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Biophys J, July 2001, p. 89-96, Vol. 81, No. 1

Ca2+ Channel Inactivation Heterogeneity Reveals Physiological Unbinding of Auxiliary beta  Subunits

Sophie Restituito, Thierry Cens, Matthieu Rousset, and Pierre Charnet

CRBM, CNRS UPR 1086, UFR 24, 34293 Montpellier Cedex 05, France


    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS AND DISCUSSION
REFERENCES

Voltage gated Ca2+ channel (VGCC) auxiliary beta  subunits increase membrane expression of the main pore-forming alpha 1 subunits and finely tune channel activation and inactivation properties. In expression studies, co-expression of beta  subunits also reduced neuronal Ca2+ channel regulation by heterotrimeric G protein. Biochemical studies suggest that VGCC beta  subunits and G protein beta gamma can compete for overlapping interaction sites on VGCC alpha 1 subunits, suggesting a dynamic association of these subunits with alpha 1. In this work we have analyzed the stability of the alpha 1/beta association under physiological conditions. Regulation of the alpha 1A Ca2+ channel inactivation properties by beta 1b and beta 2a subunits had two major effects: a shift in voltage-dependent inactivation (Ein), and an increase of the non-inactivating current (Rin). Unexpectedly, large variations in magnitude of the effects were recorded on Ein, when beta 1b was expressed, and Rin, when beta 2a was expressed. These variations were not proportional to the current amplitude, and occurred at similar levels of beta  subunit expression. beta 2a-induced variations of Rin were, however, inversely proportional to the magnitude of G protein block. These data underline the two different mechanisms used by beta 1b and beta 2a to regulate channel inactivation, and suggest that the VGCC beta  subunit can unbind the alpha 1 subunit in physiological situations.


    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS AND DISCUSSION
REFERENCES

Different Ca2+ channel auxiliary beta  subunits have been isolated from mammalian brain and heart. They can potentially be associated with any of the 6 alpha 1 pore-forming subunits of high-voltage activated Ca2+ channel (alpha 1A, alpha 1B, alpha 1C, alpha 1D, alpha 1E, alpha 1F, and alpha 1S) via conserved interaction domains: alpha -interaction domain (AID) on alpha 1 and beta -interaction domain (BID) on beta  (De Waard et al., 1995, 1996; Pragnell et al., 1994; Walker and De Waard, 1998). These beta  subunits induced generic as well as specific modifications in the expression, electrophysiological properties, and regulation of any of the alpha 1 subunits. Increased channel expression, activity, and membrane targeting of the alpha 1 subunit are common modifications induced by all beta  subunits, whereas changes in the voltage-dependence and kinetics of activation and inactivation are more specific of a given pair of alpha 1-beta subunits (Mangoni et al., 1997; Sather et al., 1993; De Waard and Campbell, 1995; Jones et al., 1998; Stea et al., 1994). These effects appeared to be mediated by high affinity interactions between the AID (located on the loop connecting domains I and II of each alpha 1 subunits) (Pragnell et al., 1994) and the BID (located on the beginning of the second conserved region of the beta  subunit) (De Waard et al., 1994). Modification of these sites, using site-directed mutagenesis, produced a complete loss of the alpha 1/beta subunits co-localization and co-immunoprecipitation, but only partially reverted the increase in current amplitude and change in electrophysiological properties of alpha 1 (Gerster et al., 1999; De Waard et al., 1994). These latter results suggest that the beta  subunit modifies channel targeting and/or current amplitude using molecular determinants distinct from those necessary for the modification of the electrophysiological properties (Gerster et al., 1999). Indeed, functional analysis of mutated and truncated alpha 1 and beta  subunits revealed that additional interaction sites of lower affinity (on the N- and C-terminal tails of the alpha 1 and beta  subunits) may also participate to these regulations (Birnbaumer et al., 1998; Cens et al., 1998; Olcese et al., 1994; Qin et al., 1996; Walker et al., 1998).

