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J. Biol. Chem., Vol. 280, Issue 13, 12474-12485, April 1, 2005
Differential Role of the
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| ABSTRACT |
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1C and auxiliary
and
2
subunits. Voltage-dependent conformational rearrangements of the
1C subunit C-tail have been implicated in Ca2+ signal transduction. In contrast, the
1C N-tail demonstrates limited voltage-gated mobility. We have asked whether these properties are critical for the channel function. Here we report that transient anchoring of the
1C subunit C-tail in the plasma membrane inhibits Ca2+-dependent and slow voltage-dependent inactivation. Both
2
and
subunits remain essential for the functional channel. In contrast, if
1C subunits with are expressed
2
but in the absence of a
subunit, plasma membrane anchoring of the
1C N terminus or its deletion inhibit both voltage- and Ca2+-dependent inactivation of the current. The following findings all corroborate the importance of the
1C N-tail/
interaction: (i) co-expression of
restores inactivation properties, (ii) release of the
1C N terminus inhibits the
-deficient channel, and (iii) voltage-gated mobility of the
1C N-tail vis à vis the plasma membrane is increased in the
-deficient (silent) channel. Together, these data argue that both the
1C N- and C-tails have important but different roles in the voltage- and Ca2+-dependent inactivation, as well as
subunit modulation of the channel. The
1C N-tail may have a role in the channel trafficking and is a target of the
subunit modulation. The
subunit facilitates voltage gating by competing with the N-tail and constraining its voltage-dependent rearrangements. Thus, cross-talk between the
1C C and N termini,
subunit, and the cytoplasmic pore region confers the multifactorial regulation of Cav1.2 channels. | INTRODUCTION |
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1C subunit C-terminal tail (14). CaM signals Ca2+ for transcription activation (5) or Ca2+-induced intracellular Ca2+ release (6) by the voltage-gated rearrangement of the
1C subunit C terminus, thus linking Ca2+-dependent inactivation (CDI) and Ca2+ signal transduction (7). With these voltage- and Ca2+-gated rearrangements, the role of the Cav1.2 cytoplasmic termini may be further defined when the
1C subunit tails are uncoupled from the channel regulation by transient immobilization in the plasma membrane.
The association of
1C with the auxiliary
2
and
subunits is important for the functional expression of Cav1.2 channels. The cytoplasmic
subunit binds to a conserved "
-interaction domain" in the
1C subunit cytoplasmic linker between transmembrane repeats I and II (8, 9). The extracellular
2 subunit is bound via an SS bridge to its post-translationally cleaved transmembrane
peptide (10, 11) that renders association with
1C. Both
2
(1214) and
subunits (1519) modulate the channel. In particular,
subunits affect the time course of the Ba2+ current decay up to 3-fold depending on the type of the
subunit.
To study conformational rearrangements in the channel in response to depolarization, measurements of differential changes in fluorescence resonance energy transfer (FRET) between the cyan (ECFP) and yellow (EYFP) fluorescent proteins fused to the
1C and
subunit termini have been an effective approach. The current findings begin to specify the central features of conformational rearrangements associated with the transition of the channel from the resting (90 mV) to the inactivated state of Cav1.2. With the (EYFP)N-
1C,77-(ECFP)C/
1a/
2
channel as a model, FRET microscopy showed reversible voltage-gated rearrangements between the
1C,77 tails and pointed to a role for the C-terminal mobile tail in intracellular Ca2+ signal transduction (5). Another study (20) characterized the voltage-gated rearrangements between the N-terminal tails of the
1C and
subunits associated with differential
subunit modulation of inactivation and demonstrated limited rearrangements of both N-tails with regard to the plasma membrane.
To investigate further the role of voltage-gated mobility of the
1C,77 N-terminal tail for function of the Cav1.2 channel, here we have investigated the effects of N-terminal deletion or plasma membrane immobilization on Ca2+- and voltage-dependent inactivation, as well as
subunit regulation of the channel. Most interestingly, if the
1C/
2
channel is assembled without a
subunit, either deletion or anchoring of the
1C,77 N-terminal tail results in high amplitude non-inactivating Ba2+ or Ca2+ currents. This provides a mechanism to explain how limited mobility of the
1C subunit N-terminal tail integrates the
subunit and the
1C subunit C terminus in inactivation of the channel.
| MATERIALS AND METHODS |
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1C subunit (see Supplemental Material) showed substantial diversity of the transcripts because of alternative splicing. The exon-22 isoform (GenBankTM accession number Z34815
[GenBank]
) of the human hippocampus
1C subunit, known as
1C,77 (21), was selected for this study because it was identified in other human tissues and cells. (EYFP)N-
1C,77, (PH-EYFP)N-
1C,77,
1C,77-(PH-ECFP)C, and (ECFP)N-PH and (EYFP)N-PH (22) expression plasmids (N and C indicate the N and C terminus of a subunit, respectively) were prepared in the pcDNA3 vector for eukaryotic expression as described earlier (5) by using pEYFP and pECFP vectors (Clontech). To delete the N-terminal amino acids 2120 of the
1C,77 subunit, the PCR product obtained by amplification of pHLCC77 (21) with the sense 5'-tggatccgccaccATGGTCGAATGGAAACCATTTG-3' and antisense 5'-AGCCATGATCCCATCATACATCAC-3' primers (noncoding nucleotides are shown in lowercase letters) was digested by BamHI and SgrAI and ligated at the respective sites into 77-pcDNA3 (23). Nucleotide sequences of all PCR and ligation products were confirmed at the DNA sequencing facility of the University of Maryland. The
1a and
2
subunits in pcDNA3 vector were prepared as described by Soldatov et al. (24).
