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Proceedings of the National Academy of Sciences of the United States of America logoLink to Proceedings of the National Academy of Sciences of the United States of America
. 1999 Jul 6;96(14):7650–7657. doi: 10.1073/pnas.96.14.7650

Calcium regulation of a slow post-spike hyperpolarization in vagal afferent neurons

Ruth Cordoba-Rodriguez *, Kimberly A Moore *, Joseph P Y Kao , Daniel Weinreich *,
PMCID: PMC33596  PMID: 10393875

Abstract

Activation of distinct classes of potassium channels can dramatically affect the frequency and the pattern of neuronal firing. In a subpopulation of vagal afferent neurons (nodose ganglion neurons), the pattern of impulse activity is effectively modulated by a Ca2+-dependent K+ current. This current produces a post-spike hyperpolarization (AHPslow) that plays a critical role in the regulation of membrane excitability and is responsible for spike-frequency accommodation in these neurons. Inhibition of the AHPslow by a number of endogenous autacoids (e.g., histamine, serotonin, prostanoids, and bradykinin) results in an increase in the firing frequency of vagal afferent neurons from <0.1 to >10 Hz. After a single action potential, the AHPslow in nodose neurons displays a slow rise time to peak (0.3–0.5 s) and a long duration (3–15 s). The slow kinetics of the AHPslow are due, in part, to Ca2+ discharge from an intracellular Ca2+-induced Ca2+ release (CICR) pool. Action potential-evoked Ca2+ influx via either L or N type Ca2+ channels triggers CICR. Surprisingly, although L type channels generate 60% of action potential-induced CICR, only Ca2+ influx through N type Ca2+ channels can trigger the CICR-dependent AHPslow. These observations suggest that a close physical proximity exists between endoplasmic reticulum ryanodine receptors and plasma membrane N type Ca2+ channels and AHPslow potassium channels. Such an anatomical relation might be particularly beneficial for modulation of spike-frequency adaptation in vagal afferent neurons.

Keywords: spike frequency adaptation, ryanodine receptor, autacoids, allergic inflammation, mast cell


Activation and sensitization of primary afferent nerve fibers during allergic inflammation are orchestrated by inflammatory mediators released from various cells, including tissue mast cells. Inflammatory mediators provoke excitability changes in sensory nerves through diverse mechanisms, including (i) modification of the density and coupling efficacy of ligand-gated ionic channels; (ii) alteration in voltage-gated sodium, potassium, and calcium channels; and (iii) manipulation of cellular mechanisms that control spike-frequency adaptation.

After immunologic activation of mast cells in airway in vivo or in sensory ganglia in vitro, a wide range of electrophysiological changes can be detected in peripheral sensory nerve terminals of the vagus (1) and in vagal primary afferent somata (located in the nodose and jugular ganglia) (2). These changes range from transient (minutes) membrane depolarizations that sometimes reach action potential (AP) threshold (3) to a sustained (days) unmasking of functional NK-2 tachykinin receptors (4, 5). One electrical membrane property that is particularly sensitive to inflammatory mediators is a slow post-spike afterhyperpolarization (AHPslow; see Fig. 1) (3). This slow afterpotential influences neuronal excitability and determines the frequency and pattern of neuronal discharge. We have found that the amplitude and duration of the AHPslow are exquisitely sensitive to known inflammatory mediators such as prostanoids, amines, and kinins applied exogenously (Table 1) or released endogenously (i.e., after immunologic activation of mast cells) (3, 6). Inhibition of the AHPslow is accompanied by a loss of spike-frequency adaptation. Thus, modulation of the AHPslow amplitude and duration provides a mechanism for neuronal sensitization.

Figure 1.

Figure 1

A single AP can evoke three types of AHP in nodose neurons. (Top) A neuron with a single-component afterpotential lasting ≈30 ms. This AHP is designated AHPfast. All neurons have this short duration afterpotential. (Middle) Example of a neuron with two afterpotentials, an AHPfast followed by a longer lasting afterpotential (≈300 ms), the AHPmedium. In approximately half of the neurons, the AHPmedium is Ca2+-dependent. (Bottom) In a subset of C fiber type nodose neurons, a slowly developing (hundreds of ms) and long-lasting (2–15 s) afterpotential is observed. This slow afterpotential (AHPslow) is always Ca2+-dependent. Intracellular recordings were obtained at room temperature from adult neurons isolated from rabbit nodose ganglia. The values near the horizontal lines are resting membrane potentials. The calibration in the Top also applies to the Middle. Similar results have been recorded in guinea pig and ferret nodose neurons.

Table 1.

Inflammatory mediators that block AHPslow in vagal afferent neurons

Mediator Receptor type EC50, nM
Bradykinin B2 72
Histamine H1 2,000
Serotonin nd 300
PGD2, PGE2 nd ∼20
Leukotriene C4 nd ∼100

Bradykinin (26), histamine (27), serotonin (28), PGD2 and PGE2 (12), and leukotriene C4 (3) block the AHPslow. nd, not determined; PG prostaglandin. 

We are interested in identifying the ionic channels and second-messenger transduction pathways that participate in the initiation and maintenance of the AHPslow in vagal primary afferent neurons. In this report, we describe the general properties of this slow afterpotential and our progress in its characterization. Our working hypothesis is that a close functional proximity between three separate channels [N type voltage-sensitive calcium channels, ryanodine (RY)-sensitive Ca2+-induced Ca2+ release (CICR) calcium channels, and AHPslow K+ (SK) channels that underlie the AHPslow] is essential for the initiation of the AHPslow.

