Abstract
Inner hair cells (IHCs), the primary sensory receptors of the mammalian cochlea, fire spontaneous Ca2+ action potentials (APs) only before the onset of hearing. Although a role for APs in the developing auditory system has not been determined it could, by analogy with other sensory systems, guide the functional maturation of the cochlea before experience-driven activity begins. Spontaneous APs in immature IHCs are shaped by a variety of ion channels including that of the small conductance Ca2+-activated K+ current (SK2), which is only transiently expressed in immature cells. Using SK2 knockout mice we found that SK2 channels are not required for generating APs but are essential for sustaining continuous repetitive spontaneous AP activity in pre-hearing IHCs. Therefore we used this mutant mouse as a model to study possible developmental implications of disrupted AP activity. Immature mutant IHCs showed impaired exocytotic responses, which are likely to be due to the expression of fewer Ca2+ channels. Exocytosis was also impaired in adult mutant IHCs, although in this case it resulted from a reduced Ca2+ efficiency and increased Ca2+ dependence of the synaptic machinery. Since SK2 channels can only have a functional influence on IHCs during immature development and are not directly involved in neurotransmitter release, the altered Ca2+ dependence of exocytosis in adult IHCs is likely to be a consequence of their disrupted AP activity at immature stages.
The small-conductance Ca2+-activated K+ (SK) current is expressed in auditory hair cells (HCs) of various vertebrates (Tucker & Fettiplace, 1996; Yuhas & Fuchs, 1999; Oliver et al. 2000; Marcotti et al. 2004b). Although three different genes encoding SK channels have been found in the mammalian brain (SK1–SK3, Köhler et al. 1996) only SK2 type channels are present in the cochlea (Nie et al. 2004), confirming previous electrophysiological findings (Oliver et al. 2000; Katz et al. 2004; Marcotti et al. 2004b). SK channels are voltage independent and can be activated by local increases in intracellular Ca2+, which in HCs is provided by voltage-gated Ca2+ channels (Tucker & Fettiplace, 1996; Marcotti et al. 2004b), or α9α10 nAChRs (Elgoyhen et al. 2001) activated by the efferent neurotransmitter ACh (Glowatzki & Fuchs, 2000; Oliver et al. 2000). The SK2 current is expressed in both inner (IHCs) and outer (OHCs) hair cells of the mammalian cochlea although at different stages of development, corresponding to when the cells become sensitive to ACh (He & Dallos, 1999; Katz et al. 2004; Marcotti et al. 2004b). This temporal difference observed between the two cell types is most likely due to the arrival of efferent synaptic connections below the cells (Pujol et al. 1998) and the expression of nAChRs (Morley & Simmons, 2002). OHCs begin to respond to ACh (≥ P6–P8: Dulon & Lenoir, 1996; He & Dallos, 1999; Marcotti et al. 2004b) from around their onset of electromotility (He et al. 1994; Marcotti & Kros, 1999). In contrast, IHCs only respond to ACh prior to their functional maturation (≤ P12–P14: Glowatzki & Fuchs, 2000; Katz et al. 2004; Marcotti et al. 2004b), which corresponds to the onset of hearing in mice (≥ P12: Mikaelian & Ruben, 1965; Shnerson & Pujol, 1982).
During pre-hearing stages of development IHCs are capable of firing spontaneous and evoked Ca2+-dependent action potentials (Kros et al. 1998; Beutner & Moser, 2001; Marcotti et al. 2003b; Katz et al. 2004). Although action potentials mainly result from the interplay of a Ca2+ current (Cav1.3; Platzer et al. 2000) and the delayed rectifier K+ current (IK,neo, Marcotti et al. 2003a), many other transiently expressed conductances contribute to shape their activity (Marcotti et al. 2004b). Among these, the SK2 current has been shown to play a role in modulating the firing activity of evoked action potentials when activated intrinsically by voltage-gated Ca2+ channels (Marcotti et al. 2004b) or extrinsically via efferent stimulation (Goutman et al. 2005). Although the role of action potentials in immature IHCs is currently unknown it has been suggested that they could serve, in analogy with other systems (Zhang & Poo, 2001; Moody & Bosma, 2005), as a developmental tool for the functional maturation of the cochlea. The aims of this paper, using SK2 knockout mice (Bond et al. 2004), was to determine whether the absence of SK2 channels affected the spontaneous action potential activity and whether this might have an impact on the functional maturation of IHCs.
Methods
Tissue preparation
Apical-coil IHCs (n = 124) of SK2 Δ/Δ mutant mice (Bond et al. 2004) and their littermate controls (+/Δ and +/+) were studied in acutely dissected organs of Corti from postnatal day 2 (P2) to P50, where the day of birth is P0. Mice were killed by cervical dislocation in accordance with UK Home Office regulations. The cochleae were dissected in normal extracellular solution (mm): 135 NaCl, 5.8 KCl, 1.3 CaCl2, 0.9 MgCl2, 0.7 NaH2PO4, 5.6 d-glucose, 10 Hepes–NaOH. Sodium pyruvate (2 mm), amino acids and vitamins (Eagle's MEM) were also added from concentrates (Invitrogen, UK). The pH was adjusted to 7.5 (osmolality ∼308 mmol kg−1). The dissected cochleae were transferred to a microscope chamber, immobilized under a nylon mesh attached to a stainless steel ring, and continuously perfused with a peristaltic pump using the above extracellular solution. The organs of Corti were viewed using an upright microscope (Leica DMLFS, Germany) with Nomarski optics (×63 objective). In situ recordings were made by exposing the basolateral surfaces of IHCs using a suction pipette (tip diameter about 4 μm), which was filled with extracellular solution. In some experiments 300 nm apamin (Calbiochem, UK) was locally applied to block the SK current (ISK). Extracellular solutions containing drugs were applied through a multibarrelled pipette positioned near the preparation. Animals were genotyped as previously described (Bond et al. 2004).
