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J Physiol Volume 530, Number 1, 35-45, January 1, 2001
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Journal of Physiology (2001), 530.1, pp. 35-45
© Copyright 2001 The Physiological Society

The amino side of the C-terminus determines fast inactivation of the T-type calcium channel alpha1G


Mik Staes, Karel Talavera, Norbert Klugbauer*, Jean Prenen, Lubica Lacinová*, Guy Droogmans, Franz Hofmann* and Bernd Nilius


Laboratorium voor Fysiologie, Campus Gasthuisberg, KU Leuven, B-3000 Leuven, Belgium and *Institut für Pharmakologie und Toxikologie, Technische Universität München, D-80802 Munich, Germany

MS 11287 Received 21 June 2000; accepted after revision 22 September 2000

  ABSTRACT
Top
Abstract
Introduction
Methods
Results
Discussion
References

  1. We analysed the kinetic properties of the fast inactivating T-type calcium channel alpha1G in HEK 293 cells transfected with different alpha1G chimeras, containing the N-terminus, III-IV linker or various C-terminal regions of the slowly inactivating L-type alpha1C.

  2. A highly negatively charged region of 23 amino acids at the amino side of the intracellular carboxy terminus of alpha1G was found to be critical for fast inactivation.

  3. The N-terminus of alpha1G does not seem to be necessary for inactivation of the T-type calcium channel because replacement of the alpha1G N-terminus with the alpha1C N-terminus did not influence channel kinetics at all.

  4. Replacing the III-IV linker of alpha1G with that of alpha1C decreased the rate of inactivation at -20 mV from 15.8 ± 1.8 to 8.5 ± 1.1 ms, and shifted the potential for half-maximal inactivation from -69.6 ± 0.8 to -54.0 ± 1.7 mV. However, these parameters were not significantly different at other potentials.

  5. We suggest a putative 'ball-and-chain'-like mechanism for inactivation in which the negative charges function as an acceptor domain for a ball, hypothetically located at a different intracellular part of the channel. In addition, transferring the IQ motif and EF hand of alpha1C to alpha1G does not confer Ca2+-dependent inactivation on alpha1G, suggesting that other sequences besides the C-terminus are needed for Ca2+-dependent inactivation of alpha1C.

  INTRODUCTION
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Abstract
Introduction
Methods
Results
Discussion
References

Voltage-dependent Ca2+ channels (or voltage-operated Ca2+ channels, VOCCs) cause a rapid influx of Ca2+ into cells upon membrane depolarisation. They play an important role in neurons, and skeletal, cardiac and smooth muscle, but also in non-excitable cells like endocrine cells, lymphocytes and spermatocytes. These channels are involved in synaptic signal transduction, excitation-contraction coupling, excitation-secretion coupling, pacemaker function, cell growth, cell proliferation and apoptosis (Cohen et al. 1988; Tsien et al. 1991; Hofmann et al. 1994; Zhang et al. 1994).