RESULTS

General Properties of Vagal Afferent AHPslow.

The AHPslow is observed in a wide variety of peripheral and central neurons (for review, see ref. 7). In nodose neurons, AHPslow is always preceded by a fast post-spike afterhyperpolarization (AHPfast, 10–50 ms) that occurs at the end of the AP repolarization. In some neurons, the AHPfast is followed by a second afterpotential that lasts 50–300 ms (AHPmedium). The AHPmedium is voltage- and Ca2+- dependent and blocked by 10 mM tetraethylammonium in ≈50% of neurons, suggesting that it is mediated by large-conductance Ca2+-activated K+ channels (BK channels) (8).

In vagal afferent somata, the AHPslow is particularly robust. After a single AP, the AHPslow displays a delayed onset (100–500 ms), a slow rise time to peak (0.3–5 s), and a long duration (2–15 s; see Fig. 1). The proportion of AHPslow neurons within nodose ganglia varies among species: ≈20% in the guinea pig, ≈35% in rabbit, and ≈85% in ferret. Only nodose neurons classified as C fibers (conduction velocity <1 m/s) possess AHPslow. To date, there have been few species differences in the pharmacological or physiological properties of the AHPslow. An analogous slow AHP has also been recently described in ≈25% of C type dorsal root ganglion neurons of the rat (9, 10).

The AHPslow in vagal afferent neurons influences cellular excitability and controls AP frequency over the physiological range from 0.1 Hz to 10 Hz (11, 12). One interesting property of the AHPslow is that its amplitude is tuned to both AP number and frequency. Over the range of 1–100 Hz, the amplitude of the AHPslow increases with the number of APs until it plateaus after ≈15 APs (Fig. 2); similar results were observed when the current underlying the AHPslow was monitored. For reasons still unresolved, 10 Hz (100-msec interspike intervals) consistently evokes the largest responses.

Figure 2.

Figure 2

Effects of varying numbers of APs and frequency on the amplitude of the AHPslow. All data points were recorded from a single acutely dissociated adult rabbit nodose neuron at room temperature. Resting potential and membrane input resistance were −55 mV and 53 MΩ, respectively. APs were evoked by transmembrane depolarizing current pulses (2 nA, 3 ms) at the frequencies indicated. Similar results were obtained when measuring IAHP by using the hybrid voltage-clamp technique in rabbit, guinea pig, and ferret nodose neurons.

The current generating the AHPslow (IAHP) is a voltage-insensitive Ca2+-dependent K+ current (13, 14) that is unaffected by a wide range of K+ channel antagonists: 100 nM apamin, 10 μM d-tubocurarine, 5 mM Cs+, 30 mM tetraethylammonium, 10 mM Ba2+, 4 mM 4-aminopyridine, and 10 nM charybdotoxin. The magnitude of the AHPslow (or the IAHP) is linearly related to the concentration of extracellular Ca2+ (Fig. 3) and requires a rise in cytosolic free Ca2+ ([Ca2+]i) for activation. Buffering intracellular Ca2+ with 1,2-bis(2-aminophenoxy)ethane-N,N,N,N′-tetraacetic acid (BAPTA) abolishes the AHPslow (Fig. 4). Noise analysis of the IAHP suggests a single-channel conductance of ≈10 pS (unpublished observations). These features are consistent with the properties of a small-conductance Ca2+-activated K+ channel (SK channel; ref. 8). Of the several SK channels recently cloned from mammalian brain (15), the hSK1 channel has a pharmacological and biophysical profile compatible with the K+ current underlying the AHPslow in nodose neurons.

Figure 3.

Figure 3

Effects of varying [Ca2+]o on the amplitude of the AHPslow recorded in isolated nodose neurons. (A) Sample traces of AHPslow evoked by a train of four APs in the presence of different [Ca2+]o. APs are evoked by transmembrane depolarizing current pulses (2 nA, 3 ms, 10 Hz) and are truncated. [Ca2+]o was varied from 2.0 to 0.0 mM in 0.5 mM decrements. The AHPslow is completely blocked when [Ca2+]o is reduced to nominally zero. On returning to 2.0 mM [Ca2+]o, the AHPslow recovers to its original amplitude. (B) Relation between [Ca2+]o and AHPslow amplitude recorded in several neurons. Values are means ± SEM of the number of observations indicated near each data point. Data are normalized to the maximum response recorded in a given neuron. Linear regression analysis yields the solid line (r = 0.993).

Figure 4.

Figure 4

Effects of BAPTA on the AHPslow and on the excitability of an acutely dissociated rabbit nodose neuron. (A) Bath-applied BAPTA/acetomethylester (10 μM) blocks the AHPslow within 5 min without changing the resting membrane potential or membrane input resistance. APs were evoked by transmembrane depolarizing current pulses (4 nA, 1.5 ms, 10 Hz) and are truncated. (B) Responses recorded at a faster sweep speed to illustrate the kinetics of the AHPfast and AHPmedium, which precede the AHPslow. The AHPfast is unaffected by 10 μM BAPTA/acetomethylester (compare a with b). The Ca2+ dependence of the AHPmedium is illustrated in c, where the neuron is superfused with 100 μM CdCl2 for 30 s, which blocks most of the AHPmedium. The residual component of the AHP recorded in CdCl2 is the AHPfast, which is mediated by delayed rectifier K+ channels. (C) Depression of the AHPslow markedly increases neuronal excitability. The average AP firing frequency induced by a current ramp protocol (1 nA, 2 s) increased from 1 to 5.5 Hz when the AHPslow was blocked. Similar loss of spike-frequency adaptation was observed with bradykinin, prostaglandin D2, histamine, and other inflammatory autacoids (see Table 2). The scale bar represents 3 mV, 2 s in A; 15 mV, 0.25 s in B; and 15 mV, 0.5 s in C. The dashed line represents the resting membrane potential (−60 mV). Resting membrane input resistance was 70 MΩ. Data is from ref. 19 with permission from the American Physiological Society.

