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1 Department of Physiology, University of British Columbia, 2177 Wesbrook Mall, Vancouver, BC, Canada V6T 1Z3 2 Department of Anatomy & Cell Biology, University of British Columbia, 2177 Wesbrook Mall, Vancouver, BC, Canada V6T 1Z3
| Abstract |
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(Received 18 June 2003;
accepted after revision 3 November 2003;
first published online 7 November 2003)
Corresponding author J. Church: Department of Anatomy & Cell Biology, University of British Columbia, 2177 Wesbrook Mall, Vancouver, BC, Canada V6T 1Z3. Email: jchurch{at}interchange.ubc.ca
| Introduction |
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As befits their important roles in determining the excitability and firing patterns of central neurones, each of the above AHPs can be modulated by neurotransmitters acting through a variety of signal transduction pathways (Madison & Nicoll, 1986; Charpak et al. 1990; Holm et al. 1997; Haug & Storm, 2000; Melyan et al. 2002). They can also be modulated by changes in pH. Thus, reductions and increases in pHo, respectively, attenuate and augment the fast AHP in CA1 neurones, effects that cannot be ascribed in their entirety to pHo-induced changes in Ca2+ influx (Church & McLennan, 1989; Church, 1999). Rather, neuronal pHi is steeply dependent on pHo (e.g. Ou-Yang et al. 1993; Church et al. 1998) and, in agreement with findings in a variety of non-neuronal cell types (e.g. Cook et al. 1984; Kume et al. 1990; Copello et al. 1991; Laurido et al. 1991; Hayabuchi et al. 1998), changes in [H+]i affect directly the unitary properties of the BK-type channel that underlies the fast AHP in CA1 neurones (Church et al. 1998; also see Liu et al. 1999). Changes in pHo also modulate the medium and slow AHPs in CA1 neurones, effects that can be mimicked by changes in pHi at a constant pHo (Church & McLennan, 1989; Church, 1992, 1999). However, the pH sensitivities of the currents that contribute to the medium and slow AHPs have not been investigated and it remains unclear whether the effects of changes in pHo and/or pHi on these AHPs might be secondary to changes in Ca2+ influx.
In the present study we used the whole-cell patch-clamp technique to investigate the modulation of mIAHP and sIAHP by extra- and intracellular pH changes in CA1 pyramidal neurones in rat hippocampal slices. The results indicate that sIAHP and, to a lesser extent, mIAHP are sensitive to changes in pHi and suggest that these effects may contribute to high pHo-evoked increases in the currents. In contrast, a reduction in Ca2+ influx appears to be the major determinant of the inhibition of mIAHP and sIAHP observed at low pHo.
| Methods |
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All procedures conformed to guidelines established by the Canadian Council on Animal Care and were approved by The University of British Columbia Animal Care Committee.
Transverse hippocampal slices (400 µm) were prepared from 17- to 21-day-old (patch pipette recordings) or
40-day-old (sharp microelectrode recordings) Wistar rats as previously described (Church & McLennan, 1989). In brief, animals were anaesthetized with 3% halothane in air, decapitated and the brains rapidly removed. Hippocampal slices were then cut and allowed to recover for at least 1 h in a holding chamber at room temperature (RT, 1923°C). Individual slices were transferred as needed to the recording chamber and placed on a nylon mesh at the interface between a humidified atmosphere and a continuously (2 ml min-1) superfusing medium at RT (patch pipette recordings) or 34°C (sharp microelectrode recordings).
