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1 Division of Neuroscience, John Curtin School of Medical Research, Australian National University, Canberra, ACT, Australia
2 Department of Physiology, Monash University, Clayton, Victoria, Australia
3 Department of Pharmacology, Graduate School of Medical Sciences, Kyushu University, Fukuoka, 812-8582, Japan
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Abstract |
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(Received 21 March 2004;
accepted after revision 11 June 2004;
first published online 11 June 2004)
Corresponding author G. D. S. Hirst: Division of Neuroscience, John Curtin School of Medical Research, Australian National University, Canberra, ACT, Australia. Email: david.hirst{at}anu.edu.au
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Introduction |
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In the stomach, ICCIM also form an essential part of the pathway by which neuronal information is transferred to smooth muscle cells, with the responses to either inhibitory or excitatory nerve stimulation being greatly attenuated in murine gastric antral and fundal tissues devoid of ICCIM (Burns et al. 1996; Ward et al. 2000; Beckett et al. 2002; Suzuki et al. 2003; Hirst & Ward, 2003). When membrane potential recordings were made from bundles of circular muscle isolated from either the antrum or fundus, the recordings were dominated by discharges of membrane noise but only if ICCIM were present (Dickens et al. 2001; Beckett et al. 2002, 2004). The membrane noise results from a discharge of spontaneous depolarizing potentials, termed unitary potentials (Edwards et al. 1999). In the gastric antrum unitary potentials result from Ca2+ release from IP3-dependent intracellular Ca2+ stores (Suzuki & Hirst, 1999; van Helden et al. 2000; Suzuki et al. 2000), followed by the activation of anion-selective channels (Hirst et al. 2002b). In the fundus unitary potentials appear to have a similar origin but the channels activated by each increase in the internal concentration of calcium ions ([Ca2+]i) differ from those in the antrum in that they are not blocked by blockers of anion selective channels (Beckett et al. 2004). In many regions of the gut, inhibitory nerve stimulation evokes a biphasic inhibitory junction potential, IJP, consisting of an apamin-sensitive fast IJP which is followed by longer-lasting, apamin-insensitive nitrergic IJP (Niel et al. 1983a; Dalziel et al. 1991; Lyster et al. 1992; He & Goyal, 1993; Zhang & Patterson, 2002; Suzuki et al. 2003). In the antrum analyses of the nitrergic component show that it results from a suppression of the resting discharge of unitary potentials by ICCIM, with neurally released nitric oxide (NO) causing the formation of cyclic GMP (Suzuki et al. 2003; Teramoto & Hirst, 2003). Similarly, analyses of antral cholinergic excitatory junction potentials indicate that they result from an increased rate of discharge of unitary potentials by ICCIM (Hirst et al. 2002c).
The present experiments were carried out with the aim of analysing the properties of IJPs recorded from the proximal colon. In this tissue inhibitory nerves preferentially innervate ICCIM (Wang et al. 2000) but the functional correlate of these structural findings is not known. The experiments reported here have reconfirmed the biphasic nature of colonic IJPs and have examined the properties of the two separate components. The results are discussed in relation to the idea that the initial component results from an increase in potassium conductance (gK) whereas the secondary nitrergic component of the IJP results from a suppression of the discharge of unitary potentials by colonic ICCIM.