Transient Expression in COS1 CellsCOS1 cells were maintained at 37 °C and 5% CO2 in Dulbecco's modified Eagle's medium supplemented with 10% (v/v) fetal calf serum (Invitrogen). For transient Ca2+ channel expression, cells were plated on poly-D-lysine-coated coverslips (MatTek) 18 h before transfection with cDNAs coding for the indicated
1C,
1a, and
2
subunits of the Ca2+ channel (1:1:1, w/w) using an Effectene kit (Qiagen) according to the protocol described previously (20). Transfected cells were visualized by ECFP or EYFP tags genetically fused to the
1C subunits. In some experiments, the G
q Q209L mutant (The Guthrie Research Institute, Sayre, PA) was co-expressed with Ca2+ channel subunits.
Electrophysiological ExperimentsWhole-cell patch clamp recordings were performed at room temperature (2022 °C) using the Axopatch 200B amplifier (Axon Instruments) 4872 h after transfection. The extracellular bath solution contained the following (in mM): 100 NaCl, 20 BaCl2, 1 MgCl2, 10 glucose, 10 HEPES, adjusted to pH 7.4, with NaOH. Borosilicate glass pipettes were fire-polished and showed a typical resistance of 36 megohms when filled with pipette solution containing the following (in mM): 110 CsCl, 5 MgATP, 10 1,2-bis(2-aminophenoxy)ethane-N,N,N',N'-tetraacetic acid, 20 tetraethylammonium, 0.2 cAMP, and 20 HEPES, adjusted to pH 7.4 with CsOH (24). Capacitance compensation and series resistance were set at 60%. Currents were sampled at 2.55 kHz and filtered at 1 kHz. Voltage protocols were generated, and data were digitized, recorded, and analyzed using pClamp 8.1 software (Axon Instruments). The holding potential (Vh) was 90 mV, and test pulses were applied at 30-s intervals. Current-voltage (I-V) curves were obtained by step depolarizations to test potentials in the range of 60 to +50 mV (with 10-mV increments) applied from the holding potential. Statistical values are given as means ± S.E.
Single channel recordings were carried out in cell-attached configurations at 24 °C in the bath solution containing the following (in mM): 110 L-aspartic acid, 20 KCl, 2 MgCl2, 2 EGTA, and 20 HEPES, adjusted to pH 7.4 with KOH. The pipette solution contained the following (in mM): 110 BaCl2, 5 HEPES, adjusted to pH 7.4 with NaOH. The pipettes were heat-polished and showed resistances of 34.5 megohms. Step depolarizations to the indicated potentials were applied from Vh = 90 mV for 1 s followed by inter-pulse intervals of 5 s. Currents were sampled at 40 kHz and low pass-filtered with a gauss filter at 500 Hz. Histograms with a bin size of 0.03 pA were fit with a sum of two gauss functions. Single channel data were analyzed using Clampfit 9.2 software (Axon Instruments)
FRET measurements were combined with whole-cell patch clamp as described in detail by Kobrinsky et al. (5, 20). Images were recorded with a Hamamatsu digital camera C4742-95 mounted on the Nikon epifluorescent microscope TE200 (60 x 1.2 N.A. objective) equipped with an excitation 75-watt xenon lamp and multiple filter sets (Chroma Technology). Acquisition and analysis of FRET images were carried out with C-Imaging (Compix) and MetaMorph (Universal Imaging) software packages. Conditions for the measurements of corrected images of FRET between (ECFP)N-PH and (EYFP)N-
1C,77 in the absence or on the presence of the
1a subunit closely matched those described recently (20).
| RESULTS |
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1C,77 subunit C- and N-terminal tails in inactivation of the Cav1.2 channel and its regulation by
subunits. To simplify the interpretation of the results, in most of this series of experiments we used the protein kinase C-insensitive Cav1.2 assembled with the
1C,77 subunit identified in human hippocampus (see Supplemental Material). Our previous experiments (5, 20, 25) provided evidence that electrophysiological properties of the channel remained essentially unaltered by the N- and/or C-terminal fusion of the green fluorescent protein analogs to the
1C,77 subunit. Measurements of state-dependent FRET, as an indicator of the voltage-gated rearrangements of the ECFP/EYFP-labeled channel, have demonstrated significant mobility of the
1C subunit C-terminal tail and its crucial role for Ca2+ signal transduction, contrasting with a relatively weak
subunit dependent mobility of the
1C N terminus.