Solutions and chemicals
The standard HCO-3/CO2-buffered media employed at RT and 34°C (in parentheses) contained (mM): NaCl 123 (129), KCl 3, NaHCO3 26 (20), NaH2PO4 1.5, MgSO4 1.5, D-glucose 10 and CaCl2 2 (pH 7.4 after equilibration with 5% CO295% O2). Low pH HCO-3/CO2-buffered solutions contained either 5 mM or 4.5 mM NaHCO3 (pH 6.7 at RT and 34°C, respectively) and high pH HCO-3/CO2-buffered solutions contained either 55 mM or 47 mM NaHCO3 (pH 7.7 at RT and 34°C, respectively); changes in [NaHCO3] were balanced by equimolar changes in [NaCl]. For Ca2+-free medium, Ca2+ was omitted, [Mg2+] was increased to 3.5 mM and 200 µM EGTA was added. In solutions containing 2 mM CoCl2, H2PO-4 and SO2-4 were omitted. HCO-3/CO2-buffered solutions containing Hepes (100 mM), the weak acid sodium propionate (40 mM) or the weak bases NH4Cl or trimethylamine HCl (TMA) (40 mM in each case) were prepared by equimolar substitution for NaCl. In HCO-3 free media, 30 mM Hepes or 30 mMN-[tris(hydroxymethyl)methyl]glycine (tricine) isosmotically replaced NaHCO3 and an appropriate concentration of NaCl; these media were saturated with O2 and titrated to the appropriate temperature-corrected pH with 10 M NaOH. Hepes and tricine were employed at 30 mM to prevent the reduction in slice interstitial pH that would otherwise occur upon the transition from a HCO-3 containing to a HCO-3 free medium (see Cowan & Martin, 1995). During perfusion with HCO-3 containing media, the atmosphere in the recording chamber contained 5% CO295% O2; this was switched to 100% O2 upon the introduction of HCO-3 free media. The pH of each solution was re-checked at the appropriate temperature following every experiment.
Salts and experimental compounds, which were applied by superfusion, were obtained from Sigma-Aldrich Canada Ltd (Oakville, ON, Canada), with the exceptions of potassium methylsulphate (ICN Pharmaceuticals Canada Ltd, Montréal, QC, Canada) and XE991 (a gift from Bristol-Myers Squibb Co., Wilmington, DE, USA).
Recording techniques
Whole-cell patch pipette current- and voltage-clamp recordings were obtained from CA1 neurones by the blind technique. Patch pipettes were pulled from 1.2 mm o.d. x 0.9 mm i.d. borosilicate tubing (World Precision Instruments Inc., Sarasota, FL, USA) and heat-polished; open pipette resistance was 25 M
when filled with one of the solutions detailed in Table 1. After a seal >1 G
was achieved, recordings were made (Axoclamp 2, Axon Instruments Inc., Union City, CA, USA) when the application of light suction revealed a resting membrane potential (Vm) of at least 50 mV (after subtraction of the 57 mV junction and tip potentials; Neher, 1992), overshooting action potentials, an input resistance (Rin, measured at 50 mV) >100 M
and a stable series resistance (830 M
). The reference bath electrode was a 3 M KCl, 4% agar bridge. Voltage and current waveforms were low-pass filtered at 2.7 kHz and 1.2 kHz, respectively, and digitized at 510 kHz using a Digidata 1200, controlled by pCLAMP software (v.6, Axon Instruments). Leakage currents were subtracted off-line. In a small number of initial control experiments, conventional intracellular recordings were obtained with sharp microelectrodes (see Church & McLennan, 1989; Church, 1999). In brief, microelectrodes were pulled from thin-walled borosilicate tubing, filled with 4 M potassium acetate (final resistance 60100 M
) and connected to an active bridge circuit. Sharp microelectrode recordings were included in data analysis if, under control conditions, neurones exhibited a stable Vm of at least 55 mV with overshooting action potentials and Rin measured at Vm > 20 M
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During current-clamp recordings, the effects of changes in perfusate composition on the medium and slow AHPs which followed a 300 ms depolarizing current-evoked train of action potentials were quantified by comparing the amplitudes of the corresponding AHPs under control and test conditions as described (Church, 1999). The magnitude of the depolarizing current pulse employed to evoke the spike train was varied to elicit the same number of action potentials under each condition. Test measurements were conducted at the original control membrane potential by passing, when necessary, steady current through the recording electrode. In experiments conducted in the presence of 1 µM TTX and 5 mM TEA, a 40100 ms depolarizing current pulse was employed to elicit a Ca2+-dependent depolarizing potential that was followed by a slow AHP; the half-amplitude duration of the Ca2+ potential and the peak amplitude of the subsequent slow AHP were measured (see Church, 1999).
