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Journal of Physiology (2002), 545.2, pp. 355-373
© Copyright 2002 The Physiological Society
DOI: 10.1113/jphysiol.2002.032151
o- and G
i-coupled muscarinic m2 receptors in Xenopus oocytes: the role of receptor precoupling in RGS modulation| ABSTRACT |
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'Regulators of G protein Signalling' (RGSs) accelerate the activation and deactivation kinetics of G protein-gated inwardly rectifying K+ (GIRK) channels. In an apparent paradox, RGSs do not reduce steady-state GIRK current amplitudes as expected from the accelerated rate of deactivation when reconstituted in Xenopus oocytes. We present evidence here that this kinetic anomaly is dependent on the degree of G protein-coupled receptor (GPCR) precoupling, which varies with different Gi/o-RGS complexes. The gating properties of GIRK channels (Kir3.1/Kir3.2a) activated by muscarinic m2 receptors at varying levels of G protein expression were examined with or without the co-expression of either RGS4 or RGS7 in Xenopus oocytes. Different levels of specific m2 receptor-G
coupling were established by uncoupling endogenous pertussis toxin (PTX)-sensitive G
i/o subunits with PTX, while expressing varying amounts of a single PTX-insensitive subunit (G
i1(C351G), G
i2(C352G), G
i3(C351G), G
oA(C351G), or G
oB(C351G)). Co-expression of each of the PTX-insensitive G
i/o subunits rescued acetylcholine (ACh)-elicited GIRK currents (IK,ACh) in a concentration-dependent manner, with G
o isoforms being more effective than G
i isoforms. Receptor-independent 'basal' GIRK currents (IK,basal) were reduced with increasing expression of PTX-insensitive G
subunits and were accompanied by a parallel rise in IK,ACh. These effects together are indicative of increased G
scavenging by the expressed G
subunit and the subsequent formation of functionally coupled m2 receptor-G protein heterotrimers (G
(GDP)
). Co-expression of RGS4 accelerated all the PTX-insensitive G
i/o-coupled GIRK currents to a similar extent, yet reduced IK,ACh amplitudes 60-90 % under conditions of low G
i/o coupling. Kinetic analysis indicated the RGS4-dependent reduction in steady-state GIRK current was fully explained by the accelerated deactivation rate. Thus kinetic inconsistencies associated with RGS4-accelerated GIRK currents occur at a critical threshold of G protein coupling. In contrast to RGS4, RGS7 selectively accelerated G
o-coupled GIRK currents. Co-expression of G
5, in addition to enhancing the kinetic effects of RGS7, caused a significant reduction (70-85 %) in steady-state GIRK currents indicating RGS7-G
5 complexes disrupt G
o coupling. Altogether these results provide further evidence for a GPCR-G
-GIRK signalling complex that is revealed by the modulatory affects of RGS proteins on GIRK channel gating. Our functional experiments demonstrate that the formation of this signalling complex is markedly dependent on the concentration and composition of G protein-RGS complexes.
(Resubmitted 6 September 2002; accepted 16 September 2002; first published online 4 October 2002)
Corresponding author C. A. Doupnik: Department of Physiology and Biophysics, University of South Florida College of Medicine, 12901 Bruce B. Downs Blvd/MDC 8, Tampa, FL 33612-4799, USA. Email: cdoupnik{at}hsc.usf.edu
| INTRODUCTION |
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G protein-gated inwardly rectifying K+ (GIRK) channels mediate slow inhibitory post-synaptic potentials (sIPSPs) in the central and peripheral nervous system and are activated by a variety of G protein-coupled receptors (GPCRs) that selectively interact with pertussis toxin (PTX)-sensitive G
i/o proteins (for recent reviews see (Dascal, 1997; Yamada et al. 1998; Mark & Herlitze, 2000). Both the amplitude and the distinguishing slow time course for GIRK-mediated sIPSPs are inherently coupled to the kinetics of the G protein activation-deactivation cycle. The time course for GIRK channel activation is dependent on the receptor catalysed production of free G
dimers that interact directly with the channel and increase open probability (Logothetis et al. 1987; Krapivinsky et al. 1995). Deactivation of GIRK currents is determined by the reaction rate for G
sequestration, a process rate limited by the GTPase activity of associated G
i/o proteins, G
(GTP)
G
(GDP), with a rate constant for GTP hydrolysis of kGTPase (Breitwieser & Szabo, 1988).
Given the large diversity and ubiquitous expression of heterotrimeric G proteins (Simon et al. 1991), several studies have begun investigating whether functional differences exist among the various G

subunits that may participate in GPCR
GIRK channel signalling (5 G
i/o isoforms, 5 G
genes, and 12 G
genes) (Lledo et al. 1992; Wickman et al. 1994; Schreibmayer et al. 1996; Sowell et al. 1997; Takano et al. 1997; Valenzuela et al. 1997; Fernandez-Fernandez et al. 1999; Greif et al. 2000; Leaney et al. 2000; Leaney & Tinker, 2000; Lei et al. 2000; Blake et al. 2001; Fernandez-Fernandez et al. 2001). Adding to this molecular complexity is the recently identified 'Regulators of G protein Signalling' (RGSs) that accelerate the termination of G protein signalling by increasing kGTPase through a direct interaction with G
subunits (for recent reviews see De Vries et al. 2000; Ross & Wilkie, 2000). Several RGS proteins, of which there are now more than 20 mammalian genes identified, are capable of accelerating receptor-dependent GIRK activation and deactivation kinetics in heterologous expression systems (Doupnik et al. 1997; Saitoh et al. 1997; Granneman et al. 1998; Herlitze et al. 1999; Saitoh et al. 1999; Kovoor et al. 2000; Burgon et al. 2001). RGS-accelerated GIRK currents more closely resemble the properties of neuronal and cardiac GIRK currents, indicating native RGS proteins are likely to be important determinants of GIRK-mediated synaptic signalling.