Electrical recording
Patch clamp recordings were performed near body temperature (34–37°C) using an Optopatch amplifier (Cairn Research Ltd, UK). Patch pipettes were made from soda glass capillaries (Harvard Apparatus Ltd, UK) and had a typical resistance in extracellular solution of 2–3 MΩ. In order to reduce the electrode capacitance, patch electrodes were coated with surf wax (Mr Zoggs SexWax, USA). Patch electrodes were positioned on the IHC membrane using a PatchStar micromanipulator (Scientifica, UK). The whole-cell patch pipette filling solution was (mm): 131 KCl, 3 MgCl2, 1 EGTA–KOH, 5 Na2ATP, 5 Hepes–KOH, 10 Na2-phosphocreatine (pH 7.3, 294 mmol kg−1). The perforated-patch technique (Rae et al. 1991) was used on a few immature IHCs (n = 9) in order to support the whole-cell voltage response findings. For these experiments the pipette filling solution contained (mm): 21 KCl, 110 potassium aspartate, 3 MgCl2, 5 Na2ATP, 1 EGTA–KOH, 5 Hepes–KOH, 10 sodium phosphocreatine (pH 7.3, 295 mmol kg−1). The antibiotic amphotericin B (Calbiochem, UK) was dissolved in dry dimethylsulfoxide (DMSO) prior to its dilution into the above intracellular solution to a final concentration of 120 μg ml−1 or 240 μg ml−1 (DMSO final dilution was 1: 500 or 1: 250, respectively). The patch pipette was tip-filled with the above normal potassium aspartate intracellular solution before back-filling with the amphotericin B containing solution. This was performed in order to prevent leakage of the antibiotic into the bath prior to sealing onto the IHC membrane. Data were acquired (sampling: 5 kHz, filtering: 2.5 kHz, 8-pole Bessel) using pCLAMP software and a Digidata 1320A (Molecular Devices, USA) and stored on computer for off-line analysis (Origin: OriginLab Corp., USA; Mini Analysis Program: Synaptosoft, USA). Statistical comparisons of means (quoted ± s.e.m.) were made by Student's two-tailed t test where P < 0.05 indicates statistical significance.
Current recordings were corrected off-line for the linear leak conductance (gleak). In immature IHCs (P2–P6) gleak was typically calculated between −84 mV and −74 mV (+/+ and +/Δ: 1.3 ± 0.2 nS, n = 15; Δ/Δ: 1.5 ± 0.2 nS, n = 9), as the outward K+ currents activate positive to around −60 mV. For adult IHCs (P20) gleak (+/+ and +/Δ: 1.0 ± 0.2 nS, n = 4; Δ/Δ: 0.9 ± 0.2 nS, n = 5) was usually calculated between −84 mV and −94 mV, as the outward K+ currents IK,s and IK,f activate positive to about −80 mV. gleak was not significantly different between control and mutant IHCs. In voltage-clamp recordings, membrane potentials were corrected for residual series resistance (Rs) after compensation (immature IHCs: +/+ and +/Δ: 5.2 ± 0.4 MΩ, n = 31; Δ/Δ: 4.4 ± 0.5 MΩ, n = 19; adult: +/+ and +/Δ: 1.2 ± 0.1 MΩ, n = 4; Δ/Δ: 1.1 ± 0.1 MΩ, n = 5) and for a liquid junction potential (LJP), measured between electrode and bath solutions. The LJP was −4 mV for the KCl-based and −11 mV for the potassium aspartate-based intracellular solution. Voltage recordings in current clamp were also corrected for the LJP.
Membrane capacitance measurement
Real-time changes in membrane capacitance (ΔCm) were measured using the Optopatch as previously described (Johnson et al. 2002, 2005). Briefly, a 4 kHz sine wave of 13 mV RMS was applied to IHCs from −81 mV and was interrupted for the duration of the voltage step. The amplitude of the sine wave was chosen to be small enough not to activate any significant current since membrane capacitance measurements require a high and constant membrane resistance. The capacitance signal from the Optopatch was amplified (×50), filtered at 250 Hz, and sampled at 5 kHz. ΔCm was measured by averaging the Cm trace over a 200 ms period following the voltage step and subtracting from prepulse baseline. For these experiments the intracellular solution contained (mm): 110 caesium glutamate, 20 CsCl, 3 MgCl2, 1 EGTA-CsOH, 5 Na2ATP, 0.3 Na2GTP, 5 Hepes-CsOH, 10 Na2-phosphocreatine (pH 7.3, 294 mmol kg−1). ΔCm was recorded while applying 30 mm TEA (Fluka, UK), and additionally 300 nm apamin in immature IHCs or 60–100 μm linopirdine (Tocris, UK) in adult cells, to reduce K+ currents. In mature IHCs the Ca2+ dependence of ΔCm was studied by superfusing a Ca2+-free solution (containing 0.5 mm EGTA) or different Ca2+ concentrations (1.3, 5 and 10 mm). When the concentration of the blockers or Ca2+ that were added to or removed from the solution was > 1 mm, NaCl was adjusted to keep the osmolality constant. Membrane potentials were corrected for Rs (4.9 ± 0.1 MΩ, n = 55, P6–P50) and the LJP (−11 mV).
Results
SK2 current is required for sustaining action potential activity in immature IHCs
Before the onset of hearing, mouse IHCs generate Ca2+ APs spontaneously (Kros et al. 1998; Beutner & Moser, 2001; Marcotti et al. 2003a, 2003b). To determine whether ISK2, which is transiently expressed during immature stages, exerts a critical role in maintaining repetitive spontaneous APs, we investigated voltage responses from SK2 knockout mice (Bond et al. 2004). For these experiments early postnatal-day mice (P2–P4) were used to increase the likelihood of finding IHCs that fired spontaneous APs (Marcotti et al. 2003a). Figure 1A shows an example of spontaneous APs from an immature control IHC. Since there were no apparent differences between wild-type (+/+) and heterozygous (+/Δ) IHCs, the results from the two cell populations were pooled. Control IHCs fired spontaneous APs with a frequency of 4.2 ± 0.5 Hz (n = 12, P2–P4), similar to that previously found in IHCs from CD-1 mice (Marcotti et al. 2003b). The presence of ISK2 in control cells was confirmed by the slowly activating, apamin-sensitive current (Marcotti et al. 2004b) recorded in voltage-clamp (Fig. 1B, +/+).
Figure 1. Repetitive spontaneous action potentials in immature IHCs require ISK2.