Ca2+ Injection Evokes Two Temporally Distinct Outward Currents.

To test whether the K+ channels associated with the AHPmedium and the AHPslow are directly activated by Ca2+, we iontophoretically injected Ca2+ into nodose neurons. Independent of the AHPslow, a large outward current with rapid activation and decay kinetics was elicited by Ca2+ injection. This current (IK-medium) was evoked at holding potentials between −2 mV and −45 mV. It was completely blocked by 5 mM tetraethylammonium but unaffected by inhibitors of the AHPslow (100 nM prostaglandins D2 or E2 or 1 μM forskolin). IK-medium was strongly voltage-dependent, requiring membrane holding potentials more positive than −55 mV. Assuming a reversal potential of −80 mV, IK-medium had an e-fold increase in peak conductance for each 8.0 ± 1.0 mV (mean ± SEM; n = 8) depolarization, as calculated from semilogarithmic plots of peak chord conductance versus voltage-clamp holding potential. These properties are similar to those of large-conductance BK (AHPmedium) channels.

In neurons that exhibited AHPslow, Ca2+ injection provoked a slowly developing and protracted outward current (IK-slow). Fig. 5 shows an overlay of the outward current responses evoked by Ca2+ injection in a single nodose C type neuron at holding potentials of −20 mV and −50 mV. The kinetic differences between IK-medium and IK-slow after Ca2+ injection are dramatic. In contrast to the rapid activation of IK-medium, the onset of IK-slow is delayed, and the decay of IK-medium is nearly complete before the peak amplitude of the IK-slow is reached. These two outward currents mirror the temporal and pharmacological differences between AHPmedium and AHPslow. IK-slow, like the AHPslow, was blocked by 100 nM prostaglandin D2. The data shown in Table 2 summarize quantitative differences between these two Ca2+-induced outward currents.

Figure 5.

Figure 5

Comparison of two outward K+ currents evoked by intracellular Ca2+ injection. Recordings were made in a single acutely isolated adult rabbit nodose neuron. A slow outward current (IK-slow) was activated by a 5-nA, 1-s iontophoretic Ca2+ injection at a holding potential of −50 mV. A second outward current (IK-medium) was activated at −20 mV (5 nA, 0.5 sec). IK-medium activates and decays completely before IK-slow reaches peak amplitude. IK-medium was blocked by 10 mM tetraethylammonium; IK-slow was blocked by 100 nM prostaglandin D2. The iontophoretic pipette was filled with a 0.2 M CaCl2 solution. Voltage-clamp currents were recorded with a second intracellular pipette. The discontinuous (switched) current injection mode of an Axoclamp II amplifier was used for both currentand voltage-clamp applications. The larger calibration value is for IK-medium. Population data is shown in Table 2.

Table 2.

Comparison of IK-slow and IK-medium

Current Peak conductance, nS n Holding potential, mV n Time-to-peak, ms n Decay time constant, ms n Duration, s n
IK-slow 27.9  ±  6.5 14 −55.4  ±  2.7 14 6,570  ±  1085 12 6,735  ±  789 5 23  ±  3.4 14
IK-medium 53.2  ±  16.5 6 −20  ±  3.7 6 958  ±  56 6 818  ±  97 6 2.5  ±  0.16 6

IK-slow and IK-medium are outward currents elicited by iontophoretic injection Ca2+ into acutely isolated nodose neurons of the rabbit. The peak conductance is the largest conductance elicited, independent of membrane potential. The holding potential is the potential at which the peak conductance was measured. The decay time constant was measured by fitting a line, by eye, to the log transform of the decay of the current. The duration was calculated from the onset of Ca2+ injection to the time at which the current had decayed to 20% of its peak value. Data are summarized as the mean ± SEM. 

It is possible that the delayed onset of IK-slow compared with IK-medium results from unequal Ca2+ diffusion distances from the injection site to the two types of K+ channels. This cause seems unlikely because the orientation of impalement was random, and the plasma membranes of dissociated nodose neurons appear devoid of processes that would provide semi-isolated regions where IK-slow might be generated. An alternative possibility is that additional intermediate steps, such as the synthesis or release of a second messenger, are required to activate IK-slow. The large Q10 (>3.0; ref. 14) supports the latter alternative. One candidate is mobilization of intracellularly stored Ca2+.

Ca2+ Released by the CICR Pool Is Essential for the Generation of the AHPslow.