Initial studies of RGS-accelerated GIRK channel kinetics revealed an apparent paradox where the RGS-accelerated activation phase, an expected consequence of accelerated deactivation according to standard kinetic concepts, was not accompanied with a reduction in steady-state current amplitude (Doupnik et al. 1997; Saitoh et al. 1997). These findings suggested that RGS proteins have actions on GPCR
GIRK signalling beyond the well-established GTPase-activating function of the RGS domain on G
(GTP) subunits (Zerangue & Jan, 1998). To further explore the effects of RGS proteins on receptor-dependent GIRK channel gating, we examined the actions of two distinct RGS proteins (RGS4 and RGS7) on GIRK channels (Kir3.1/Kir3.2a heteromers) activated by muscarinic m2 receptors coupled to varying concentrations and compositions of G
i/o
heterotrimers in Xenopus oocytes. Muscarinic m2 receptor-G

-GIRK channel coupling was established by expressing varying levels of PTX-insensitive G
i/o subunits (Wise et al. 1997) while uncoupling oocyte G
i/o subunits (xG
i/o) with PTX. Our findings indicate that GPCR-G protein-RGS-GIRK precoupling is a critical determinant in the anomalous channel gating, and is dependent on the concentration and composition of G
i/o-RGS proteins.
| METHODS |
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Isolation of Xenopus oocytes
All procedures for the use and handling of Xenopus laevis (Xenopus One, Ann Arbor, MI, USA) were approved by the University of South Florida Institutional Animal Care and Use Committee in accordance with NIH guidelines. Oocytes were isolated from ovarian tissue surgically removed during hypothermia and 0.2% tricaine (MS-222)-induced anaesthesia. After recovery from anaesthesia, frogs were returned to their tanks in the institutional animal housing facility where they were monitored daily. Frogs were killed after a second procedure by exsanguination while under anaesthesia. The time between surgeries was 1-3 weeks.
The oocytes were enzymatically dissociated by a 50 min collagenase A (Boehringer Mannheim) digestion (1.8 %) at room temperature on a rocker platform in Ca2+-free oocyte Ringer (OR) solution. The OR solution was composed of 82.5 mM NaCl, 2.5 mM KCl, 1.0 mM CaCl2, 1.0 mM MgCl2, 1.0 mM NaHPO4 and 5.0 mM Hepes, at pH 7.5 (NaOH). Isolated stage V-VI oocytes were then maintained in oocyte culture medium (OCM) at 19 °C in 35 mm dishes on an orbital shaker. OCM was composed of OR solution containing 2.5 mM sodium pyruvate and 5 % heat-inactivated horse serum. OCM was changed 1-2 times daily.
Heterologous expression in Xenopus oocytes
Linearized cDNA-containing vectors (Table 1) were used to transcribe cRNA in vitro using the appropriate RNA polymerase (T7 or T3) as described by the manufacturer (mMessage mMachine, Ambion, Austin, TX, USA). Concentrations and quality of the cRNAs were determined by spectrophotometric absorbance at 260 nm and denatured (formaldehyde) agarose gel electrophoresis. On the first day after enzymatic isolation (Day 1), oocytes were injected with a mixture of cRNAs dissolved in DEPC-treated H2O at a final injection volume of 50 nl (Nanoliter2000, World Precision Instruments). All oocytes were injected with cRNAs for Kir3.1 (0.5 ng), Kir3.2a (0.5 ng), and the m2 receptor (0.5 ng). The amounts of other cRNAs, including PTX-insensitive G
subunits and RGSs, were varied as described in the Results section. The PTX-insensitive G
cDNAs were all constructed by PCR (kindly provided by Stephen Ikeda, NIAAA, Bethesda, MD, USA), having a 5' Kozak sequence followed by the G
coding region containing the C-terminal C
G mutation. The 5' and 3' untranslated regions of the G
cDNAs were not included in the constructs, and therefore ribosomal binding and translation initiation of each PTX-insensitive G
cRNA are expected to be equivalent.

Two methods were used to inactivate endogenous oocyte G
i/o subunits by PTX-mediated ADP ribosylation. Initially we injected the PTX holotoxin (containing S1, S2, S3, S4 and S5 subunits from Bordetella pertussis, Sigma-Aldrich Chemical) at 1 ng/oocyte on Day 2 of culture (1 day after cRNA injection), and then recorded GIRK currents on Day 4. This method inhibited > 80 % of the m2 receptor-activated GIRK currents coupled to endogenous G
i/o subunits that was determined for each batch of oocytes to monitor the efficiency of endogenous G protein uncoupling. In subsequent experiments we included cRNA (1 ng/oocyte) encoding the catalytically active PTX-S1 subunit (kindly provided by Eitan Reuveny, Weizmann Institute, Israel) with the mixture of other cRNAs in the initial Day 1 cRNA injection (Vivaudou et al. 1997). This produced a much more effective > 95 % uncoupling of endogenous G
i/o subunits which also was determined for each batch of oocytes tested.