A, spontaneous voltage responses (25 s) from a control (+/+) IHC. AP frequency: 2.7 Hz. The two insets show expanded regions of the trace above (blue and red horizontal lines). t = 20 s indicates the time from the beginning of the recording. B, currents in voltage clamp from control (+/+), mutant (Δ/Δ) and control superfused with 300 nm apamin (+/+ and Apa). Recordings were in response to a voltage step from −84 mV to −34 mV. Note the presence of the slowly activating ISK2(arrow) only in the +/+ IHC. C, spontaneous APs from a mutant (Δ/Δ) IHC. Spike frequency: 4.2 Hz (left panel) and 2.4 Hz (right panel). The time specified at the break point along the trace represents the actual time omitted from the recording, i.e. 52 s is the time that the cell remained depolarized, 1 s transition to the resting potential and 74 s time before trace resumes. D, APs from a control IHC during the superfusion of apamin. AP frequency: 3.2 Hz and 2.5 Hz. E, APs from different time points (colour coded) shown in panels A, C and D. F, AP width as a function of recording time for the cells shown above. Cell properties were, +/+: Cm 7.6 pF; Rs 6.1 MΩ; gleak 1.4 nS; Δ/Δ: Cm 8.9 pF; Rs 6.8 MΩ; gleak 1.6 nS. +/+ and Apa: Cm 8.4 pF; Rs 7.8 MΩ; gleak 1.9 nS. All recordings in this and following figures were obtained at body temperature and are single traces.
Despite the absence of ISK2 (Figs 1B, Δ/Δ), mutant IHCs were able to generate spontaneous APs (Fig. 1C) for several seconds (48 ± 12 s, n = 9, P2–P4) with a frequency of 3.4 ± 0.3 Hz. However, with time APs gradually became wider until a sustained depolarization occurred (Fig. 1C, red inset) in all P3–P4 IHCs investigated (n = 8) but in only 1 out of 7 P2 cells. This indicates that from around P2–P3 ISK is essential for sustaining continuous and rapid firing activity by providing a more robust AP repolarization. This also agrees with previous findings indicating that ISK2 becomes expressed in IHCs from around P2–P3 (Katz et al. 2004; Marcotti et al. 2004b). In addition to differences in width, mutant APs were significantly (P < 0.04) smaller in amplitude (32.6 ± 2.2 mV, n = 9, P2–P4) compared to those of control cells (39.1 ± 1.9 mV, n = 12, P2–P4). The sustained depolarization observed in mutant IHCs (which lasted for 32 ± 6 s, n = 7, P2–P4) was not permanent since they were able to repolarize completely within a few seconds and fired spontaneously again (Fig. 1C and green inset) after an additional 53 ± 10 s with a frequency of 2.3 ± 0.4 Hz. This pattern was repeated three times in one of the longest recordings made. A similar behaviour was also observed when a fully blocking concentration of apamin (300 nm), a selective blocker of SK channels (Sah & Faber, 2002), was superfused onto control IHCs (Fig. 1D). The block of ISK2 was confirmed by voltage-clamp recordings (Fig. 1B, +/+ and Apa). The change in the AP waveform with time, recorded in the three different situations (Fig. 1A, C and D), is shown in Fig. 1E. The gradual widening of APs in both mutant and control (in the presence of apamin) IHCs was evident when the width of the APs (at 20% from baseline) was plotted as a function of time (Fig. 1F). Qualitatively similar results to those shown in Fig. 1 were obtained for all cells investigated (+/+ and +/Δ: n = 13; +/+ and Apa: n = 3; Δ/Δ: n = 12). To ensure that possible differences in resting membrane potential between control and mutant IHCs did not bias our observations we studied evoked APs. In control IHCs (Fig. 2A), the frequency of APs increased with the amount of depolarizing current injection applied as previously described in CD-1 mice (Marcotti et al. 2003a). In contrast a gradual disappearance of the firing activity in mutant IHCs (Fig. 2B) and control cells superfused with apamin (Fig. 2C) was seen when current injections were applied. It is also worth noting that in control IHCs the contribution of ISK was evident by the more robust AP repolarization occurring towards the beginning of each current step (Fig. 2A, arrowheads). The absence/block of ISK, together with the progressive inactivation of IK,neo, is likely to be responsible for the gradual increase in the input resistance during large current steps (e.g. +60 pA and +70 pA in Fig. 2B and C).
Figure 2. SK2 is also essential for sustaining induced action potentials.
A–C, voltage responses induced by depolarizing current injections from control (+/Δ, A), mutant (Δ/Δ, B) and control with 300 nm apamin (+/+ and Apamin, C) immature IHCs. Current steps were applied between 0 pA and +100 pA from the resting potential, and for clarity only a few responses are shown (see values next to panels in C). Recordings of injected currents are shown above the voltage traces. Subsequent current steps were separated by about 5 s. Arrowheads in A indicate a more robust AP repolarization most likely caused by the SK2 current. +/Δ: Cm 8.8 pF; Rs 5.1 MΩ; gleak 1.0 nS; Δ/Δ: not known. +/+ and Apa: Cm 9.1 pF; Rs 1.9 MΩ.
To determine whether the whole-cell configuration, a condition that could modify the intracellular milieu, had an effect on action potential activity (Figs 1 and 2) we recorded from a few IHCs using the perforated-patch technique, a condition closer to the in vivo situation. The results shown in Fig. 3 clearly indicate that spontaneous action potentials from control and mutant IHCs (Fig. 3A and B, respectively) were comparable to those recorded in whole-cell conditions. Mutant IHCs exhibited difficulties in repolarizing completely following an AP upstroke and with time a sustained depolarization occurred (Fig. 3B). Interestingly, APs with a long-lasting ‘plateau’, as seen in whole-cell experiments (Fig. 1C), could be recorded following membrane perforation (Fig. 3B), indicating that mutant IHCs are likely to fire prolonged APs and therefore spend a considerable amount of time depolarized in vivo. It is worth noting that a persistent depolarization was never observed at the beginning of current clamp recordings. This could occur if the membrane potential cycle observed in mutant IHCs is initially reset by voltage clamping the cells near their resting potential for patch break-in/perforation. Evoked APs were also similar between whole-cell (Fig. 2A and B) and perforated patch (Fig. 3C and D) with mutant IHCs losing the ability to fire APs with time and current injection.