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Methods |
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The procedures described were approved by the Animal Experimentation Ethics Committee at the Australian National University. Guinea-pigs of either sex, weight range 250–400 g, were stunned, exsanguinated and the proximal colon removed. The proximal colon was opened along its mesenteric border. Segments of colon were pinned out in a dissecting chamber filled with oxygenated physiological saline (composition, mM): NaCl, 120; NaHCO3, 25; NaH2PO4, 1.0; KCl, 5; MgCl2, 2; CaCl2, 2.5; and glucose, 11; bubbled with 95% O2–5% CO2. After removing the mucosa and the longitudinal muscle layer, two distinct types of preparation were made. For some experiments, sheets of tissue, approximately 5 mm square were dissected free and pinned in a recording chamber, mucosal surface downwards. For other experiments thin strips of circular muscle (diameter 80–150 µm, length 400–600 µm) were isolated as previously described (Suzuki & Hirst, 1999) and pinned in a recording chamber. These strips of tissue contained some three to five individual bundles of smooth muscle. However when recordings were made from adjacent bundles in the same strip, they appeared to be electrically isolated from each other. Thus the discharge patterns of membrane noise were different and current injected into one bundle failed to produce an electrotonic potential in the second bundle. With either preparation, intramuscular nerve terminals were stimulated using a pair of platinum stimulating electrodes, positioned one on either side of the preparation (Hirst et al. 2002c). The sheet preparations were impaled with single sharp microelectrodes (resistance 90–150 M
, filled with 0.5 M KCl). Individual bundles of muscle were impaled with two independently mounted sharp electrodes; one was used to record membrane potential changes and the other to inject current. Membrane potential changes and membrane currents were amplified using an Axoclamp-2B amplifier (Axon Instruments, Foster City, CA, USA), low pass filtered (cut-off frequency, 100 Hz) digitized and stored on computer for later analysis. During each experiment the preparation was constantly superfused with physiological saline solution warmed to 37°C; nifedipine (1 µM) was added to the physiological saline to reduce muscle contractility: atropine (1 µM) was also added to abolish the effects of stimulating excitatory cholinergic nerves. In several experiments spectral density curves were constructed from membrane potential recordings obtained from the isolated bundles of colonic muscle (see Edwards et al. 1999). In other experiments, the standard deviation time course was determined for baseline recordings and during the nitrergic IJP (Baylor & Hodgkin, 1973; Edwards et al. 1976). All data are expressed as means ± standard error of the means (S.E.M.). Student's t tests were used to determine if data sets differed, P values of less than 0.05 were taken to indicate significant differences between sets of observations.
Simulations of IJPs
A segment of a single bundle of circular muscle was assumed to be electrically isopotential so that its electrical behaviour could be modelled by a single equivalent cell. In the first instance, resting membrane conductances were represented as ohmic leaks of K+ (gK), Cl– (gCl) and Na+ (gNa) with equilibrium potentials of –90, –20 and 40 mV, respectively (Fig. 1A). Absolute values of gK (98 nS), gCl (73 nS) and gNa (30 nS) were chosen to give a resting membrane potential of –45 mV (see Results) and an input resistance of 5 M. Membrane capacitance (Cm) was set to 30 nF which gave a membrane time constant of 150 ms, close to the mean value for circular smooth muscle bundles, determined experimentally. The early purinergic component of the IJP was modelled as a transient increase in gK (Fig. 5B and C). The time course of the modulation was defined as the difference between two exponential functions, raised to a power, N:
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Iionic is the sum of resting membrane currents and transient membrane currents resulting from imposed transient membrane conductance modulations. Ielectrode represents current injected into the bundle via a microelectrode. No attempt was made to simulate the rebound depolarization that was evident in recordings of IJPs.
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, and the resting membrane potential at –45 mV. Accordingly, the resting membrane conductances were made 94 nS (gK), 56 nS (gCl) and 5 nS (gNa). Ratios between these conductance values were in approximate concordance with the permeability coefficients cited by Casteels (1969). At a resting discharge rate of 270 Hz, the mean value of gcation(t) was 42 nS, giving the equivalent cell the required input resistance and resting membrane potential. When gcation(t) was reduced to zero, the resting membrane potential hyperpolarized to –60 mV. Thus, gcation(t) contributed some 15 mV to the resting membrane potential. The purinergic K+ conductance (gKP) proposed in the first model (Fig. 1A) was made explicit in Fig. 1B and is shown connected via a switch indicating that current via this conductance was reduced to zero in the presence of apamin. Values used for gKP modulation were as in the first model. Similarly the nitrergic K+ conductance (gKN) proposed in the first model (Fig. 1A) is also made explicit in Fig. 1B and is shown connected by dashed lines indicating that it is a candidate model for the late phase of the IJP. Values used for gKN modulation were as in the first model to obtain the simulations shown in Fig. 7A. Current injection via a microelectrode was simulated by setting Ielectrode in eqn (2) to –3 nA to obtain 15 mV of hyperpolarization and to –6 nA to obtain 30 mV of hyperpolarization.