Under voltage-clamp conditions, 80200 ms depolarizing voltage steps from the holding potential (VH, 50 mV) to 020 mV, applied approximately once per minute, elicited partially clamped inward currents that were followed by early (mIAHP) and late (sIAHP) outward K+ tail currents. Experimentally evoked changes in mIAHP and sIAHP were quantified by comparing the peak amplitudes of the currents obtained under control and test conditions; if a distinct sIAHP peak was not evident, current amplitudes were compared isochronally at 400 ms after the end of the depolarizing voltage step. Larger depolarizing steps (from VH to +2040 mV) were employed to elicit Co2+ and Co2+- and XE991-resistant currents. The influence of time-dependent changes in current amplitude was minimized by comparing the computed means of responses obtained prior to and after recovery from the test condition with the test response. In experiments conducted in the presence of 1 µM TTX and 5 mM TEA, the depolarizing voltage step elicited a robust inward Ca2+ current (ICa) that was followed by a sIAHP; the ICas evoked under control and test conditions were compared qualitatively whereas the peak amplitudes of the subsequent sIAHPs were measured and compared statistically.
To examine the effects of experimental manoeuvres on IAHP in relative isolation, the current was evoked by a previously described protocol (Stocker et al. 1999) in the presence of 1 µM TTX and 1 mM TEA to block voltage-gated Na+ channels and Ca2+ and voltage-dependent K+ channels, respectively. Given previous findings that cAMP, acting via protein kinase A, modulates the activities of the Na+H+, Na+-dependent Cl--HCO-3 and Na+-independent Cl--HCO-3 exchangers found in rat CA1 neurones and thereby changes pHi (see Brett et al. 2002), we avoided the use of cAMP analogues in the patch pipette to suppress sIAHP in these experiments (cf. Stocker et al. 1999). Rather, the decay phase of IAHP and the rising phase of sIAHP were fitted by a double exponential and sIAHP was subtracted off-line (see Fig. 3A). The double exponential had the form
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1 and
2 are the time constants of current 1 and current 2, respectively. Parameters were seeded with estimates obtained from the experimental record and allowed to run free in a Levenberg-Marquardt algorithm; r2 values were typically > 0.90.
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| Results |
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The medium and slow AHPs (and their underlying currents) recorded under whole-cell conditions may differ from those obtained with sharp microelectrodes (see Zhang et al. 1994). Initially, therefore, we performed a limited series of experiments to assess the characteristics of the AHPs and currents under our experimental conditions.
In 21 CA1 neurones impaled with sharp microelectrodes under control pHo 7.4 HCO-3/CO2-buffered conditions, Vm was -65 ± 1 mV and Rin was 27 ± 2 M
, values similar to those reported previously by this laboratory (e.g. Church & McLennan, 1989; Church, 1999) and others (e.g. Azouz et al. 1996) under similar experimental conditions. Corresponding values for Vm and Rin obtained in whole-cell patch pipette recordings (n= 48) were -55 ± 1 mV and 160 ± 4 M
, respectively. Under both recording conditions, 300 ms depolarizing current pulses elicited trains of action potentials that were followed by medium and slow AHPs (Fig. 1A and B). Despite the use of the methylsulphate anion in the pipette solution (see Zhang et al. 1994), the peak amplitudes of the medium and slow AHPs in the whole-cell patch configuration (5.2 ± 0.4 mV and 4.0 ± 0.3 mV, respectively) were significantly (P < 0.05 in each case) smaller than those obtained in sharp microelectrode recordings (medium AHP, 6.7 ± 0.9 mV; slow AHP, 5.5 ± 0.8 mV). Because of these differences, all subsequent recordings were obtained with patch pipettes in the whole-cell configuration.