Single APs produce transient increases in [Ca2+]i (ΔCat) as measured by the fluorescent indicator fura-2. The magnitude of the ΔCat depends on both [Ca2+]o and the number of APs. Over the range of one to eight APs, there is an approximately linear relation between the magnitude of the ΔCat and the number of APs (Fig. 6). In the presence of drugs that block CICR but do not significantly affect AP-induced Ca2+ influx [(RY, 10 μM), 2,5,-di(t-butyl)hydroquinone (DBHQ, 10 μM), or thapsigargin (TG, 100 nM)], we found that at least eight APs were required to evoke a detectable ΔCat (Fig. 6). In the presence of RY, DBHQ, and TG, the ΔCat–AP relation exhibits slopes of 0.5, 1.1, and 0.8 nM per AP, respectively. When compared with the slope of 9.6 nM per AP in control neurons, Ca2+ influx produced by a single nodose AP is amplified by 5- to 10-fold by CICR (16). Nodose neurons demonstrate a relatively low stimulus threshold for eliciting CICR. For instance, a robust CICR response can be observed after a single AP stimulus in nodose neurons, whereas many tens of APs are required in dorsal root ganglion neurons (17). The greater CICR response in nodose neurons is not due to greater Ca2+ influx through voltage-dependent Ca2+ channels (VDCCs); a single AP produces comparable Ca2+ influx in nodose and dorsal root ganglion neurons (39 vs. 49 pC, respectively; refs. 16 and 18). Rather, the more responsive CICR pool in nodose neurons may reflect either a closer proximity between plasma membrane Ca2+ influx channels and endoplasmic reticulum RY receptors or a more sensitive RY receptor.

Figure 6.

Figure 6

(Upper) Effect of RY on AP-induced Ca2+ transients. Traces are Ca2+ transients evoked by varying numbers of APs, as indicated below each trace. In control neurons, distinct Ca2+ transients can be elicited by very few APs. In contrast, in the presence of 10 μM RY, a CICR inhibitor, at least eight APs are required to generate a discernible change in [Ca2+]i. Suppression of the Ca2+ transient by RY is due to its effect on CICR and not the result of nonspecific effects on Ca2+ channels; the kinetics and amplitude of ICa elicited by APs are completely unaffected by RY. (Lower) Effect of RY on the relation between the amplitude of Ca2+ transients and number of APs. ○ and ● are mean amplitudes of Ca2+ transients evoked by varying numbers of action potentials for control (n = 10) and for RY-treated nodose neurons (n = 3), respectively. Linear regression of data from control (≤4 action potentials) and RY-treated cells yielded slopes of 9.6 ± 0.01 and 0.5 ± 0.23 nM per AP, respectively. Comparison of the slopes illustrates that CICR is capable of amplifying the “trigger” Ca2+ resulting from AP-induced Ca2+ influx by 20-fold. Data is modified from ref. 16 with permission from Journal of Physiology (London).

By using physiological stimuli (APs) in conjunction with pharmacological manipulations of CICR, we have demonstrated that CICR is essential for the development of the AHPslow. Over the range of 1–16 APs, the magnitudes of the AP-induced AHPslow and the ΔCat (a monitor of CICR in these neurons) were highly correlated (r = 0.985). Simultaneous recordings of ΔCat and AHPslow before and during bath application of CICR inhibitors (RY, TG, DBHQ, or 10 μM cyclopiazonic acid) revealed that both responses were blocked in a parallel fashion (Fig. 7; see also Table 1 in ref. 19). These data indicate that a CICR pool is essential for the generation of the AHPslow. They also provide a potential explanation for the slow kinetics of the AHPslow, namely Ca2+ mobilization from CICR.

Figure 7.

Figure 7

Effect of DBHQ, a functional CICR inhibitor, on the AP- induced Ca2+ transient and on the AHPslow recorded simultaneously in an acutely isolated rabbit nodose neuron. Upper traces represent superimposed Ca2+ transients evoked by a train of four APs (10 Hz) recorded in control Locke solution and 7 min after switching to Locke solution containing 10 μM DBHQ. The lower pair of traces shows AHPslow. DBHQ treatment completely blocked both the Ca2+ transient and the AHPslow. Resting [Ca2+]i was 91 nM. Fluorescence data were acquired at 10 Hz. Resting membrane potential was −67 mV. AP amplitudes are truncated. Data are from ref. 19 with permission from the American Physiological Society.

Effects of Changing [Ca2+]o on the AHPslow, ΔCat, and Ca2+ influx.

If the AHPslow depends on Ca2+ released from the CICR pool triggered by AP-induced Ca2+ influx, it would follow that changes in [Ca2+]o should produce corresponding effects on both the AHPslow and the ΔCat. The data shown in Fig. 3A illustrate the effects of progressively lowering [Ca2+]o from 2.0 mM to nominally zero on the amplitude of the AHPslow recorded in a single nodose neuron. As [Ca2+]o was decreased, the amplitude of the AHPslow was reduced proportionally. When the results from this and five additional neurons were plotted (Fig. 3B), the relation between [Ca2+]o and the amplitude of the AHPslow was linear (r = 0.993; n = 6, pooled data from three current-clamp and three hybrid voltage-clamp experiments).