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L-Nitroarginine (NOLA) and acetoxymethyl ester tris-(2-amino-S-phenoxy) ethane-N,N,N',N'-tetracetic acid (MAPTA-AM) (obtained from Calbiochem, San Diego, CA, USA), apamin, atropine sulphate, glibenclamide, iberiotoxin (IbTX), nifedipine, niflumic acid (NFA), oxadiazolo quinoxalin-1-one (ODQ), 4,4'-diisothiocyano-2,2'-stilbene disulphonic acid (DIDS), anthracene-9-carboxylic acid (9-AC) (each obtained from Sigma Chemical Co., St Louis, MO, USA) and pyridoxalphosphate-6-azophenyl-2',4'-disulphonic acid (PPADS, obtained from Research Biochemical International, Natick, MA, USA) were used in these experiments.
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Results |
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When intracellular recordings were made from sheets of the circular layer of the proximal colon, cells had resting potentials in the range –35 to –52 mV (–44.9 ± 1.0 mV, n= 44: mean ±S.E.M., where each n value represents an observation made on a separate preparation). In most preparations the membrane potential recordings displayed an ongoing discharge of membrane noise: in a further nine preparations, which are not included in the report, regular discharges of rhythmical depolarizing potentials with amplitudes of up to 35 mV were detected. The nature of these oscillations has not been investigated further. In the quiescent preparations, when nerve terminals present in the circular layer were stimulated with a single pulse (pulse width 0.02–0.1 ms, intensity 10–70 mA) an IJP was evoked. The amplitude of the IJP could be graded by altering the stimulus strength up to a maximum value: in all experiments the stimulus strength was set some 20% higher than that used to evoke the largest amplitude IJP and left unchanged for the duration of the experiment. In control solutions IJPs, evoked by supramaximal stimuli, had a mean peak amplitude of 22.1 ± 0.9 mV (n= 44), a mean latency, defined as the time to 5% of their peak amplitudes, of 140 ± 10 ms, a mean rise time, defined as the time taken from 5 to 95% of the peak amplitudes of 190 ± 15 ms and a mean half-width, defined as the time the signals spends beyond 50% of the peak amplitude of 850 ± 40 ms (Fig. 2). Invariably the decaying phase of the IJP was interrupted by a rebound potential. We are unclear about the events underlying the rebound potential. Rebound potentials were unaffected by adding caesium ions (2 mM) or nickel ions (0.1 mM) (n= 3 for each agent) and were not triggered by periods of membrane hyperpolarization (see Fig. 3). The rebound potential was invariably abolished when both components of the IJP were abolished: on occasions the rebound potential was abolished when the slow component was abolished (Fig. 2E) but this was not always the case (Fig. 2H). This phenomenon has not been examined further. In some preparations, the rebound potential was followed by a long-lasting depolarization which persisted after the IJP had been abolished (Fig. 2D–F). This slow potential appeared to result from the release of substance P from excitatory nerves; it was abolished by desensitizing the preparations with substance P (10 µM) for 20 min (n= 3; Niel et al. 1983b; Lyster et al. 1992).
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The NOLA-resistant component of the IJP was abolished by the further addition of apamin (0.1 µM; n= 5; Fig. 2F). The NOLA-resistant component was also reduced in amplitude by PPADS, a blocker of purinergic receptors in the gut (Windscheif et al. 1995). At a concentration of 100 µM the amplitude of the NOLA-resistant component was reduced from a value of 16.8 ± 4.8 mV to 13.0 ± 4.1 mV; increasing the concentration of PPADS to 200 µM further reduced the amplitude to 6.9 ± 2.3 mV (n= 4). The effects of NOLA were not reversed by washing the preparations with drug-free solution for up to 3 h. On the other hand the effects of apamin were completely reversed by washing with drug-free solutions for 1–1.5 h. In several experiments, attempts were made to separate the two components of the IJP by varying the stimulus strength, this was never successful. Thus whatever stimulus strength was applied, a part of the biphasic response was removed by the addition of apamin to the physiological saline. Clearly if the two components result from transmitter release from two separate populations of nerve fibres, the two sets of fibres have very similar thresholds for excitation. The apamin-resistant component was unaffected by IbTX (0.1 µM; n= 3), 9-AC (1 mM; n= 3), NFA (100 µM; n= 3), or glibenclamide (10 µM; n= 3).