Based on their electrophysiological and pharmacological properties, VOCCs can be functionally classified into different subtypes (L-, N-, P/Q-, R- and T-type) (Tsien et al. 1991; Zhang et al. 1993; Hofmann et al. 1999). T-type calcium channels show some unique biophysical properties, which are absent in other VOCCs. They activate at much more negative potentials, ranging from -50 to -30 mV with a peak current around -20 mV (Droogmans & Nilius, 1989; Chen & Hess, 1990; Huguenard, 1996) and are therefore also called low voltage-activated (LVA) channels. Inactivation of the macroscopic current is voltage dependent but Ca2+ independent, resulting in a typical criss-crossing current pattern (Droogmans & Nilius, 1989; Chen & Hess, 1990). T-type channels also deactivate slowly, giving rise to long-lasting tail currents during repolarisation (Droogmans & Nilius, 1989; Chen & Hess, 1990). These properties are functionally important for induction of large inward Ca2+ currents following short depolarisations during an action potential (Nilius et al. 1985; Huguenard, 1996). T-type channels may play a critical role in the generation of electrophysiological rhythms, such as the cardiac pacemaking of sino-atrial node cells (Nilius, 1986; Tseng & Boyden, 1989; Lei et al. 1996) and are part of an internal clockwork system controlling oscillations in thalamocortical networks (Destexhe et al. 1993; Tsien, 1998). They are also involved in excitation-induced secretion processes (Barrett et al. 1996; Chen et al. 1999). The subunit composition of LVA channels is still unknown, but they contain at least one alpha1 subunit, responsible for voltage sensing, ion selectivity, ion conduction and binding of some channel blockers (Hofmann et al. 1999). Three different alpha1 subunits of T-type channels have been identified and cloned: alpha1G, alpha1H and alpha1I (Perez-Reyes et al. 1998; Cribbs et al. 1998; Klugbauer et al. 1999; Lee et al. 1999). The alpha1G subunit of the T-type calcium channel contains four homologous domains (repeats I to IV) each of them consisting of six transmembrane alpha-helices (S1 to S6). Interactions between alpha1G co-expressed with an alpha2delta and/or beta subunit have not (Lacinova et al. 1999) or have (Dolphin et al. 1999) been observed.

At present, the structure-function relationship for the gating mechanism of T-type calcium channels is not known. To investigate the fast inactivation mechanism of T-type channels, we have created different chimeras by replacing parts of the T-type alpha1G protein (Klugbauer et al. 1999) with the corresponding sequences of the slowly inactivating L-type alpha1Cb Ca2+ channel (Biel et al. 1990). Inactivation of the L-type Ca2+ channel is also Ca2+ dependent, a process that is controlled by intracellular sequences in the carboxy terminus, which have been identified as calmodulin (IQ motif) and calcium (EF hand) binding sites (Wei et al. 1994; de Leon et al. 1995; Qin et al. 1999; Zühlke et al. 1999). We have therefore also constructed different C-terminal chimeras containing either or both of the IQ and EF motifs to investigate whether Ca2+ dependency of inactivation can be transferred from alpha1C to alpha1G.

The voltage-gated Na+ channel is, like the T-type Ca2+ channel, composed of four homologous internal repeats, each of them consisting of six putative transmembrane segments (Noda et al. 1984). Since the hydrophobic IFM motif in the intracellular linker between region III and IV is involved in the fast inactivation of voltage-dependent sodium channels (Stühmer et al. 1989; Patton et al. 1993; Catterall, 1999), we have also removed this region from alpha1G and replaced it with the corresponding part of alpha1C in order to investigate if the fast inactivation of alpha1G is also due to specific apolar residues in the III-IV linker.

The intracellular amino terminus of K+ channels is involved in their inactivation mechanism based on a ball-and-chain interaction (Armstrong & Bezanilla, 1977; Hoshi et al. 1990; Zagotta & Aldrich, 1990). We have therefore replaced this terminus of alpha1G with that of alpha1C with the purpose of investigating whether the T-type N-terminus is necessary for inactivation.

  METHODS
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Abstract
Introduction
Methods
Results
Discussion
References

Construction of calcium channel chimeras

Chimeras were obtained using the standard PCR overlap extension technique with the mouse alpha1G cDNA, pc3LVA1, accession number AJ012569 (Klugbauer et al. 1999) and the rabbit alpha1Cb cDNA, accession number X55763 (Biel et al. 1990) as the template DNA. If necessary, subfragments of alpha1G or alpha1Cb were first subcloned into pUC18 (New England Biolabs) or pBluescript II KS+ (Stratagene) as follows. GCDeltaN: Hind III alpha1G fragment (1292 bp) in pUC18 (Subclone 1); GCDeltaL: Hind III-Acc65 I alpha1G fragment (4539 bp) in pUC18 (Subclone 2); GCDeltaC1-GCDeltaC4: EcoR I-Xho I alpha1Cb fragment (4496 bp) in pBluescript II KS+ (Subclone 3); GCDeltaC5: Xho I alpha1G fragment (1767 bp) in pBluescript II KS+ (Subclone 4).

