathing solution without TTX, in an attempt to augment reverse-mode NCX, did not result in greater SR Ca2+ accumulation upon application of caffeine (not shown). The amount of Ca2+ accumulated by the SR did not significantly increase when stimulating pulses (either control pulses or 1 s pulses to +50 mV) were applied in the presence of 1 or 10 μmol l-1 isoprenaline, although ICa was augmented. Thus, SR Ca2+ content in burbot ventricular myocytes was at a steady-state between 100 and 300 μmol l-1 Ca2+under the conditions of our study. It should be noted, however, that a few cells (11 out of 119 at 4°C and 2 out of 20 at 11°C) had an SR Ca2+ content in excess of 1000 μmol l-1 upon the first application of caffeine. Although these cells were Ca2+overloaded, it does suggest that the maximal Ca2+ storage capacity of the burbot SR can be large.

Fig. 6.

SR Ca2+ release in burbot myocytes does not affect the inactivation kinetics of ICa. Representative recordings of ICa at 4°C (A) or 11°C (B) on the first pulse after caffeine application (SR empty) and the 25th pulse after caffeine application (steady-state SR Ca2+ content). Recordings are superimposed. Tau of inactivation was calculated by fitting a single exponential function to the decaying portion of ICa. For clarity, only the fit for 25th pulse is shown at each temperature (red lines).(C) Values are means ± s.e.m. from 9 myocytes at 4°C and 16 myocytes at 11°C, 1, 5, 10 and 25 pulses after caffeine application. *Inactivation of ICa was faster at 11°C than at 4°C (Student's t-test, P<0.05).

Fig. 6.

SR Ca2+ release in burbot myocytes does not affect the inactivation kinetics of ICa. Representative recordings of ICa at 4°C (A) or 11°C (B) on the first pulse after caffeine application (SR empty) and the 25th pulse after caffeine application (steady-state SR Ca2+ content). Recordings are superimposed. Tau of inactivation was calculated by fitting a single exponential function to the decaying portion of ICa. For clarity, only the fit for 25th pulse is shown at each temperature (red lines).(C) Values are means ± s.e.m. from 9 myocytes at 4°C and 16 myocytes at 11°C, 1, 5, 10 and 25 pulses after caffeine application. *Inactivation of ICa was faster at 11°C than at 4°C (Student's t-test, P<0.05).

SR Ca2+ levels were considerably reduced (∼70%) when control loading pulses were applied during blockade of ICa (with 100 μmol l-1 CdCl2) or INCX (with 10 mmol l-1 NiCl). For example, SR Ca2+ content decreased from 244±72 μmol l-1 (N=13) under control conditions, to 73±20 and 75±41 μmol l-1when the 25 stimulation pulses were applied in the presence of CdCl2 (100 μmol l-1) or NiCl2 (10 mmol l-1), respectively. This suggests equal SR Ca2+ loading capabilities of these two Ca2+ influx pathways. However, because CdCl2 at a concentration of 100 μmol l-1 can potentially impact NCX activity, we examined SR Ca2+ accumulation in the presence of 30 μmol l-1 CdCl2 and 10 μmol l-1 verapamil, which has been shown to quickly and effectively block l-type Ca2+ channel currents in crucian carp(Carassius carassius) myocytes without inhibiting the NCX(Vornanen, 1999). We found less of a reduction (∼56%) in SR Ca2+ content under these conditions, suggesting that reverse-mode NCX contributes a greater amount of Ca2+ to SR stores than ICa in burbot ventricular myocytes. It is important to note that these experiments were conducted with 0.025 mmol l-1 EGTA in the pipette to better simulate in vivo cytosolic Ca2+ buffering(Hove-Madsen and Tort, 1998)and thus peak ICa was reduced by ∼65% (to 0.28±0.02 and 0.48±0.04 pA pF-1 at 4°C and 11°C, respectively) compared with the values presented in Fig. 4, possibly reducing ICa contribution to SR Ca2+ loading. On the other hand, the lack of an increase in SR Ca2+ content during isoprenaline stimulation, despite augmented ICa,emphasizes the limited role of ICa and the potential importance of Ca2+ influx via NCX during excitation-contraction coupling in this species.

Inactivation kinetics of ICa were examined to assess the impact of SR Ca2+ release on excitation-contraction coupling in burbot myocytes at 4°C and 11°C. ICa records initiated immediately after depletion of SR Ca2+ by caffeine allowed the effects of subsequent progressive accumulation and release of SR Ca2+ on ICa to be monitored. Single exponential fits (tau, τ) to the decaying portion of ICa revealed no change in inactivation kinetics as Ca2+ was loaded into the SR(Fig. 6), indicating a lack of SR-Ca2+-release dependent inactivation of ICaat either temperature.

