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J. Biol. Chem., Vol. 283, Issue 28, 19301-19313, July 11, 2008
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From the
Neurosciences Institute, Division of Pathology and Neuroscience, Ninewells Hospital and Medical School, University of Dundee, Dundee DD1 9SY, Scotland, United Kingdom and the
Departments of Pharmacology and Physiology and ¶Anesthesiology and Critical Care Medicine, George Washington University, Washington, D. C. 20037
Received for publication, March 27, 2008 , and in revised form, May 8, 2008.
| ABSTRACT |
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| INTRODUCTION |
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-aminobutyric acid, the exocytosis of which is enhanced by direct Ca2+ influx through the ionophore of presynaptic 5-HT3 receptors (8, 9).
5-HT3 receptors can be assembled in vitro as pentamers from a selection of five gene products, namely the 5-HT3A, 5-HT3B, 5-HT3C, 5-HT3D, and 5-HT3E subunits (10–16). The 5-HT3A subunit assembles as a functional homopentamer and is mandatory for cell surface expression of any of the other 5-HT3 receptor subunits (10, 14, 17). Only homopentameric 5-HT3A and heteropentameric 5-HT3A/5-HT3B subunit complexes have been characterized in detail (10–12). These two receptor types differ in their sensitivity to activation by 5-HT, antagonism by certain agents, and allosteric modulation by some general anesthetics and 5-substituted indole analogues (11, 12, 18, 19). Strikingly, the human homomeric 5-HT3A receptor exhibits an unusually small single channel conductance within the range of 0.3 to 1 pS (20–22), whereas the corresponding range of 16 to 30 pS for the human 5-HT3A/5-HT3B heteromer (11, 23) is more akin to the single channel conductance of most native 5-HT3 receptors and other members of the Cys-loop receptor superfamily family. Heteromeric 5-HT3A/5-HT3B receptors additionally differ from the homomeric 5-HT3A isoform by exhibiting a reduced relative permeability to Ca2+, no measurable permeability to Mg2+, faster agonist-induced desensitization kinetics, and a propensity to spontaneous channel opening (11, 12, 18). Diversity within the human 5-HT3A and 5-HT3B subunit structure occurs through alternative splicing and polymorphisms, some of which impact significantly upon receptor expression and function and are linked to human pathologies (23–25).
Cys-loop receptor subunits share a common overall topology of extracellular, transmembrane (TM), and intracellular domains, which represent functionally interacting modules (26, 27) (Fig. 1A). The TM domain consists of four
-helices (TM1–4), the second of which (TM2) lines the ion channel (26, 27). A wealth of evidence across both cation- and anion-selective channels of the Cys-loop family implicate specific amino acid residues within TM2 and the adjacent sequences as fundamental determinants of ionic selectivity and single channel conductance (2, 26, 28–30) (Fig. 1B).
Notwithstanding the importance of the TM2 domain, we have identified an additional
-helical structure (the MA helix) within the large intracellular loop linking TM3 and TM4 that greatly influences single channel conductance (2, 22, 31, 32) (Fig. 1C). In particular, the peculiarly small single channel conductance of the human homomeric 5-HT3A receptor is due to the unique presence of three arginine residues (Arg-432, Arg-436, and Arg-440) that impede cation conductance by both steric and repulsive electrostatic influences (32). The combined substitution of these residues by those aligned in the human 5-HT3B receptor subunit (i.e. R432Q, R436D, R440A, generating a construct coined 5-HT3A(QDA)) enhances single channel conductance by
40-fold (22, 33) (Fig. 1C). Importantly, arginine residues engineered into the corresponding locations of both subunit species of the nicotinic ACh
4β2 receptor depress single channel conductance (22). Such findings have been rationalized in the light of the 4 Å resolution model of the nicotinic ACh receptor of Torpedo marmorata in which the five MA-stretch helices manifest as an inverted pentagonal cone that projects from the plasma membrane into the cytoplasm forming the intracellular vestibule of the channel (26). Narrow (
8 Å) lateral windows (or "portals") situated at the subunit interfaces, which are lined by the MA helices, form an obligate pathway for ion permeation (26) (Fig. 1A).