Effect of Plasma Membrane Immobilization of the
1C C Terminus on CDI, Voltage-dependent Inactivation, and Ion Selectivity of the ChannelIn the first set of experiments, the C terminus of the
1C,77 subunit was immobilized to the plasma membrane via the pleckstrin homology (PH) domain of phospholipase C
1. To prepare the plasmid encoding
1C,77-(PH-ECFP)C, the PH domain was genetically fused to the last C-terminal Leu-2138 residue of the
1C,77 subunit, and the reading frame was completed with the ECFP-coding sequence. The
subunit-deficient
1C,77-(ECFP)C/
2
channel was predominantly localized in the cytoplasm and did not show substantial membrane targeting (for details, see Harry et al. (26)). The C-terminal fusion of the PH domain was sufficient to direct the plasma membrane insertion of the channel, as one can see from the distribution of the ECFP fluorescence across the cell (Fig. 1A, inset). When co-expressed in COS1 cells with the
2
subunit but in the absence of
subunits (Fig. 1A), the
1C,77-(PH-ECFP)C/
2
channel generated only a minute Ba2+ current in response to a +10-mV depolarization applied from Vh = 90 mV. However, when
2
and
1C,77-(PH-ECFP)C were co-expressed with the
1a subunit (Fig. 1B), the amplitude of the Ba2+ current increased severalfold, and the current decay exhibited a distinctly prolonged plateau at approximately half-maximum of the current. Fig. 1C shows a set of the representative traces of the Ba2+ current evoked by 600-ms test pulses in the range of 0 to +50 mV (10-mV increments) applied from Vh = 90 mV. The corresponding averaged I-V relation is presented in Fig. 1D. The most prominent feature of the Ba2+ current through the channel with the plasma membrane-anchored
1C subunit C terminus was the sustained component of the current (Fig. 1D, open circles in the I-V curve) that, in a wide range of the current-evoking potentials, composed 35.5 ± 3.5% (n = 7) of the total Ba2+ current (from 31.4% at 10 mV to 56.1% at +50 mV). The sustained current was preceded by a rapidly inactivating component with the fast time constant
f of 20.0 ± 5.0 ms (at +20 mV; n = 9). Overall, the anchoring of the
1C subunit C terminus in the plasma membrane accelerated fast inactivation and inhibited slow inactivation of the Ba2+ current.
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1C,77 subunit C-tail could be stimulated by the hydrolysis of the PH domain PIP2 upon activation of phospholipase C. In previous studies, we demonstrated that activation of PIP2 hydrolysis by epidermal growth factor-mediated stimulation of the co-expressed epidermal growth factor receptors helped to fully restore the CDI and voltage-dependent slow inactivation of the channel (5). Because the epidermal growth factor-mediated recovery was transient and additionally complicated by inhibition of the channel activity (27), we analyzed the effects of the co-expression of the constitutively active mutant (Q209L) of the G
q protein that depletes the plasma membrane PIP2 (e.g. see Howes et al. (28)). Fig. 1E (inset) shows the fluorescence image of a COS1 cell co-expressing the
1C,77-(PH-ECFP)C,
2
, and
1a subunits, the G
q Q209L mutant, and representative traces of the Ba2+ current generated in response to step depolarizations in the range of +10 to +40 mV applied from Vh = 90 mV. Co-expression of the G
q Q209L mutant shifted inactivation of the channels to the normal phenotype with a prominent slow component. Single exponential fitting shows the time constant of the Ba2+ current decay of 200 ± 38 ms (at +10 mV; n = 9) and the lack of sustained component.
The inability of the channel with the immobilized C-terminal tail to complete inactivation was corroborated by the analysis of steady-state inactivation properties (Fig. 1F). Approximately 70% of the Ba2+ current through the
1C,77-(PH-ECFP)C/
2
/
1a channel evoked by a +10-mV depolarization remained non-inactivated after a depolarizing prepulse in a range of 10 to +50 mV was applied from Vh = 90 mV prior to the +10-mV test pulse (Fig. 1F, closed circles). The release of the
1C,77 C-tail restored inactivation of the channel, as can be seen from a comparison of the Ba2+ current decay (Fig. 1E) and steady-state inactivation curves recorded in the absence and in the presence of the constitutively active G
q Q209L mutant (Fig. 1F).
Cav1.2 channels classically inactivate by a combination of the voltage- and Ca2+-dependent mechanisms. One of the main consequences of the replacement of Ba2+ for Ca2+ as the charge carrier is an acceleration of the macroscopic current decay or CDI (29). However, this was not found to hold true for the C-terminal tail-anchored Ca2+ channel. Indeed, the representative traces of the Ca2+ current through the
1C,77-(PH-ECFP)C/
2
/
1a channel (Fig. 1G), recorded from the same cell as Ba2+ currents in Fig. 1C, show both inactivating and sustained components of the decay. Similar to the Ba2+ current, the large sustained Ca2+ current components lasted for the duration of depolarization at all indicated test pulses (+20 to +50 mV). Although the fast component of inactivation was not as prominent as in the case of the Ba2+ current, the average fraction of the sustained currents (44.9 ± 2.3%, from 33.3% at 10 mV to 48.6% at +50 mV, Fig. 1H) was essentially the same as with Ba2+ as the charge carrier. All these features of the C-terminal tail-anchored
1C,77-(PH-ECFP)C channel closely matched the phenotype of the
1C,IS-IV channel, which has the slow inactivation mechanism inhibited by the specific mutation in the cytoplasmic pore region (30).