Electrophysiological properties of burbot ventricle

In general, the RMP and AP of the burbot ventricle are similar to those recorded from other vertebrate hearts(Jaeger, 1965; Anderson et al., 1977; Morad et al., 1983; Venditti et al., 1996). However, there are several features of SL ion currents in the burbot ventricle that are not especially typical for vertebrate heart. These characteristics include (i) very small IK1, (ii) large IKr, (iii) small ICa and (iv) large INCX.

In cardiac myocytes, IK1 maintains the negative RMP and contributes to final phase 3 repolarisation(Christie, 1995; Barry and Nerbonne, 1996). IK1 of the burbot ventricle is small, only one third of those found in cold-acclimated (4°C) trout and even less than the values measured in warm-acclimated (18°C) trout and crucian carp(Paajanen and Vornanen, 2002; Paajanen and Vornanen, 2004; Vornanen et al., 2002a), which explains its 7-10 mV less negative RMP in comparison with these species. Because IK1 is small, it cannot contribute very much to the repolarisation of the AP. It is perhaps not unexpected then, that the other repolarising current, IKr, is about five times larger than IK1 in burbot ventricular myocytes. The relative sizes of K+ currents in burbot ventricular myocytes resemble those of cold-acclimated trout but are in fact more extreme, with burbot ventricular K+ currents showing an electrical excitability phenotype similar to atrial K+ currents in other fish species(Vornanen et al., 2002a). The similarity of K+ currents, i.e. small IK1 and large IKr, in cold-acclimated trout and burbot suggest that this might be a physiologically significant mechanism by which excitability is maintained at low temperatures. Studies on other cold-adapted species are necessary to assess the universality of this strategy and its influence on factors such as maintenance of RMP, AP duration and the prevention of cardiac arrhythmias.

Sarcolemmal Ca2+ transport in burbot ventricular myocytes

Fish cardiac myocytes have a large surface area-to-volume ratio, increasing the efficacy of SL ion exchange in cytosolic Ca2+ management. This is especially true in myocytes of the burbot heart, which are 30% smaller in both length and width than those from similarly sized rainbow trout, which should result in even smaller diffusion distances between the SL and the myofilaments (Tiitu and Vornanen,2002a). In the physiological voltage range, the NCX avidly transports Ca2+ in both directions across the SL, while l-type Ca2+ channels provide an entry pathway for extracellular Ca2+ and maintain the long AP duration. The density of ICa is very low in burbot myocytes(Fig. 4) being half of that of crucian carp myocytes under identical conditions (not shown). However, the temperature sensitivity of ICa in the burbot ventricle(Q10∼2) is similar to that of other fish(Shiels et al., 2000). The low ICa density may be related to the low density of the l-type Ca2+ channels on the burbot SL as dihydropyridine(DHPR) binding studies have indicated significantly lower Bmax compared with that of trout and carp(Tiitu and Vornanen, 2003).β-adrenergic stimulation increases the size of ICa,but at present the adrenergic tonus on the burbot heart and its impact on excitation-contraction coupling are unknown.

Despite the slow inactivation of ICa, the charge carried (QCa) was still very small. Indeed, the values for QCa after a 1 s square pulse in the burbot were similar to the values of the rainbow trout ventricular myocytes for 0.5 s pulse and 58-75% of the values of the crucian carp ventricular myocytes for 0.5 s pulse(Vornanen, 1997; Vornanen, 1998; Shiels et al., 2000) at similar temperatures and identical conditions of cytosolic Ca2+buffering. Thus, ICa and QCa in the burbot heart are smaller than in either rainbow trout or crucian carp. However, the slow inactivation of ICa may have another important role in cytosolic Ca2+ management. It increases calcium influx via the ICa-window current, which may play an important role in the long APD of burbot myocytes. We have previously shown that acute cold temperature increases the ICa-window current in trout myocytes, increasing the relative importance of SL calcium influx (Shiels et al., 2000). Here we show that the size the ICa window current in burbot ventricular myocytes at 4°C is twofold greater than in rainbow trout at 7°C (Shiels et al.,2000). Despite this, the peak density of ICais so small in the burbot that the integrated charge transfer during the duration of an AP (∼1 s at 4°C) remains smaller in burbot than trout under similar experimental conditions.

INCX density in burbot ventricular myocytes is approximately double that observed in crucian carp under identical conditions(Vornanen, 1999). INCX and ICa have been measured previously in crucian carp ventricular myocytes and it was estimated they contribute almost equally to SL Ca2+ entry(Vornanen, 1999). The present findings show that the density of INCX is clearly larger and the density of ICa much smaller in burbot than in carp myocytes. For example, the mean current density of the INCX is 0.2615 pA pF-1 at +10 mV at 4°C(see Fig. 3B), and if this current is integrated for 1000 ms, it results in 0.2615 pC pF-1 of charge transferred in 1 s. Because only one charge is carried by the NCX for each Ca2+ atom, this charge density corresponds to 0.523 pC pF-1 if it were carried by Ca2+ channels. This is substantially more than that transported by l-type Ca2+channels at peak current (0.24±0.043 pC pF-1 at the same voltage and temperature). This clearly indicates that in burbot ventricular myocytes, the NCX is much more important than l-type Ca2+ channels in trans-sarcolemmal Ca2+ influx. This is especially true when one considers that the charge transferred by the l-type Ca2+ channels given above was measured with 5 mmol l-1 EGTA in the pipette solution, which augments Ca2+ influx.