When intracellular recordings were made from electrically short strips of circular muscle dissected from the proximal colon, cells were found to have resting potentials in the range –37 to –47 mV (–44.0 ± 0.8 mV, n= 17). The recordings showed evidence of an ongoing discharge of membrane noise (Fig. 3B and C) whose spectral density curves could be described as for recordings from other regions of the gut (Edwards et al. 1999). Single supra-maximal stimuli evoked IJPs with similar characteristics to those recorded from sheets of tissue. When impaled with two independent electrodes, one being used to pass current and the other to record membrane potential changes, hyperpolarizing current pulses evoked electrotonic potentials whose time courses of onset, or offset, could be described with single exponentials having time constants in the range 70–300 ms (160 ± 20 ms, n= 14). Preparations had input resistances in the range 2.0–9.9 M (4.9 ± 0.7 M, n= 14). In each of the preparations tested, hyperpolarizing or depolarizing current pulses failed to evoke a regenerative response either during the periods of depolarization or after the break of periods of hyperpolarization (Fig. 3A). Moreover, unlike the antrum (Teramoto & Hirst, 2003), the discharge of membrane noise was not abolished by periods of hyperpolarization (Fig. 3A). Again, unlike the antrum, the discharge of membrane noise was unaffected by 9AC (1 mM; n= 3; Fig. 3B) or by NFA (200 µM;n= 3). However like the antrum, the discharge of membrane noise was reduced so that individual unitary potentials could be detected by adding MAPTA (20 µM) to the physiological saline for a period of 10 min: at the same time the amplitude of the power spectral density curve was reduced (Fig. 3C). This was associated with a membrane hyperpolarization, in the range 2–11 mV (7.1 ± 1.6 mV, n= 5).
Properties of IJPs recorded from the circular layer of guinea-pig proximal colon
That the IJP was made up of two separate components could also be demonstrated by adding ODQ (3 µM), an inhibitor of soluble guanylate cyclase, to the physiological saline. ODQ, like NOLA reduced the amplitude of the apamin-resistant component (Fig. 4A–C). When ODQ (3 µM) was applied before apamin the rapid component persisted and this was in turn blocked by apamin (0.1 µM; Fig. 4D–F). In these experiments, the ODQ-resistant component had a mean peak amplitude of 18.0 ± 1.4 mV (n= 8), a mean latency of 160 ± 10 ms, a mean rise time of 160 ± 5 ms and a mean half-width of 370 ± 15 ms.
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Clearly the two components of the IJP could result if two transmitters, presumably ATP and NO (Watson et al. 1996) were released by intrinsic inhibitory nerve terminals and activated two distinct sets of potassium-selective channels. For this to be the case ATP must activate an apamin-sensitive K+ channel and NO must activate a novel potassium-selective channel that is insensitive to both IbTX and glibenclamide. Alternatively, ATP could activate apamin-sensitive K+ channels and NO could produce a hyperpolarization by decreasing a resting inward current. Attempts were made to distinguish between these two possibilities by calculation (see Methods and Fig. 1A). Firstly the rapid component was attributed to a brief increase in gK and the second component was attributed to a slower-in-onset longer-lasting increase in gK (Fig. 5B). When the conductances, adjusted so that they had similar time courses and amplitudes to those of the separate components recorded experimentally, were summed, an IJP resembling that recorded from intact tissues was generated (Fig. 5A and B). In the second simulation, the rapid component was attributed to a brief increase in gK and the second component was attributed to a slower-in-onset longer-lasting decrease in gNa (Fig. 1A). Again when these two distinct conductance changes were summed together, an IJP resembling that recorded from intact tissues was generated (Fig. 5A and C). Clearly these simple simulations were unable to cast further light on the nature of the conductance changes underlying the biphasic IJP. All of the subsequent experiments were designed to test whether both components of the IJP resulted from an increase in gK, or whether the nitrergic component resulted from a decreased inward current.
