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J Physiol Volume 510, Number 1, 63-70, July 1, 1998
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The Journal of Physiology (1998), 510.1, pp. 63-70
© Copyright 1998 The Physiological Society

The erg inwardly rectifying K+ current and its modulation by thyrotrophin-releasing hormone in giant clonal rat anterior pituitary cells

Christiane K. Bauer

Physiologisches Institut, Universitätskrankenhaus Eppendorf, Martinistraße 52, D-20246 Hamburg, Germany

Received 7 November 1997; accepted after revision 20 March 1998.

  ABSTRACT
Top
Abstract
Introduction
Methods
Results
Discussion
References

  1. The voltage-dependent inwardly rectifying K+ current (IK,IR) of clonal rat anterior pituitary cells (GH3/B6) was investigated in solutions with physiological K+ gradient using giant polynuclear cells.

  2. IK,IR was isolated by the use of the selective erg (ether-à-go-go-related gene) channel blocker E-4031. In external 5 mM K+ solution, IK,IR carried steady-state outward current in the potential range between -60 and 0 mV, with a maximum current amplitude at -40 mV. Negative to the K+ equilibrium potential, EK, large transient inward currents occurred.

  3. A selective pharmacological block of IK,IR induced a sustained depolarization of the membrane potential when Ca2+ action potentials were blocked, confirming the contribution of IK,IR to the resting membrane potential of GH3/B6 cells.

  4. Thyrotrophin-releasing hormone (TRH) reduced effectively the sustained outward and the transient inward IK,IR. The magnitude of a TRH-induced depolarization of the membrane potential was consistent with an almost complete reduction of IK,IR.

  5. The results demonstrate that the TRH-induced reduction of IK,IR is able to mediate the resting potential depolarization, suggesting that the increase in the frequency of action potentials occurring during the second phase of the TRH response in GH cells should be sustained by IK,IR inhibition. Moreover, this is the first evidence of a ligand-induced physiological modulation of an erg-mediated current.

  INTRODUCTION
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Abstract
Introduction
Methods
Results
Discussion
References

Lactotroph cells of the anterior pituitary respond to the hypothalamic neuropeptide thyrotrophin-releasing hormone (TRH) with an increase in prolactin secretion. The underlying intracellular signal cascade activated by TRH has been studied mainly in the somatomammotrophic GH cell lines. Since TRH induces secretion predominantly via an increase in the cytosolic free Ca2+ concentration ([Ca2+]i), the TRH-induced biphasic secretory response is mirrored in a biphasic increase in [Ca2+]i, which is accompanied by a biphasic electrical response. The hyperpolarization due to opening of Ca2+-dependent K+ channels during the first phase results from the release of stored intracellular Ca2+ producing a transient rise in [Ca2+]i, whereas the second phase of the electrical response causes or at least contributes to the subsequent plateau-like increase in [Ca2+]i (for reviews, see Ozawa & Sand, 1986; Corrette, Bauer & Schwarz, 1995). The second-phase electrical response is characterized by a depolarization or an onset of action potentials in silent cells and an increase in the frequency of action potentials in spontaneously active cells. These effects have been explained by a decrease in K+ conductance (Ozawa & Sand, 1986).

The voltage-dependent inwardly rectifying K+ current IK,IR is suggested to contribute to the resting membrane potential of GH cells (Bauer, Meyerhof & Schwarz, 1990). A similar voltage-dependent inwardly rectifying K+ current is present in native rat lactotrophs (Corrette, Bauer & Schwarz, 1996). It has already been shown that IK,IR can be modulated by TRH (Bauer et al. 1990; Barros, Delgado, del Camino & de la Peña, 1992; Corrette et al. 1996; Barros, del Camino, Pardo, Palomero, Giráldez & de la Peña, 1997), but these studies have been carried out in high external potassium to increase the current amplitude. Under these conditions, the physiologically relevant IK,IR outward currents could not be investigated.