Studies using non-teleost expression systems demonstrate that the trout NCX temperature-sensitivity is quite low (Q10∼1.1)(Elias et al., 2001), whereas the NCX of a tropical fish species, the tilapia Oreochromis mossambicus, shows a similar temperature-sensitivity to mammals(Marshall et al., 2005). Surprisingly, the burbot INCX shows a relatively strong temperature dependence (Q10=2.47) between 4°C and 11°C when recorded in native myocytes. This is interesting in light of the cold stenothermic environment in which the burbot lives and the predominance of the NCX in mediating SL Ca2+ flux. It should be noted, however, that regardless of the Q10-effect, the activity of the NCX at 4°C is still high in burbot in comparison with other fish species. Further studies are necessary to assess the impact of this temperature sensitivity on excitation-contraction coupling.

SR Ca2+ cycling in burbot ventricular myocytes

We found the SR Ca2+ content in burbot ventricular myocytes was at a steady state between 100 and 300 μmol l-1, which is comparable to that observed in mammals [100-150 μmol l-1(Bassani et al., 1995; Negretti et al., 1995)] but smaller than that reported for rainbow trout myocytes (>500 μmol l-1) (Hove-Madsen et al.,1998; Shiels et al.,2002b).

In the present study we examined the effect of SR Ca2+ content on the inactivation kinetics of ICa as an indirect means of assessing Ca2+-induced Ca2+-release (CICR). Despite the modest total SR Ca2+ content, we had expected to see evidence of CICR in burbot myocytes given that (i) isolated muscle experiments show that SR Ca2+ contributes significantly to contractility(Tiitu and Vornanen, 2002b),(ii) electron micrographs of burbot ventricle show that peripheral couplings between the SR and the SL are bridged by distinct foot particles akin to ryanodine receptors, indicating the structural organization necessary for CICR(Tiitu and Vornanen, 2002a),and (iii) [3H]ryanodine binding studies in cardiac vesicles indicate that the burbot ventricle has a substantial number of ryanodine receptors (65% of the value of the rat heart) whose opening is very Ca2+ sensitive (Vornanen,2006). However, we saw no effect of SR Ca2+ content on the inactivation kinetics of ICa, which suggests limited CICR in burbot ventricular myocytes. This apparent contradiction may be related to the low density of the l-type Ca2+ channels,which may preclude sufficient trigger signal for propagative CICR (see Shiels and White, 2005). Alternatively, as the NCX can provide the trigger Ca2+ in both mammal and fish hearts (Vornanen et al.,1994; Hove-Madsen et al.,2003), it is possible that the large INCX of the burbot ventricular myocytes overwhelms ICa as a trigger in the dyadic junction and, at the same time, masks the effect of CICR on ICa inactivation. According to this proposal the relative roles of ICa and INCX in triggering SR Ca2+ release would be quite different in fish and mammalian hearts. Obviously further studies examining the time course of intracellular Ca2+ transients in burbot ventricle with and without SR inhibition would provide valuable insight into the physiological role and mechanism of SR Ca2+ cycling during excitation-contraction coupling in this species.

Conclusions

Electrical excitation of burbot ventricular myocytes suggest that cold stenothermy and compensative cold-acclimation involve many of the same subcellular mechanisms. In particular, burbot K+ currents are organised similarly to those of cold-acclimated active species, demonstrating a small delayed rectifier K+ current (IKr) and a large inward rectifier K+ current (IK1). This data strongly suggests that K+ current reorganisation may be necessary for AP regulation in cold-adapted species. Based on inactivation of ICa, we found no evidence of an upregulation of SR Ca2+ flux pathways in burbot ventricular myocytes, which is contrary to previous findings from other cold-acclimated fish. This may be related to the fluminous Ca2+ influx through the NCX, which probably provides the major part of the contractile Ca2+.

    List of abbreviations
     
  • AP

    action potential

  •  
  • APD

    action potential duration

  •  
  • CICR

    Ca2+-induced Ca2+-release

  •  
  • NCX

    Na2+-Ca2+ exchange

  •  
  • RMP

    resting membrane potential

  •  
  • SL

    sarcolemma

  •  
  • SR

    sarcoplasmic reticulum

We thank Jaakko Haverinen for his help with some of the experiments and acknowledge the support of a Journal of Experimental Biology Travel Fellowship to H.A.S. and by the Academy of Finland to V.P. and M.V.

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