Effect of changing [K+]o on IJPs recorded from the circular layer of guinea-pig proximal colon
In the first series of experiments the effect of changing the external concentration of potassium ions, [K+]o, without osmotic compensation, on the amplitudes of the two components was examined. In each experiment, the preparation was bathed in a solution containing apamin (0.1 µM) and the effect of changing [K+]o (from 5 to 2.5 mM and from 5 to 10 mM) on the amplitudes of the nitrergic component of the IJP was determined. Subsequently the preparations were washed with drug-free solution for 1.5 h and ODQ (0.3 µM) was then added to the bathing medium. The effect of changing [K+]o on the amplitudes of the purinergic component of the IJP was then determined. These changes in [K+]o had little effect on the resting membrane potential of the preparations, with the membrane potential being –39.5 ± 1.0, –42.7 ± 1.0 and –38.5 ± 0.9 mV when [K+]o was 2.5, 5 and 10 mM, respectively (n= 5). The results of one experiment are illustrated in Fig. 6A and C. It can be seen that the amplitude of the nitrergic component of the IJP, recorded in apamin, was little changed by changing [K+]o in the range 2.5–10 mM (Fig. 6A): the results from this experiment and four experiments are shown graphically in Fig. 6B. In contrast the amplitude of the purinergic component of the IJP, recorded in ODQ, increased when [K+]o was decreased and decreased when [K+]o was increased (Fig. 6C): the grouped results are plotted in Fig. 6D. Statistical analysis showed that the slope of the relationship between the amplitudes of the purinergic IJPs and [K+]o was negative, –5.2 ± 1.0 mV (pK)–1, and significantly different to zero (P < 0.01): this was not the case for the relationship between nitrergic IJPs and [K+]o.
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Effect of changing membrane potential on IJPs recorded from the circular layer of guinea-pig proximal colon
The effect of changing the membrane potential of bundles of circular muscle on the amplitude of the nitrergic component of the IJP was explored in two ways. Firstly two simulations were constructed which would predict the behaviour of nitrergic IJPs if they resulted from an increase in gK or if they resulted from a suppression of the discharge of membrane noise (see Methods and Fig. 1B). As expected the amplitudes of computed IJPs decreased as the membrane potential was made more negative when they were assumed to result from an increase in gK (Fig. 7A): when nitrergic IJPs were simulated by assuming that they resulted from a suppression of the discharge of membrane noise, they increased in amplitude as the membrane potential was made more negative (Fig. 7B). Secondly the effect of changing the membrane potential on the amplitude of nitrergic IJPs was determined experimentally by impaling a segment with two independent electrodes, one being used to pass current and the other to record membrane potential changes: in these experiments preparations were bathed in solutions containing apamin (0.1 µM) to abolish the purinergic component of the IJP. When this was done, the amplitude of the nitrergic IJP increased as the membrane potential was made more negative (Fig. 7C and D). Over the limited range of membrane potentials examined, the relationship between peak amplitude of the nitrergic IJP was well described by a straight line with, in the experiment shown in Fig. 7, an extrapolated reversal potential of +35 mV (Fig. 7D). From this and the other experiments in this series the mean reversal potential obtained by extrapolation was +12.5 ± 5.6 mV (n= 6). These experiments suggest that the nitrergic component of the IJP results from a reduction in inward current flow rather than from an increased outward flow of K+.
In the second series of experiments the effects of changing membrane potential on the time course of two component IJPs were examined. Again simulations were constructed and the results of the simulations were compared with physiological measurements. In the two simulations shown in Fig. 8 the biphasic IJP was assumed to result from two kinetically distinct increases in gK (Fig. 8A) and from an initial increase in gK augmented by a slower suppression of the discharge of membrane noise (Fig. 8B). When the effect of changing the membrane potential on simulated IJPs resulting from two separate increases in gK was examined, the amplitudes of both components were found to be reduced with no overall change in the shape, hence the time to peak amplitude of the IJP was unchanged (Fig. 8A). In contrast when the simulated IJPs resulted from an increase in gK and a suppression of membrane noise, hyperpolarization increased the time to peak of the simulated IJP as the contribution made by the initial increase in gK reduced and that made by slower suppression of inward current increased (Fig. 8B). When the effect of changing the membrane potential on the two-component IJP was determined experimentally the time to peak of the composite IJP was found to increase as the membrane potential was made more negative (Fig. 8C). In the experiment illustrated, hyperpolarizing the membrane from –47 to –77 mV increased the time to peak from 450 to 820 ms. From this and the other experiments in this series the mean time to peak was found to increase from 455 ± 25 to 650 ± 50 ms (n= 6) with a hyperpolarizing step of approximately 30 mV; these values were significantly different using a paired t test. These experiments support the idea that the purinergic and nitrergic components of the IJP result from two quite distinct changes in membrane conductance.