Here, we demonstrate that residues within the MA helices also strongly affect the permeability of Ca2+ relative to monovalent ions (e.g. PCa/PCs) but do not influence charge selectivity (e.g. PNa/PCl). Additionally, we describe the influence of Ca2+ on 5-HT-evoked single channel conductance using the 5-HT3A(QDA) construct as a model, which, unlike the wild-type receptor, mediates unitary events that can be directly resolved in outside-out patch recordings. Finally, we have examined the role of an aspartate residue, located at the extracellular end of the conduction pathway, which is known to influence ionic conductance and selectivity in other Cys-loop receptors (28) and contributes to an inhibitory effect of Ca2+ on macroscopic currents mediated by 5-HT3A receptors (34). The introduction of a D293A mutation into the 5-HT3A(QDA) receptor (yielding the 5-HT3A(QDA D293A) construct) markedly suppressed PCa/PCs and reduced inwardly directed single channel conductance.
| EXPERIMENTAL PROCEDURES |
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Electrophysiological Recordings—Whole-cell and outside-out patch configurations were used to record macroscopic and single channel currents, respectively, from transfected cells. All experiments were performed at room temperature (20–23 °C). The recording chamber was routinely superfused (5 ml min–1) with an extracellular solution (E1) comprising (in mM): NaCl 140, KCl 2.8, MgCl2 2.0, CaCl2 1.0, glucose 10, HEPES 10 (pH 7.2, adjusted with 1 M NaOH; final [Na+]o = 146 mM). Patch electrodes (resistance = 2–8 megohms when measured in solution E1) were filled with an intracellular solution (I1) containing (in mM): CsCl 140, CaCl2 0.1, EGTA 1.1, HEPES 10 (pH 7.2, adjusted by 1 M CsOH, final [Cs+]i = 143 mM). In solution I2, CsCl was totally replaced by NaCl (pH 7.2, adjusted by 1 M NaOH, final [Na+]i = 145 mM). The intracellular free calcium concentration ([Ca2+]i) for I1 and I2 was estimated to be 10 nM (35). To determine the relative permeability of Na+ versus Cs+ (PNa/PCs), in solution E2, additional NaCl totally replaced KCl in the extracellular solution, and the concentrations of CaCl2 and MgCl2 were each reduced to 0.1 mM to minimize the influence of divalent cations upon the reversal potential of the macroscopic current response to 5-HT (E5-HT). The permeability of Ca2+ relative to Cs+ (PCa/PCs) was determined using an extracellular solution (E3) containing (in mM): CaCl2 100, L-histidine 5, glucose 10 (pH 7.2) (20). To prevent changes in reference electrode potential during the superfusion of media with altered ionic composition, a bridge containing 3 M KCl in agar (4% w/v) was employed. Liquid junction potentials arising at the tip of the patch pipette were measured as described by Fenwick et al. (35), and potential measurements were corrected post hoc.
E5-HT was determined by two methods. In the first, the membrane potential was stepped from –60 mV to –100 mV for 100 ms and subsequently ramped to +60 mV within 1 s at the peak of the macroscopic current response to pressure-applied 5-HT (1 µM). Care was taken to ensure that the agonist-induced current recorded at –60 mV before and immediately following the voltage ramp did not change. Subtraction of the leakage current recorded in the absence of 5-HT from the current recorded in the presence of the agonist yielded the current-voltage (I-V) relationship attributable to the 5-HT-evoked conductance increase. In the second method, peak current responses to pressure-applied 5-HT (10 µM) were recorded at steady holding potentials closely bracketing E5-HT, which was subsequently determined by interpolation. The two methods gave similar results.