A part of the insert was replaced by the corresponding sequence of the alpha1Cb cDNA. Replacement sequences were created by standard PCR overlap extension. The primers and template DNA for each chimera are given below (Table 1).

eq01

The chimerical overlap PCR fragments were inserted into the respective subclones using the following restriction enzymes: GCDeltaN: BamH I (in Subclone 1); GCDeltaL: PinA I/Bgl II (in Subclone 2); GCDeltaC1 and GCDeltaC4: EcoR I/BstE II (in Subclone 3); GCDeltaC5: BspM I/Esp I (in Subclone 4). The chimerical overlap PCR fragments for GCDeltaC2 and GCDeltaC3 were cloned into the vector pCR-Blunt II-TOPO (Invitrogen) for further storage and amplification.

In a final step, the chimerical fragments were transferred to the full-length alpha1G clone pc3LVA1 using the following restriction enzymes: GCDeltaN: Hind III; GCDeltaL: PinA I/Acc65 I; GCDeltaC1: Xho I; GCDeltaC2 and GCDeltaC3: Acc65 I/Not I; GCDeltaC4 and GCDeltaC5: Xho I.

The sequence of each chimera was verified by sequence analysis. The exact locations of sequence exchanges between alpha1G and alpha1Cb are shown in Fig. 1.

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    Figure 1 Schematic representation of alpha1G-alpha1C chimeras

    Black boxes indicate intracellular parts from alpha1G. Open boxes represent fragments of alpha1C. The exact locations of the exchanges between alpha1G and alpha1C are given by the numbers of the corresponding amino acids (AA).

Cell culture and transfection of HEK 293 cells

Human embryonic kidney cells (HEK 293 cell line) were grown in Dulbecco's modified Eagle's medium containing 10% (v/v) human serum, 2 mM L-glutamine, 2 U ml-1 penicillin and 2 mg ml-1 streptomycin at 37°C in a humidity controlled incubator with 10% CO2. The cells were transiently transfected with the expression vectors using LipofectAMINE PLUS reagent according to the instructions of the manufacturer (Gibco-BRL Life Technologies). Expression vector pc3LVA1 was used for expression of the wild-type (WT) alpha1G channel in HEK 293 cells.

Solutions

The standard extracellular solution was Krebs solution, containing (mM): 150 NaCl, 6 KCl, 1 MgCl2, 1.5 CaCl2, 10 glucose, 10 Hepes, titrated to pH 7.4 with 1 M NaOH, with an osmolarity of 320 ± 5 mosmol l-1. While measuring calcium currents, the cells were perfused with a bath solution containing (mM): 130 N-methyl-D-glucamine, 20 CaCl2 or BaCl2, 5 CsCl, 10 Hepes, 1 MgCl2, 5 glucose, titrated to pH 7.4 with 1 M HCl, with an osmolarity of 320 ± 5 mosmol l-1. The pipettes were filled with a solution containing (mM): 102 CsCl, 5 Hepes, 5 MgCl2, 5 Na2-ATP, 10 TEA-Cl, 10 EGTA, titrated to pH 7.4 with 1 M CsOH, with an osmolarity of 270 ± 5 mosmol l-1.

Electrophysiology

Currents were recorded in the whole-cell configuration of the patch-clamp technique using an EPC-7 (List Electronics, Darmstadt, Germany) or EPC-9 (HEKA Electronics, Lambrecht/Pfalz, Germany) patch-clamp amplifier and filtered with an eight-pole Bessel filter (Kemo, Bekenham, UK). For control of voltage-clamp protocols and data acquisition, we used pCLAMP 6 software (Axon Instruments, Foster City, CA, USA) run on an IBM-compatible PC connected to the amplifier via a TL-1 DMA interface (Axon Instruments). Rapid exchange of bath solution occurred via a multi-barrelled pipette connected to solution reservoirs and was controlled by a set of magnetic valves. Patch electrodes were pulled from Vitrex capillary tubes (Modulohm, Herlev, Denmark) using a DMZ-Universal puller (Zeitz-instruments, Augsburg, Germany). When filled with pipette solution they had a DC resistance between 2 and 5 MOmega. An Ag-AgCl wire was used as the reference electrode. The cell capacitance and series resistance were electronically compensated. Current traces were filtered at 2 kHz and digitised at 5-10 kHz. The experiments were performed at room temperature (20-25°C).