The I-V relations for the Ba2+- and Ca2+-conducting
1C,77-(PH-ECFP)C channel show a number of common patterns (Fig. 1, D and H). Immobilization of the
1C,77 subunit C-terminal tail caused a shift in activation of ion conductance by 1015 mV to more positive potentials. Currents reached the peak of the I-V relationship at +20 (Ca2+) or +30 mV (Ba2+), exhibiting a 1020-mV shift of the maximum toward more positive voltages as compared with the
1C,77-(ECFP)C/
2
/
1a channel. The apparent reversal potential was also notably changed. Both the Ba2+ and Ca2+ currents reversed direction at much higher voltages than in the wild-type channel. Although this effect was not investigated in detail, it may be due to altered ion selectivity and/or decreased permeability to Cs+ ions (introduced in electrodes) in the outward direction that contributed significantly to the apparent reversal potential of the wild-type channel (
+65 mV) (31). Release of the
1C,77-(PH-ECFP)C subunit C-terminal tail by co-expression of the G
q Q209L mutant reversed these changes in the I-V relationship to parameters that are more characteristic for the
1C,77-(ECFP)C/
2
/
1a channel, including ion selectivity and the peak current voltage (Fig. 1D, filled squares). The permeability of the wild type
1C,77 channel to Ba2+ is on average 2.8 times greater than that of the Ca2+ ions (24, 30). Immobilization of the
1C subunit C-tail reduced the difference between the maximum amplitudes of the Ba2+ and Ca2+ currents (compare traces in Fig. 1, C and G), again indicating that the anchoring of the
1C subunit C-terminal tail may affect the ion conductance of the channel. Taken together, these data support the model (7) that links CDI and slow inactivation of the Cav1.2 channel to specific folding of the
1C subunit C terminus vis à vis the cytoplasmic pore region.
Subunit Facilitation of the Cav1.2 Channel Gating Is Revealed by Immobilization of the
1C Subunit N-terminal TailIn the second set of experiments, the N-terminal tail of the (EYFP)N-
1C,77 subunit was anchored to the plasma membrane via the PH domain. The (PH-EYFP)N-
1C,77 channel was expressed in COS1 cells in different combinations with auxiliary
1a and
2
subunits. Fig. 2 shows a collection of representative traces of the Ba2+ current elicited by depolarization to +10 mV from Vh = 90 mV in a set of COS1 cells of approximately similar size. The insets in Fig. 2 are fluorescent images of the expressing cells showing subcellular localization of the EYFP-tagged
1C subunits. Confirming earlier data (32, 33), COS1 cells did not show appreciable endogenous expression of Cav1.2 (Fig. 2A). Transfection of COS1 cells with a mixture of cDNAs coding for the (EYFP)N-
1C,77,
1a and
2
subunits (Fig. 2B) renders the current with characteristics (Fig. 3, curves 3) closely resembling those of the wild-type channel (24). Anchoring of the
1C subunit N terminus by co-expression of (PH-EYFP)N-
1C,77 with the
1a and
2
subunits (Fig. 2C) accelerated the kinetics of inactivation of the Ba2+ current by
15% (5). An acceleration of inactivation was also seen when the PH domain was separately co-expressed with the (EYFP)N-
1C,77,
1a, and
2
subunits (Fig. 2D). Making no assumptions about the nature of these variations, we investigated the effect of the deletion of the
1a subunit from the expressed constituents of the channel.
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1C,77 was expressed alone, the fluorescent-tagged channel protein was diffusely distributed over the cytoplasm and did not generate measurable voltage-gated current (Fig. 2E). The N-terminal fusion of the PH domain caused robust surface membrane targeting by the labeled (PH-EYFP)N-
1C,77 protein, but the channel remained essentially silent (Fig. 2F). A similar result was obtained when
2
was co-expressed with the (EYFP)N-
1C,77 subunit (Fig. 2G, note poor membrane targeting of the channel complex). However, the membrane anchoring of the
1C subunit N-terminal tail by co-expression of the (PH-EYFP)N-
1C,77 and
2
subunits stimulated membrane targeting of the
-deficient channel that generated large slowly activating and non-inactivating Ba2+ current in response to depolarization (Fig. 2H). This result is consistent with the idea that
1C and
2
are sufficient for the expression of a conducting L-type Ca2+ channel if the N-terminal tail of the
1C subunit is immobilized by the plasma membrane anchoring. To find whether or not release of the PH-tagged N-terminal tail would compromise the channel activity in the
subunit-deficient channel, we investigated the effect of co-expression of the constitutively active Q209L mutant of G
q. AG
q-mediated depletion of PIP2 in the plasma membrane did abolish the plasma membrane targeting by inhibiting the immobilization of the
1C,77 subunit N-terminal tail, and precluded expression of the conducting channel (Fig. 2I). Together, these data suggest that the
1C N-terminal tail may act as a silencer of the channel voltage-gated conductance and block it in the absence of the
subunit. Results obtained with the
1C subunit having a genetically immobilized N-terminal tail further corroborate this suggestion by demonstrating robust current of the
subunit-deficient Cav1.2 channel composed of the (PH-EYFP)N-
1C,77 and
2
subunits.