Next, we examined the relation between [Ca2+]o and the magnitude of the AP-induced ΔCat. Fig. 8A illustrates ΔCats elicited by varying numbers of APs recorded from a single neuron in Locke solution containing 2.2 or 1.1 mM Ca2+. The population results relating the normalized amplitude of the ΔCats recorded in four neurons to the number of APs is shown in Fig. 8B. In 1.1 mM [Ca2+]o, the first few APs did not elicit a measurable ΔCat. For the neuron shown in Fig. 8A, at least eight APs were necessary to evoke a detectable ΔCat. In three additional neurons, the minimum number of APs necessary to elicit a detectable ΔCat ranged from 4 to 32. The ΔCat–AP relation recorded in 1.1 mM [Ca2+]o, as in Locke solution containing normal [Ca2+]o, followed a hyperbolic relation (χ2 = 6.75 and 0.31; r = 0.988 and 0.999 for 2.2 and 1.1 mM Ca2+,respectively; Fig. 8B and see also Fig. 1 in ref. 16). Given the hyperbolic nature of the ΔCat–AP relation, deducing the effects of altered [Ca2+]o on the magnitude of the ΔCat clearly depends on where along this relation the comparison is made. At one extreme, there is a ≈2-fold change when comparing the plateau phases of the curves in normal and one-half normal [Ca2+]o. It is also possible to calculate the limiting initial slopes for the rising phase of the curves (dashed lines in Fig. 8B). The limiting slopes, which represent the full Ca2+ release potential of the CICR pool before any release has actually occurred, were 15 ± 3.8 and 2 ± 0.7 nM per AP in 2.2 and 1.1 mM [Ca2+]o, respectively. Thus, reducing [Ca2+]o by a factor of 2 results in a reduction of the ΔCat by a factor of 7 ± 2.8 when the rising phases of the two curves are compared. The ≈7-fold reduction of the ΔCat associated with halving [Ca2+]o is much larger than the 2-fold reduction in the AHPslow amplitude (Fig. 3), suggesting that some, but not all, of the Ca2+ released from the CICR pool is required for the generation of the AHPslow.

Figure 8.

Figure 8

Effect of varying [Ca2+]o on the amplitude of AP -induced Ca2+ transients. (A) Representative traces of Ca2+ transients evoked by varying numbers of APs in normal (2.2 mM) and reduced (1.1 mM) [Ca2+]o. APs were elicited by transmembrane depolarizing current pulses (2 nA, 1.5 ms, 10 Hz). The number of APs is indicated below each trace. (B) The normalized (mean ± SEM) amplitude of Ca2+ transients recorded in four neurons is plotted against varying numbers of APs. Data are normalized to the maximal response recorded in a given neuron. ○ represents Ca2+ transients recorded in 2.2 mM [Ca2+]o; ● represents Ca2+ transients recorded in the same neurons in 1.1 mM [Ca2+]o. Continuous curves are rectangular hyperbolas fit to the data (χ2 = 6.75 and 0.31, r = 0.988 and 0.999 for 2.2 and 1.1 mM [Ca2+]o, respectively). The dashed lines represent the limiting initial slopes (15 ± 3.8 and 2 ± 0.7 nM per AP for 2.2 and 1.1 mM [Ca2+]o, respectively).

The disproportionate effect of reduced [Ca2+]o on the ΔCat versus the AHPslow could arise from a nonlinear reduction of Ca2+ influx per AP and/or from a decreased Ca2+ release from CICR pool per unit Ca2+ influx. To study these possibilities, we examined the effect of lowering [Ca2+]o on AP-induced Ca2+ influx. The amount of Ca2+ entering a neuron with each AP in normal and in reduced [Ca2+]o was determined by using a prerecorded AP as whole-cell voltage-clamp command under experimental conditions where the major inward charge carrier is Ca2+ (for details, see Fig. 2 in ref. 16). When [Ca2+]o was decrementally reduced from 2 mM to nominally zero, the magnitude of the ICa decreased proportionally. The charge movement caused by Ca2+ influx, normalized to cell membrane capacitance (pC/pF), was plotted against varying [Ca2+]o for 12 neurons. Over the range of 0–2.0 mM [Ca2+]o, Ca2+ influx varied linearly with [Ca2+]o (r = 0.974). These results indicate that changes in Ca2+ influx alone cannot account for the disproportionate reduction in the ΔCat relative to the AHPslow that is observed when [Ca2+]o is reduced.

The disproportionate effect of reduced [Ca2+]o on the ΔCat–AHPslow relation could arise from a diminution in the amount of Ca2+ released from the CICR pool. Caffeine, a known agonist of CICR, is traditionally used to assess the releasable content of the CICR pool. In 8 of the 13 neurons studied, halving [Ca2+]o reduced the caffeine-induced ΔCat by 20–79% (100% vs. 47 ± 7.2% in 2.2 and 1.1 mM [Ca2+]o, respectively; P = 0.0002). In other words, decreasing [Ca2+]o by a factor of 2 caused a 1.25- to 5-fold reduction in the caffeine response. On returning to normal Locke solution, the caffeine response was restored to near control values. In the remaining five neurons, the caffeine-induced ΔCat was unaffected by reducing [Ca2+]o (100% vs. 112 ± 8.4% in 2.2 and 1.1 mM [Ca2+]o, respectively; P = 0.690). There was no significant difference in resting levels of [Ca2+]i between these two groups of neurons (93 ± 29.5 nM vs. 111 ± 29.7 nM; P = 0.530). Unfortunately, the wide variability in the effects of reduced [Ca2+]o on the caffeine responses prevents a meaningful interpretation of the effect of [Ca2+]o on the releasable content of the CICR pool.

Ca2+ Influx Through N Type Calcium Channels Selectively Elicits AHPslow.