Data analysis

Electrophysiological data were analysed and fitted using the WinASCD software package (G. Droogmans, Laboratory of Physiology, KU Leuven). Peak I-V relations were fitted to:

I = ( gmax(V - Vrev) ) / ( 1 + exp[-(V - Vact)/sact] )

where I is the measured current (in pA pF-1), gmax the slope conductance (in nS pF-1), V the test potential, Vrev the reversal potential, Vact the potential of half-maximal activation (all in mV) and sact (in mV) the slope parameter for activation.

Steady-state inactivation (h ) was determined from the peak current during an 80 ms test pulse to -20 mV following a long-lasting pre-pulse (5120 ms) to various potentials from -100 to -25 mV in steps of 5 mV. This protocol was repeated every 2 s from a holding potential of -100 mV. These peak currents were normalised to that following a pre-pulse to -100 mV, i.e.:

h = Ipeak(Vpre)/Ipeak(-100).

Current traces were first corrected for linear background currents. The voltage dependence of this parameter was fitted to the Boltzmann equation:

h (V) = 1/{1 + exp[(V - Vinact)/sinact]}, (2)

where Vinact represents the potential for half-maximal inactivation and sinact is a slope factor.

For statistical analysis and graphical presentation of the data we used Origin version 5.0. Pooled data are given as means ± S.E.M. of all the measurements. Results were tested for significance using Student's unpaired t test with P < 0.05 and P < 0.01 as the level of significance. To account for variations in cell size, we have expressed the current amplitudes per unit of membrane capacitance in Fig. 7A.

  RESULTS
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Abstract
Introduction
Methods
Results
Discussion
References

Molecular structure of alpha1G-alpha1C chimeras

Figure 1 gives a shematic representation of all discussed chimeras, in which a fragment of the alpha1G channel has been replaced by the corresponding part of alpha1C. In GCDeltaN, the 80 amino acids in the amino terminal part of alpha1G have been replaced with 124 amino acids from the N-terminus of alpha1C. Amino acids 1542 to 1618 from alpha1G have been replaced with amino acids 1195 to 1243 from alpha1C in chimera GCDeltaL. GCDeltaC1 is composed of the alpha1G channel in which the C-terminal amino acids 1863 to 2295 have been replaced with those of alpha1C from 1505 to 2166. In the C-terminal chimeras GCDeltaC2, GCDeltaC3 and GCDeltaC4, fewer amino acids have been replaced compared to GCDeltaC1. For GCDeltaC2 amino acids 2024 to 2295 from alpha1G have been replaced by those from 1690 to 2166 in alpha1C, while in GCDeltaC3 only the distal 126 amino acids at the C-terminus have been replaced with amino acids 1929 to 2166 from alpha1C. In GCDeltaC4, only the first 23 amino acids of the C-terminus have been conserved while the following distal part of alpha1G has been replaced with amino acids 1540 to 2166 from alpha1C. The C-terminus of chimera GCDeltaC5 is exactly the opposite of the C-terminus of GCDeltaC2: the first 161 amino acids have been replaced by amino acids 1505 to 1689 from alpha1C.