It should be noted that although the AID-BID interaction occurs through high-affinity sites, the recent identification of a G protein beta gamma binding site overlapping the AID suggests that this interaction can be disrupted in certain circumstances, such as when G proteins are activated (De Waard et al., 1997; Zamponi et al., 1997). Indeed, in an heterologous expression system, the Ca2+ channel block by G protein is decreased by expression of an auxiliary beta  subunit (Bourinet et al., 1996) suggesting competition between overlapping sites and possible disruption of the AID-BID interaction. In normal conditions however, such unbinding has never been observed.

Slowing of inactivation has been reported when the beta 2a subunit is co-expressed with the neuronal alpha 1A, alpha 1B, alpha 1C, and the alpha 1E subunits (Sather et al., 1993; Mangoni et al., 1997, De Waard and Campbell, 1995; Stea et al., 1994; Jones et al., 1998; Cens et al., 1999). The mechanism underlying this effect has recently been proposed to be due to immobilization of the channel inactivation gate by a membrane-anchoring site (Restituito et al., 2000) constituted of two palmitic acid bound to cysteines 3 and 4 of the amino-terminal tail of the beta 2a subunit (Chien et al., 1996, 1998; Qin et al., 1998).

Here we report a significant heterogeneity in the voltage-dependence and kinetics of inactivation of the alpha 1A P/Q-type Ca2+ channel expressed with the beta 2a or beta 1b subunits. Variable parameters are the fraction of non-inactivating current (Rin) for beta 2a and the voltage for half-inactivation (Ein) for beta 1b. However, expression of alpha 1A and alpha 2 - delta  without beta  results in more homogeneous inactivation properties. A more complete analysis of voltage-dependent activation and inactivation and G protein regulation was performed using different mutated beta  subunits at different alpha 1A/beta 2a cDNA ratios and suggested unbinding of the beta  subunit from the alpha 1 subunit. Altogether these results provide evidences for a dynamic association between these two subunits.


    MATERIALS AND METHODS
TOP
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS AND DISCUSSION
REFERENCES

Preparation of mutated beta  subunits

The following calcium channel subunits were used: alpha 1A (Starr et al., 1991), beta 1b (Pragnell et al., 1991); beta 2a (Perez-Reyes et al., 1992), and alpha 2delta . All these cDNAs were inserted into the pMT2 expression vector (Stea et al., 1994). The chimera CD8-beta 2aC3,4S construction was produced as described previously (Restituito et al., 2000).

Xenopus oocyte preparation and injection

Xenopus oocyte preparation and injection (5-10 nl of a mixture of alpha 1, alpha 2-delta , or beta  subunits cDNAs at approx 0.3 ng/nl each) were performed as described elsewhere (Cens et al., 1996). For Fig. 4, starting cDNA concentration was either 1 or 0.1 ng/nl for alpha 1A and beta 2a subunits, giving a final concentration of 0.3 or 0.03 ng/nl after dilution. Oocytes were selected as expressing slow- or fast-inactivating currents after individual recordings in voltage-clamp. Oocytes from each pool (fast, slow, non-expressing, and non-injected) were then frozen in liquid nitrogen and kept for Western blotting. Each line was loaded with the equivalent of three oocytes expressing the same quantity of currents. µ opioid receptor and alpha O G protein RNA (1 µg/µl) were injected 1 day after cDNA injection. Oocytes were then incubated for 2 to 7 days at 19° C under gentle agitation before recording.

Western blot

Frozen oocytes were homogenized in 5 µl/oocytes of the following lysis buffer [20 mM Tris (pH 7.5), 50 mM NaCl, 50 mM NaF, 10 mM beta glycerophosphate, 5 mM Na4P2O7, 5 mM EDTA; 5 mM EGTA, 10 mg/ml PMSF, 0.2 mg/ml pepstatin, 0.2 mg/ml leupeptin, and 0.2 mg/ml aprotinin] and centrifuged for 3 min at 20,000 × g at 4°C. The supernatant was boiled in sodium dodecyl sulfate (SDS) gel loading buffer (Laemmli), electrophoresed on 10% SDS-polyacrylamide gel, and transferred to nitrocellulose filter. Filters were blocked 1 h at room temperature (8% skim milk powder), rinsed in distilled water, incubated overnight at 4°C with the beta -com rabbit polyclonal primary antibody in 0.1% bovine serum albumin (CW24; Vance et al., 1998), washed 3 times, incubated 1 h with an anti-rabbit antibody, and detected by chemiluminescence (Renaissance NEN, Boston, MA).