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Changes in pHo modulate mIAHP and sIAHP
Lowering pHo from 7.4 to 6.7 (HCO-3/CO2-buffered conditions) significantly decreased the peak amplitudes of mIAHP and sIAHP (Fig. 2A and C). Conversely, increasing pHo from 7.4 to 7.7 significantly increased mIAHP and, to a greater extent, sIAHP (Fig. 2B and D). Corresponding changes were observed in the medium and slow AHPs recorded from the same neurones under whole-cell current-clamp conditions (data not shown; see Church, 1999). The augmented sIAHP observed at pHo 7.7 remained sensitive to manoeuvres that reduced the current at pHo 7.4. Thus, sIAHP at pHo 7.7 was reduced from 109 ± 14 pA (n= 12) to 10 ± 4 pA (n= 4) under [Ca2+]o-free conditions (Fig. 2B; the corresponding current measured in the absence of external Ca2+ at pHo 7.4 was 10 ± 3 pA; n= 2); to 10 ± 2 pA (n= 8) in the presence of 2 mM Co2+ (8 ± 2 pA at pHo 7.4; n= 14); and to 42 ± 7 pA (n= 4) by the application of 24 µM isoprenaline (at pHo 7.4, sIAHP was reduced to 30 ± 9 pA by 8 µM isoprenaline; n= 3). The results indicate that decreases and increases in pHo reduce and enhance sIAHP, respectively. However, because sIAHP overlaps temporally with mIAHP(see Storm, 1990), the potential effect of changes in pHo to modulate mIAHP is less clear. This difficulty is compounded by the fact that a number of currents, including IAHP and IM, contribute to mIAHP. Therefore, to further explore the effects of changes in pHo on mIAHP, IAHP and IM were studied in relative isolation.
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To study the effects of changes in pH on mIAHP without contributions from Ca2+-activated currents, 2 mM Co2+ was applied (Fig. 3C). The residual current observed in the presence of Co2+ at pHo 7.4 was insensitive to 100 nM apamin (n= 2; data not shown) but was reduced by 10 µM XE991 from 69 ± 10 pA to 40 ± 5 pA (a 40 ± 5% reduction; n= 4; P < 0.05; Fig. 3C), consistent with the involvement of not only IM but also other early outward currents. Decreasing pHo to 6.7 decreased the Co2+-resistant current whereas increasing pHo to 7.7 increased it (Fig. 3D). However, when pHo was reduced to 6.7 in the presence of 2 mM Co2+ and 10 µM XE991, the decline in the residual current was not significantly different (P > 0.17) to that observed in the presence of 2 mM Co2+ alone (Fig. 3D). Similarly, there was no significant difference between the increases in the Co2+-resistant current observed at pHo 7.7 in the absence and presence of 10 µM XE991 (Fig. 3D).
Taken together, the results indicate that mIAHP and sIAHP are sensitive to changes in pHo and further suggest that the effect of pHo to modulate mIAHP reflects changes in IAHP and current(s) other than IM that also contribute to the medium AHP.
Changes in pHi modulate mIAHP and sAHP
In rat CA1 neurones, changes in pHo lead to changes in pHi in the same direction (see Introduction). Therefore, we examined whether changes in pHi affect mIAHP and sIAHP and, if so, whether these effects might contribute to pHo-induced changes in the currents.
Decreasing pHi at a constant pHo.
Initially, slices were exposed to a pH 7.4 HCO-3/CO2-buffered medium containing 40 mM sodium propionate, a manoeuvre that leads to a transient fall in pHi in hippocampal neurones (Church et al. 1998; Bonnet et al. 2000). As illustrated in Fig. 4A, this manoeuvre reduced mIAHP by a maximum of 39 ± 2% and sIAHP by a maximum of 56 ± 9% (n= 3 in each case), thereby resembling the effects of reducing pHo on both currents. In contrast to the transient effects of externally applied weak acids, the transition from a HCO-3/CO2-buffered medium to a HCO-3 free medium buffered with either 30 mM Hepes or 30 mM tricine (pHo constant at 7.4) produces a transient increase in pHi (reflecting CO2 washout) followed by a sustained reduction in pHi consequent upon the blockade of HCO-3 dependent acid extrusion mechanism(s) (Church, 1992; Cowan & Martin, 1995; Bonnet et al. 1998; Brett et al. 2002). Therefore, in the next series of experiments we examined the effects of this manoeuvre on mIAHP and sIAHP; test measurements in the absence of HCO-3 were obtained
20 min after the start of perfusion with HCO-3 free medium to allow pHi to stabilize at the new lower resting level. The effects of switching to HCO-3 free Hepes- (n= 11) or tricine- (n= 2) buffered media were indistinguishable and the results were pooled.