Figure 3. Action potentials in immature IHCs under perforated patch conditions.
A, spontaneous voltage responses (8.5 s) from a control (+/Δ) IHC. AP frequency: 6.4 Hz. The two insets show expanded regions of the trace above. Cm 10.4 pF; Rs 3.4 MΩ. B, spontaneous APs from a mutant (Δ/Δ) IHC. Spike frequency: 3.5 Hz. Cm 7.5 pF; Rs 7.3 MΩ. t = 0 in both A and B indicates the time from the beginning of the recording (immediately after membrane perforation). C and D, evoked voltage responses elicited using depolarizing current injections from control and mutant immature IHCs, respectively. Current-clamp protocol shown above the traces. +/Δ: Cm 9.1 pF; Rs 6.2 MΩ; Δ/Δ: 7.1 pF; Rs 5.8 MΩ.
Potassium currents in SK2 mutant IHCs develop normally
It has been suggested that AP activity in pre-hearing IHCs could serve as a developmental signal by influencing the expression of ion channels and other proteins within the cells themselves (Beutner & Moser, 2001; Marcotti et al. 2003a, b). Since the absence of ISK2 from mutant IHCs disrupted the normal spontaneous and evoked firing activity of immature cells (Figs 1–3), we investigated some of the cell's biophysical properties in order to verify whether they matured normally. Typical examples of outward (delayed rectifier IK,neo: Marcotti et al. 2003a) and inward (inward rectifier IK1: Marcotti et al. 1999) K+ currents characteristic of immature IHC are shown in Fig. 4. The size of both K+ currents was found to be indistinguishable between control and mutant IHCs (Fig. 4C and F and see Table 1). Although the inward Na+ current was not studied in isolation, in some recordings (e.g. Fig. 4A and B) it was seen to precede the much slower outward K+ current of both control and mutant IHCs. Table 1 also shows that the basolateral membrane properties of immature IHCs were not significantly different between control and mutant cells. Furthermore, the K+ currents characteristic of adult IHCs (Fig. 5A–C, F and G; IK,s and IK,n: Marcotti et al. 2003a, 2004a; Oliver et al. 2003; IK,f: Kros et al. 1998), voltage responses (Fig. 5D and E) and resting membrane potentials (Fig. 5H) did not differ significantly between control and mutant adult cells, indicating that the normal development of K+ currents and the general biophysical properties of IHCs were unlikely to be affected by the mutation.
Figure 4. Membrane currents in immature IHCs.
A and B, membrane currents recorded from a control (A) and a mutant (B) P3 IHC. Currents were elicited by hyperpolarizing and depolarizing voltage steps (10 mV nominal increments) from −84 mV. Actual test potentials, corrected for voltage drop across uncompensated Rs, are shown next to some of the traces. Note the presence of both Ca2+ and Na+ currents preceding the slower activating K+ current IK,neo (Marcotti et al. 2003a, 2003b). +/Δ: Cm 7.7 pF; Rs 3.8 MΩ; gleak 2.0 nS. Δ/Δ: Cm 7.4 pF; Rs 1.3 MΩ; gleak 1.3 nS. C, average steady-state current–voltage (I–V) curves for IK,neo obtained from 12 control and 7 mutant IHCs, including those shown in A and B. D and E, inwardly rectifying K+ current (IK1: Marcotti et al. 1999) in control and mutant IHCs, respectively. Current responses are from P3 IHCs recorded by using 10 mV voltage steps nominally between −44 mV and −54 mV starting from a holding potential of −64 mV. +/Δ: Cm 7.4 pF; Rs 4.6 MΩ; gleak 2.0 nS. Δ/Δ: Cm 8.1 pF; Rs 1.6 MΩ; gleak 0.6 nS. F, average I–V curves at the steady-state currents (IK,1) from control (n = 3) and mutant (n = 4) IHCs, including those shown in D and E.
Table 1.
Properties of immature apical-coil IHCs from SK2 mutant mice
+/+ and +/Δ (P2–P4) | Δ/Δ (P2–P4) | |
---|---|---|
Membrane capacitance (pF) | 7.4 ± 0.2 (21) | 7.3 ± 0.3 (15) |
Resting potential (mV) | −57.5 ± 0.8 (31) | −56.5 ± 1.1 (11) |
IK1 at −124 mV (pA) | −112 ± 12 (10) | −117 ± 20 (7) |
IK,neo at 0 mV (nA) | 3.1 ± 0.1 (12) | 3.1 ± 0.3 (12) |
g at −84 mV (nS) | 1.2 ± 0.1 (13) | 1.5 ± 0.3 (8) |
IK,neo: steady-state activation | ||
Vhalf(mV) | −32.9 ± 0.7 (12) | −33.5 ± 1.6 (7) |
Slope factor, S (mV) | 6.6 ± 0.2 (12) | 6.6 ± 0.5 (7) |
IK,neo: steady-state inactivation | ||
Vhalf(mV) | −45.1 ± 3.3 (5) | −39.4 ± 6.6 (3) |
Slope factor, S (mV) | 16.2 ± 1.4 (5) | 12.2 ± 1.5 (3) |
Steady-state activation and inactivation values (see Marcotti et al. 2003a for comparisons with normal CD-1 mice) are from fits using a first-order Boltzmann equation. Values are means ± s.e.m.; number of hair cells is in parentheses. None of the values shown above were significantly different between control and mutant IHCs.
Figure 5. Membrane currents and voltage responses in adult IHCs.