Six types of VDCCs have been described in neurons: L, N, P, Q, R, and T (20). Nodose neurons express several types of VDCCs. By using a panel of pharmacologic reagents that are selective for different types of VDCCs, we tested the contribution of each to the total AP-induced Ca2+ current. Our results, summarized in Table 3, reveal that ≈85% of the AP-induced inward Ca2+ current is shared by L and N type Ca2+ channels (Fig. 9). P, Q, and T type Ca2+ channel antagonists were ineffective, suggesting that the remaining Ca2+ current is associated with Ca2+ influx through R type channels. Nifedipine (10 μM), an L type Ca2+ channel blocker, produced no measurable effect on either the AHPfast, the AHPmedium, or the AHPslow. By contrast, ω-conotoxin-GVIA (0.5 μM), a selective N type Ca2+ channel blocker, always obliterated the AHPslow, and in ≈50% of the neurons abolished the AHPmedium (about half of the AHPmedium are Ca2+-sensitive, see above), while leaving the AHPfast unaffected (Fig. 9 and Table 4.). These results indicate that the SK and BK type K+ channels are both regulated by Ca2+ influx through N type channels. BK channels are gated by influx Ca2+ directly (8), whereas SK channels are affected by influx Ca2+ indirectly (i.e., Ca2+ entering through N type VDCC triggers RY receptors to release Ca2+ from CICR pools). Such a sequence implies a functional coupling between N type Ca2+ channels and RY channels in the endoplasmic reticulum. We tested this proposition by examining the effects of VDCC antagonists on the magnitude of AP-induced ΔCat.

Table 3.

Effects of Ca2+ channel blockers on action potential-induced inward Ca2+ currents

Channel type Channel blocker Concentration μM Reduction n
T Amiloride 500 0  ±  0 18
L Nifedipine 10 44  ±  5.6 9
P/Q ω-AGA IVA 0.2 0  ±  0 2
Q ω-CTX MVIIC 0.25 0  ±  0 6
N ω-CTX GVIA 1 40  ±  4.0 15

The blocking effect of amiloride, nifedipine, ω-agatoxin (AGA) IVA, ω-conotoxin (CTX) MVIIC, and ω-conotoxin (CTX) GVIA is expressed as percent reduction in the peak amplitude of the total calcium current ± SEM. n corresponds to the number of cells for each condition. 

Figure 9.

Figure 9

Effects of VDCC antagonists on AP-induced calcium currents, AHPslow and AP-induced Ca2+ transients. (A) Inward calcium currents recorded in isolated nodose neurons evoked by a prerecorded AP waveform from a holding potential of −60 mV. From Left to Right, control inward current in the presence of 2 mM [Ca2+]o and in the presence of 10 μM nifedipine. After reestablishing control conditions, the neuron was exposed to 1 μM ω-conotoxin-GVIA. The effects of 500 μM cadmium were recorded in another neuron; the control current for this cell was similar to the first trace. (B) AHPslow evoked by a train of four APs (10 Hz) recorded in another nodose neuron. From Left to Right, AHPslow evoked in control conditions, in the presence of 100 μM CdCl2, after washout, in the presence of 500 nM ω-conotoxin-GVIA, and after washout. (C) AP-induced Ca2+ transients recorded in two nodose neurons. From Left to Right, Ca2+ transients evoked by a train of eight APs in normal Locke solution, and in Locke solution containing 10 μM nifedipine. In another neuron, 1 μM ω-conotoxin-GVIA reduced the Ca2+ transient ≈50% (see Table 4). APs were evoked by 2.5-ms, 10-Hz depolarizing current pulses.

Table 4.

Actions of specific Ca2+ channel blockers on the action potential-induced Ca2+ transient and the AHPslow

Channel type Channel blocker Reduction, %
Ca2+ transient n AHPslow amplitude n
L Nifedipine 57  ±  7.7 21 0  ±  0 5
N ω-CTX GVIA 39  ±  6.2 4 100  ±  0 6
T, R Nickel nd 0  ±  0 5
All Cadmium 100  ±  0 2 100  ±  0 6

The following concentrations of antagonists were used: nifedipine (10 μM), ω-conotoxin GVIA (0.5 μM or 1 μM), nickel (50−500 μM), and cadmium (100 μM). nd, not determined. 

Ca2+ influx through both L and N type Ca2+ channels triggers CICR. The magnitude of the ΔCat is a sensitive indicator of Ca2+ release from the CICR pool. To determine the relative influence of Ca2+ influx through L and N type channels on release from the CICR pool, we applied selective VDCC antagonists and monitored the amplitude of ΔCat. Nifedipine (10 μM) and ω-conotoxin-GVIA (0.5–1.0 μM) diminished the amplitude of the ΔCat by 57% and 39%, respectively (Fig. 9 and Table 4). These results reveal that Ca2+ entering through either L or N type Ca2+ channels provides “trigger” Ca2+ to stimulate CICR. Given that the amount of Ca2+ influx through L and N type Ca2+ channels is comparable (44% and 40%, respectively, of total AP-induced Ca2+ influx; see Table 3), there must be a remarkable spatial arrangement between plasma membrane N type Ca2+ channels, endoplasmic reticulum RY receptors, and plasma membrane SK channels. Our working hypothesis concerning the regulation of the AHPslow by Ca2+ is illustrated schematically in Fig. 10.

Figure 10.

Figure 10

Schematic diagram of the relation between plasma membrane Ca2+ channels, BK, and SK potassium channels and endoplasmic reticulum RY receptors in primary vagal afferent neurons. Single APs evoke Ca2+ influx through L and N type VDCCs. Ca2+ influx through either of these channels can trigger release of Ca2+ from the endoplasmic reticulum via RY receptors. Whereas BK channels are activated directly by Ca2+ entering the neuron via N type VDCC, SK channels are activated indirectly. SK channels require Ca2+ from CICR pools released after Ca2+ influx through N type channels.