Electrophysiological recordings
Macroscopic GIRK currents were measured using a two-electrode voltage clamp amplifier (GeneClamp 500, Axon Instruments) and standard recording techniques (Stuhmer & Parekh, 1995). Electrodes were fabricated from borosilicate glass tubes (1.5 outside diameter, 0.86 inside diameter, GC150F-10, Warner Instruments) by a programmable microelectrode puller (P-97, Sutter Instruments). Electrodes were filled with 3 M KCl and had tip resistances of 0.8-1.0 M
. Membrane currents from voltage clamped oocytes were digitized using a Digidata 1200 acquisition system (Axon Instruments) and a Dell PC computer running pCLAMP 7.0 software (Axon Instruments).
Oocytes were placed in a recording chamber continuously perfused with a minimal Ringer solution composed of 98 mM NaCl, 1 mM MgCl2 and 5 mM Hepes at pH 7.5 (NaOH). After electrode impalement and clamping the membrane potential to -80 mV, the perfusion solution was changed to a high K+ solution composed of 20 mM KCl, 78 mM NaCl, 1 mM MgCl2, and 5 mM Hepes at pH 7.5 (NaOH). The resulting increase in inward current represents a 'basal' K+ current (IK,basal) that is due primarily to receptor-independent GIRK channel activity (Dascal et al. 1993). Rapid application and washout of acetylcholine (ACh, Sigma-Aldrich Chemical) produced the receptor-dependent GIRK current (IK,ACh), and was performed with a computer controlled perfusion system (SF-77B, Warner Instruments) that rapidly switched the position of two perfusion barrels (barrel A and barrel B) located next to the oocyte. The perfusion barrels contained high K+ solution (barrel A) and high K+ solution plus ACh (barrel B). For barrel B, a range of ACh concentrations was tested for each oocyte via a manifold that connected multiple reservoirs containing different ACh concentrations. Flow through the perfusion barrels was gravity driven, and the time constant for solution exchange was ~1 s as determined by the time course change in receptor-independent GIRK current with switching between 20 and 40 mM external K+. All recordings were performed at room temperature (21-23 °C).
Electrophysiological data analysis
Time-dependent GIRK current kinetics were analysed using non-linear curve fitting software that fit single exponential functions to derive activation time constants (
act) and deactivation time constants (
deact) (Clampfit software, Axon Instruments). Dose-response relations were analysed by fitting peak GIRK current amplitudes with the following Hill function:

where the effective concentration producing a 50 % response (EC50) and Hill coefficient value (nH) were derived from the best fit (Origin 6.0 software, OriginLab Corp., Northampton, MA, USA). In some cases where the GIRK current did not reach a steady-state level at the end of the agonist application period (i.e. low agonist concentrations), the steady-state current amplitude was estimated by the fit of the activation time course to an extrapolated steady-state value.
Statistical comparisons between the various experimental groups were performed by one-way ANOVA where P < 0.05 was considered significant. Experiments were each replicated in oocytes from 2-4 separate batches (dissections) of oocytes.
Radiolabelling, immunoprecipitation and Western blotting of G
i/o proteins
To compare the relative expression levels of PTX-insensitive G
i/o proteins, [35S]Met/Cys (Pro-mix, Amersham Pharmacia, Piscataway, NJ, USA) was added to OCM (0.5 mCi ml-1) 1-2 h after cRNA injection to initiate radiolabelling of proteins. Fresh OCM containing [35S]Met/Cys was added on a daily basis, and 3 days after cRNA injection ~20 oocytes from each experimental group were washed with label-free OR solution and homogenized in the following lysis buffer (150 mM NaCl, 50 mM Tris-Cl, 1 mM dithiothreitol (DTT), 1.0 % Trition X-100, and protease inhibitor cocktail (Boehringer Mannheim), pH 7.5) at 50 µl/oocyte. The oocyte lysate was then centrifuged at 10 000 g for 10 min to clear insoluble debris.
G
i/o subunits were immunoprecipitated from oocyte lysates using a rabbit polyclonal antibody that recognizes an internal epitope (GAGESGKSTIVKQMK) identical among G
i/o isoforms (SA-126, BIOMOL Research Laboratories, Plymouth Meeting, PA, USA). To expose the internal epitope, the supernatant from the equivalent of five oocytes (250 µl) was diluted in SDS denaturing buffer (50 mM NaPO4, 2 mM EDTA, 1 mM DTT, 0.5 % SDS, pH 8.0) and boiled for 3 min. The denaturated supernatants were then diluted and solubilized further in RIPA buffer (150 mM NaCl, 50 mM NaPO4, 2 mM EDTA, 1 mM DTT, 1.0 % Triton X-100, 1.0 % deoxycholate, 0.5 % SDS, pH 7.2). Denatured oocyte lysates (~700 µl each) were then pre-cleared with 10 µl of non-immune rabbit serum (1 h incubation at 4 °C) and 20 µl Protein A/G-agarose beads (Santa Cruz Biotechnology, Inc.). G
i/o proteins were immunoprecipitated in an overnight incubation at 4 °C using the SA-126 antibody precoupled to Protein A/G-agarose beads. We initially tested different amounts of oocyte lysate (0.5, 1, 2 and 4 oocytes) with a fixed amount of SA-126 antibody (2 µl) and Protein A/G-agarose (20 µl) to establish non-saturating binding conditions, which was determined to be
1 oocyte. All immunoprecipitations were then performed using the lysate equivalent of a single oocyte. At the end of the overnight incubation period, beads were washed three times with lysis buffer and the immunoprecipitated proteins eluted by boiling in 40 µl of SDS loading buffer (62.5 mM Tris-Cl pH 6.8, 10 % glycerol, 5 %
-mercaptoethanol, 2 % SDS, 0.05 % bromophenol blue).