When recordings were made from isolated bundles of the circular layer of the proximal colon, as pointed out previously, a discharge of membrane noise was apparent. In these preparations when the nitrergic component of the IJP was inspected, it appeared to be associated with a cessation of the discharge of membrane noise (Fig. 9E). To test this idea, the standard deviation time course was determined for baseline recordings, during the nitrergic IJP and during the rebound depolarization. When this was done, the standard deviation fell during the nitrergic component of the IJP and increased during the rebound depolarization (Fig. 9G). The mean fall in the standard deviation, determined at the average peak of the nitrergic IJP (Fig. 9F) was 1.05 ± 0.3 mV (n= 5).
A fall in standard deviation during the nitrergic IJP may result from a conductance increase which had shorted out the discharge of membrane noise or if the discharge of membrane noise had been interrupted, and attempts were therefore made to distinguish between these two possibilities using a mathematical simulation. Again the nitrergic IJP was presumed to result either from an increase in gK (Fig. 9A) or from a suppression of the discharge of membrane noise (Fig. 9C). In the simulation when an increase in gK was applied, no change in the standard deviation of the membrane noise was detected (Fig. 9B). This implies that as the membrane noise is shorted out by the increase in membrane conductance, the associated hyperpolarization increases the amplitude of the membrane noise by increasing its driving potential. Conversely when the IJP was calculated to arise from a suppression of noise discharge, the standard deviation of the membrane noise fell dramatically (Fig. 9D). Together these observations indicate that the depression in standard deviation detected during the nitrergic component of the IJP is unlikely to result from an increase in gK.
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Discussion |
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Control recordings from short segments of colonic circular muscle detected an ongoing discharge of membrane noise with a characteristic frequency spectrum (Fig. 3B and C). Such spectral density curves have been obtained from the circular layer of other regions of the gastrointestinal tract but only when the preparations contain ICCIM. Thus a discharge of membrane noise is detected in the antral circular layer of control animals but not in tissues taken from W/WV mice which lack ICCIM (Dickens et al. 2001; Beckett et al. 2004). Similarly discharges of membrane noise are detected in fundal tissues which contain ICCIM but are absent in both W/WV and Sl/Sld mice, each of which lack ICCIM (Beckett et al. 2002). On this basis it seems likely that the discharge of noise detected in the colon results from ongoing activity generated by colonic ICCIM. Unlike antral ICCIM, the frequency of discharge of fundal ICCIM is little affected by changes in membrane potential, suggesting that fundal ICCIM either lack a voltage sensor or the cells are held at a membrane potential that is well away from their voltage-sensitive range (Beckett et al. 2004). The same also appears to apply to colonic ICCIM. Regenerative responses, like those detected in antral tissue were not triggered by membrane depolarization or by the releasing the ICCIM from hyperpolarized levels (Fig. 3A). Furthermore, unlike the antrum, periods of hyperpolarization failed to inhibit the discharge of membrane noise (Fig. 3A; Teramoto & Hirst, 2003). Similarly, unlike the antrum (Hirst et al. 2002b), but like the fundus (Beckett et al. 2004), the application of chloride channel blockers failed to block the discharge of membrane noise. Together these observations support the view that ICCIM in different regions of the gut may have quite distinct properties with colonic ICCIM appearing to resemble more closely those found in the fundus (Beckett et al. 2004).
Virtually all IJPs recorded from many different regions of the gut consist of two components, an initial purinergic, apamin-sensitive component, followed by a nitrergic, apamin-insensitive, component (Niel et al. 1983a; Lyster et al. 1992; He & Goyal, 1993; Teramoto & Hirst, 2003). When tested the nitrergic component has been found to be abolished by ODQ, an inhibitor of soluble guanidine cyclase (Ward et al. 1992; Teramoto & Hirst, 2003), suggesting that neurally released NO causes the formation of cyclic GMP in target cells.