Electrophysiological recordings

Whole-cell Ba2+ currents (<5 µA) were recorded under two electrodes voltage-clamp using the GeneClamp 500 amplifier (Axon Instruments, Burlingame, CA). Current and voltage electrodes (<1 MOmega ) were filled with 2.8 M CsCl and 10 mM BAPTA, pH = 7.2, with CsOH. Ba2+ current recordings were performed after injection of BAPTA (around 50 nl of (mM): BAPTA-free acid (Sigma), 100; CsOH, 10; HEPES, 10; pH 7.2 CsOH) using the following solution (in mM): BaOH, 10; TEAOH, 20; NMDG, 50; CsOH, 2; HEPES, 10; pH 7.2 with methanesulfonic acid. Currents were filtered and digitized using a Digidata 1200 interface (Axon Instruments), and subsequently stored on a Pentium II-based personal computer by using the version 6.02 of the pClamp software (Axon Instrument). Ba2+ currents were recorded during a test pulse from -80 mV to +10 mV of 2.5 sec duration. Current amplitudes were measured at the peak of the current. Pseudo steady-state inactivation (2.5 s of conditioning depolarization followed by a 400 ms test pulse to +10 mV) was fitted using the following equations
I/I<SUB><UP>max</UP></SUB>=R<SUB><UP>in</UP></SUB>+(1−R<SUB><UP>in</UP></SUB>)/(1+<UP>exp</UP>((V−E<SUB><UP>in</UP></SUB>)/k)) (1)
where I is the current amplitude measured during the test pulse at +10 mV for conditioning depolarization varying from -80 to +50 mV; Imax, the current amplitude measured during the test-pulse for a conditioning depolarization of -80 mV; Ein, the potential for half-inactivation; V, the conditioning depolarization; k, the slope factor; and Rin, the proportion of non-inactivating current. Current to voltage curves were fitted using the following equation
I/I<SUB><UP>max</UP></SUB>=G*(V−E<SUB><UP>rev</UP></SUB>)<UP>/</UP>(<UP>1 + exp</UP>((V−V<SUB><UP>act</UP></SUB>)/k)) (2)
where I is the current amplitude measured during depolarizations varying from -80 to +50 mV; Imax, the peak current amplitude measured of the current-voltage curve; G, is the normalized macroscopic conductance; Erev, is the apparent reversal potential, Vact: the potential for half-activation; V, the value of the depolarization; and k, a slope factor.

Activation of G protein-coupled µ opioid receptor was performed by perfusion of 10 µmol of the specific agonist Tyr-D-Ala-Gly-N-Methyl-Phe-Gly-ol (DAMGO; Sigma-Aldrich, Saint Quentin Fallavier, France). % block induced by DAMGO was calculated by dividing the current amplitude in control conditions by the current amplitude recorded at the steady state effect of 10 µM DAMGO during train of 50-ms depolarizations at 0 mV. All values are presented as mean ± SEM.