Immunoprecipitated proteins were separated by SDS-polyacrylamide (8 %) gel electrophoresis and then transferred to a polyvinylidene difluoride (PVDF) membrane by overnight electrophoretic transfer at 4 °C. 35S-labelled proteins were resolved by autoradiography. Western blot analysis was performed using a polyclonal goat antibody that recognizes a conserved region in G
i/o/t/z proteins (sc-12798, Santa Cruz Biotechnology). A ~41 kDa band corresponding to G
i/o proteins was readily detected by an HRP-conjugated donkey anti-goat secondary antibody (sc-2033, Santa Cruz Biotechnology) and enhanced chemiluminescence. Relative radiolabelling and G
i/o protein levels were quantified by densitometric analysis (GS-700 Imaging Densitometer, Bio-Rad) of the 41 kDa band following normalization to a sample control.
| RESULTS |
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Conferring specific m2 receptor-G
-coupling in Xenopus oocytes
To assess the properties of receptor-dependent GIRK channel gating elicited by specific G
-coupled m2 receptors, oocyte G
i/o subunits were inactivated by PTX while expressing one of five different PTX-insensitive G
i/o subunits (G
i1(C351G), G
i2(C352G), G
i3(C351G), G
oA(C351G), or G
oB(C351G)) (Wise et al. 1997). As reported previously, expression of PTX-S1 blocked > 95 % of IK,ACh and effectively abolished endogenous G
i/o protein coupling (Vivaudou et al. 1997). Shown in Fig. 1, co-expression of G
i2(C352G) rescued the m2 receptor-coupled GIRK currents and was dependent on the level of G
i2(C352G) expression (Fig. 1B). Injection of 5 or 10 ng of G
i2(C352G) cRNA per oocyte produced ACh-evoked GIRK currents that were ~50 and 95 %, respectively, the peak amplitude of GIRK currents recorded from paired oocytes utilizing endogenous G
i/o subunits (i.e. no PTX-S1 or G
i2(C352G) cRNA). The G
i2(C352G)-dependent GIRK currents represent channels activated by m2 receptors coupled specifically to G
i2(C352G) subunits and endogenous G
dimers. G
i2(C352G)-dependent IK,ACh was also associated with a parallel 50-60 % decrease in IK,basal (Fig. 1D). The reduction in IK,basal by G
i2(C352G) is likely due to the sequestration of free G
dimers that mediate receptor-independent basal GIRK channel activity (Lim et al. 1995; Vivaudou et al. 1997; Jeong & Ikeda, 1999).
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Figure 1. Specific coupling of G A, typical ACh-evoked GIRK currents (IK,ACh) recorded from different oocytes from three separate experimental groups. Upper traces: IK,ACh from a 'control' oocyte expressing muscarinic m2 receptors and Kir3.1/Kir3.2a channel subunits, utilizing endogenous G | ||
ACh dose-response curves derived from oocytes expressing different levels of G
i2(C352G) were not significantly different with respect to their EC50 value as shown in Fig. 1C, and this is consistent with previous studies where EC50 values were shown to be relatively unaffected by overexpressed G
subunits, but most sensitive to levels of GPCR expression (Henry et al. 1995). Since the same amount of m2 receptor cRNA was injected for all experimental groups (0.5 ng cRNA/oocyte), m2 receptor protein levels were assumed to be roughly equivalent across groups and this was supported by the equivalent EC50 values with varying G
i2(C352G) expression levels. The ACh dose-response curves for G
i2(C352G)-coupled m2 receptors, however, were notably shifted rightward compared to the ACh dose-response relation from m2 receptor coupling to endogenous G
i/o subunits (Fig. 1B). The higher EC50 value for G
i2(C352G) versus endogenous G
i/o-coupled receptors may be attributable to the mixed coupling of oocyte G
o and G
i subunits, and/or a lower level of m2 receptors precoupled to heterotrimeric G proteins (Shea & Linderman, 1997; Shea et al. 2000) (see Results below and Discussion).
One readily apparent feature of the m2 receptor- G
i2(C352G)-coupled GIRK current was the significantly slower activation and deactivation kinetics as compared to GIRK currents coupled to endogenous xG
i/o subunits (Fig. 1A). The time constants for IK,ACh activation and deactivation over a range of ACh concentrations are shown in Fig. 1E and F. The slower kinetics for m2 receptor-G
i2(C352G)-coupled GIRK currents were not attributable to the level of G
i2(C352G) expression since increasing amounts of G
i2(C352G) cRNA, which nearly doubled maximal IK,ACh amplitudes, did not result in significantly different GIRK activation or deactivation time constants. The slower GIRK gating properties may be caused by altered coupling properties of the C
G mutated G
i2 subunit, or alternatively the faster properties in the absence of overexpressed G
subunits may reflect the influence of endogenous RGS proteins (Saitoh et al. 2000).