Concentration-response relationships to 5-HT (0.3–100 µM) were determined from the peak inward whole-cell current response recorded in the presence of solutions E1 and I1 at a holding potential of –60 mV. The data were fitted iteratively using SigmaPlot 8 (Systat Software Inc., San Jose, CA) by an equation of the form
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Single channel currents evoked by pressure application of 5-HT (10 µM) were recorded from excised outside-out membrane patches clamped at steady holding potentials within the range of –100 to +100 mV as specified under "Results." The solutions used in such experiments were I1 and E1, E2, and E3, as appropriate. Additionally, in experiments that determined E5-HT and single channel conductance in mixtures of extracellular Na+ and Ca2+, NaCl was held at a constant concentration of 95 mM in the presence of variable concentrations of CaCl2 (10–8–3 x 10–2 M), sucrose (0–90 mM, as appropriate to maintain constant osmolarity), glucose (10 mM), and L-histidine (5 mM; pH 7.2). Currents were recorded using an Axopatch-1D amplifier (Axon Instruments, Union City, CA), low pass-filtered (5 KHz, Bessel characteristic), and recorded onto magnetic tape using a Bio-Logic DAT recorder (Bio-Logic, Claix, France) for subsequent offline analysis.
Data Analysis—Permeability ratios (relative to Cs+) were determined from measurements of E5-HT and calculated ion activities (i.e. the ionic concentration multiplied by ion activity coefficient (
ion)). The latter were estimated (following the Guggenheim convention) to be:
Cs 0.72 (140 mM Cs+)
Na 0.76 (140 mM Na+), and
Ca 0.26 (100 mM Ca2+). For varying concentrations of Ca2+ in the presence of 95 mM Na+, the mean molal activity coefficients for CaCl2 in the presence of 100 mM NaCl, as tabulated by Butler (36), allowed calculation of
Ca. Sucrose had a negligible influence upon
Na over the range of sugar concentrations employed (37). The permeability ratio PNa/PCs was calculated from the Goldman-Hodgkin-Katz (voltage) equation,
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The permeability ratio, PCa/PCs, was calculated from a modified Goldman-Hodgkin-Katz (voltage) equation (38) which, with both Na+ and Ca2+ present as permeant species in the extracellular medium but only Cs+ and negligible Ca2+ present in the pipette (`intracellular') solution, can be written as (20)
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When Ca2+ was the sole cation in the extracellular medium, the term PNa/PCs was omitted. For simplicity, in the text we routinely refer to ion concentrations (in square brackets) rather than activities (in parentheses), although the latter were used in all calculations of relative permeability and are presented in the figures where relevant.
Single channel currents were low pass-filtered offline at 1 KHz, digitized at 10 KHz via a DigiData 1302A (Axon Instruments) interface. Using the WinEDR V2 7.6 electrophysiology data recorder (J. Dempster, Dept. of Physiology and Pharmacology, University of Strathclyde, UK), single channel current amplitude histograms were constructed from sections of single channel activity in which unitary events predominated. A transition detection threshold of 30–40% of the predominant unitary event amplitude was employed to capture events for inclusion within the amplitude histogram. Events less than 1 ms in duration (classified as incompletely resolved), obvious artifacts, and those corresponding to multiple openings were rejected. The resulting mean open state amplitude histogram was fitted using an iterative least squares algorithm with a single Gaussian probability density function from which unitary event amplitude (i) was determined. The analysis was restricted to the dominant unitary current state, as events of differing amplitude were relatively rare. Single channel conductance (
) is routinely reported as the chord conductance, i.e.
= i/(Vm – E5-HT), where Vm is the holding potential (including liquid junction potential correction) and E5-HT is the reversal potential of the agonist-evoked macroscopic response determined as described above under the appropriate ionic conditions.