DISCUSSION

Whether recorded in intact vagal sensory ganglia or in acutely isolated vagal afferent somata (nodose neurons), single APs can elicit an AHPslow that exhibits a delayed onset (50–300 ms), a slow time to peak amplitude (0.3–0.5 s), and a particularly long duration (2–15 s) (14, 21). Inhibition of the AHPslow by numerous inflammatory mediators (e.g., bradykinin, prostanoids, histamine, serotonin, leukotriene C4; see Table 1) results in an increased neuronal excitability and a loss of spike-frequency adaptation. Thus, modulation of the AHPslow by these mediators provides a mechanism for peripheral nociceptor sensitization that may underlie allergic inflammation-induced hyperalgesia.

One unresolved but important mechanistic question revolves around the delayed onset and protracted duration of the AHPslow. Many of our studies of nodose AHPslow were performed with acutely dissociated adult neurons, which are essentially spherical structures lacking dendritic and axonal processes. Thus, the delayed onset of the AHPslow cannot be due to slow diffusion of Ca2+ from distal sites of influx to somal SK channels. The high temperature coefficient (Q10 > 3.0) for the rising phase and the decay time constant of the nodose AHPslow (14) also argues against simple Ca2+ diffusion as an explanation for the slow kinetics of the AHPslow. The time course of the AHPslow could arise from unusual channel kinetics of the SK channels. This also appears unlikely if SK channels in nodose neurons have activation kinetics similar to those cloned from rat brain (22). Recombinant SK channels from rat brain have activation time constants that are orders of magnitude shorter than the rise time of the AHPslow. It is more likely that the time course of the AHPslow is a consequence of the ΔCat because of CICR.

If the AHPslow is directly dependent on Ca2+ released from the CICR pool, the AHPslow and the AP-induced rise in [Ca2+]i should display similar kinetics. Quantitative kinetic comparisons between these two variables are subject to some uncertainty, because the time course of the ΔCat reflects global changes in [Ca2+ ]I, whereas the kinetics of the AHPslow are determined by events at the plasma membrane. Nonetheless, we determined the time-to-peak and 10-to-90% decay time for both the AHPslow and the ΔCat elicited by one to eight APs (19). The time-to-peak for AHPslow was significantly slower than the ΔCat by nearly a factor of a two (1.0 s vs. 1.9 s); the ΔCat also decayed more rapidly than the AHPslow (3 s vs. 7 s). Analogous temporal discrepancies have been reported between the ΔCat and AHPslow in vagal motoneurons (23). Such temporal differences suggest that Ca2+ released from CICR pools does not act alone to gate AHPslow K+ channels. Cloned SK channels contain many potential phosphorylation sites (15); Ca2+-dependent phosphorylation and/or dephosphorylation may thus be additional processes in the signal-transduction pathway of AP-evoked AHPslow.

Unambiguous data now exist showing that Ca2+ can directly activate SK channels in hippocampal neurons (24) and in Xenopus oocytes (22). In nodose neurons, it is less clear whether Ca2+ alone is sufficient to activate and sustain the AHPslow after an AP. In hippocampal neurons, flash photolysis of a “caged” Ca2+ chelator immediately truncates AP-induced AHPslow, suggesting that elevated intracellular Ca2+ is required to maintain the AHPslow (25). These results do not, however, distinguish between continuous Ca2+ gating of SK channel and the involvement of other Ca2+-dependent factors sustaining the longevity of the AHPslow. It is also possible that Ca2+-dependent factors act synergistically with Ca2+ to control SK channels (23). The nearly spherical morphology and large size of acutely isolated adult nodose neurons provide a favorable preparation to determine the nature of second messengers required to activate and sustain the AHPslow.

In conclusion, a subset of vagal primary afferent neurons possess a slowly developing and long-lasting spike afterhyperpolarization, the AHPslow, that can profoundly affect the discharge frequency of these visceral afferent neurons. Although AP-evoked Ca2+ influx via both L and N type Ca2+ channels triggers CICR, only Ca2+ flux through N type channels activates the CICR-dependent AHPslow. This type of specificity suggests that spatial coupling between N type Ca2+ channels and SK channels may be critical for the generation of the AHPslow in nodose neurons. The exact mechanism coupling ΔCat to the AHPslow current remains to be determined.

Acknowledgments

We thank our coworkers who participated in many of the experiments described in this manuscript: Drs. Akiva Cohen, Samir Jafri, and Bill Wonderlin, and Mr. Glen Taylor. The authors also thank Dr. Liz Katz and Mr. Eric Lancaster for their constructive suggestions on an earlier draft of this manuscript. This work was supported by National Institutes of Health Grants GM-46956 to J.P.Y.K., NS-22069 to D.W. and Training Grant NS-07375 to K.A.M.