GIRK channel gating properties via G
o- and G
i-coupled m2 receptors
The gating properties of GIRK currents elicited by m2 receptors coupled to each of the PTX-insensitive G
i/o subunits are shown in Fig. 2. Since there were no noticeable differences in GIRK current kinetics at different levels of G
i2(C352G) expression, comparisons between the five different G
i/o isoforms were initially made using 5 ng cRNA/oocyte for each G
isoform. The three G
i isoforms (G
i1(C351G), G
i2(C352G) and G
i3(C351G)) each produced ACh-elicited GIRK currents that were indistinguishable from each other with regard to the five parameters analysed (maximal IK,ACh, IK,basal, EC50,
act and
deact) (Fig. 2). G
oA(C351G) and G
oB(C351G) also produced equivalent GIRK responses but were distinct from G
i-coupled GIRK currents in several respects. First, G
o-coupled GIRK currents were significantly larger than G
i-coupled currents, with maximal IK,ACh amplitudes being ~2-fold greater (Fig. 2B). Second, expression of G
oA(C351G) and G
oB(C351G) more prominently inhibited IK,basal compared to G
i1(C351G), G
i2(C352G), or G
i3(C351G) (Fig. 2B). Third, the EC50 values for G
oA(C351G) and G
oB(C351G) were more similar to the EC50 values with endogenous xG
i/o coupling than with G
i1(C351G), G
i2(C352G), or G
i3(C351G) (Fig. 2C). And finally, the activation of G
o-coupled GIRK currents was faster compared to G
i-coupled currents and had a more prominent sigmoidal time course (Fig. 2D). The deactivation time course for IK,ACh was not significantly different among all five G
i/o isoforms (Fig. 2D).
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Figure 2. Properties of ACh-evoked GIRK currents activated by m2 receptors coupled to five different G A, typical ACh-evoked GIRK currents for each PTX-insensitive G | ||
The differences between G
i and G
o-coupled GIRK currents were not attributable to cDNA/vector construction (i.e. untranslated regions), cRNA quantification, or batch-to-batch oocyte variability (see Methods). Several factors could conceivably contribute to these differences and include (1) differences in G
i/o biosynthesis or degradation (Li et al. 1996), (2) preferential G
o coupling to m2 receptors (Leaney & Tinker, 2000), (3) preferential G
o association with oocyte G
subunits (Fernandez-Fernandez et al. 2001), and (4) different G
i/o subcellular distributions (Devic et al. 1996).
Biochemical analysis of PTX-insensitive G
i/oprotein expression levels
To determine whether PTX-insensitive G
i/o subunits are differentially expressed following cRNA injection (5 ng cRNA/oocyte, as in Fig. 2), G
i/o proteins were immunoprecipitated from oocytes following metabolic labelling with [35S]Met/Cys. The PTX-insensitive G
i/o proteins each contain an equivalent number of Met/Cys sites (19) for potential radiolabelling. As shown in Fig. 3A, a prominent ~41 kDa band that corresponds to G
i/o proteins was radiolabelled in each experimental group. A significant portion represents radiolabelling of endogenous xG
i/o proteins over the 3 day incubation period as indicated by the oocyte groups that were not injected with PTX-insensitive G
i/o cRNA. Quantitative comparisons of the 35S-labelled 41 kDa band via densitometric analysis indicate a small 10-20 % elevation in oocytes injected with PTX-insensitive G
i/o cRNAs (Fig. 3B). The observed changes in 35S labelling were also paralleled by densitometric changes in the bands detected by Western blot analysis (Fig. 3B). Since the peak IK,ACh amplitudes for G
o-coupled m2 receptors were ~2 times higher compared to G
i-coupled m2 receptors under equivalent expression conditions (cf. Fig. 2B), the ~2-fold difference in G
oB(C351G) versus G
i2(C352G) or G
i3(C351G) protein expression could potentially account for the differences in m2 receptor-GIRK channel coupling. G
oA(C351G)-elevated protein levels, however, were similar to G
i2(C352G) and G
i3(C351G) levels (Fig. 3B), and resolving small expression changes was clearly limited by the biochemical approach. Thus despite equivalent cRNA injections (5 ng cRNA/oocyte each), differences in G
i/o biosynthesis and/or degradation may result in different steady-state G
i/o protein levels that account for the distinct gating properties of G
o- versus G
i-coupled GIRK currents.
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Figure 3. Biochemical analysis of PTX-insensitive G A, radiolabelling (upper panel) and Western blot analysis (lower panel) of oocytes injected with cRNAs encoding five different PTX-insensitive G | ||
The GIRK activation time course is dependent on free G
levels
A sigmoidal time course for GIRK activation, as observed with G
o expression (Fig. 2), is well documented in cardiomyocytes and neurons and indicative of a multi-step process in channel opening (Inomata et al. 1989; Sodickson & Bean, 1996). Tetrameric GIRK channels can bind up to four G
dimers, and functional studies indicate at least two G
dimers are necessary for channel opening (Nemec et al. 1999; Corey & Clapham, 2001). We questioned whether the sigmoidal GIRK activation time course via G
o-coupled receptors was a consequence of a markedly reduced free G
concentration as indicated by the low IK,basal level. As illustrated in Fig. 4A, conditions favouring high free G
concentrations (high IK,basal) would yield a single exponential time course for receptor activation, where the binding of a single G
dimer leads to channel opening. At low free G
concentrations (i.e. low IK,basal), GIRK channels would instead be occupied by fewer G
dimers (less than 3 G
) and require multiple G
binding events during receptor activation (2-4 G
). According to this hypothesis, reducing G
o expression levels should increase IK,basal and promote a single exponential time course for IK,ACh activation.