A and B, membrane currents recorded from a control (A) and a mutant (B) adult IHC (P20). Currents were elicited by hyperpolarizing and depolarizing voltage steps (10 mV nominal increments) from −64 mV. Note the presence of all three K+ currents characteristic of adult IHCs (IK,s, IK,n and IK,f). +/Δ: Vm−76 mV; Cm 13.5 pF; Rs 1.4 MΩ; gleak 1.3 nS. Δ/Δ: Vm−72 mV; Cm 13.8 pF; Rs 1.0 MΩ; gleak 1.5 nS. C, average steady-state current-voltage (I–V) curves obtained from 4 control and 5 mutant IHCs, including those shown in A and B. D and E, voltage responses under current clamp from +/Δ (D) and Δ/Δ (E) IHCs. Current steps were applied between −20 pA and +2000 pA, from the resting potential. +/Δ: Vm−72 mV; Cm 10.8 pF; Rs 1.1 MΩ; gleak 1.2 nS. Δ/Δ: same cell as in B. F, size of IK,n in +/Δ and Δ/Δ IHCs measured as the deactivating tail currents at −124 mV (difference between instantaneous and steady-state inward currents) from the holding potential of −64 mV. G, size of IK,s and IK,f in +/Δ and Δ/Δ IHCs was measured by using a voltage step to −25 mV from the holding potential of −84 mV. IK,f was measured at 1.0–1.5 ms from the start of the voltage step, a time point at which IK,s is not active (Marcotti et al. 2004a). IK,s was obtained by subtracting IK,f from the total outward current (IK,f+IK,s) measured at 160 ms. H, resting membrane potential in control and mutant IHCs. Number of cells investigated in F–H are shown in line with the columns.
Exocytosis in IHCs from SK2 mutant mice fails to mature
Since the maturation of K+ currents was normal in mutant IHCs, we investigated whether the development of ICa and the induced exocytosis was altered by the mutation. Exocytosis was estimated by measuring increases in cell membrane capacitance (ΔCm) following depolarizing voltage steps, which is generally interpreted as a sign of neurotransmitter release from presynaptic cells (Parsons et al. 1994; von Gersdorff et al. 1998; Moser & Beutner, 2000; Schnee et al. 2005). Figure 6A and B shows ICa and the corresponding ΔCm recorded in response to a 100 ms depolarizing voltage step from control and mutant immature IHCs, respectively. The ICa in pre-hearing mutant IHCs was significantly (P < 0.0005) smaller than that recorded in control cells (Fig. 6C, current–voltage (I–V) relation) and is likely to be responsible for the reduced AP amplitude observed in these cells (Fig. 1). As a consequence of the smaller ICa a significant reduction (P < 0.005) in the Ca2+-induced ΔCm (Fig. 6D, capacitance–voltage (ΔCm–V) relation) was also seen in mutant IHCs (10.4 ± 1.0 fF, n = 8, P6–P8) compared to that in control cells (37.2 ± 6.9 fF, n = 11, P6–P8).
Figure 6. Ca2+ currents and ΔCm in immature IHCs from SK2 mutant mice.
A and B, ICa (middle) and ΔCm (bottom) responses in immature control (P7 +/+) and mutant (P8 Δ/Δ) IHCs, respectively. Recordings were obtained in response to 100 ms voltage steps, in 10 mV increments, from −81 mV. For clarity, only responses at −11 mV and −81 mV are shown. The voltage protocol is shown in the top panel above the traces. +/Δ: Cm 8.5 pF; Rs 5.5 MΩ; gleak 1.4 nS. Δ/Δ: Cm 8.5 pF; Rs 5.3 MΩ; gleak 1.7 nS. C and D, average peak current–voltage (I–V) and capacitance–voltage (ΔCm–V) curves from immature IHCs (+/+ and +/Δ, n = 11; Δ/Δ, n = 8). E and F, synaptic transfer functions describing the relation between ΔCm and ICa were obtained by plotting average ΔCm against the corresponding ICa from the I–V (C) and ΔCm–V (D) curves for immature control and mutant IHCs, respectively. Single data points are also shown (grey symbols). In this and the next figure, data plotted are from values at membrane potentials from −71 mV to −21 mV. Fits to the single grey data points are according to eqn 1. R2 of the fits were 0.9 and 0.6 in control and mutant cells. G, direct comparison of the synaptic transfer functions from control and mutant IHCs in panels E and F.
Figure 6E and F shows synaptic transfer functions that show the relation between the peak ICa and exocytosis for control and mutant IHCs, at different membrane potentials (Augustine et al. 1985; Johnson et al. 2005). For the above comparison, peak ICa was preferred to the time integral since ICa is likely to be contaminated by the presence of residual unblocked K+ currents (IK,neo in immature IHCs and IK,s and IK,Ca in adult cells), which are known to be difficult to block completely (Marcotti et al. 2003a, 2004a). While slowly activating K+ currents are absent or relatively small at the peak ICa, their interference would become more prominent towards the end of the voltage steps causing variability in the apparent ICa inactivation (Fig. 6A and B; see also Johnson et al. 2005). This is particularly true when working near body temperature since the activation kinetics of the contaminating outward K+ currents become faster.
The single data points shown in Fig. 6E and F were approximated using a power function:
![]() |
(1) |
where c is a scaling coefficient and the exponent n is the power. In immature IHCs, the power obtained from fitting the single data points from each control (Fig. 6E; 2.7 ± 0.1, n = 11) and mutant (Fig. 6F; 2.7 ± 0.4, n = 8) IHC indicates that each release event requires around three Ca2+ binding steps to occur (Dodge & Rahamimoff, 1967; Johnson et al. 2005). This suggests that mutant IHCs, despite the reduced ΔCm, show a normal Ca2+ dependence of exocytosis at this stage of development (see the complete overlap of the two synaptic transfer functions: Fig. 6G).
An example of ICa and corresponding ΔCm recorded in adult control and mutant IHCs is shown in Fig. 7A and B, respectively. In contrast to immature IHCs, depolarizing voltage steps elicited a similar peak ICa between mutant and control cells (Fig. 7C) although the former showed a significantly (P < 0.0001) smaller ΔCm (Fig. 7D, mutant: 17.8 ± 1.4 fF, n = 10, P31–P49; control: 34.0 ± 2.2 fF, n = 12, P28–P50). The power value of the synaptic transfer functions in control adult cells (Fig. 7E) was 0.9 ± 0.1 (n = 13), suggesting a near linear relation between Ca2+ entry and exocytosis as previously described in normal CD-1 mice (Johnson et al. 2005). Surprisingly, the mutant transfer function (Fig. 7F) was best approximated using a power of 2.3 ± 0.2 (n = 9), significantly larger (P < 0.0001) than that found in the controls but similar to that of immature IHCs. A direct comparison of the synaptic transfer function between control and mutant IHCs is shown in Fig. 7G.