Activation and Inactivation Properties of the (PH-EYFP)N-
1C,77/
2
ChannelThe effects of the
1C subunit N-tail immobilization in the plasma membrane on electrophysiological properties of the channel are presented in Fig. 3. For comparison with the channel that has the
1C subunit N-terminal tail EYFP-tagged but not anchored, Fig. 3, AC, includes data for Ba2+ currents through the (EYFP)N-
1C,77/
1a/
2
channel (curves 3). Fig. 3A shows superimposed traces of Ba2+ currents (normalized to the same amplitude) through the (PH-EYFP)N-
1C,77/
1a/
2
channel (trace 1), (PH-EYFP)N-
1C,77/
2
channel (trace 2), and the control channel (trace 3). When co-expressed with the
1a and
2
subunits, the (PH-EYFP)N-
1C,77 channel showed notable acceleration of inactivation (Fig. 3A, trace 1) compared with the control. However, expression of the same channel in the absence of the
subunit (Fig. 3A, trace 2) significantly delayed activation and inhibited inactivation of the current. A single-exponential fit of the activation time course (+20 mV) showed a substantial increase in the time constant of activation (
a) of the Ba2+ current through the
subunit-deficient (PH-EYFP)N-
1C,77/
2
channel (34.0 ± 10.5 ms, n = 13) as compared with the (PH-EYFP)N-
1C,77/
1a/
2
channel (
a = 2.4 ± 0.3 ms; n = 6; p < 0.005). The respective I-V relationships are shown in Fig. 3B. The voltage-dependent characteristics, obtained from the fit of the I-V curve for the control (EYFP)N-
1C,77/
1a/
2
channel, were typical for the L-type Ca2+ channel current, including Erev = 60 ± 2 mV, V0.5 = 0.02 ± 0.95 mV, and kI-V = 7.8 ± 0.5 (n = 6). The plasma membrane immobilization of the
1C,77 subunit N-terminal tail shifted the voltage dependence of activation (V0.5) to more negative potentials by 15.5 ± 2.4 (+
1a; n = 6) and 23 ± 4.5 mV (
1a; n = 13). The threshold of activation of the Ba2+ current was shifted by
10 mV toward more negative voltages in the
-deficient channel (Fig. 3B, filled circles) as compared with the (PH-EYFP)N-
1C,77/
1a/
2
channel (open circles). In the
-deficient channel, the voltage that elicited the maximum Ba2+ current (+10 mV) was shifted by
10 mV to more positive potentials. However, the most notable change was the increase of the apparent reversal potential in both (PH-EYFP)N-
1C,77/
2
±
1a channels. A similar effect was also induced by immobilization of the
1C subunit C-terminal tail (Fig. 1) and may be a result of altered ion selectivity.
To characterize further the inactivation characteristics of the Ba2+ current through the (PH-EYFP)N-
1C,77/
2
±
1a channels, we measured steady-state inactivation curves by using a two-step voltage clamp protocol (Fig. 3C). Steady-state inactivation properties point to differences in voltage dependence of inactivation of the Ba2+ current as compared with the control (EYFP)N-
1C,77/
1a/
2
channel (Fig. 3C, curve 3). Voltage at the half-maximum of inactivation was shifted from 7.9 ± 0.7 mV (n = 6) in control to 15.9 ± 3.4 (n = 3) in the (PH-EYFP)N-
1C,77/
1a/
2
channel (Fig. 3C, curve 1). Although the voltage dependence of availability (20.1 ± 1.5%) was not significantly changed by the plasma membrane immobilization of the
1C,77 N-terminal tail (21.0 ± 5.9%), the slope k of the steady-state inactivation curve (fitted by the Boltzmann equation) decreased from 6.3 ± 0.6 to 13.5 ± 3.8 (p < 0.05). Thus, cooperativity in voltage gating leading to inactivation is significantly affected by the plasma membrane immobilization of the
1C subunit N-terminal tail. Steady-state inactivation analysis also confirmed that the voltage dependence of inactivation of the
subunit-deficient channel is inhibited in the range of conditioning pulses of up to +60 mV (Fig. 3C, curve 2).
The single channel analysis corroborated the macroscopic data (Fig. 4, A and B). Recordings of the Ba2+ current in the cell-attached configuration (110 mM Ba2+) revealed rarely occurring activations of the (PH-EYFP)N-
1C,77/
2
channel that were characterized by low probabilities of both opening and closing (Fig. 4B). Openings of the channel were preceded by a large number of blank traces. The loss of inactivation of this channel was evidenced by continuous bursting of a single Ca2+ channel activity during long lasting depolarizations (mean burst length was 154 ± 18 ms, n = 39). In the presence of the
subunit (Fig. 4A), the appearance of bursts was as low as 1 burst for 100 traces, whereas in the absence of the
subunit, we observed bursts almost in every trace with the channel activity (Fig. 4B). The first latency was significantly prolonged (
= 55.4 ms) compared with the control (EYFP)N-
1C,77/
1a/
2
channel (
= 28.4 ms). This explains the delay in activation of the whole-cell current in the anchored (PH-EYFP)N-
1C,77/
2
channel.
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subunit-deficient (PH-EYFP)N-
1C,77/
2
channel was also found to hold true with Ca2+ as the charge carrier. Fig. 5A shows superimposed traces of the Ca2+ current evoked by depolarization in the range of 20 to +50 mV applied from Vh = 90 mV. A remarkable feature of the
-deficient channel is the striking similarity in the properties of the Ba2+ and Ca2+ currents. A single-exponential fit of the activation time course (+20 mV) shows a marked increase (p < 0.05) in the time constant of activation of the Ca2+ current through the
-deficient (PH-EYFP)N-
1C,77/
2
channel (
a = 69.0 ± 12.5 ms, n = 32) as compared with the (PH-EYFP)N-
1C,77/
1a/
2
channel (
a = 2.0 ± 0.2 ms; n = 5; Fig. 5C). These data are not significantly different (unpaired t test) from those obtained for the Ba2+ current (see above). The
subunit-deficient channel exhibits unusually high Ca2+ current amplitude but did not reveal appreciable decay of the Ca2+ current even when the test pulse duration was prolonged to 30 s (Fig. 5B). These data indicate that CDI was lost by the
subunit-deficient Cav1.2 channel when its
1C subunit N-tail was immobilized in the plasma membrane. Release of the N terminus of the (PH-EYFP)N-
1C,77 subunit by the co-expression of a constitutively active Q209L mutant of G
q to activate PIP2 hydrolysis (Fig. 5D) sharply reduced the size of the Ca2+ current through the
subunit-deficient channel in response to a +20-mV depolarization that corresponds to other controls discussed above (Fig. 2, G and I). A small residual non-inactivating current with the average amplitude of 30 pA may be due to incomplete PIP2 hydrolysis rendering plasma membrane immobilization of the
1C subunit N-tail in a small fraction of the channels (see also Fig. 2I). Taken together, these data suggest that inactivation by both the voltage-dependent and CDI mechanisms is missing in the
subunit-deficient (PH-EYFP)N-
1C,77/
2
channel.