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Figure 4. Activation kinetics of G A, kinetic scheme for GIRK channel activation via G | ||
To test this, we compared the activation time course of IK,ACh at two different levels of G
oB(C351G) expression (Fig. 4). As expected, lower expression of G
oB(C351G) (1 ng G
oB(C351G) cRNA/oocyte) produced smaller IK,ACh amplitudes compared to high G
oB(C351G) expression, and had significantly higher receptor-independent basal GIRK activity (Fig. 4C and D). The activation time course for IK,ACh was clearly affected by the level of G
oB(C351G) expression and was consistent with the gating scheme shown in Fig. 4A. Low G
oB(C351G) expression yielded GIRK currents whose activation time course was well described by a single exponential function. In contrast, high G
oB(C351G) expression yielded GIRK currents whose activation time course had a significant delay and were best described by a 3rd order exponential function, suggesting the binding of three G
subunits in receptor-dependent GIRK activation (see Fig. 4A). The
act was smaller for high G
oB(C351G) expression versus low G
oB(C351G) expression, and single exponential fits to the rising phase of the sigmoidal time course underestimate the activation rate constant (1/
act) under these conditions. Comparisons of
deact and EC50 values from ACh dose-response curves indicated the these properties were not significantly affected by these levels of G
oB(C351G) expression (data not shown).
RGS4 reduces GIRK currents at low G
i/o coupling levels
We next evaluated the effects of RGS4 at saturating expression levels (10 ng RGS4 cRNA/oocyte; Doupnik et al. 1997; Keren-Raifman et al. 2001) on both G
o- and G
i-coupled m2 receptors as described in Fig. 2. As shown in Fig. 5, RGS4 accelerated the receptor-dependent GIRK activation and deactivation kinetics for each G
i/o isoform, consistent with the non-selective GTPase activating properties of RGS4 on G
i/o subunits in vitro (Berman et al. 1996; Watson et al. 1996). Interestingly, however, RGS4 suppressed 60-70 % of the IK,ACh amplitude for G
i-coupled m2 receptors, yet had no effect on the peak IK,ACh amplitude of G
o-coupled receptors. RGS4 did not significantly affect the EC50 for channel activation via G
i-coupled receptors, but did cause a small shift the EC50 value for G
oA(C351G)-coupled GIRK currents towards a higher ACh concentration, which more closely corresponded to the EC50 values of G
i-coupled GIRK currents (Fig. 5F). Kinetic analysis indicated the RGS4-mediated reduction in G
i-coupled IK,ACh (Fig. 5E) was fully explained by the RGS4-accelerated GIRK deactivation rate (see Table 2 and Discussion).

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Figure 5. Effects of RGS4 on GIRK currents coupled to specific PTX-insensitive G All data are from oocytes injected with 5 ng G | ||
To determine whether the higher degree of G
o versus G
i coupling (cf. Fig. 2) could account for the RGS4-dependent effects on steady-state GIRK currents, we examined the effects of RGS4 at a lower level of G
oA expression (0.5 ng cRNA/oocyte). At low G
oA expression levels, RGS4 significantly reduced ~90 % of both IK,ACh (G
oA alone, 0.76 ± 0.11 µA, n = 17; G
oA + RGS4, 0.07 ± 0.03 µA, n = 9; P < 0.05) and IK,basal (G
oA alone, 2.34 ± 0.18 µA, n = 19; G
oA + RGS4, 0.25 ± 0.07 µA, n = 14; P < 0.05). Thus the effect of RGS4 on steady-state GIRK current amplitudes is dependent on the level of G
i/o expression and GPCR precoupling. At high levels of m2 receptor-G
o coupling (i.e. Fig. 5), RGS4 accelerates GIRK activation and deactivation without significantly reducing steady-state GIRK current amplitudes and resembles the effects of RGS4 with endogenous xG
i/o coupling (Doupnik et al. 1997).
RGS7 selectively accelerates G
o-coupled GIRK currents
RGS7 belongs to a distinct subfamily of RGS proteins that contain a G
-like (GGL) domain that specifically binds G
5 subunits (Snow et al. 1998; Sondek & Siderovski, 2001). RGS7 has relatively weak effects on GIRK current kinetics when expressed without G
5 in Xenopus oocytes (Saitoh et al. 1999), but is significantly enhanced by G
5 co-expression (Kovoor et al. 2000; Keren-Raifman et al. 2001). We examined whether RGS7 (10 ng cRNA/oocyte), with or without co-expressed G
5 subunits, differentially affected G
o- versus G
i-coupled GIRK currents. In the absence of coexpressed G
5, RGS7 preferentially accelerated G
o-coupled GIRK currents having little effect on G
i-coupled GIRK kinetics (Fig. 6), which is consistent with other studies indicating RGS7 selectively interacts with G
o subunits (Posner et al. 1999; Lan et al. 2000; Rose et al. 2000). Interestingly, RGS7 acceleration of G
o-coupled IK,ACh was greater than that caused by RGS4 (cf. Fig. 5C and D) and was evident for both the IK,ACh activation and deactivation time course as well as the desensitization rate. As observed with RGS4, RGS7 did not cause a significant reduction in the maximal G
o-coupled GIRK current despite accelerating the GIRK channel gating kinetics (Fig. 6E), but did cause a small shift in the ACh dose-response curve (Fig. 6B and F). Yet in contrast to RGS4, RGS7 did not reduce steady-state GIRK currents when G
oA expression was markedly reduced (0.5 ng cRNA/oocyte): IK,basal (G
oA alone, 2.34 ± 0.18 µA, n = 19; G
oA + RGS7, 2.18 ± 0.20 µA, n = 18) and IK,ACh (G
oA alone, 0.76 ± 0.11 µA, n = 17; G
oA + RGS7, 1.25 ± 0.21 µA, n = 17).