Figure 7. Ca2+ currents and ΔCm in adult SK2 mutant IHCs.
A and B, ICa and ΔCm responses in adult control (+/+ P37) and mutant (Δ/Δ P32) IHCs, respectively. Recordings were obtained as described for Fig. 6. +/+: Cm 8.3 pF; Rs 4.1 MΩ; gleak 1.9 nS. Δ/Δ: Cm 9.2 pF; Rs 4.9 MΩ; gleak 1.0 nS. C and D, average peak I–V and ΔCm–V curves, respectively, from adult IHCs (+/+ and +/Δ: P28–P50, n = 13; Δ/Δ: P31–P49, n = 9). E and F, synaptic transfer functions of adult control and mutant IHCs, respectively. Single data points are shown in grey. Fits to single data points are according to eqn (1). R2 was 0.7 and 0.9 in control and mutant cells. G, direct comparison of the synaptic transfer functions from control and mutant IHCs in panels E and F.
Since the Ca2+ dependence of exocytosis was altered in adult mutant IHCs (using physiological 1.3 mm extracellular Ca2+), we investigated this finding in greater detail by recording responses while superfusing cells with different Ca2+ concentrations (Augustine & Charlton, 1986). Changing the extracellular Ca2+ concentration over the range from zero to 10 mm gradually increased the size of both ICa and ΔCm in control (Fig. 8A, +/+) and mutant (Figs 8B, Δ/Δ) IHCs. However, in mutant IHCs the increase in ΔCm was less linear than that in control cells. Figure 8C and D shows the peak I–V (bottom panel) and ΔCm–V (top panel) curves from control and mutant IHCs, respectively. The direct relation between the size of ICa and elicited ΔCm (Fig. 8E and F) can be obtained by plotting the maximum responses in different Ca2+ concentrations and membrane potentials from each individual cell tested, similar to the synaptic transfer functions shown in Figs 6 and 7, where ICa and ΔCm were varied by membrane potential in only 1.3 mm extracellular Ca2+. The power values obtained by fitting the data using eqn (1) for control (+/+ and +/Δ,Fig. 8E) and mutant (Δ/Δ, Fig. 8F) adult IHCs were 1.2 ± 0.1 (n = 5) and 2.5 ± 0.1 (n = 4, significant at P < 0.0001), respectively, which are similar to those obtained in Fig. 7E and F. The direct comparison between the two fits is shown in Fig. 8G.
Figure 8. Ca2+ dependence of exocytosis in adult IHCs.
A and B, ICa and ΔCm responses from a control and mutant IHC during the application of different Ca2+ concentrations. +/Δ: Cm 10.7 pF; Rs 4.9 MΩ; gleak 0.7 nS. Δ/Δ: Cm 8.1 pF; Rs 5.4 MΩ; gleak 2.5 nS. C and D, average I–V (bottom) and corresponding ΔCm–V (top) curves recorded using different Ca2+ concentrations from control and mutant IHCs, respectively (+/+ and +/Δ: P28–P50, n = 5; Δ/Δ: P31–P49, n = 4). Note that for clarity the values for 0 mm Ca2+ have been omitted. E and F, synaptic transfer functions of adult control and mutant IHCs, respectively. Single data values are shown in grey. For each IHC ΔCm values are plotted against the corresponding ICa recorded between −71 mV and the membrane potential where the peak current occurred in different extracellular Ca2+ concentrations. Fits to the single data points are according to eqn (1). R2 was 0.7 and 0.9 in control and mutant cells. G, direct comparison of the synaptic transfer functions from control and mutant IHCs in panels E and F.
The altered Ca2+ dependence of exocytosis in adult SK2 mutant IHCs would theoretically affect the release kinetics of their different vesicle pools. In order to investigate this hypothesis, the rate of neurotransmitter release in mutant and control IHCs was studied by measuring ΔCm in response to depolarizing voltage steps, from 2 ms to 3 s in duration, to −11 mV from the holding potential of −81 mV (Fig. 9). This allowed us to study the emptying of different synaptic vesicle pools (Moser & Beutner, 2000; Johnson et al. 2005). While relatively short stimuli reveal the number of vesicles docked at the active zones (readily releasable pool: RRP), longer steps induce the release of vesicles from a secondarily releasable pool (SRP) that is located further away from the Ca2+ channels (von Gersdorff et al. 1996; Moser & Beutner, 2000; Beutner & Moser, 2001). Figure 9A and B shows ΔCm responses from a control and mutant adult IHC, respectively, in response to depolarizing voltage steps of varying duration using physiological 1.3 mm extracellular Ca2+. The average ΔCm responses to voltage steps of varying duration from control (P28–P31, n = 5) and mutant (P31–P32, n = 6) IHCs are shown in Fig. 9C. Similar to previous findings in normal CD-1 mice using similar recording conditions (body temperature and 1.3 mm Ca2+: Johnson et al. 2005) voltage steps of up to about 100 ms are likely to recruit mainly the RRP in both control and mutant IHCs since the increase of capacitance responses (Fig. 9D) could be approximated with a single exponential. The SRP (evident from the slower additional increase of ΔCm > 100 ms, Fig. 9C) was isolated (Fig. 9E) by subtracting the RRP. The cross-over in the size of control and mutant ΔCm responses associated with the SRP (Fig. 9C and E) is likely to reflect the higher Ca2+ dependence in mutant IHCs. The fact that mutant IHCs showed large ΔCm responses following prolonged Ca2+ entry, similar to those of control cells, indicates that the number of available vesicles and/or release sites is unlikely to be affected by the mutation in adult cells. This might also suggest that the smaller ΔCm responses observed for the RRP in mutant IHCs (Fig. 9D) could simply be due to a reduced Ca2+ efficiency of exocytosis (Figs 7 and 8) rather than a difference in the relative number of active zones and/or docked vesicles.
Figure 9. Kinetics of neurotransmitter release in control and mutant adult IHCs.