ABBREVIATIONS

AP

action potential

BK

large-conductance Ca2+-activated K+ channels

SK

small-conductance Ca2+ -activated K+ channels

CICR

Ca2+-induced Ca2+ release stores

RY

ryanodine

VDCC

voltage-dependent Ca2+ channels

L

N, R, L type, N type, and R-type VDCC

AHP

afterhyperpolarization

DBHQ

2,5,-di(t-butyl)hydroquinone

References

  • 1.Undem B J, Riccio M M. In: Asthma. Barnes P J, Grunstein M M, Leff A, Woolcock A J, editors. Philadelphia: Lippincott; 1997. pp. 1009–1026. [Google Scholar]
  • 2.Weinreich D. Pulm Pharmacol. 1995;8:173–179. doi: 10.1006/pulp.1995.1023. [DOI] [PubMed] [Google Scholar]
  • 3.Undem B J, Hubbard W, Weinreich D. J Auton Nerv Syst. 1993;44:35–44. doi: 10.1016/0165-1838(93)90376-6. [DOI] [PubMed] [Google Scholar]
  • 4.Weinreich D, Moore K A, Taylor G E. J Neurosci. 1997;17:7683–7693. doi: 10.1523/JNEUROSCI.17-20-07683.1997. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 5.Moore K A, Taylor G E, Weinreich D. J Physiol (London) 1999;514(1):111–124. doi: 10.1111/j.1469-7793.1999.111af.x. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 6.Greene R, Fowler J C, MacGlashlan D, Jr, Weinreich D. J Appl Physiol. 1988;64:2249–2253. doi: 10.1152/jappl.1988.64.5.2249. [DOI] [PubMed] [Google Scholar]
  • 7.Sah P. Trends Neurosci. 1996;19:150–154. doi: 10.1016/s0166-2236(96)80026-9. [DOI] [PubMed] [Google Scholar]
  • 8.Blatz A L, Magleby K L. Trends Neurosci. 1987;10:463–467. [Google Scholar]
  • 9.Gold M S, Shuster M J, Levine J D. Neurosci Lett. 1996;205:161–164. doi: 10.1016/0304-3940(96)12401-0. [DOI] [PubMed] [Google Scholar]
  • 10.Villière V, McLachlan E M. J Physiol (London) 1996;76:1924–1941. doi: 10.1152/jn.1996.76.3.1924. [DOI] [PubMed] [Google Scholar]
  • 11.Coleridge J C G, Coleridge H M. Rev Physiol Biochem Pharmacol. 1984;99:1–110. doi: 10.1007/BFb0027715. [DOI] [PubMed] [Google Scholar]
  • 12.Weinreich D, Wonderlin W F. J Physiol (London) 1987;394:415–427. doi: 10.1113/jphysiol.1987.sp016878. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 13.Higashi H, Morita K, North R A. J Physiol (London) 1984;355:479–492. doi: 10.1113/jphysiol.1984.sp015433. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 14.Fowler J C, Greene R, Weinreich D. J Physiol (London) 1985;365:59–75. doi: 10.1113/jphysiol.1985.sp015759. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 15.Köhler M, Hirschberg B, Bond C T, Kinzie J M, Marrion N V, Adelman J P. Nature (London) 1996;273:1709–1714. doi: 10.1126/science.273.5282.1709. [DOI] [PubMed] [Google Scholar]
  • 16.Cohen A S, Moore K A, Bangalore R, Jafri M S, Weinreich D, Kao J P Y. J Physiol (London) 1997;499:315–328. doi: 10.1113/jphysiol.1997.sp021929. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 17.Shmigol A, Verkhratsky A, Isenberg G. J Physiol (London) 1995;489:627–636. doi: 10.1113/jphysiol.1995.sp021078. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 18.Scroggs R S, Fox A P. J Neurosci. 1992;12:1789–1801. doi: 10.1523/JNEUROSCI.12-05-01789.1992. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 19.Moore K A, Cohen A S, Kao J P Y, Weinreich D. J Neurophysiol. 1998;79:688–694. doi: 10.1152/jn.1998.79.2.688. [DOI] [PubMed] [Google Scholar]
  • 20.Dunlap K, Luebke J I, Turner T J. Trends Neurosci. 1995;18:89–98. [PubMed] [Google Scholar]
  • 21.Leal-Cardosa H, Koschorke G M, Taylor G, Weinreich D. J Auton Nerv Syst. 1993;45:29–39. doi: 10.1016/0165-1838(93)90359-3. [DOI] [PubMed] [Google Scholar]
  • 22.Hirschberg B, Maylie J, Adelman J P, Marrion N V. J Gen Physiol. 1998;111:565–581. doi: 10.1085/jgp.111.4.565. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 23.Lasser-Ross B, Ross W N, Yarom Y. J Neurophysiol. 1997;78:825–834. doi: 10.1152/jn.1997.78.2.825. [DOI] [PubMed] [Google Scholar]
  • 24.Marrion N V, Tavalin S J. Nature (London) 1998;395:900–905. doi: 10.1038/27674. [DOI] [PubMed] [Google Scholar]
  • 25.Lancaster B, Zucker R S. J Physiol (London) 1994;475:229–239. doi: 10.1113/jphysiol.1994.sp020064. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 26.Weinreich D, Koschorke G M, Undem B J, Taylor G E. J Physiol (London) 1995;483(3):735–746. doi: 10.1113/jphysiol.1995.sp020618. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 27.Jafri M S, Moore K A, Taylor G E, Weinreich D. J Physiol (London) 1997;503(3):533–546. doi: 10.1111/j.1469-7793.1997.533bg.x. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 28.Christian E P, Taylor G E, Weinreich D. J Appl Physiol. 1989;67:584–591. doi: 10.1152/jappl.1989.67.2.584. [DOI] [PubMed] [Google Scholar]

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