Recently it has been shown that IK,IR exhibits a high sensitivity to several class III antiarrhythmic agents, which made it possible to isolate IK,IR as a drug-sensitive current (Weinsberg, Bauer & Schwarz, 1997; Barros et al. 1997). These antiarrhythmics, including methanesulphonanilides like E-4031 and WAY-123,398, are suggested to be specific blockers of the rapidly activating component of the cardiac delayed rectifier current (IKr) and HERG(human ether-à-go-go-related gene) K+ channels which are believed to be the basis of IKr (Spector, Curran, Keating & Sanguinetti, 1996). IKr and the heterologously expressed HERG current exhibit time-dependent inward rectification. This distinctive property is suggested to result from rapid inactivation being faster than activation at depolarized potentials and to recovery from inactivation being faster than deactivation (Shibasaki, 1987; Wang, Liu, Morales, Strauss & Rasmusson, 1997). We have recently cloned the rat homologue of HERG (rerg) and shown that the IK,IR channel in GH3/B6 cells is most probably encoded by rerg (Bauer, Engeland, Wulfsen, Ludwig, Pongs & Schwarz, 1998a). As a result of this finding, the voltage-dependent gating of IK,IR which has been described up to now using the classical inward rectifier model (e.g. activation for the current increase upon hyperpolarization) will now be described using the HERG current model (e.g. recovery from inactivation for the current increase upon hyperpolarization; Smith, Baukrowitz & Yellen, 1996).

In the present study, specific erg channel blockers were used to investigate IK,IR in solutions with physiological K+ gradients in polynuclear giant GH3/B6 cells which exhibit a high IK,IR amplitude. It was demonstrated that the TRH-induced reduction of IK,IR occurred within a potential range that is important for the control of the electrical activity of the cells.

Part of this work has been published in abstract form (Bauer, 1997).

  METHODS
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Abstract
Introduction
Methods
Results
Discussion
References

Cell culture

Giant clonal rat anterior pituitary (GH3/B6) cells were routinely cultured in Ham's F10 medium supplemented with 15 % horse serum and 2·5 % fetal calf serum. The cells were incubated at 37°C in an atmosphere of 95 % air and 5 % CO2. GH3 cells, which contain fewer giant polynuclear cells, were grown under identical conditions.

Solutions and chemicals

The external '150 mM K+' solution contained (mM): 140 KCl, 4 MgCl2, 1 CaCl2, 2·5 EGTA, 10 Hepes, 10 glucose, 10 KOH to adjust pH to 7·3. The standard external '5 mM K+' solution contained (mM): 5 KCl, 135 NaCl, 4 MgCl2, 1 CaCl2, 2·5 EGTA, 10 Hepes, 10 glucose, 10 NaOH to adjust pH to 7·3. TTX (500 nM) was added to both external solutions to block Na+ channels. The concentration of free Ca2+ was low (estimated free Ca2+ was 75 nM; EQCAL, Biosoft, Cambridge, UK) to reduce Ca2+ currents and Ca2+-dependent K+ currents. NiCl2 was added to the 5 mM K+ solution at 200 µM, a concentration which does not affect IK,IR (Bauer et al. 1990), to block Ca2+ channels. Patch pipettes were filled with (mM): 140 KCl, 2 MgCl2, 1 CaCl2, 2·5 EGTA, 10 Hepes, 10 glucose, 10 KOH to adjust pH to 7·3. The estimated free Ca2+ concentration of the pipette solution was 66 nM (EQCAL). Where indicated, MgCl2 was omitted; the contamination of this intracellular solution with Mg2+ was estimated to be less than 1 µM. The estimated free Mg2+ in the normal intracellular solution was 1·8 mM (EQCAL). For most TRH experiments, 2 mM MgATP and 0·2 mM Na2GTP were added to the intracellular solution. There was no difference in the observed TRH response with and without these nucleotides in the pipette solution.

The antiarrhythmic drugs E-4031 and WAY-123,398 were generous gifts from Eisai, Tokyo, Japan, and from Wyeth-Ayerst, Princeton, NJ, USA, respectively. Both drugs were dissolved in water to yield a stock solution of 10 mM.

Electrophysiology

Cells were used 1-5 days after passaging. Electrophysiological recordings were performed in the whole-cell mode to render the TRH-induced reduction of IK,IR irreversible (Bauer et al. 1990; Barros, Mieskes, del Camino & de la Peña, 1993). This was necessary to obtain the complete I-V relationship of the TRH-sensitive current component. In addition, voltage-dependent, spontaneous or TRH-induced changes in [Ca2+]i were reduced in the whole-cell recording mode. The pipette resistance ranged from 2·5 to 4 MOmega. Prior to recording, fast and slow capacitances were compensated; the value of the slow capacitance was taken to represent the cell capacitance. Series resistance errors were compensated to at least 70 %. Stimulation, data acquisition and analysis were carried out with an EPC9 patch-clamp amplifier and the 'Pulse' software (HEKA Elektronik, Lambrecht, Germany). All experiments were performed at room temperature (20-26°C).