A and B, ΔCm recordings from a control (A) and a mutant (B) adult IHC in response to voltage steps (to around −11 mV) of different duration shown next to the traces. +/Δ: Cm 7.9 pF; Rs 4.7 MΩ; Δ/Δ: Cm 9.2 pF; Rs 4.9 MΩ. C, average ΔCm responses recorded for each voltage step applied (2 ms to 3 s) from control (P28–P31, n = 5) and mutant (P31–P32, n = 6) IHCs. RRP: readily releasable pool; SRP: secondarily releasable pool. D, average ΔCm responses (expanded version of the first 100 ms shown in C) approximated with a single exponential function (control: maximal ΔCm= 28 ± 2 fF, τ= 46 ± 9 ms; mutant: maximal ΔCm= 17 ± 2 fF, τ= 40 ± 13 ms). The available RRP consisted of 757 (control) and 459 (mutant) synaptic vesicles (significant at P < 0.005) using a conversion factor of 37 aF per vesicle (Lenzi et al. 1999). The initial release rate was 612 fF s−1 (16542 vesicles s−1) and 418 fF s−1 (11305 vesicles s−1) in control and mutant IHCs, respectively (not significant). E, the isolated secondarily releasable pools (where responses to the 100 ms step in C have been subtracted to zero) fitted with single exponentials (maximal ΔCm: control 189 ± 11 fF, mutant 291 ± 52 fF; τ: control 387 ± 73 ms, mutant 1163 ± 455 ms, both not significantly different) consisted of 5096 (control) and 7852 (mutant) synaptic vesicles. The initial release rates of the SRP were 487 fF s−1 (13155 vesicles s−1) and 249 fF s−1 (6732 vesicles s−1) in control and mutant IHCs, respectively. Dotted lines in D and E represent 95% confidence intervals for the fits.
Discussion
SK2 channels are essential for sustaining continuous repetitive spontaneous action potentials in pre-hearing IHCs
Small conductance Ca2+-activated K+ (SK) channels have a crucial role in modulating the excitability of neuronal cells (Bond et al. 2005). This is achieved by the ability of these channels to hyperpolarize the cell membrane potential when activated by transient and small increases in cytosolic Ca2+ resulting from the activation of voltage-gated Ca2+ channels (Tucker & Fettiplace, 1996; Marcotti et al. 2004b) or α9α10 nAChRs (Glowatzki & Fuchs, 2000; Oliver et al. 2000; Elgoyhen et al. 2001). In IHCs the SK current, which is carried by SK2 channels (Nie et al. 2004), is only transiently expressed during pre-hearing stages of development (Katz et al. 2004; Marcotti et al. 2004b). Using SK2 knockout mice (Bond et al. 2004) we have shown that repetitive spontaneous and evoked AP activity was gradually abolished when the SK2 current was absent (Figs 1C, 2B and 3B and D) or blocked by apamin (Figs 1D and 2C) leading to a sustained depolarization. Similar results, with apamin, have also been described on evoked APs from normal CD-1 mice, which was found to result from the direct coupling between SK2 and Ca2+ channels (Marcotti et al. 2004b). However, the disappearance of APs (Figs 1C and 3B) was not permanent since mutant IHCs were able to repolarize completely and fire spontaneously again. Therefore, the membrane potential of IHCs appears to cycle between periods of AP activity and maintained depolarization, probably causing periodical prolonged Ca2+ influx into these cells. Although we did not look for the presence of nAChRs in immature mutant IHCs, any efferent transmission onto these cells in vivo would, if anything, cause the cells to depolarize because of the absence of SK2 channels and most likely facilitate the appearance of wide APs and sustained depolarizations (Marcotti et al. 2004b).
Immature IHCs fire spontaneous APs from just before birth up to the end of the first postnatal week (Marcotti et al. 2003a). The generation and modulation of these APs depends on a variety of ion channels expressed in their basolateral membrane, most of which are only present transiently during pre-hearing stages of development (Housley et al. 2006). Although both Ca2+ and Na+ channels are expressed in IHCs, only the former is essential for the generation of APs (Marcotti et al. 2003b). Moreover, ICa together with a delayed rectifier K+ current (IK,neo) determines the rates of rise and fall of APs, while INa reduces the interspike interval by speeding up the time required for the membrane potential to reach spike threshold (Marcotti et al. 2003a, b). The inward rectifier K+ current IK1 is mainly involved in setting the cell's resting membrane potential (Marcotti et al. 1999). ISK2 first appears in immature IHCs at around P2–P3 (Katz et al. 2004; Marcotti et al. 2004b), a period when APs change from wide and small to become narrower and much taller (Marcotti et al. 2003a). This suggests that soon after birth the presence of ISK could be required for sustaining continuous and rapid firing activity by providing a more robust AP repolarization. Although IK,neo is initially sufficient to sustain repetitive APs, ISK2 (when activated by Ca2+ channels: Marcotti et al. 2004b) ensures IHCs repolarize completely following each AP and consequently prevents the progressive inactivation of IK,neo. A transient role for SK2 in development is not unique to IHCs since ISK2 is also known to be involved in modulating spontaneous firing activity in both retinal and cerebellar neurons where its expression is confined to early developmental stages (Klöcker et al. 2001; Cingolani et al. 2002).
Physiological consequences of the absence of SK2 channels in IHC development
Although the function of spontaneous APs in pre-hearing IHCs in currently unknown, the influx of Ca2+ during AP activity (Beutner & Moser, 2001) is likely to regulate a variety of cellular responses involved in their functional maturation (Berridge et al. 2000). Therefore, any alteration in the frequency, amplitude and duration of APs, as observed in SK2 mutants (Figs 1–3), could have major consequences on the normal developmental maturation of IHCs. In the developing nervous system spontaneous firing has been implicated in the refinement of neural circuits before the onset of externally driven activity (Zhang & Poo, 2001). In addition to this extrinsic role, spontaneous activity could also influence intrinsic cell development by modulating the expression of ion channels or other proteins implicated in normal cell maturation (Moody & Bosma, 2005). Indirect evidence for the latter has come from experiments on IHCs implying that the expression of the BK current IK,f is induced by elevations in [Ca2+]i from APs (Brandt et al. 2003). Although immature SK2 mutant IHCs expressed a smaller ICa, this is likely to be of minor relevance compared to the prolonged Ca2+ influx during sustained depolarizations (Figs 1–3). However, this Ca2+ elevation had no significant effects on the normal developmental expression of K+ currents (Figs 4 and 5) characteristic of immature (IK,neo and IK1: Marcotti et al. 2003a, 2003b) and adult (IK,n: Marcotti et al. 2003a; Oliver et al. 2003 and IK,f: Kros et al. 1998; Marcotti et al. 2004a) IHCs.