    RESULTS AND DISCUSSION
TOP
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS AND DISCUSSION
REFERENCES

Xenopus oocytes were injected with cDNA encoding the alpha 1A + alpha 2 - delta  and either the beta 1b or beta 2a subunit, and Ba2+ currents were recorded 2-5 days later. As seen in Fig. 1, A and B (left), and as already shown by others (De Waard and Campbell, 1995; Stea et al., 1994), these two combinations of subunits induced the expression of P/Q type Ba2+ currents with fast and slow inactivation, respectively. The voltage protocol applied to the oocytes (shown on top of Fig. 1) allows for the same recording to calculate current-voltage and inactivation curves as well as inactivation kinetics. The slowing of inactivation by the beta 2a subunit was clear for depolarized (>-20 mV) potentials, and the inactivation curves allow to calculate the potential for half-inactivation (Ein) and the proportion of non-inactivating current (Rin) for each combination of subunits. Averaged values gave an Ein of -28.2 ± 9.8 mV and -12.8 ± 5 mV and an Rin of 0.098 ± 0.002 and 0.48 ± 0.004 for beta 1b (n = 28) and beta 2a (n = 56). Comparison with the values obtained in the absence of expressed beta  subunit (alpha 1A + alpha 2 - delta ; Ein = -12.2 ± 2.2mV and Rin = 0.08 ± 0.002, n = 16) demonstrate that the major effect of beta 1b subunit was to decrease the availability of the channel by hyperpolarizing Ein, whereas the major effect of beta 2a was to prevent inactivation by increasing Rin. However, when typical individual inactivation curves recorded for each combination were plotted on the same graph (Fig. 1, right), a large variation in the Ein and Rin values can be seen for each subunit combination. This variation was better seen in Fig. 2 A, in which individual Rin values are plotted against their corresponding Ein value for all combinations of subunits tested (n > 200 oocytes). From such a plot, 3 groups can be identified. The control alpha 1A group (open square), corresponds to oocytes expressing the alpha 1A alpha 2-delta subunits without beta  subunit. For this group, the inactivation parameters (Ein and Rin) are well centered around their average values, as expected for an homogeneous population. The beta 2 group (triangle) represents oocytes injected with alpha 1A + alpha 2-delta and the beta 2a subunit cDNAs. This group displays low variability in their Ein values (which are almost similar to Ein of the alpha 1A group), but large variations in Rin ranging from 0.1 to 0.9. In this group, smaller values of Rin are close to the average Rin value of the alpha 1A group. In the case of the beta 1 group (oocytes injected with alpha 1A + alpha 2 - delta  + beta 1b cDNA; Fig. 2 A, open circle) the variations are more pronounced for Ein (starting from -10 mV, the average value of the control alpha 1A group, and decreasing up to -55 mV), whereas Rin appeared almost unchanged when compared to alpha 1A group. Hyperpolarization of the inactivation curve and reduction of inactivation, the two fundamental effects of the beta 1b and beta 2a subunits, respectively, are therefore subject to large variations in vivo despite the known high-affinity interaction between the alpha 1A and the beta  subunits. Such variations has also been found in chromaffin cells and tsA201 cells transfected with the alpha 1B, or alpha 1A and beta 2a subunits (Cahill et al., 2000; Hurley et al., 2000).



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FIGURE 1   Heterogeneity of voltage-dependent inactivation. Voltage-dependent inactivation curves recorded from oocytes expressing the alpha 1A and alpha 2 - delta  Ca2+ channel subunits with either the beta 1b (A) or beta 2a (B) auxiliary subunits. (Left) Typical current traces recorded on oocytes expressing alpha 1A + alpha 2 - delta  + beta 1b or alpha 1A + alpha 2 - delta  + beta 2a subunit during the voltage protocol shown on top. The conditioning depolarisation had a duration of 2.5s, test-pulse (+10 mV) duration was 0.4 s. Scale bar, 0.5 µA. (Right) Example of 8 typical steady-state inactivation curves recorded on different oocytes for each of the two combinations of subunits. Note the variability in the voltage for half-inactivation (Ein) and in the proportion of the non-inactivating current (Rin).