  RESULTS
Top
Abstract
Introduction
Methods
Results
Discussion
References

Occurrence of giant polynuclear GH3/B6 cells and recording of IK,IR in isotonic KCl

In cell cultures of GH3/B6 cells, large round cells of up to 40 µm diameter occur infrequently, but regularly. These cells contain several nuclei (Fig. 1). Recordings of hyperpolarization-elicited K+ currents in external 150 mM K+ solution demonstrated that these giant cells exhibited high amplitudes of the voltage-dependent inwardly rectifying K+ current (IK,IR) previously described in 'normal' mononuclear GH3/B6 cells (Bauer et al. 1990). In the standard pulse protocol, a 2 s depolarizing pulse to +20 mV preceded every test pulse in order to achieve maximum IK,IR amplitudes due to a maximum steady-state activation of the erg channels (Wang et al. 1997).

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    Figure 1. Hyperpolarization-elicited K+ currents recorded from a mononuclear and a giant polynuclear GH3/B6 cell in isotonic KCl

    Left: micrograph of GH3/B6 cells with a giant polynuclear cell which contained at least 12 nuclei. Right: membrane currents recorded from a big mononuclear cell (20 pF) and from a giant polynuclear cell (60 pF) in symmetrical (150 mM) K+ solution. The K+ inward currents were elicited with the standard pulse protocol shown at the top; in this and subsequent figures voltages are given in mV. The complete pulse sequence consisted of variable 200 ms test pulses to potentials between 0 and -120 mV preceded by a 2 s prepulse to +20 mV and a 500 ms pulse to -20 mV. Test pulses were followed by a 100 ms pulse to -20 mV before returning to the holding potential of -40 mV.

A strong dependence of the deactivation process on external divalent cations has been found in two other native erg-mediated currents (Faravelli, Arcangeli, Olivotto & Wanke, 1996; Ho, Earm, Lee, Brown & Noble, 1996), but not in heterologously expressed HERG currents (Wang et al. 1997). Therefore, additional experiments were performed in external 150 mM K+ solution containing 2 mM Ca2+ and 4 mM Mg2+ (but without EGTA) and in a solution without free divalent cations (CaCl2 and MgCl2 omitted, 2·5 mM EGTA added). The increase in external free Ca2+ made the recordings of IK,IR more difficult due to an increase in overlapping currents, but did not induce a clear acceleration of the IK,IR deactivation process (taudeact,-120: 30 ± 3·2 ms (n = 4) vs . 35·7 ± 4·0 ms in external solution with 75 nM free Ca2+(n = 6); time constants obtained by fitting single exponential curves to the current decay during the hyperpolarization to -120 mV; series resistance compensation 90 %). In the absence of external divalent cations, IK,IR deactivation at potentials more negative than -60 mV was still evident (taudeact,-120: 63 ± 18 ms, n = 3; series resistance compensation 50-70 %), although the recordings were impeded by huge steady-state and tail currents, probably due to K+ permeation through Ca2+ channels. These results suggested that IK,IR deactivation is not very sensitive to external divalent cations.

Isolation of IK,IR as an E-4031-sensitive current in solutions with a physiological K+ gradient

Giant polynuclear GH3/B6 cells were used for recording in external 5 mM K+ solution because of they exhibit high-amplitude IK,IR. Figure 2A demonstrates the presence of IK,IR in the control currents: upon hyperpolarization, a time-dependent current increase occurred, which reversed direction at about -80 mV. Application of 10 µM E-4031, which has been shown to block IK,IR fast and completely (Weinsberg et al. 1997), abolished this current increase, confirming that it was due to IK,IR.

Since the rerg channels were most probably 'fully activated' (Wang et al. 1997; Bauer et al. 1998a) by the depolarizing pulse prior to the test pulses, IK,IR isolated as the E-4031-sensitive current exhibited, during the 200 ms test pulses, sustained outward currents in the potential range between -60 and 0 mV with a maximum amplitude at about -40 mV (Fig. 2C and D). At more negative potentials IK,IR deactivated and demonstrated a strong voltage dependence of the deactivation kinetics. The I-V relationship of the peak currents showed a clear inward rectification. Similar results were obtained when IK,IR was isolated as a WAY-123,398-sensitive current.