Although most of the biophysical properties were indistinguishable between control and mutant IHCs, the absence of ISK was accompanied by the abnormal development of Ca2+-induced exocytosis. In immature IHCs the similar Ca2+ dependence of exocytosis between control and mutant cells (Fig. 6) suggests that the smaller ICa and ΔCm observed in the latter is simply due to the expression of fewer Ca2+ channels compared to control cells. This is likely to result from fewer presynaptic active zones since the disrupted AP activity in these cells may not facilitate the survival of as many newly formed synaptic connections in the immature organ (Zhang & Poo, 2001; Moody & Bosma, 2005). If this is the case then the Ca2+ elevation at each active zone in pre-hearing IHCs is unlikely to be affected by the mutation, explaining the similar Ca2+ dependence observed between control and mutant IHCs (Fig. 6G). In adult IHCs while the size of ICa was similar between controls and mutants (Fig. 7) the induced ΔCm was smaller in the latter, indicating a reduction in the Ca2+ efficiency of exocytosis in mutant cells. This was also evident from the release kinetics of the readily releasable pool of vesicles (Fig. 9D). The reduced efficiency (for ICa smaller than about 150 pA; Figs 7G and 8G) in mutant IHCs resulted from a higher order Ca2+ dependence of exocytosis (power N≈ 2.3–2.5) compared to control cells (near linear: N≈ 0.9–1.2) (Figs 7 and 8). This higher order Ca2+ dependence caused exocytosis in mutant IHCs to become more Ca2+ efficient than control cells following large Ca2+ currents (> 150 pA: Fig. 8G) or prolonged stimulation (> 1.5 s: Fig. 9E). The Ca2+ dependence of exocytosis in control IHCs changes with development from a third order relation in pre-hearing IHCs (Fig. 6E) to be approximately linear in adult cells (Fig. 7E), similar to previous studies in mice (Johnson et al. 2005). A linear relation of the stimulus–secretion coupling has also been confirmed in adult mouse IHCs (Brandt et al. 2005), turtle auditory hair cells (Schnee et al. 2005) and bullfrog papillae (Keen & Hudspeth, 2006). The higher-order Ca2+ dependence of exocytosis and the lower Ca2+ efficiency in adult mutant IHCs is again indicative of a failure in the normal functional development of the exocytotic machinery, most likely caused by the disrupted AP activity (rather than the smaller ICa) in immature cells. A recent investigation has shown that the complete absence of APs in pre-hearing IHCs of Cav1.3 knockout mice did not prevent robust exocytotic responses to flash photolysis of caged Ca2+ (Brandt et al. 2003). Although these findings suggest that the presence of synaptic machinery in IHCs is unlikely to be affected by a reduced number of Ca2+ channels and/or AP activity, the Ca2+-sensitivity of exocytosis in Cav1.3 mutant cells was not determined. While the factors that lead to the developmental linearization in the Ca2+ dependence of exocytosis in normal IHCs remains unknown, the Ca2+ nanodomain control of the stimulus–secretion coupling (Brandt et al. 2005; for a recent review see Moser et al. 2006) as well as the specific expression of Ca2+ sensing molecules such as otoferlin (Roux et al. 2006), are likely to play a crucial role.
The adult cochlea is specialized to encode acoustic signals with high temporal precision over a wide dynamic range of stimuli. In order to achieve these tasks, IHCs have developed synaptic specializations named ribbon synapses (Sterling & Matthews, 2005) that allow continuous release of neurotransmitter both spontaneously and in response to changes in membrane potential. Although SK2 mutant mice are not deaf (they showed a positive Preyer's reflex, authors' personal observations), the higher Ca2+ dependence of exocytosis in IHCs would elevate the threshold for neurotransmitter release, such that they would respond less efficiently for small stimuli and thus narrow their dynamic range. The direct influence of the altered Ca2+ dependence of exocytosis on the animals hearing sensitivity has yet to be determined. A high order Ca2+ dependence of exocytosis has recently been described in adult IHCs from Beethoven and deafness mutant mice (Marcotti et al. 2006) in which the transmembrane cochlear-expressed gene 1 (tmc1) is mutated. Both mutants exhibit absent (dn) or elevated (Bth) compound action potentials (CAP), although in this case the concomitant failure in the normal development of K+ currents characteristic of adult IHCs (IK,f and IK,n) is likely to have a prominent effect on the CAP.
The data presented here indicate that SK2 channels are essential for supporting continuous repetitive spontaneous Ca2+-dependent AP activity in pre-hearing IHCs. In the absence of SK2 channels, immature IHCs expressed fewer Ca2+ channels although the Ca2+ dependence of exocytosis was normal. One possible explanation for this finding is the presence of fewer afferent synaptic contacts in immature mutant IHCs. Despite having a normal ICa, adult IHCs from SK2 mutant mice exhibited an altered (higher-order) Ca2+ dependence of exocytosis. Since SK2 channels can only have a functional influence during immature stages of development and are not directly involved in neurotransmitter release, our results suggest that the disrupted spontaneous APs in mutants could affect the normal maturation of the exocytotic machinery. The results presented here give the first indication of a possible direct link between the spontaneous firing activity of pre-hearing IHCs and their normal intrinsic development.
Acknowledgments
This work was supported by the Wellcome Trust, Deafness Research UK and The Royal Society. W.M. is a Royal Society University Research Fellow. We would like to thank J. Engel, M. C Holley and T. D. Parsons for their careful assessment of the manuscript. We would also like to thank the reviewers for their perceptive and constructive comments, M. Juusola and E. Seward for commenting on an earlier version of the manuscript and B. D. Nutton for her excellent assistance with the SK2 mice.
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