Statistical Analysis—Data are presented as mean ± S.E. Statistical analysis was conducted using one-way analysis of variance with the post hoc Dunnett or Tukey test as appropriate. A value of p < 0.05 was considered significant.
| RESULTS |
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In subsequent experiments, we evaluated the contributions of the individual mutations R432Q (MA –4'), R436D (MA 0'), and R440A (MA 4') to the enhancement of PCa/ PCs. The R436D charge reversal mutation produces an
6-fold increase in single channel conductance compared with the wild-type 5-HT3A receptor (22). The 5-HT3A(R436D) receptor also had a significantly enhanced relative permeability to Ca2+ (PCa/PCs = 3.13 ± 0.31, n = 7, Fig. 3A, Table 1). By contrast, the introduction of aspartate did not significantly affect PNa/PCs compared with wild-type 5-HT3A receptors (Fig. 3A, Table 1). Notably, the PCa/PCs of the 5-HT3A(QDA) receptor was not significantly greater than that of the 5-HT3A(R436D) receptor. The individual replacement of Arg-432 by the equivalent 5-HT3B subunit residue glutamine had no significant effect on single channel conductance (22). Likewise, the permeability of Ca2+ relative to Cs+ of the 5-HT3A(R432Q) mutant was similar to that of the wild-type 5-HT3A receptor, suggesting that this MA helix residue has little influence on ion selectivity (Fig. 3A, Table 1). Substitution of Arg-440 residue by alanine significantly increased single channel conductance (22). Although the 5-HT3A(R440A) mutant exhibited a trend toward an increased PCa/PCs ratio relative to the wild-type receptor, the effect failed to reach statistical significance (Fig. 3A, Table 1).
The validity of the above estimates of PNa/PCs and PCa/PCs for the 5-HT3A(QDA) receptor construct relies upon the mutant retaining the near perfect cation versus anion selectivity of the wild-type receptor (PNa/PCl = 53) (30). We tested this assumption rigorously by dilution experiments in which the NaCl content of the extracellular solution E2 was reduced to 95, 50, and 20 mM by replacement with sucrose. Under such conditions a plot of E5-HT as a function of the logarithm of extracellular Na+ activity, (Na+)o, was linear and yielded a slope of 59 mV/decade change in (Na+)o (Fig. 3B). A similar dependence upon (Na+)o was observed under simplified bi-ionic conditions in which Na+ totally replaced Cs+ within the intracellular solution. Because only a slope of less than 58 mV/decade change in (Na+)o is compatible with anion permeation (28), we concluded that for the 5-HT3A(QDA) receptor construct PNa/PCl =
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The foregoing results indicate that the arginine residues present at positions 436 (MA 0') and to a lesser extent 440 (MA 4') of the human wild-type 5-HT3A receptor collectively suppress the permeability of Ca2+, but not Na+, relative to Cs+, revealing that the large intracellular loop of a Cys-loop receptor is an important determinant of divalent versus monovalent cation selectivity.
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With Na+ as the predominant extracellular cation, the single channel current-voltage relationship (i-V) for the 5-HT3A (QDA) receptor shows a very mild outward rectification over a wide range of holding potentials (–100 to 100 mV) and yields chord conductance levels of 46 and 40 pS at holding potentials of +100 and –100 mV, respectively (Fig. 4, A and B). The latter is slightly larger than previously reported by us (22); this minor difference is due to the reduced concentration of divalent cations in the extracellular medium E2. Inclusion of 1 mM Ca2+ and 2 mM Mg2+ (medium E1) also yielded an essentially linear i-V relationship but with a slope conductance corresponding to our previous estimate (22).