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    Figure 2. Isolation of IK,IR as an E-4031-sensitive current recorded in physiological K+ gradients

    A, inward and outward membrane currents recorded from a giant GH3/B6 cell (54 pF) in external 5 mM K+ solution using the standard pulse protocol described in Fig. 1. The holding potential was -40 mV. B, membrane currents recorded from the same cell as in A after addition of 10 µM E-4031. C, isolation of IK,IR as the E-4031-sensitive current obtained by subtraction of the currents recorded in the presence of E-4031 (B) from the control currents shown in A. D, I-V plot of the peak and late (measured at the end of the 200 ms test pulses) outward and inward E-4031-sensitive currents shown in C. E, time- and voltage-dependent increase and decrease of E-4031-sensitive currents recorded from two cells using intracellular solutions prepared with differing amounts of MgCl2. The '0' mM Mg2+ solution was estimated to contain less than 1 µM free Mg2+. F, I-V plots of the peak and late outward and inward E-4031-sensitive currents recorded with differing amounts of Mg2+ in the intracellular solutions; shown are mean current values ± S.D. obtained from each 5 giant GH3/B6 cells with a comparable range of cell sizes (43·2 ± 6·9 pF and 43·6 ± 5·5 pF for 1·8 mM and '0' mM Mg2+, respectively). In the voltage range from -50 to 0 mV, peak values were omitted because they did not differ from late current values.

In contrast to classical inward rectifiers, the gating of HERG channels has been shown to be independent of intracellular Mg2+ (Smith et al. 1996). To investigate the Mg2+ dependence of the rerg-mediated IK,IR, experiments were performed with and without MgCl2 in the pipette solution. The kinetics of inactivation (time constant, tauinact) and recovery from inactivation (time constant, taurecov) were similar in the two groups (Fig. 2E; taurecov at -40 mV: 6·9 ± 1·1 ms vs. 8·0 ± 1·3 ms; taurecov at -50 mV: 7·2 ± 1·0 ms vs. 8·6 ± 1·4 ms; tauinact at -20 mV: 11·0 ± 2·5 ms vs. 12·8 ± 3·1 ms; data obtained for 1·8 mM (n = 5) and '0' mM (n = 5) free Mg2+, respectively). Also the voltage dependence of peak and late current amplitudes of IK,IR (Fig. 2F) did not significantly differ.

A few experiments were performed on GH3 cells. In this cell line, giant polynuclear cells occurred less frequently. The characteristics of IK,IR recorded as the E-4031-sensitive or WAY-123,398-sensitive current in 5 mM K+ from giant GH3 cells were identical to those observed in GH3/B6 cells.

Correlation of IK,IR with the membrane potential of the cells

In order to relate a specific block of IK,IR to changes in membrane potential, experiments were performed in which alternating recordings were made of membrane currents and membrane potential in the voltage-clamp and current-clamp mode, respectively. The standard external 5 mM K+ solution was used in which Ca2+ action potentials were blocked. Figure 3 shows one of five experiments, where 10 µM WAY-123,398 induced a depolarization which could be clearly attributed to a block of IK,IR. The average depolarization amounted to 4·4 ± 0·96 mV, from -45·6 to -41·2 mV (n = 5). Most experiments of this kind could not be evaluated due to either an increase or a decrease in the amplitude of a hyperpolarization-activated current (Ih) during the critical period of membrane potential recording.

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    Figure 3. Block of IK,IR depolarizes the membrane potential

    Recordings of membrane currents and membrane potential from a 70 pF giant GH3/B6 cell in external 5 mM K+ solution. The voltage-clamp recordings in the absence (A) and presence of WAY-123,398 (C) were separated by a period in which the effect of 10 µM WAY-123,398 on the membrane potential was monitored in the current-clamp mode (B).

Effects of TRH on IK,IR

Membrane currents of giant GH3/B6 cells were recorded with the standard pulse protocol before and about 3 min after the addition of TRH. In between, the TRH response was traced with a double-pulse sequence applied every 10 s. The standard protocol lasted less than 1 min and TRH was applied within 3 min of patch rupture to enable measurement of the effects of TRH on IK,IR in the whole-cell recording mode (Barros et al. 1993). The time course of the TRH-induced reduction of IK,IR was similar to that previously described for experiments in isotonic KCl (Bauer, Davison, Kubasov, Schwarz & Mason, 1994), with a maximal reduction of IK,IR achieved about 150 s after the application of TRH. Figure 4A-D shows that the TRH-sensitive current closely resembled IK,IR, isolated as the E-4031-sensitive current. This implies that TRH selectively reduced IK,IR under these experimental conditions, and that this effect occurred over the whole voltage range.