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1C Subunit N-terminal Deletion on the
Subunit Modulation of the Ca2+ Channel GatingWe have next explored another way of uncoupling the
1C subunit N-tail from its apparent silencing function by a genetically encoded deletion of 120 out of a total 124 N-terminal amino acids of
1C,77 (
N-
1C,77). Shistik et al. (34) made a similar attempt in Xenopus oocytes by expressing a rabbit cardiac
1C where all but 15 N-terminal tail amino acids were deleted. However, because Xenopus oocytes are known to express endogenous Ca2+ channels (3538), there was ambiguity in their findings. Interpretation was also obscured by the continuous application of 1 µM ()-BayK8644 to artificially increase the amplitude of the single channel Ba2+ current. More substantial deletion of the
1C subunit N-terminal tail as well as the use of COS1 cells, free of endogenous Ca2+ channel subunits, helped us to eliminate these ambiguities. Fig. 6 shows Ca2+ channel activity of the
N-
1C,77/
2
channel assembled with (A) or without (B) the
subunit. As was observed with the full size
1C,77 (for details see Refs. 20 and 26), the co-expression of
N-
1C,77 and
2
increased the plasma membrane targeting by the (ECFP)N-
1a subunit (Fig. 6A, panel a). The surface membrane targeting by the labeled
N-
1C,77-(ECFP)C subunit (and the (ECFP)N-
2
; Fig. 6B, panel a) was prominent independently on the presence of the
subunit (Fig. 6, A and B, panel b). The presence of
was not crucial for the functional expression of the
N-
1C,77/
2
±
1a channels. In both channels, Ca2+ currents were activated by stepwise depolarization from Vh = 90 mV (shown are traces recorded in response to +20-mV test pulses). This result supports the data on the
1C,77 N-tail anchoring that a
subunit is not essential for the expression of an active conducting channel if the N-terminal tail of the
1C subunit is uncoupled from the channel regulation. Although the
subunit was crucial for inactivation of the (PH-EYFP)N-
1C,77/
2
/
1a channel (Fig. 2C), this effect was essentially missing in the
N-
1C,77/
2
/
1a channel (Fig. 6A). The Ca2+ current evoked by the +20-mV step depolarization had rather small amplitude and did not show accelerated decay that would be characteristic for CDI. This result indicates that the functional uncoupling of the
1C subunit N-terminal tail through the plasma membrane anchoring or deletion influences the interaction with the
subunit in different ways.
|
-deficient (PH-EYFP)N-
1C,77/
2
channel that shows non-inactivating Ca2+ currents (Fig. 5B), inactivation of the
N-
1C,77/
2
±
1a channels was impaired (Fig. 6, A and B). In addition, removal of the
subunit from the channel complex significantly delayed activation of the Ca2+ current (Fig. 6B). However, analysis of the respective I-V relations (Fig. 6C) showed that the voltage sensors responsible for activation of the
N-
1C,77/
2
±
1a channels were not strongly affected by the removal of the
subunit from the oligomeric complex, despite other signature changes also seen with the N-tail-anchored
1C,77 channel (Fig. 5A), including broadening of the I-V curves and a shift of the peak currents to more positive potentials (Fig. 6C). Single channel recordings (Fig. 4D) revealed a relatively large number of empty swipes corresponding to low probability of opening of the
subunit-deficient
N-
1C,77/
2
channel. First latencies were significantly shorter in the presence of the
subunit,
= 48.5 ms (Fig. 4C), than without it,
= 139.4 ms (Fig. 4D). However, the important difference with the effect of the transient anchoring of the
1C subunit N-terminal tail (Fig. 4, A and B) is clearly visible; the N-tail uncoupling through a deletion essentially stabilized the open state of the
subunit-deficient channel, which showed long opening of a single Ca2+ channel activity during long lasting depolarizations (Fig. 4D). With either type of uncoupling of the
1C subunit N-terminal tail, a delay in the activation of the whole-cell current appears to be associated with prolongation of the first latency.