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Figure 6. Effects of RGS7 on GIRK currents coupled to specific PTX-insensitive G All data are from oocytes injected with 5 ng G | ||
RGS7-G
5 disrupts G
o-coupled GIRK currents
G
5 binds with high affinity to the GGL domain of RGS7, enhancing the GAP activity and protein stability of RGS7 (Levay et al. 1999; Kovoor et al. 2000; Keren-Raifman et al. 2001). We examined the effects of G
5 expression on the RGS7- mediated regulation of both G
o- and G
i-coupled GIRK currents, with comparisons made using G
1 as a negative control which does not bind to RGS7 (Levay et al. 1999; Kovoor et al. 2000). As shown in Fig. 7, co-expression of G
5 with RGS7 caused a significant reduction (70-80 %) in G
o-coupled GIRK current amplitudes, yet had no effect on G
i-coupled currents. The lack of effect of G
5 on G
i-coupled GIRK currents indicates the level of G
5 (or G
5
formation) does not cause a direct inhibition of GIRK currents as observed in transfected HEK-293 cells (Lei et al. 2000). In addition to reducing G
o-coupled GIRK currents, G
5 enhanced the RGS7-accelerated GIRK kinetics consistent with RGS7-G
5 complexes having greater GAP activity compared to RGS7 alone (Kovoor et al. 2000; Keren-Raifman et al. 2001). Thus the formation of RGS7-G
5 complexes apparently disrupts G
o coupling (either to m2 receptors and/or GIRK channels) and is supported by the effects of G
5 on RGS7-G
o interactions in vitro (Levay et al. 1999).
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Figure 7. Effects of G All data are from oocytes injected with 5 ng G | ||
| DISCUSSION |
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The goal of this study was to determine whether functional differences exist in the GPCR-dependent gating properties of GIRK channels coupled to specific G
i/o subunits and RGS proteins. Our findings reveal that m2 receptors coupled to G
i and G
o subunits are differentially regulated by RGS4 and RGS7. A significant finding of our study is the identification of G protein coupling levels as a critical determinant in mediating the anomalous kinetic effects of RGS proteins on GIRK channel gating (Doupnik et al. 1997; Saitoh et al. 1997; Zerangue & Jan, 1998; Kovoor & Lester, 2002). Incremental increases in G
o
coupling by increased G
o expression revealed a transition in the RGS4-accelerated GIRK currents from 'expected' steady-state properties, characterized by a large reduction in maximal GIRK current amplitude, to 'anomalous' gating kinetics which displayed accelerated activation and deactivation kinetics with no effect on steady-state GIRK amplitude. We propose that this transition in steady-state GIRK channel kinetics is a functional indicator of the formation of a GPCR-G protein-GIRK channel signalling complex (Huang et al. 1995; Slesinger et al. 1995) that is precipitated at a critical level of G
i/o expression and revealed by the modulatory actions of co-expressed RGS proteins.
RGS proteins reveal GPCR-G protein-GIRK coupling levels via steady-state gating properties
RGS proteins were originally identified as 'negative regulators' of G protein signalling causing reduced GPCR signalling in yeast, fungi, nematodes and mammals (Dohlman et al. 1995, 1996; Druey et al. 1996; Koelle & Horvitz, 1996; Yu et al. 1996). These findings were readily explained by RGS proteins behaving as GTPase-activating proteins and accelerating the termination of G protein signalling (Berman et al. 1996; Chen et al. 1996; Hunt et al. 1996; Watson et al. 1996). Initial studies of the effects of RGS proteins on GPCR-evoked GIRK currents revealed the anticipated acceleration in current deactivation, which was well explained by the RGS-accelerated GTPase activity of G
i/o subunits causing a more rapid sequesteration of channel-activating G
dimers (Doupnik et al. 1997; Saitoh et al. 1997). Unexpectedly, however, the accelerated deactivation was also accompanied with an accelerated activation phase in the absence of reduced current amplitude.
We analysed the temporal and steady-state GIRK current kinetics for the various conditions tested in this study using a simplified two-state gating scheme (Doupnik et al. 1997):

where the forward rate constant for GIRK channel opening (kopen) is dependent on the rate of G
production during GPCR activation (Breitwieser & Szabo, 1988; Yamada et al. 1998), and the closing rate constant (kclose) is dependent on G
clearance, which is rate-limited by the GTP hydrolysis rate of G
subunits. Accordingly, the time constant for GIRK channel deactivation (
deact) is equal to kclose-1, and the time constant for GIRK activation (
act) is equal to (kopen + kclose)-1 (Doupnik et al. 1997). Using these relations and an empirically derived kopen value of 0.03 s-1 (held constant to simulate a saturating agonist concentration), the experimentally derived
deact values were used to calculate 'expected' values of
act and steady-state GIRK current amplitudes (kopen/[kopen + kclose]) in the absence and presence of RGS expression according to the kinetic model. The 'expected' values were then compared to the experimentally 'observed' values (Table 2).