The amount of TRH-induced IK,IR reduction is most probably underestimated in the above experiments, since they were carried out with a depolarizing prepulse and we have previously shown that the magnitude of a TRH-induced reduction of IK,IR can be decreased by a preceding depolarization (Bauer et al. 1990). Double pulses with and without a prepulse to +20 mV (see Fig. 4, top right) were used to investigate whether this phenomenon also occurred in cells in 5 mM K+ solution exhibiting outward IK,IR. Before application of TRH, the membrane currents recorded with and without a depolarizing prepulse were almost identical (Fig. 4E) in the majority of the cells. TRH reduced inward and outward membrane currents and a difference between current traces elicited with and without prepulse became evident (Fig. 4F). Both the TRH-sensitive and the small prepulse-sensitive current components (Fig. 4G and H) exhibited characteristic inactivation of IK,IR upon depolarization and recovery upon hyperpolarization. In most experiments of this kind, after application of TRH, the current response to hyperpolarization to -100 mV without preceding depolarization resembled tail currents only (Fig. 4F), with no indication of the characteristic hook representing recovery from inactivation which is observed with erg channels. This suggested that, in the absence of depolarizing pulses to potentials more positive than those occurring physiologically in GH3/B6 cells, TRH produces an almost complete reduction of IK,IR.

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    Figure 4. TRH selectively reduces IK,IR

    A, membrane currents were recorded in a giant GH3/B6 cell (39 pF) using the standard pulse protocol described in Fig. 1. The holding potential was -40 mV. B, membrane currents recorded from the same cell as in A about 3 min after the application of 500 nM TRH. C, TRH-sensitive current obtained by subtraction of the currents recorded after the addition of TRH (B) from the control currents shown in A. D, I-V plot of the peak and late outward and inward TRH-sensitive currents shown in C. E-H, time- and voltage-dependent increase and decrease of membrane currents recorded from a 43 pF giant cell before (E) and after (F) addition of 500 nM TRH. The TRH-sensitive current (G) and the prepulse-sensitive current after TRH (H) were obtained by subtraction (G = E - F, H = F* - F). The asterisks mark current traces elicited by pulse sequences with depolarizing prepulses. The sequence of voltage pulses is shown on top. A sequence with a 1·5 s depolarizing prepulse to +20 mV delivered 2 s before the pulse to -20 mV was followed by two pulse sequences without a prepulse. Pulse sequences were repeated every 10 s.

Another set of experiments was therefore performed to investigate the effects of TRH on the resting membrane potential induced by a specific reduction of IK,IR. Before and after a period of monitoring the effects of TRH application in the current clamp mode, membrane currents were recorded in the standard 5 mM K+ solution using a holding potential of -20 mV, a potential at which rerg currents are almost 'fully activated' and no deactivation occurs (Bauer et al. 1998a). The pulse protocol consisted of 200 ms test pulses to different potentials followed by a short pulse to -100 mV. Using this protocol, an estimation could be made of the deactivation of IK,IR during the test pulses by measuring the amplitude of the current which could be recovered during hyperpolarization. In experiments in which the presence of IK,IR was clearly visible in the control currents (Fig. 5A), TRH (500 nM or 1 µM) induced an irreversible depolarization of the membrane potential (Fig. 5B). The depolarization induced by TRH amounted to 4·4 ± 0·4 mV (n = 3; values obtained from the experiment shown in Fig. 5 and two comparable experiments), a value which is similar to the depolarizing effect of WAY-123,398 and which was due to a complete block of IK,IR. In one further experiment, where IK,IR clearly dominated the control currents, the TRH-induced depolarization amounted to 7·3 mV. A distinct TRH-induced first-phase hyperpolarization was observed in only one of these experiments, suggesting that the recording conditions (EGTA-buffered low Ca2+ concentrations in the extracellular and the pipette solutions) inhibited a rise in [Ca2+]i produced by the TRH-induced release of Ca2+ from intracellular stores. Membrane currents recorded after the addition of TRH showed no indications of the presence of IK,IR (Fig. 5C) in three of four experiments. The TRH-sensitive currents always exhibited the characteristic properties of IK,IR (Fig. 5E), demonstrating that the TRH-induced depolarizations were produced by a selective inhibition of IK,IR. As already shown in the above experiments, a long depolarizing prepulse was able to partially restore IK,IR (Fig. 5D and F). This effect might be explained by a strong TRH-induced shift of the voltage dependence of activation of IK,IR to more positive potentials. This was indicated by a shift to more positive potentials of the inflection points of Boltzmann functions fitted to the values of the peak inward currents during hyperpolarization to -100 mV after the addition of TRH (Fig. 5F, from -59·6 to -48·2 mV). Due to contamination by tail currents resulting from the deactivation of other K+ currents (visible in Fig. 5C and F : cir), these curves do not accurately represent the voltage dependence of IK,IR activation. For the TRH-sensitive currents, the mean value of the inflection point of the fitted Boltzmann functions was -78·2 ± 2·9 mV (n = 3).