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Given the variable effects of exposure to HCO-3 free medium on mIAHP, IAHP was studied in isolation using the protocol described earlier. Examined in the presence of 1 µM TTX and 1 mM TEA, decreasing pHi at a constant pHo significantly reduced IAHP in 5 out of 5 neurones tested (Fig. 4C). Under the same conditions, sIAHP remained sensitive to reductions in pHi, being reduced from 85 ± 15 pA to 36 ± 9 pA (a 58 ± 1% reduction) upon exposure to HCO-3 free medium (n= 5; P < 0.05). To study the effects of changes in pHi on mIAHP without contributions from Ca2+-activated currents, 2 mM Co2+ was again employed. When the transition to HCO3- free medium was conducted in the presence of 2 mM Co2+, the Co2+-resistant current was reduced in 4 out of 4 neurones tested (Fig. 4D). Four additional neurones were treated with 2 mM Co2+ and 10 µM XE991. In three of these cells, reducing pHi at a constant pHo caused a decline in the residual current that was not significantly different (P > 0.5) to the decrease observed in the presence of 2 mM Co2+ alone (Fig. 4D). Interestingly, in the remaining neurone, reducing pHi at a constant pHo caused a 15% increase in the Co2+- and XE991-resistant early outward current, an effect that may contribute to the increased mIAHP observed in 2 out of 13 cells when pHi was reduced at a constant pHo in the absence of either Co2+ or XE991 (see above).
Taken together, these observations indicate that reductions in pHi at a constant pHo inhibit sIAHP and, less consistently, mIAHP. The variable effects of low pHi on mIAHP may reflect the net effect of the pHi change on IAHP (which consistently declined, albeit to a lesser extent than sIAHP) and the Co2+- and XE991-resistant current(s) that also contribute to mIAHP (which sometimes exhibited an increase).
Increasing pHi at a constant pHo. In rat hippocampal neurones, the external application of a weak base transiently increases pHi at a constant pHo (see Church et al. 1998; Bonnet & Wiemann, 1999). Therefore, in an attempt to examine the effects of increasing pHi at a constant pHo on mIAHP and sIAHP, slices were exposed to a pH 7.4 HCO-3/CO2-buffered medium containing 40 mM TMA (n= 6). Unexpectedly, TMA reduced mIAHP and sIAHP in a manner that was independent of the increase in pHi, most likely reflecting a direct effect of TMA to block the currents (T. Kelly & J. Church, unpublished observations; also see Bruening-Wright et al. 2002). Similar results, which are reminiscent of the effects of the weak base 4-aminopyridine (Andreasen, 2002), were obtained with 40 mM NH4Cl (n= 2; also see Díaz et al. 1996). In light of these difficulties, we employed an alternative approach to assess the potential contribution of increases in pHi to the effects of increasing pHo on mIAHP and sIAHP, i.e. to prevent the change in pHi by including a high concentration of H+ buffer in the patch pipette solution.
Buffering pHi changes.
High internal H+ buffer concentrations (
50 mM) must be employed in the whole-cell configuration to effectively control pHi in the face of a change in pHo (e.g. Byerly & Moody, 1986; Korn & Horn, 1991; Kapus et al. 1993). Initially, therefore, we examined the effects of changing pHo on mIAHP and sIAHP recorded with 100 mM Hepes in the patch pipette; under these conditions, increasing pHo from 7.4 to 7.7 failed to significantly increase either mIAHP or sIAHP (P > 0.1 and P > 0.2, respectively; Fig. 5A). Although these results are consistent with the possibility that a rise in pHi consequent upon a rise in pHo contributes to the effects of increasing pHo to augment mIAHP and sIAHP, it is also apparent that mIAHP and sIAHP recorded at pHo 7.4 with 100 mM internal Hepes were significantly reduced compared to the amplitudes of the currents measured with the standard pipette solution containing 10 mM Hepes, also at pHo 7.4 (Fig. 5A and B). In turn, this raised the possibility that the lack of effect of increasing pHo on mIAHP and sIAHP recorded with 100 mM internal Hepes might simply reflect an effect of high internal [Hepes] to modify the currents (also see Wanke et al. 1979). This possibility was supported by findings that the amplitudes of mIAHP(not shown) and sIAHP (Fig. 5B) recorded at pHo 7.4 with 50 mM internal Hepes or 50 mM internal Tes (a structurally related buffer; not shown) were also significantly reduced, compared to the currents measured with 10 mM internal Hepes.