In contrast to the mild outward rectification of the i-V relationship observed with Na+, when Ca2+ was the sole extracellular cation, 5-HT-evoked single channel events mediated by the 5-HT3A(QDA) receptor displayed marked outward rectification (Fig. 4, A and B) similar to that seen in whole-cell current recordings (Fig. 2C). At all negative holding potentials, single channel current amplitudes were greatly reduced in comparison to when Na+ was the permeant cation. At the most negative potential studied (–100 mV), where it can be assumed that single channel currents reflect inward movement of Ca2+ with little opposing outwardly directed monovalent cation flux, a single channel chord conductance of 5.7 pS was calculated, assuming an E5-HT of 9.4 mV obtained from macroscopic currents recorded under identical ionic conditions. The disparity between single channel current amplitudes recorded in Na+- and Ca2+-containing solutions decreased as the holding potential was progressively shifted to more positive values (Fig. 4, A and B). This is most clearly appreciated by inspection of Fig. 4C, which plots unitary current amplitude against driving force (i.e. holding potential minus E5-HT). Indeed, at the most positive potentials examined, where an outwardly directed flux of Cs+ predominates, single channel current amplitudes were indistinguishable between Na+- and Ca2+ - based extracellular solutions (Fig. 4C). The data indicate that the 5-HT3A(QDA) receptor construct, despite selecting for Ca2+ over Na+, conducts the former less efficiently, thus predicting that extracellular Ca2+ will (at negative holding potentials) reduce single channel conductance in mixtures of Na+ and Ca2+ as we previously inferred for the human wild-type 5-HT3A receptor by fluctuation analysis (20).
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65% over the range [Ca2+]o = 0.1 mM (41.3 ± 0.88 pS) to [Ca2+]o = 30 mM (14.8 ± 0.63 pS; Fig. 5, B and C). However, it should be noted that Ca2+ will itself contribute to inward current amplitude, particularly at high [Ca2+]o. For this reason the calculation of an IC50 value for the suppressant effect of Ca2+ upon single channel conductance was inappropriate. A simple interpretation of such data is that Ca2+ reduces single channel conductance by binding to a site(s) of comparatively low affinity within the permeation pathway and thereby occludes the flux of Na+. In agreement with such a violation of the independent movement of Na+ and Ca2+ within the permeation pathway, the ratio PCa/PCs was found to be concentration-dependent. With [Na+]o fixed at 95 mM (and assuming PNa/PCs = 0.9; see above), PCa/PCs was calculated from determinations of E5-HT to be 0.5 and 1.8 in the presence of 10 and 30 mM extracellular Ca2+, respectively, versus the value of 3.7 found with Ca2+ as the sole extracellular charge carrier. Extracellular Ca2+ Reduces Single Channel Conductance of the 5-HT3A(QDA) Receptor in a Voltage-independent Manner—Blockade by Ca2+ of macroscopic current responses mediated by the 5-HT3A receptor expressed in mammalian cell hosts is voltage-independent (20, 21, 34, 40, 41). The readily resolvable single channel conductance of the 5-HT3A(QDA) receptor allowed direct measurements of the influence of extracellular Ca2+ upon single channel current amplitudes over a range of membrane potentials. Fig. 6 depicts the results of such studies where [Ca2+]o was varied between 0.3 and 10 mM in the presence of 95 mM Na+ and single channel events evoked by pressure-applied 5-HT (10 µM) were recorded from outside-out membrane patches at holding potentials in the range of –40 to –100 mV. At all concentrations of extracellular Ca2+ studied the single channel i-V relationship was well fitted by a linear function and showed no evidence of a region of negative slope conductance or outward rectification (Fig. 6). In addition, the single channel conductances derived from the slope of the i-V relationships (i.e. 35.8, 29.4, 25.0, and 20.0 pS in the presence of 0.3, 1, 3, and 10 mM Ca2+, respectively) were in excellent agreement with the chord conductances reported in Fig. 5C. Thus, the reduction in single channel conductance by extracellular Ca2+ is voltage-independent over the range of negative potentials examined.