When the role of ICCIM in inhibitory neurotransmission has been examined, it has been found that the nitrergic component is absent in tissues devoid of ICCIM (Burns et al. 1996; Beckett et al. 2002; Suzuki et al. 2003), suggesting that neurally released NO selectively targets ICCIM. In the antrum, neurally released NO reduces the ongoing discharge of unitary potentials by ICCIM and this results in a small hyperpolarization (Teramoto & Hirst, 2003). In the colon nitrergic nerve stimulation also causes a fall in discharge of membrane noise and this is reflected as a fall in the standard deviation of the membrane potential recordings (Fig. 9). However the nitrergic component of inhibitory responses in the colon is of much larger amplitude than those of the antrum. One explanation for this could simply be that colonic ICCIM produce a larger mean inward current than do those of the antrum. Some support for this suggestion comes from the finding that in the antrum, when the discharge of membrane noise is blocked by buffering [Ca2+]i to low levels a small depolarization is detected (Fukuta et al. 2002). This presumably reflects the balance between the suppression of inward current, generated by antral ICCIM, and the suppression of Ca2+-dependent outward currents, generated either by ICCIM or smooth muscle cells. In the colon, buffering [Ca2+]i, to low levels produce a hyperpolarization of some 7 mV (Fig. 3C). An increased contribution of inward current flow by colonic ICCIM could result from the conductance change they generate having a more positive reversal potential than that of antral ICCIM. Alternatively the density of colonic ICCIM could be higher or their rates of discharge of unitary potentials could be greater than those of antral ICCIM.
In the antrum unitary potentials involve ion channels which are blocked by chloride channel antagonists; when unitary potentials are abolished by such agents nitrergic IPJs are also abolished (Teramoto & Hirst, 2003). In the colon the discharge of membrane noise, by ICCIM, is little affected by chloride channel blockers and the nitrergic component is similarly unaffected. In the antrum hyperpolarization abolishes the resting discharge of membrane noise by ICCIM and at the same time abolishes the nitrergic component of the IJP (Teramoto & Hirst, 2003). In the colon the resting discharge of membrane noise was little changed by membrane hyperpolarization (Fig. 3) and the amplitude of the nitrergic component was increased (Fig. 7). An increase in amplitude of a hyperpolarizing synaptic potential with increased membrane polarization can most simply be explained if the hyperpolarizing potential was initiated by a decrease in conductance to an ongoing inward conductance. Whilst such a phenomenon has been described in neuronal tissues (Weight & Padjen, 1973) and in cardiac cells (Bywater et al. 1990), a similar voltage dependency of IJPs has not been demonstrated in smooth muscle preparations. This type of behaviour is, however, implicit in the suggestion that in some regions of the gut nitrergic IJPs result from a suppression of chloride conductance (Crist et al. 1991a,b; Teramoto & Hirst, 2003). In the colon the extrapolated reversal potential for the IJP was some +12.5 mV. It would be unwise to assume that this reflected the reversal potential of the conductance being inhibited by neurally released NO. Quite clearly although this will represent the functional slope conductance change for the nitrergic component of the IJP at potentials near rest, any non-linearity in the conductance/membrane potential relationship will give a different absolute reversal potential. Furthermore, it is an implicit assumption that during the experiments described here, the preparations were isopotential. If this were not the case, even without non-linearities, the extrapolated reversal potential would be in error. Having made this point, however, it is clear that current polarization did effectively change the membrane potential of the preparations under test. If this were not the case, it is difficult to see how the nitrergic IJP would increase in amplitude when the membrane was hyperpolarized (Fig. 7) and it is difficult to understand how the time course of the composite IJP would change in the expected manner with hyperpolarization (Fig. 8).
In summary, the simplest explanation for our findings is that in the colon inhibitory nerve stimulation releases two separate transmitters, ATP which activates an apamin-sensitive potassium conductance and NO which selectively targets colonic ICCIM and inhibits their resting discharge of unitary potentials. The two components can be distinguished on pharmacological grounds and on a kinetic basis with the slower nitrergic component involving the formation of a second messenger, cyclic GMP. The two components can be further distinguished on the basis of their ion selectivity in that the purinergic component involves an increase in gK whereas the nitrergic involves a decreased inflow of depolarizing current, presumably by inhibiting the discharge of unitary potentials by colonic ICCIM.
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) to the physiological saline; the resting potential of the preparation remained unchanged at –40 mV throughout. C, the discharge of membrane noise (•) was reduced by adding MAPTA-AM (20 µM; 