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    Figure 5. The TRH-induced reduction of IK,IR depolarizes the membrane potential

    Recordings of membrane currents and membrane potential from a 38 pF giant GH3/B6 cell in external 5 mM K+ solution. The voltage-clamp recordings shown in A and C were separated by a period in which the effect of 1 µM TRH on the membrane potential was monitored in the current-clamp mode (B). Membrane currents in A and C were elicited by the pulse protocol shown below A without a depolarizing prepulse, whereas the membrane currents in D were obtained with a 2 s depolarizing prepulse to +20 mV. The gap between prepulse and test pulses was 500 ms. The holding potential was -20 mV. E, TRH-sensitive current obtained by subtraction of the currents recorded after the addition of TRH, shown in C, from the control currents, shown in A; note the expanded current scale in E. F, peak amplitudes of the currents obtained with the constant 20 ms pulse to -100 mV are plotted against the preceding test pulse potential. Continuous and dotted lines represent Boltzmann functions fitted to the data points; values for the inflection point and steepness are, respectively: -59·6 mV and -17·5 mV (Control; continuous line), -48·2 mV and -11·5 mV (TRH*), -75·1 mV and -9·15 mV (TRH-sensitive). Please note that the current level at -100 mV differed slightly in A and D due to a moderate activation of Ih in D.

  DISCUSSION
Top
Abstract
Introduction
Methods
Results
Discussion
References

The investigation of IK,IR in solutions with a physiological K+ gradient was enabled by the combined use of erg-specific pharmacological blockers and giant polynuclear GH3/B6 cells, which exhibit a high IK,IR amplitude. It could be demonstrated that IK,IR reaches its maximum outward value in the range of the resting potential of these cells, and that TRH drastically reduces the physiologically relevant sustained outward IK,IR. Nevertheless, in future investigations of IK,IR in normal-sized cells, external solutions with elevated K+ concentrations will need to be used because of the low IK,IR density.

Another endogenous erg current has been described in neuroblastoma cells using a high-K+ external solution (Arcangeli et al. 1995), and recently this erg current has been shown to be crucial for spike-frequency adaptation in F-11 dorsal root ganglion neurone × neuroblastoma hybrid cells (Chiesa, Rosati, Arcangeli, Olivotto & Wanke, 1997). Like neuroblastoma cells, lactotroph cells lack classical inward rectifier currents. Therefore IK,IR is able to contribute to the resting potential of these cells which ranges from about -60 to -40 mV.

In giant GH3/B6 cells, the average IK,IR density at -40 mV amounted to only 1·5 pA pF-1 (64 pA/43 pF). Therefore, the importance of IK,IR depends strongly on the input resistance of the cells, which is probably linked to their physiological state. In cells with high basal [Ca2+]i, for example, Ca2+-dependent K+ channels contribute essentially to the resting conductance of the cells. This might explain why Weinsberg et al. (1997) observed an effect of E-4031 on the membrane potential of normal GH3/B6 cells in only two out of three experiments. In comparable experiments performed in giant GH3/B6 cells, only one out of nine cells did not respond to E-4031, and TRH was unable to produce a second phase in this cell (A. Winkelmann, C. K. Bauer & J. R. Schwarz, unpublished observations). The lack of a second phase in the TRH response has been described in about one out of six GH cells (reviewed in Corrette et al. 1995).