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Application of 1 µM 5-HT to cells transfected with the 5-HT3A(QDA D293A) receptor cDNA elicited only small inward current responses. Hence, we constructed full concentration-response relationships to 5-HT for both the 5-HT3A(QDA) and 5-HT3A(QDA D293A) receptors to determine whether the D293A mutation was associated with a reduction in the agonist potency of 5-HT. Such experiments demonstrated that relative to the 5-HT3A(QDA) receptor (EC50
1.1 µM), the 5-HT3A(QDA D293A) construct is less sensitive to 5-HT (EC50
3.6 µM; supplemental Fig. 1A). Similarly, a comparison of wild-type 5-HT3A and 5-HT3A(D293A) receptors revealed that the D293A mutation decreases the potency of 5-HT, as the EC50 value was shifted dextrally from
3 to 7 µM (supplemental Fig. 1B). In subsequent experiments, 2 µM 5-HT was employed to elicit macroscopic currents from cells expressing the 5-HT3A(D293A) and 5-HT3A(QDA D293A) receptor constructs.
In common with the 5-HT3A(QDA) construct, the 5-HT3A(QDA D293A) mutant maintained exclusive selectivity for cations because the slope of the relationship between the logarithm of (Na+)o and E5-HT was determined to be 61 mV/decade change in (Na+)o (Fig. 8A). Using solutions E3 and I2 and the voltage ramp protocol, macroscopic currents mediated by the 5-HT3A(QDA D293A) construct in response to 5-HT demonstrated an E5-HT of –40.5 ± 0.8 mV (n = 6), corresponding to a PCa/PCs ratio of only 0.25 ± 0.01 (n = 6) compared with that of 3.7 for the 5-HT3A(QDA) receptor (Fig. 8B). Similarly, the E5-HT of –30.6 ± 4.7 mV (n = 6) for the 5-HT3A(D293A) mutant indicates a PCa/PCs of 0.44 ± 0.08 (n = 6), which is also significantly reduced versus the wild-type receptor (1.4). The PCa/PCs ratios of the 5-HT3A(D293A) and 5-HT3A(QDA D293A) receptors were not significantly different. The PNa/PCs ratio of either construct was unchanged by the D293A mutation (Fig. 8B). Thus, for both the wild-type 5-HT3A and 5-HT3A(QDA) constructs, neutralization of the negatively charged 20' residue greatly reduces the PCa/PCs ratio but has no effect upon PNa/PCs.
In addition to reducing the relative permeability of Ca2+, as evidenced by a decreased sensitivity of E5-HT to changes in [Ca2+]o (Fig. 8C), the introduction of the D293A mutation into the 5-HT3A(QDA) receptor construct also decreased single channel conductance. In the presence of 0.1 mM Ca2+ and 95 mM Na+, the single channel chord conductance of the 5-HT3A(QDA D293A) receptor was 25.8 ± 1.9 pS (n = 4) at a holding potential of –80 mV in comparison with 41.3 pS for the 5-HT3A(QDA) construct. Similarly, the single channel chord conductance (at –80 mV) of the 5-HT3A(QDA D293A) receptor determined with solution E2 (29.8 ± 0.5, n = 7) was significantly less than that of the 5-HT3A(QDA) construct (40.8 pS). However, no difference in single channel conductance was observed between the 5-HT3A(QDA) and 5-HT3A(QDA D293A) constructs over a range of positive holding potentials (60 to 100 mV), indicating that the D293A mutation preferentially suppresses inwardly directed cation flux (Fig. 8D). As found for the 5-HT3A(QDA) receptor, elevated [Ca2+]o (0.1–30 mM) also depressed the single channel conductance of the 5-HT3A(QDA D293A) construct in a concentration-dependent manner (Fig. 8E). At all values of [Ca2+]o studied, the single channel chord conductance of the 5-HT3A(QDA D293A) construct was significantly less than that of the 5-HT3A(QDA) receptor. Clearly, the alleviation of macroscopic current block by the D293A mutation (34) cannot be attributed to a reduced influence of Ca2+ upon single channel conductance.