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FIGURE 2   beta 1 and beta 2-induced regulation of inactivation. (A and B) Scatter plot of Rin versus Ein for different batches of oocytes (n>200) injected with the alpha 1A and alpha 2 - delta  subunits alone or in combination with beta 1b, beta 2a (A), CD8-beta 2C3,4S or beta 2C3,4S (B; see Results and Discussion). Note that these oocytes can be divided into 3 groups. The control alpha 1A group included oocytes expressing the alpha 1A + alpha 2 - delta  subunits and show limited variability in either Ein and Rin. The beta 2 group, displays the same Ein than alpha 1A + alpha 2 - delta  but with higher Rin (includes oocytes expressing alpha 1A+ alpha 2 - delta  + beta 2a, or CD8-beta 2C3, 4S). Currents recorded from oocyte belonging to the beta 1 group have the same Rin than alpha 1A + alpha 2 - delta , but more hyperpolarized Ein (group of oocytes expressing alpha 1A + alpha 2 - delta  + beta 1b or beta 2C3, 4S). For the beta 1b group, variability is more pronounced for Ein, while for the beta 2 group, Rin was the most variable parameter. (C) Scatter plot of Ein versus Vact, the potential of half activation for the oocytes shown on A. The two groups of oocytes induced an hyperpolarization of the IV curves. This hyperpolarization was correlated with a negative shift of Ein for the beta 1 group that was less pronouned for the beta 2 group. (D) Scatter plot of Rin versus Vact, the potential of half activation, for the currents recorded from the same oocytes shown on A. Hyperpolarizing shift of the IV curve (Vact) was correlated with an increase in Rin for the beta 2, but not the beta 1 group. Lines are drawn to show tendencies. Symbols in C and D are the same as in A and B.

The slowing of inactivation by beta 2a has been attributed to palmitoylation of cysteines at position 3 and 4 in the beta 2a subunit (Qin et al., 1998). Modulation of this post-translational modification can thus be a reason for variations in the voltage-dependence and kinetics of inactivation (Chien et al., 1998; Hurley et al., 2000; Qin et al., 1998). To assess this, we have injected cDNA of the beta 2a subunits mutated at cysteines 3,4 (beta 2C3, 4S subunit) with the alpha 1A and alpha 2 - delta  subunits and analyzed the inactivation parameters of the expressed channels. Mutation of Cys3,4 to Ser decreases Rin to values normally recorded with the alpha 1A+ alpha 2 - delta  subunits expressed alone or with beta 1b (Fig. 2 B, diamond). The mutation also shifts Ein toward hyperpolarized values to varying degrees. Thus, the effect of the mutation on the beta 2a subunits seems to transfer the variability in Rin associated to beta 2a subunit to variability in Ein normally recorded with the beta 1b subunit, suggesting that variations of these two parameters arise from a common mechanism. Further analysis of the role of Cys3,4 was done by expressing a chimera where a transmembrane CD8 domain was added at the N terminus of this beta 2C3,4S mutated subunit (CD8-beta 2C3, 4S subunit). This subunit is able to slow alpha 1A channel inactivation without being palmitoylated (Restituito et al., 2000). Interestingly, this CD8-beta 2C3,4S subunit expressed with the alpha 1A + alpha 2 - delta  subunits gave slowly inactivating channels that behaved exactly like the beta 2a subunit, i.e., displaying large variations in their Rin values but low variability in Ein (Fig. 2 B, inverted triangle). Such results clearly argue against any participation of the palmitoylation of the beta 2a subunit in the variability recorded with Rin as can be seen in other systems (Hurley et al., 2000).

Inspection of the ability of these subunits to modulate the activation properties of the alpha 1A subunit (Fig. 2 C) has been done by plotting Ein versus the potential for half-activation (Vact) for each oocyte. As seen in Fig. 2 C, all subunit combinations are capable of hyperpolarizing the voltage-dependence of activation of the channel. In the case of the beta 1b group, however, this shift was graded with the hyperpolarizing shift in Ein. In the case of the beta 2 group, almost no change in Ein could be recorded. Similarly, when Rin was plotted versus Vact (Fig. 2 D), the same type of relation appeared, i.e., the hyperpolarizing shift in Vact was graded with the increase in Rin value for the beta 2 group, but not for the beta 1 group. The alpha 1A group (open square) still displays a low degree of variability.