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pH effects on Ca2+ influx
Changes in pHo and pHi modulate the activities of neuronal high-voltage-activated Ca2+ channels (e.g. Tombaugh & Somjen, 1996, 1997; Church et al. 1998; Kiss & Korn, 1999). Because the modulation of sIAHP(and, to a lesser extent, mIAHP) by changes in pHo and/or pHi might simply reflect changes in Ca2+ influx through voltage-activated Ca2+ channels, we examined the effects of changes in pH on Ca2+-dependent depolarizing potentials (Ca2+ spikes) and inward Ca2+ currents recorded in the presence of 1 µM TTX and 5 mM TEA.
Current-clamp recordings. In agreement with previous reports (e.g. Higashi et al. 1990; Church, 1999), a 40100 ms depolarizing current pulse applied under control pHo 7.4 HCO-3/CO2-buffered conditions (10 mM internal Hepes) elicited a Ca2+-dependent, Co2+- and nifedipine-sensitive depolarizing potential followed by a slow AHP (see Fig. 7AC). A reduction in pHo to 6.7 significantly inhibited both the half-amplitude width of the Ca2+ spike and the peak amplitude of the subsequent slow AHP, which declined from 4.0 ± 0.4 mV to 0.3 ± 0.2 mV (n= 5; Fig. 7A and D). Conversely, as illustrated in Fig. 7B and D, at pHo 7.7 both the half-amplitude width of the Ca2+ spike and the peak amplitude of the subsequent slow AHP increased significantly (the latter from 4.0 ± 1.0 mV to 6.8 ± 1.0 mV; n= 7). Finally, slices were exposed to HCO-3 free medium to reduce pHi at a constant pHo; this manoeuvre significantly reduced the peak amplitude of the slow AHP (from 7.5 ± 0.8 mV to 3.9 ± 1.3 mV; n= 3) but, in contrast to the effect of a reduction in pHo, the half-amplitude width of the preceding Ca2+ spike was not significantly affected (Fig. 7C and D).
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Voltage-clamp recordings. Depolarizing from VH to 020 mV in the presence of 1 µM TTX and 5 mM TEA revealed a robust partially clamped inward current that could be blocked by 2 mM Co2+(n= 3) and which was followed by a sIAHP (Fig. 8A). Consistent with results obtained under current-clamp conditions, decreasing pHo to 6.7 decreased the magnitude of the Ca2+ current (ICa) in 9 out of 9 neurones examined and significantly reduced sIAHP by 76% (Figs 7D and 8A). Conversely, increasing pHo to 7.7 increased ICa in 8 out of 8 neurones and significantly enhanced sIAHP by 76% (Figs 7D and 8B). Also consistent with the current-clamp results, reducing pHi at a constant pHo by exposing slices to HCO-3 free medium significantly reduced sIAHP by 51% in 9 out of 9 neurones with little apparent change in ICa (Figs 7D and 8C).