As seen in Table 2, the 'observed' effects of RGS4 on
act and steady-state amplitude for G
i-coupled GIRK currents closely correlate with the 'expected' consequences of the RGS4-accelerated deactivation rate, but not so for the G
o-coupled GIRK currents. Similarly, a correlation was seen for the effects of G
5 on RGS7-accelerated GIRK currents activated by G
o-coupled receptors. Thus during reduced levels of G protein coupling, GIRK channels behave according to standard kinetic concepts in response to RGS modulation and are consistent with the collision coupling model of G protein activation (Shea & Linderman, 1997; Shea et al. 2000). In contrast, RGS4 and RGS7 modulate G
o-coupled GIRK currents in a manner similar to previous descriptions of the anomalous kinetic effects of RGS proteins on GIRK channel gating which do not correlate with the kinetic model (Table 2) (Doupnik et al. 1997; Saitoh et al. 1997). We propose that these expression conditions promote the formation of a precoupled m2 receptor-G
o
-GIRK channel complex (Huang et al. 1995; Slesinger et al. 1995), having altered activation properties that are revealed by the modulatory effects of RGS proteins and effectively preserve maximal GIRK current amplitudes (see Fig. 8).
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Figure 8. RGS modulation of GPCR A, collision coupling model (low G | ||
GIRK activation kinetics revealed at low levels of basal activity
GIRK channels are composed of four Kir3.0 subunits with each subunit capable of binding a single G
dimer, thus a maximum of four G
dimers can bind to a single GIRK channel (Corey & Clapham, 2001). Several studies indicate GIRK channel activation is a multi-step process and may represent the binding of multiple G
dimers leading to channel opening (Hosoya et al. 1996; Sodickson & Bean, 1996; Nemec et al. 1999). Assuming four bound G
dimers promote the channel open state, receptor-independent basal GIRK activity represents channels transiently occupied by four G
dimers, excluding the potential influence of phosphatidylinositol-4,5-bisphosphate (PIP2), arachidonic acid, and intracellular Na+, Mg+2 and polyamines (Dascal, 1997; Yamada et al. 1998). IK,basal activity is directly related to the concentration of free G
in the cell membrane based on the effectiveness of G
scavengers to lower IK,basal amplitudes (Lim et al. 1995; Vivaudou et al. 1997; Jeong & Ikeda, 1999; Fernandez-Fernandez et al. 2001). According to the GIRK channel gating scheme shown in Fig. 4A, basal GIRK activity reflects channels transiently occupied by three to four G
dimers where random association of a single free G
subunit causes channel opening. Receptor activation of GIRK channels with high free G
concentrations predict a single G
binding event is necessary to activate the channels and IK,ACh will thus follow a single exponential time course. Conversely, receptor activation with low concentrations of free G
predict multiple binding events are necessary for channel opening, producing a sigmoidal IK,ACh time course analogous to the sequential movement of multiple gates during the activation of voltage-gated ion channels (Hodgkin & Huxley, 1952). The observed time course for receptor-dependent GIRK activation at the different levels of basal activity produced by high and low levels of G
o expression are in agreement with this and similar GIRK gating schemes (Destexhe & Sejnowski, 1995; Hosoya et al. 1996; Ivanova-Nikolova et al. 1998; Yamada et al. 1998). Different levels of GIRK-G
occupancy may also influence the voltage-dependent relaxation phenomena associated with RGS4 expression, which is only observed at low agonist concentrations (Inanobe et al. 2001). Although we deliberately express low levels of m2 receptors to slow GIRK activation rates (Herlitze et al. 1999), it should be emphasized that the GIRK activation and deactivation kinetics measured in the oocyte expression system, even with RGS expression, are consistently slower than native mammalian cells and may be limited by solution exchange rates and/or other intrinsic oocyte factors.
Interestingly, overexpression of a PTX-insensitive and RGS-resistant G
o mutant (G
oA(G184S:C351G)) in rat sympathetic neurons also reveals a prominent sigmoidal GIRK activation time course via
2-adrenergic receptor activation, and could be dramatically accelerated by coexpression of the N-terminal region of RGS8 (i.e. no RGS domain) (Jeong & Ikeda, 2001). The results of Jeong & Ikeda indicate the RGS8 N-terminal domain facilitates coupling of heterotrimeric G
oA(G184S:C351G)
subunits to
2-adrenergic receptors, and as a consequence greatly accelerates the GIRK activation time course. Based on our observations of RGS7 reported here, we speculate that N-terminal regions of RGS7 may similarly interact with m2 receptors and facilitate coupling to G
o in the absence of G
5.
Physiological implications
GIRK channels mediate sIPSPs in the nervous system where the time course and amplitude of inhibitory synaptic events are dependent on the G protein cycle (Luscher et al. 1997). Thus RGS proteins are likely to play an important role in determining the amplitude and temporal properties of GIRK-mediated sIPSPs. Our findings demonstrate GIRK-mediated sIPSPs may be determined by specific GPCR-G
-RGS signalling complexes that activate postsynaptic GIRK channels, where certain G
-RGS precoupled complexes accelerate GIRK activation and deactivation kinetics without compromising amplitude. Perturbation of these signalling complexes would reduce inhibitory synaptic transmission and promote cellular excitability. The consequences of these events in the mammalian nervous system remain to be elucidated, yet the demonstrated role of RGS complexes in coordinating locomotion and egg laying behaviour in Caenorhabditis elegans highlight their potential impact on mammalian neural signalling (Chase et al. 2001; Robatzek et al. 2001).
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