One obvious explanation for these large variations in Ein and Rin is the variable degree of expression of auxiliary beta  subunit between different oocytes. In this case, since the primary effect of beta  subunits is to increase channel expression, the magnitude of the effect (shift in Ein or increase in Rin) is expected to be correlated to the amplitude of the current, because this latter parameter is proportional to the number of functional channels expressed. Plots of Ein and Rin values against current amplitude (Fig. 3, A and B) for these different mutations clearly show that this was not the case, and the lack of clear relation between changes in Ein and Rin and current amplitude therefore argues against a deficit in beta  subunit expression as a possible mechanisms to account for the observed effects. For the same reasons, any technical artifacts due to a poor voltage-control also appears very unlikely in these oocytes. Moreover, the fact that small Rin values in the beta 2 group have Ein comparable to the alpha 1A group (Fig. 2 A), suggest that these variations are not due to over-expression of an endogenous beta 3 subunits (Tareilus et al., 1997) which one would expect to also hyperpolarize Ein.



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FIGURE 3   (A and B) Scatter plots of Ein (A) and Rin (B) versus the maximum amplitude of the corresponding current. In each case variations in Ein (for the beta 1 group, A), or Rin (for the beta 2 group, B) were not related to the amplitude of the current suggesting that deficient expression of the channel auxiliary subunits was not the cause of the variability. (C and D) Individual and averaged Ba2+ current amplitude (C) and inactivation (Rin, D) recorded on oocytes expressing different ratios of alpha 1A/beta 2 subunits cDNA. Ten nl of a v/v mixture of alpha 1A, beta 2 (at a concentration of 0, 0.1, or 1 µg/µl, as indicated) and alpha 2 - delta  (1 µg/µl) subunit cDNAs were injected into oocytes, and currents were recorded 3-4 days later. (E) Lack of correlation between current amplitude and Rin for oocytes injected with ratios of alpha 1A/beta 2a cDNA giving the largest variability in inactivation (1/1, inverted triangle, and 1/0.1, diamond).

Indeed, the slow inactivation induced by the beta 2a subunit was never observed when beta 2a cDNA was not injected. In such conditions, expression was low (0.2-1 µA, see alpha 1/beta = 0.1/0 and 1/0, Fig. 3 C) and inactivation was fast (low Rin values, Fig. 3 D). Similar values are obtained for two concentrations of alpha 1A subunit cDNA injected (0.1 and 1ng/nl, p > 0.05), suggesting that functional expression of this subunit was already saturating at the lowest cDNA concentration. Co-injection of beta 2a subunit cDNA, either at low (0.1) or high (1) concentration induced a significant increase in current amplitude (Fig. 3 C) and a slowing of inactivation (p < 0.05; Fig. 3 D). Both effects were recorded for the two alpha 1A concentrations (alpha 1/beta = 0.1/1 and 1/1, Fig. 3 C). However, whereas variability in current amplitude was recorded at all the concentrations of the alpha 1A and beta 2a cDNA tested (maximum and minimum amplitude values were almost identical in all cases, alpha 1/beta = 0.1/1; 1/1 and 1/0.1), variability in inactivation (Rin) was more prominent for the highest alpha 1A/beta 2a subunit ratio (1/0.1), and only slow-inactivating currents were recorded at alpha 1/beta = 0.1/1. The fact that different degree of regulation of inactivation by the beta 2a subunit can be recorded at two concentrations of alpha 1A, (0.1 and 1, both saturating for expression of functional channels), and that this regulation did not correlate with the expressed current amplitude using two different beta  subunit concentrations (see 1/0.1, inverted triangle; and 1/1, diamond; n = 67 and 119, respectively, Fig. 3 E) suggested that the individual variation was not due to inter-oocyte variability in the level of expression of the beta 2a subunit.

This hypothesis was tested directly by coupling the electrophysiological measurement with the immunochemical evaluation of the beta 2a subunit expression. Oocytes were injected with a alpha 1A/beta 2a subunit:cDNA ratio of 1:1, and Ba2+ currents were recorded 2-3 days later. Current amplitude and inactivation (Rin) were then estimated and allowed the selection of the oocytes into two groups (fast and slowly inactivating). Oocytes were then homogenized, and analyzed by SDS-page electrophoresis and Western blot using a anti-beta antibody. Bottom of Fig. 4 A shows averaged current amplitude and inactivation of these two groups (n = 5 for each group). Despite differences in inactivation, the amplitude of each group was very similar. Moreover Western blot analysis (3 oocytes/line, representing ~5 µA of current) showed that the level of expression of the beta 2a subunit was almost identical between the fast and slowly inactivating oocytes, and clearly distinct from the non-expressing or non-injected oocytes. Therefore, neither defect in palmitoylation, nor deficient expression of the beta 2a subunit, could explained the observed changes in inactivation.