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| Discussion |
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Effects of changes in pHo
sIAHP. Decreases and increases in pHo reduce and augment, respectively, the Ca2+ influx through high-voltage-activated Ca2+ channels that contributes to the activation of sIAHP (Lancaster & Adams, 1986; Shah & Haylett, 2000); in rat hippocampal neurones, the pHo for 50% Ca2+ channel inhibition (pK) is 7.17.2 (Tombaugh & Somjen, 1996; Church et al. 1998). In the present study, the inhibition of sIAHP observed at pHo 6.7 was associated with a reduction in Ca2+ potentials and was not significantly affected by the inclusion of 100 mM tricine in the patch pipette. These findings indicate that when pHo is reduced, decreased Ca2+ influx is primarily responsible for the attenuation of sIAHP and reductions in pHi consequent upon reductions in pHo play little or no role. In contrast, pHo 7.7-induced increases in sIAHP appeared to reflect an action of increases in pHi to modulate sIAHP downstream from any high pHo and/or high pHi-induced changes in the priming Ca2+ signal. Thus, although increasing pHo increased the magnitudes of Ca2+ potentials and sIAHP, buffering high pHo-induced pHi changes with 100 mM internal tricine significantly attenuated only the augmented sIAHP. Although it remains possible that changes in pHo might also act to modulate sIAHP directly, in no case did pHo-induced changes in sIAHP occur in the absence of parallel changes in Ca2+ potentials. In this regard we have shown previously, in outside-out patches, that changes in pHo fail to alter the unitary properties of the BK-type Ca2+-dependent K+ channel that underlies the fast AHP in rat hippocampal neurones (cf. changes in pHi; Church et al. 1998; also see Hayabuchi et al. 1998; Pedersen et al. 2000).
The differences between the ways in which low and high pHo modulate sIAHP may be due to a number of factors. Most notably, decreasing pHo to 6.7 reduced the half-width of Ca2+ potentials by 57%, compared to the 19% increase observed at pHo 7.7. These findings are consistent with the possibility that a marked decrease in Ca2+ entry at pHo 6.7 inhibits sIAHP to such an extent that any effect of a low pHo-induced reduction in pHi to further directly reduce the current is prevented. In contrast, Ca2+ entry at pHo 7.7, although increased, may remain insufficient to maximally activate sIAHP and high pHo-induced decreases in [H+]i may act to further modulate the current. The latter possibility receives support from previous findings that high pHi-induced increases in the open probability of BK-type channels in hippocampal neurones are observed only when [Ca2+]i is below saturation (Church et al. 1998; also see Copello et al. 1991; Liu et al. 1999; Pedersen et al. 2000).
mIAHP.
Like the sIAHP, mIAHP was inhibited at pHo 6.7 and increased at pHo 7.7; these effects reflected changes in IAHP and the Co2+- and XE991-resistant component of mIAHP. Although reducing pHo to 6.7 inhibited the Co2+-resistant component of mIAHP more than the Co2+- and XE991-resistant component, the difference (which represents the contribution of IM) did not reach statistical significance; similarly, increasing pHo to 7.7 augmented the Co2+-resistant and Co2+- and XE991-resistant components of mIAHP to a similar extent. The apparent insensitivity of IM to the relatively small changes in pHo (and pHi) employed in the present study is consistent with the reported pK for the effect of changes in pH to modulate the KCNQ 2/3 heteromultimers that are believed to underlie IM(pK
6.1; Prole & Marrion, 2002; also see Peretz et al. 2002).
Also like sIAHP, changes in pHi did not contribute to low pHo-induced reductions in mIAHP (although reductions in pHi at a constant pHo usually inhibited the current; see below), whereas high-pHo-induced increases in mIAHP were attenuated by including 100 mM tricine in the patch pipette. The greater effect of pHo 6.7 to reduce mIAHP (a 59% decrease) than of pHo 7.7 to increase it (by 12%) may reflect the previously mentioned larger change in Ca2+ entry in the acidic compared to the alkaline direction (with consequent effects on IAHP, which was reduced by 58% at pHo 6.7 and increased by 16% at pHo 7.7) as well as the greater sensitivity of the Co2+- and XE991-resistant component of mIAHP to acidic versus alkaline pHo shifts. Although the current(s) that underlie the Co2+- and XE991-resistant component of mIAHP remain unknown, the effects of changes in pHo (and pHi) on this current are consistent with the pH sensitivities of, for example, a variety of voltage-gated K+ channels (e.g. delayed rectifier channels) that are expressed in hippocampal neurones and may contribute to this component (see Maletic-Savatic et al. 1995; Steidl & Yool, 1999).