Effect of the
Subunit on the Voltage-gated Mobility of the
1C Subunit N-terminal TailFinally, we assessed whether the
subunit affects the voltage-gated mobility of the
1C subunit N-terminal tail. The (EYFP)N-
1C,77/
2
channel was co-expressed with the (ECFP)N-PH in the absence (Fig. 7A) or in the presence (Fig. 7B) of the
1a subunit (for arrangement of fluorophores and subunits, see panels b). In this experiment, the EYFP-labeled N-terminal tail of the
1C,77 subunit reports its state-dependent position to the FRET partner, ECFP, fused to the plasma membrane-trapped PH domain. FRET was confined to the plasma membrane region (Fig. 7, yellow boxes in panels a) and was set to be recorded within the time windows, marked by black or red bars under the actual Ba2+ current traces on panels c, simultaneously with acquisition of the currents. An image recorded at the resting state (90 mV, Fig. 7, black bars corresponding to panels d) was followed by an image recorded at the end of a +20 mV depolarization test pulse (red bars corresponding to panels e). One can see that independent of the presence of the
1a subunit, a corrected FRET signal of different intensity was observed in Fig. 7, panels d and e. Ratios (Fig. 7, panels f) between the two consecutive images recorded at 90 and +20 mV reflect voltage-dependent conformational rearrangements of the N-tail fluorophore fused to the
1C,77 subunit with regard to the relatively small membrane-trapped PH domain probe (5). In the presence of the
1a subunit (Fig. 7B), the channel generated a Ba2+ current in response to a +20-mV depolarization (Vh =90 mV) that showed complete inactivation within 500 ms (Fig. 7B, panel c). Thus, the +20-mV corrected FRET image recorded at the end of the 600-ms depolarizing pulse (Fig. 7B, panel e) corresponds to a predominantly inactivated state of the channel. However, the ratio (Fig. 7B, panel f) shows very little if any change in corrected FRET between 90 and +20 mV (0.90 ± 0.06; n = 6). A similar result was observed with another type of
subunit, the rabbit
2 (20).
|
subunit (Fig. 7A) renders the channel to a voltage-insensitive silent state (see a zero current trace recorded in response to a +20-mV test pulse in panel c). However, the ratio of corrected FRET images recorded at 90 and +20 mV (1.70 ± 0.10; n = 5) at the time windows marked below the current trace by black and red bars, respectively, shows a substantial (p < 0.005) differential FRET signal generated in the plasma membrane by voltage-gated rearrangement of the
1C,77 subunit N-terminal tail. | DISCUSSION |
|---|
|
|
|---|
1C isoforms in voltage-, Ca2+-, and
subunit-dependent regulation of the Cav1.2 channel.
Our study is an important step forward in understanding Cav1.2 channel regulation as a multifactorial process. Here for the first time we have analyzed differential regulation of the Ca2+ channel by the C- and N-terminal tails of the
1C subunit with simultaneous assessment of the role of
subunits. To deconvolute the contribution of these parts, transient anchoring to the plasma membrane via the PH domain fused to the
1C subunit tails has been used to uncouple the
1C tails from the channel regulation. To assess the potential interplay between the tails and a
subunit, we compared properties of the channel expressed in the absence and in the presence of
. The accumulated body of data shows that inactivation of the Cav1.2 channel is mediated by a combinatorial input of these distinct parts, in which CDI is essentially additive to voltage-dependent inactivation.
Voltage-dependent slow inactivation and CDI were previously co-identified with the calmodulin-binding regions in the middle part of the
1C subunit C-tail (for review see Ref. 40). A recent picture (41) still includes an EF hand-like motif of the C-tail proximal region, although involvement of this motif in CDI has been contested by experimental evidence (29). Our findings show that CDI is not mediated solely by determinants of the
1C C-terminal tail. Investigation of other cytoplasmic constituents of the channel complex have been crucial in identifying the roles of the N-tail, the cytoplasmic pore region of
1C, and
subunits for inactivation and in understanding how slow and fast voltage-dependent inactivation and CDI evolve from their interplay. A distinct advantage of COS1 cells lacking endogenous Ca2+ channel subunits (32) over other expression systems, such as HEK293 cells or Xenopus oocytes, permits an unambiguous interpretation of our data on
subunit modulation of the channel. Because no appreciable Ca2+ channel activity was exhibited by the
1C,77/
2
channel (Fig. 2G), unless a
subunit was co-expressed, we define the
subunit modulation as a facilitation of voltage gating of the channel. Recognizing that the kinetics of inactivation of the Ba2+ current through the "wild-type"
1C,77/
1a/
2
channel is best fit by a sum of two (fast and slow) exponentials, the respective fractional components of the Ba2+ current measured at the peak of I-V curves were analyzed to assess the voltage-dependent fast and slow inactivation mechanisms.
We have shown previously that four highly conserved amino acids of the transmembrane segment S6, constituting the cytoplasmic end of the pore, jointly form the ADSI. Their simultaneous mutation (S405I in IS6, A752T in IIS6, V1165T in IIIS6, and I1475T in IVS6) generates the
1C,IS-IV channel, which does not show the slow inactivation, CDI, or differential
subunit modulation (30). Our findings have shown that the
1C subunit C-terminal tail is subject to voltage-gated conformational rearrangements that specifically deliver Ca2+ signaling to downstream targets involved in cAMP-response element-binding protein-dependent transcription activation (5). The plasma membrane anchoring of the C-tail interrupts Ca2+ signal transduction despite robust Ca2+ current through the channel. Thus, a specific position of the C-terminal tail vis à vis the polypeptide packing of the cytoplasmic channel constituents (including the
1C subunit tails and a
subunit) is crucial for CDI and slow voltage-dependent inactivation.
We now find that plasma membrane immobilization of the
1C,77 C-terminal tail alters inactivation of the channel similar to the mutation of the ADSI (Fig. 1). An interesting distinction from the electrophysiological phenotype of the
1C,IS-IV channel, however, is a shift of the I-V relationship to more positive potentials. Because these dramatic changes do not involve structural alterations of the ADSI or the calmodulin-binding regions, and are completely reversible upon the release of the
1C,77-(PH-ECFP)C subunit C-tail, stimulated by PIP2 hydrolysis, it is reasonable to assume that the plasma membrane anchoring of the
1C C-terminal tail interferes with the functional folding of the cytoplasmic polypeptide bundle in the pore region, including ADSI. This may directly affect the pore-forming transmembrane segment IVS6, connected to the
1C C-tail, and, indirectly, the ensemble of the pore conformations defining the ion selectivity of the channel.