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FIGURE 4   (A) Oocytes with currents showing fast or slow inactivation expressed the same level of beta 2a subunit. Oocytes were injected with 10 nl of cDNA with a alpha 1A/beta 2a ratio of 1/0.1. Three days later, oocytes were selected in 3 batches according to the properties of their Ba2+ currents (n.e., no expression; slow, current with an Rin > 0.5; fast, current with Rin < 0.5). For each batch, averaged current amplitude and inactivation were recorded (see histogram). Oocytes were then homogenized, centrifuged and processed for Western blotting using an anti-beta com antibody (3 oocytes/line corresponding to ~5 µA; n.i, non-injected). The mean current amplitude and Western blot suggest similar levels of expression of the alpha 1A and beta 2a subunit in the fast and slow oocytes. (B) Typical current traces recorded from oocytes expressing alpha 1A + alpha 2 - delta  or alpha 1A + alpha 2 - delta  + beta 2a subunits before and at the steady state effects of DAMGO (*, 10 µM). Holding potential was -80 mV. The second test pulse (0 mV, see voltage protocol at top) is preceded by a prepulse at +100 mV that allow partial relieve of the inhibition induced by DAMGO. Note the differences in inactivation kinetics and block by DAMGO between alpha 1A + alpha 2 -delta and alpha 1A + alpha 2 - delta  + beta 2a oocytes. Scale bar, 0.5 µA. (C) Scatter plots of the percentage of inhibition of the Ba2+ currents recorded during the perfusion of the µ opioid agonist DAMGO (10 µM), and the inactivation properties of the corresponding current. Inactivation was quantified by calculating Rin as above. Two different combinations of subunits were studied alpha 1A + alpha 2 - delta  and alpha 1A + alpha 2 - delta  + beta 2a. In the case of alpha 1A + alpha 2 - delta  + beta 2a, note the correlation between Rin and the magnitude of the inhibition by DAMGO.

Dissociation of a variable proportion of the auxiliary beta  from alpha 1A subunits, after targeting of the pore-forming subunit to the membrane, may also cause these effects. Indeed, these two different functions of the beta  subunits have recently been shown to be due to different and independent interaction sites (Gerster et al., 1999) and reversible alpha 1/beta interaction has been proposed (Bichet et al., 2000; Gerster et al., 1999). This "unbinding" hypothesis can be tested by analyzing the regulation of the Ba2+ currents by G proteins. G protein-induced inhibition of the alpha 1A Ca2+ channel has been shown to be greatly reduced by co-expression of beta  subunits (Bourinet et al., 1996), and can therefore be used as an index of association between the alpha 1A and the beta  subunits. Oocytes were co-injected with RNA encoding the µ opioid receptor and cDNA of alpha 1A and alpha 2 -delta subunits alone or with the beta 2a subunit. G protein activation was achieved by superfusion of 10 µM DAMGO, a specific µ opioid agonist, and both the level of inactivation of the Ba2+ current (determined as Rin) and the extend of G protein block of the current were calculated. Fig. 4 B shows that perfusion of DAMGO on oocytes expressing alpha 1A+alpha 2-delta subunits induced a pronounced inhibition (approx 70%) of the rapidly inactivating Ba2+ current. This inhibition was voltage-dependent, as it could be partially reversed by applying a 50-ms prepulse to positive voltages (+100 mV). When the same experiment was performed on oocytes expressing the alpha 1A + alpha 2 - delta  + beta 2a subunits, current inhibition induced by DAMGO was greatly reduced, especially on those oocytes that have the slowest inactivation kinetics (see bottom of Fig. 4 B). A scatter plot of this inhibition versus the inactivation parameter Rin (see Materials and Methods) for different oocytes is shown on Fig. 4 C. Both, the fast inactivation kinetics and the marked inhibition by DAMGO recorded with alpha 1A + alpha 2 - delta  were systematically recorded on these batches of oocytes, and therefore values for Rin and percentage of inhibition by DAMGO display a low dispersion (alpha 1A group, Fig. 4 C). However, on oocytes injected with alpha 1A + alpha 2 - delta  + beta 2a cDNA, values for both inactivation (Fig. 1) and percentage of inhibition by DAMGO were more dispersed (beta 2 group, Fig. 4 C). In this group, the decrease in the inhibition by DAMGO was correlated to a slowing of inactivation. Again, these effects were not related to the absolute amplitude of the current, since G protein-sensitive or G protein-resistant currents of similar amplitude could be recorded from oocytes expressing the alpha 1A + alpha 2 - delta  + beta 2a subunits (data not shown).