Activation properties of alpha1C and alpha1G

Figure 2A shows representative current traces for alpha1C and alpha1G expressed in HEK cells during voltage steps between -90 and 60 mV from a holding potential of -100 mV using either 20 mM Ca2+ (left) or 20 mM Ba2+ (right) as the charge carrier. Inactivation of L-type currents was much slower if the current was carried by Ba2+ (Fig. 2A, top). In contrast, inactivation of WT alpha1G was voltage dependent, but did not depend on the charge carrier, illustrating the Ca2+-independent inactivation of T-type calcium currents (Fig. 2A, bottom). Figure 2B shows the normalised I-V relations for alpha1C and alpha1G for both Ca2+ and Ba2+ as a charge carrier. Curves for alpha1C were shifted by about 50 mV to more positive potentials, consistent with the 'high threshold' nature of this channel as compared with the 'low threshold' alpha1G.

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    Figure 2 Comparison of T- and L-type currents in 20 mM Ca2+ and 20 mM Ba2+

    A, representative activation current traces for alpha1C (top) and alpha1G (bottom), in 20 mM Ca2+ (left) or 20 mM Ba2+ (right). The currents result from an activation step protocol that consists of subsequent 160 ms test pulses from -90 to 60 mV in steps of 10 mV, starting from a holding potential of -100 mV. Only traces representing visible currents are shown. The time interval between different episodes was 2 s. B, corresponding normalised current-voltage relationships for alpha1C and alpha1G for 20 mM Ca2+ (left) or 20 mM Ba2+ (right).

Involvement of III-IV linker in inactivation of alpha1G

Figure 3A shows representative current traces for alpha1G and the III-IV linker chimera GCDeltaL using 20 mM Ca2+ as the charge carrier. These traces were recorded during voltage steps between -80 and 30 mV (alpha1G) or -80 and 50 mV (GCDeltaL) applied from a holding potential of -100 mV. Inactivation time constants, tauinact, obtained from a single exponential fit to the decaying phase of the current, are shown as a function of voltage in Fig. 3B. It is obvious that substitution of the III-IV linker region has only minor effects on the rate of inactivation. Steady-state inactivation parameters for WT alpha1G and GCDeltaL, as obtained from a fit of the voltage dependence of h (not shown) to eqn (2), are summarized in Fig. 6A and B together with tauinact for a test pulse at -20 mV (Fig. 6C). Vinact and tauinact of GCDeltaL (Vinact = -54.0 ± 1.7 mV; tauinact = 8.5 ± 1.1 ms) were significantly decreased compared to alpha1G (Vinact = -69.6 ± 0.8 mV; sinact = 4.2 ± 0.3 mV; tauinact = 15.8 ± 1.8 ms), while sinact of GCDeltaL (sinact = 4.4 ± 0.3 mV) was unaffected.

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    Figure 3 Activation currents and inactivation time constants of alpha1G and GCDeltaL

    A, representative activation current traces in 20 mM Ca2+ for alpha1G (left) and GCDeltaL (right). The currents resulted from an activation step protocol that consists of subsequent 160 ms test pulses from -90 to 60 mV in steps of 10 mV, starting from a holding potential of -100 mV. Only traces representing visible currents are shown. The time interval between different episodes was 2 s. B, time constants of inactivation (tauinact) at different test potentials. Statistical analysis (Student's unpaired t test) was applied to the resulting data from at least 6 different measurements.

The amino terminus of alpha1G does not influence kinetics of inactivation

As shown at the bottom of Fig. 6, the inactivation properties of the amino terminal chimera GCDeltaN (Vinact = -66.0 ± 0.6 mV; sinact = 3.9 ± 0.2 mV; tauinact = 13.6 ± 0.8 ms) were not different from those of alpha1G and will not be discussed further.

The carboxy terminus is essential for fast inactivation of alpha1G

Figure 4 compares current traces with 20 mM Ca2+ as the charge carrier in response to voltage steps between -80 and 30 mV applied from a holding potential of -100 mV for alpha1G and the C-terminal chimeras GCDeltaC1, GCDeltaC4 and GCDeltaC5. Compared to WT alpha1G, inactivation was clearly slower in GCDeltaC1 and GCDeltaC5, containing a replacement of the complete C-terminus or only the first 161 C-terminal amino acids, respectively, while no difference was observed for GCDeltaC4. The time constants of inactivation, tauinact, plotted in Fig. 4B, were 2 to 3 times larger for GCDeltaC1 and GCDeltaC5 than the corresponding values of WT alpha1G, whereas those for GCDeltaC4 were not significantly different.