A very different role was found for the
1C subunit N-terminal tail. FRET microscopy combined with the patch clamp (20) revealed limited voltage-dependent mobility of the
1C N terminus in relationship with the plasma membrane (Fig. 7B). This may correspond to the restricted local dynamics of the adjacent S1 segment observed in other channels (42). Here we find that in the
subunit-deficient (silent) channel, voltage-gated conformational rearrangements of the
1C subunit N terminus vis à vis the plasma membrane are significantly increased (Fig. 7B). The functional importance of the conformational "rigidity" to voltage gating conferred by a
subunit to the
1C subunit N terminus was confirmed here by anchoring of the N-tail to the plasma membrane, stabilized by the fused PH domain.
The
subunit confers conformational rigidity to the
1C subunit N-tail in a manner that facilitates the channel response to voltage gating. We have found that the plasma membrane-anchoring of the
1C subunit N terminus, in the absence of
, completely inhibited inactivation of the Ba2+ (or Ca2+) current. At the same time, activation of the channel current in response to depolarization becomes slow independently of the charge carrier (Fig. 2H). The single channel study pointed to low probability of both opening and closing of the channel (Fig. 4B). Uncoupling of the N-terminal tail by its deletion from the
1C subunit also inhibited inactivation of the channel (Fig. 7). However, in this case retardation of the channel activation was enhanced to a greater extent, probably because of long lasting episodes of rare openings (Fig. 4D). Release of the plasma membrane-anchored
1C N terminus essentially blocked the channel current (Fig. 2I), leaving only some residual Ca2+ channel activity that may be generated by the remaining small fraction of channels with immobilized
1C N-tails. Overall, these data correspond to the result obtained with the
-deficient Cav1.2 channel (Fig. 2G). Conversely, co-expression of
with
2
subunits re-established both the voltage- and Ca2+-dependent inactivation of the channels despite uncoupling of the
1C subunit N-terminal tail from the regulation by its plasma membrane anchoring. These observations shed new light on the role of the
subunit. It appears that there is a
subunit-dependent desensitization of the
1C subunit N-tail to voltage, which is essential for the fast activation, CDI, and voltage-dependent inactivation of the channel.
Our data support the conclusion of Dascal and co-workers (34) that
subunits prevent inhibition of the channel by the N-tail. The results of our work demonstrate that the N-terminal tail of the
1C subunit is a channel silencer, competing with the
subunit facilitation of the channel gating. This may account for CDI and voltage-dependent inactivation and activation of the current.
Our findings add to the understanding of the
subunit regulation of the Cav1.2 channel in a number of ways. The "chaperon" hypothesis implies that
subunits ease functional expression of the Cav1.2 channel by binding to the
-interaction domain resulting in inhibition of an endoplasmic reticulum retention signal of the
1C subunit (43). The present study does not support this view. In COS1 cells, free of endogenous Ca2+ channel subunits, an uncoupling of the
1C subunit N-terminal tail (by membrane anchoring or deletion) completely eliminates the requirement of
subunits for the robust expression of functional Cav1.2 channels, but co-expression of
2
is critical.
Recent investigation of the human cardiac short
2f and
2g subunits (26) identified the C-terminal 153-amino acid sequence as essential for the functional modulation of the channel and interaction with the
1C subunit. This region includes Ser-574 that is subject to phosphorylation by phosphatidylinositol 3-kinase as necessary and sufficient to promote Ca2+ channel trafficking to the plasma membrane (44). Although the mechanism of this effect is unknown, our data put the
1C subunit N-terminal tail in play as a possible determinant of the channel trafficking and a target of the
subunit modulation.
Thus a new picture of the
subunit modulation of the Cav1.2 channel has emerged (Fig. 8), showing how
acts as a "molecular wedge" that prevents the N terminus of the
1C subunit from blocking the pore. Dependence of CDI on interaction between the
1C subunit N-tail and the
subunit led us to a hypothesis that the
subunit and the
1C C-tail may have an integrating role for the cytoplasmic polypeptide packing underlying the pore.
|
1C subunit C-terminal tail and ADSI are directly involved in this coupling, whereas the crucial correlates provided by
1C N terminus and
subunits may add more specialization via genetic variation and alternative splicing in neuronal cells (see Supplemental Materials and Ref. 26). Whether neuronal specialization evolves from such variations is an interesting question to be addressed. | FOOTNOTES |
|---|
The on-line version of this article (available at http://www.jbc.org) contains Methods, Results and Discussion, Refs. 17, Fig. 1, and Table 1. ![]()
¶ To whom correspondence should be addressed: Laboratory of Clinical Investigation, National Institute on Aging, 5600 Nathan Shock Dr., Baltimore, MD 21224. Tel.: 410-558-8343; Fax: 410-558-8318; E-mail: soldatovN{at}grc.nia.nih.gov.
1 The abbreviations used are: CaM, calmodulin; ADSI, the annular determinant of slow inactivation; CDI, Ca2+-dependent inactivation; IV, current-voltage; PH, pleckstrin homology; PIP2, phosphatidylinositol bisphosphate; ECFP, enhanced cyan fluorescent protein; EYFP, enhanced yellow fluorescent protein; FRET, fluorescence resonance energy transfer. ![]()
| ACKNOWLEDGMENTS |
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| REFERENCES |
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