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| DISCUSSION |
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1.4 to 3.7. Such an effect was selective because neither PNa/PCs nor PNa/PCl was perturbed by the mutation, the latter being inferred by comparison with values within the literature (20, 29, 30). Notably, the 5-HT3A(QDA) construct retained perfect selectivity toward cations versus anions, a finding that accords with the results of a recent study in which deletion of the entire intracellular loop of the 5-HT3A receptor had no measurable influence upon PNa/PCl (44). Indeed, residues within and adjacent to TM2 govern charge selectivity in the 5-HT3A receptor (29). In particular, the single amino acid substitution E–1'A at the intracellular border of TM2 (Fig. 1B) is sufficient to generate a 5-HT3A receptor that does not discriminate between monovalent cations and anions (PNa/PCl = 0.89) (30). In future studies, it would be of interest to generate the E–1'A mutation within the 5-HT3A(QDA) background to assess whether a role for the MA helix emerges when a primary determinant of charge selectivity is silenced.
Our results indicate that the single mutation R436D is sufficient to enhance PCa/PCs to an extent comparable with that found for the 5-HT3A(QDA) construct. Analysis of several amino acid substitutions involving neutralization, or inversion, of charge at this key locus suggests that an electrostatic repulsive effect contributes to a suppression of PCa/PCs in the wild-type receptor. The latter is consistent with the results of modeling studies that place the highly basic (pKa = 12.48) guanidinium group of Arg-436 within the intracellular permeation pathways (portals) located between adjacent MA-stretch
-helices (26, 32). Because of the small maximal width of the portals (26), interactions between partially hydrated permeating ions and Arg-436 are likely.
Previous studies of Ca2+ permeation through homomeric 5-HT3 receptor channels have, because of its very low single channel conductance, been restricted to the analysis of macroscopic currents. The latter are suppressed by extracellular divalent cations by mechanisms that potentially include a reduction in agonist binding affinity (34, 41), an acceleration of the kinetics of deactivation and desensitization (34), and depression of macroscopic and single channel current amplitudes (20, 34), the latter being inferred by fluctuation analysis (20). In the present study, we employed the 5-HT3A(QDA) receptor construct to examine directly the influence of extracellular Ca2+ upon single channel conductance. A solution (E3), in which Ca2+ was the sole extracellular cation, supported outwardly rectifying single channel currents but with a chord conductance at negative potentials (5.7 pS), which was greatly reduced in comparison with the value of 40.8 pS obtained with solution E2, in which Na+ was the permeant species. Thus, although the permeability of Ca2+ relative to Cs+ is greatly increased in the 5-HT3A(QDA) construct, the channel does not conduct Ca2+ efficiently. Moreover, the addition of Ca2+ to Na+-containing extracellular solutions caused a concentration-dependent inhibition of the inwardly directed single channel current amplitude, in a manner reminiscent of that observed for single channel currents mediated by the nicotinic ACh receptor of skeletal muscle (45). Such results are most parsimoniously explained by hypothesizing that the permeation pathway presents a low affinity binding site (or sites) for Ca2+, which confers a degree of selectivity for Ca2+ over monovalent cations, yet with an off-rate sufficient to allow significant flux of both Na+ and Ca2+. An interaction between Ca2+ and Na+ within the channel is supported by our experimental observations indicating the PCa/PNa ratio for the 5-HT3A(QDA) receptor construct varies with [Ca2+]o (i.e. the principle of independence is violated (39)). Consistent with this notion, the reduction in single channel current amplitude by extracellular divalent cations was more pronounced when [Na+]o was reduced.