Effects of changes in pHi
Although reductions in pHi did not appilie low pHo-induced reductions in mIAHP and sIAHP, changes in pHi were able to modulate both currents. Thus, high pHo-induced increases and low pHi-induced decreases in mIAHP and sIAHP were significantly attenuated when internal H+ buffering power was raised by the inclusion of 100 mM tricine in the patch pipette. The latter effects were not accompanied by significant changes in Ca2+ potentials (or ICa), indicating that they are not dependent on marked alterations in Ca2+ influx (cf. the effect of reductions in pHo). Rather, the results are consistent with the possibility that, under these conditions, pHi becomes an important factor in the control of IAHP and sIAHP.
The modulation by pHi of IAHP and sIAHP is reminiscent of previous findings that protons acting on the cytoplasmic side of the membrane are potent modulators of BK-type channels in a variety of cell types (e.g. Cook et al. 1984; Kume et al. 1990; Copello et al. 1991; Laurido et al. 1991; Hayabuchi et al. 1998; Liu et al. 1999), including rat hippocampal neurones (Church et al. 1998). Internal protons have been proposed to affect BK channels either by competing with Ca2+ at regulatory binding sites (Cook et al. 1984; Kume et al. 1990; Copello et al. 1991) and/or via an allosteric site on the channel complex (Laurido et al. 1991). Although kinetic studies at the single channel level are required to determine how protons modulate IAHP and sIAHP, it is of interest that SK-type Ca2+-activated K+ channels use calmodulin (CaM) constitutively associated with the C-terminus of the SK
-subunit as their high affinity Ca2+ sensor (Xia et al. 1998). Calcium binding to CaM is pH sensitive (e.g. increasing pH from 6.5 to 7.5 increases the affinity of CaM for Ca2+ > 4-fold; Tkachuk & Men'shikov, 1981), an effect that indirectly confers a pH dependency on the many Ca2+-dependent processes that are normally regulated by CaM. This raises the possibility that protons may affect IAHP and, possibly, sIAHP by modulating Ca2+ binding to CaM, although this could not explain the pHi sensitivity of BK-type channels (which are not gated by the interaction of Ca2+ ions and CaM; see Sah & Faber, 2002). Single channel studies might also reveal the basis for the differential sensitivity of IAHP and sIAHP to changes in pHi.
Functional implications
Given that medium and slow AHPs are important determinants of neuronal excitability, the pH-dependent modulation of mIAHP and sIAHP observed in the present study would be expected to profoundly affect neuronal function. By inhibiting mIAHP and sIAHP, decreases in pHo and/or pHi would be expected to slightly depolarize neurones, reduce spike frequency adaptation and increase the number of action potentials elicited by a depolarizing current pulse, whereas increases in pHo and/or pHi would exert opposite effects. Indeed, these are precisely the consequences of changes in pHo and pHi on neuronal firing patterns reported previously in CA1 pyramids (Church & McLennan, 1989; Church, 1992, 1999) and other mammalian neurones (e.g. CO2-sensitive medullary neurones; Wiemann et al. 1998). In addition, changes in pH may modulate the link between membrane excitability and cellular metabolism that is provided by Ca2+-activated K+ channels which, when activated, act as a negative feedback mechanism that limits Ca2+ influx into neurones (see Chono et al. 2003). It has been suggested, for example, that the inhibition of voltage-activated Ca2+ channels by reductions in pHi might help to prevent excessive rises in [Ca2+]i under conditions, such as ischaemia, which are associated with an internal acidosis (e.g. Tombaugh & Somjen, 1997). The present findings suggest, however, that reductions in pHi may uncouple [Ca2+]i increases from the activation of IAHP and sIAHP (as well as IC; see Church et al. 1998) and may thereby act to offset any effect of a reduction in pHi to reduce Ca2+ flux through voltage-activated Ca2+ channels. This possibility is supported by our previous findings (Church et al. 1998) that, in contrast to changes in pHo, changes in pHi at a constant pHo fail to significantly affect the magnitudes of depolarization-evoked [Ca2+]i transients in fura-2-loaded hippocampal neurones. Conversely, augmented Ca2+-activated K+ currents may help to limit the increases in Ca2+ entry and epileptiform burst-firing that occur in the CA1 region under high pHo conditions (Church & McLennan, 1989; Church et al. 1998).
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