The simplest explanation for these results is to propose an unbinding of the auxiliary beta  subunit from the alpha 1A. Such a dissociation removes the modulatory role of the beta  subunit on inactivation, as well as blockade of G protein modulation. Thus, for each oocyte, a mixed population of channels with or wihtout beta  subunit in variable proportions, could co-exist on the oocyte membrane. The magnitude of the beta  subunit effect may therefore result from the proportion of bound beta  subunits on the AID of channel. Because no clear relation can be found between the magnitude of this effect and current amplitude, we propose that the beta  subunit can unbind the channel after membrane targeting of the alpha 1 subunits. Moreover, considering that fast or slow inactivating kinetics could be recorded for current of similar amplitudes in the same batch of alpha 1A + alpha 2 - delta  + beta 2a-injected oocytes, lead us to suggest that this unbinding of auxiliary subunit does not affect the probability of opening of the channel, but only the transition to the inactivated state. Unbinding can occur for the beta 1 or the beta 2 subunits (as well as the different mutants presented) and is best revealed by the modulation of the inhibition by G proteins. Because the presence of a beta  subunit is an important determinant for channel regulation by G proteins, dissociation occurring in physiological conditions, therefore, represents a new pathway for modulating channel properties and regulation. Preliminary experiments using cAMP derivative and kinase inhibitors (W7, H89) suggest that PKA phosphorylation is not directly involved in this pathway. Recently, based on the different membrane distribution of the alpha 1 subunit when expressed alone or with the beta  subunit, it has been hypothesized that alpha 1/beta 2 interaction may results in secondary interactions with other cellular proteins (such as PDZ-domain-containing proteins; Gao et al., 1999) and stabilization of the complex at specific membrane location. Differential expression of such proteins between oocytes of a same batch may therefore constitute an interesting direction for future experiments. Whether beta  subunits remain bound to the alpha 1 subunit, using secondary interaction sites of minor importance regarding inactivation and G protein regulations, remains also to be determined.

    ACKNOWLEDGMENTS

We thank Dr G. Zamponi, Dr. I. Lefevre, and Dr. P. Bello for critical comments, Dr. M. de Waard for help in the construction of the CD8-beta 2C3,4S subunit, Dr. McEnery for CW24 antibody, and Dr. E. Mandart and C. Barrère for technical help. This work was supported by GRRC FRM (financial support to S.R. and T.C., respectively), Ligue Régionale Contre le Cancer, ARC and AFM.

    FOOTNOTES

Received for publication 1 August 2000 and in final form 12 April 2001.

Address reprint requests to Dr. Pierre Charnet, CRBM, CNRS UPR 1086, UFR 24, 1919 Route de Mende, Montepellier, Cedex 05, France 34293; Tel.: 33-4-67613352; Fax: 33-4-67521559; E-mail: charnet{at}crbm.cnrs-mop.fr.


    REFERENCES
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ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS AND DISCUSSION
REFERENCES

Biophys J, July 2001, p. 89-96, Vol. 81, No. 1
© 2001 by the Biophysical Society   0006-3495/01/07/89/08  $2.00



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