We considered the D293A residue of the human 5-HT3A receptor subunit, which forms the 20' negatively charged ring within the extracellular vestibule of the channel (2, 28), to be a strong candidate for the putative Ca2+ binding site that limits the rate of charge transfer through the channel (Fig. 1). Firstly, mutation of the corresponding residue (Asp-298) of the mouse 5-HT3A subunit to alanine alleviates the block of macroscopic current responses by extracellular Ca2+ (34). Secondly, Ca2+ reduced the amplitude of single channel currents mediated by the 5-HT3A(QDA) receptor construct in a voltage-independent manner. The lack of observable voltage dependence suggests a binding site for Ca2+ away from the electrical field of the membrane. The 20' residue resides within such a location. However, because Ca2+ is permeant, rather than a simple impermeant open channel blocker, it remains possible that Ca2+ does interact with a site(s) within the field but that the increased driving force provided by hyperpolarization facilitates its dissociation and inward conduction. Note that this scenario is quite different from that found for an impermeant cationic blocker, for which the dwell time within the channel would be increased by hyperpolarization because of a decreased probability of the molecule exiting the pore to the extracellular environment.
The potency of 5-HT to activate the mouse 5-HT3A(D298A) construct is less than for the murine wild-type receptor (34), a result concordant with our observation that the D293A mutation introduced into either the human wild-type or 5-HT3A(QDA) construct causes a dextral shift in the 5-HT concentration-response relationship. The D293A mutation within the 5-HT3A(QDA) receptor background caused a reduction in the amplitude of inwardly, but not outwardly, directed single channel current events. Such an effect is consistent with a simple electrostatic mechanism in which the negative charge of the five Asp-293 residues acts to increase the local concentration of permeant cations within the extracellular vestibule. Removal of such charges would thus reduce a focusing mechanism, consistent with the appearance of a enhanced outward rectification in the i-V relationship for the 5-HT3A(QDA D293A) receptor construct versus the 5-HT3A(QDA) receptor. Very similar effects of neutralizing the extracellular ring of charge upon single channel conductance and rectification have been reported for nicotinic ACh and anion-selective
-aminobutyric acid type A and glycine receptors (28). Because of the very low conductance of the wild-type 5-HT3A receptor (20, 21) and kinetic properties of the 5-HT3A(D293A) receptor, which are unfavorable to fluctuation analysis (34),5 we could not estimate the effect of the D293A mutation upon single channel conductance in this construct. However, it is notable that the pattern of inward rectification of macroscopic currents mediated by the mouse 5-HT3A(D298A) mutant resembles that of the murine wild-type receptor (34). The latter differs from the present observations comparing the human 5-HT3A(QDA) and 5-HT3A(QDA D293A) receptors at the single channel level. An important difference in our studies is the removal of positive electrostatic potential in the intracellular vestibule by the mutations R432Q, R436A, and R440A. Such charges are present in the mouse 5-HT3A and 5-HT3A(D298A) receptors studied by Hu and Lovinger (34) and would reduce the local concentration of permeant ions within the intracellular vestibule. The latter would induce a degree of inward rectification. It is possible that such an influence is dominant, masking any tendency toward linearization that might be anticipated from the 5-HT3A(D293A) mutation. Indeed, in our studies, the macroscopic current I-V relationship shifts from the pattern of inward rectification characteristic of the wild-type 5-HT3A receptor toward linearity in the 5-HT3A(QDA) construct.
For both the wild-type 5-HT3A and the 5-HT3A(QDA) constructs, the introduction of the D293A mutation drastically reduced the PCa/PCs ratio. Once more, such an effect can probably be attributed to a reduction in a local negative electrostatic potential that particularly favors the accumulation of Ca2+ at the entrance to the pore, as suggested by molecular dynamics simulations performed on models of the
7 and skeletal muscle nicotinic ACh receptors (46, 47). Such simulations indicate monovalent cations to be stabilized at the 20' position, where the ion dwells during its passage through the channel axis. The greater coulombic attraction between Ca2+ and the 20' residue would amplify such interactions. Also, heteromeric
4β2 nicotinic ACh receptors, harboring a larger complement of β2 subunits in which lysine occupies the 20' position, appear to have reduced selectivity toward Ca2+ (48). However, the D293A residue does not contribute crucially to cation versus anion selectivity because the PNa/PCl ratio for the 5-HT3A(QDA D293A) construct was best described as infinite. A previous study of mouse 5-HT3A receptors in which cysteine r