Pharmacological block of IK,IR induced only a moderate depolarization of the membrane potential of giant GH3/B6 cells, from about -45·5 to -41 mV. Nevertheless, the fact that the threshold for the initiation of action potentials is close to -40 mV in these cells, just the potential where IK,IR has its maximum outward current, suggests that this level of depolarization could be highly effective. In the physiological voltage range, TRH almost completely reduced outward and inward IK,IR and induced a depolarization of the membrane potential comparable to that induced by complete pharmacological block of IK,IR. Since the TRH-sensitive current is almost identical to IK,IR, TRH exerts its maximum IK,IR-mediated effects on the resting conductance in a voltage range critical for the electrical activity of the cell. These data, together with the sensitivity of the TRH-induced reduction of IK,IR to a depolarizing prepulse, suggest that the IK,IR-mediated effects of TRH are most apparent in silent cells.

Normal rat lactotrophs have been shown to possess an inwardly rectifying K+ current quite similar to IK,IR (Corrette et al. 1996). Using E-4031 as a specific blocker of this current, we have recently found that this inwardly rectifying K+ current is involved in the maintenance of the resting potential of normal lactotrophs and in the control of prolactin secretion (Bauer et al. 1998b).

In cardiac cells, erg channels are involved in action potential repolarization, and a selective block of IKr results in a prolongation of the action potential (Curran, Splawski, Timothy, Vincent, Green & Keating, 1995). This proven role for HERG channels suggests an additional new role for the rerg-mediated IK,IR: the reduction of IK,IR by TRH might help to mediate a prolongation of Ca2+ action potentials, an effect which occurs often during the second phase of the TRH response. Up to now, this effect has been suggested to be mediated solely by an inhibition of the Ca2+- and voltage-dependent K+ channel BK (reviewed in Corrette et al. 1995).

The mechanism by which TRH exerts its effects on IK,IR is not known, but it has been suggested that it is mediated by a phosphorylation, which is produced neither by protein kinase C nor by protein kinase A (Barros et al. 1993; Bauer et al. 1994). The irreversibility of the TRH-induced reduction of IK,IR in the whole-cell recording mode has been proposed to be due to a wash-out of phosphatases, because the reduction of IK,IR by TRH is completely reversible in perforated-patch experiments, and is partially reversible in whole-cell experiments where protein phosphatase 2A has been added to the pipette solution (Barros et al. 1993). The assumption that TRH-induced phosphorylation of erg channels mediates the reduction of IK,IR agrees well with the present results, which indicate that TRH shifts the voltage dependence of IK,IR activation to more positive potentials, since phosphorylation of voltage-dependent ion channels has been suggested to result in a shift of the activation curve towards more positive potentials simply by electrostatic interactions (Perozo & Bezanilla, 1990). The partial reversal of the TRH-induced reduction of IK,IR by a depolarizing prepulse is reminiscent of the depolarization-induced reversal of G-protein-mediated inhibition of Ca2+ currents (reviewed by Dolphin, 1996). This phenomenon has been interpreted as depolarization-induced dissociation of a complex formed by direct interaction of inhibitory G-proteins with the Ca2+ channels. However, it is suggested that the (much slower) TRH-induced reduction of IK,IR is not a membrane-delimited event and involves a diffusible second messenger, since the magnitude of the TRH response decreases with prolonged intracellular dialysis during whole-cell recordings (Barros et al. 1993).

Recently, it has been suggested that the cardiac IKr is mediated by a minK-HERG complex (McDonald et al. 1997). MinK mRNA is not present in GH3/B6 cells (I. Wulfsen, J. R. Schwarz & C. K. Bauer, unpublished observations). This suggests a direct modulatory action of a TRH-activated second messenger on the rerg protein. Up to now, IK,IR is the only example of an erg-mediated current which is modulated by a ligand. This implies that the importance of the TRH-induced reduction of IK,IR is not confined to the study of prolactin secretion, and GH3/B6 cells might serve as a model system for the study of neuropeptide-induced modulation of erg channels.

  REFERENCES
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Abstract
Introduction
Methods
Results
Discussion
References

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Acknowledgements

I gratefully acknowledge the scientific support of Professor J. R. Schwarz and Dr F. Weinsberg and the technical support of Ms W. Krüger and Ms C. Reißmann. This work was supported by a grant from the Deutsche Forschungsgemeinschaft (Ba-1436/1).

Correspondence

C. K. Bauer: Physiologisches Institut, UKE, Martinistraße 52, D-20246 Hamburg, Germany.

Email: c.bauer{at}uke.uni-hamburg.de




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