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    Figure 4 Activation currents and inactivation time constants of alpha1G and C-terminal chimeras

    A, representative activation current traces in 20 mM Ca2+ for alpha1G (top left), GCDeltaC1 (top right), GCDeltaC4 (bottom left) and GCDeltaC5 (bottom right). The currents resulted from an activation step protocol that consists of subsequent 160 ms test pulses from -90 to 60 mV in steps of 10 mV, starting from a holding potential of -100 mV. Only traces representing visible currents are shown. The time interval between different episodes was 2 s. B, time constants of inactivation (tauinact) at different test potentials. Statistical analysis (Student's unpaired t test) was applied to the resulting data from at least 6 different measurements.

Figure 5 shows representative current traces from alpha1G, GCDeltaC1, GCDeltaC4 and GCDeltaC5 with 20 mM Ca2+ as the charge carrier in response to a depolarising voltage step to -20 mV following a 5120 ms pre-pulse to potentials ranging from -100 to -25 mV in increments of 5 mV. The time courses of inactivation for GCDeltaC1 and GCDeltaC5 were again much slower compared to that of alpha1G. Steady-state inactivation curves, obtained from the peak current amplitudes, are depicted in Fig. 5B. Compared to alpha1G (Vinact = -69.6 ± 0.8 mV; sinact = 4.2 ± 0.3 mV), the curve for GCDeltaC4 (Vinact = -56.7 ± 1.0 mV; sinact = 4.5 ± 0.1 mV) was shifted 13 mV to the right, while the slope of the curve was unaffected. In contrast, for GCDeltaC1 (Vinact = -66.9 ± 1.2 mV; sinact = 5.8 ± 0.3 mV) and GCDeltaC5 (Vinact = -66.5 ± 1.5 mV; sinact = 6.2 ± 0.4 mV), the slope factors were increased, while no significant shift occurred.

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    Figure 5 Inactivation currents and steady-state inactivation curves of alpha1G and C-terminal chimeras

    A, representative inactivation current traces for alpha1G, GCDeltaC1, GCDeltaC4 and GCDeltaC5. The currents resulted from a protocol that consists of an 80 ms test pulse at -20 mV, following variable 5120 ms pre-pulses from -100 to -25 mV in steps of 5 mV. The holding potential was -100 mV. The interval between different episodes was 2 s. B, the average steady-state inactivation curves.

The average time constants of inactivation and the parameters of steady-state inactivation of the five different C-terminal chimeras are depicted in Fig. 6. Vinact was significantly shifted to less negative potentials for GCDeltaC2 (-51.5 ± 1.3 mV), GCDeltaC3 (-60.1 ± 2.1 mV) and GCDeltaC4 (-56.7 ± 1.0 mV) compared to WT alpha1G (-69.6 ± 0.8 mV) (P < 0.01), whereas sinact for GCDeltaC1 (5.8 ± 0.3 mV) and GCDeltaC5 (6.2 ± 0.4 mV) was significantly different from that of the WT channel (4.2 ± 0.3) (P < 0.01). Chimeras GCDeltaC1 (tauinact = 43.6 ± 2.9 ms) and GCDeltaC5 (tauinact = 30.5 ± 1.9 ms) inactivated significantly slower than alpha1G (tauinact = 15.8 ± 1.8 ms) (P < 0.01) as already shown in Fig. 5.

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    Figure 6 Kinetic characteristics of inactivation of different T-channel chimeras

    A, potentials of half-maximal steady-state current inactivation (Vinact). B, slopes of the mean inactivation curves (sinact). C, time constants for inactivation at a test pulse of -20 mV (tauinact). Columns and corresponding error bars represent mean and S.E.M. values, respectively. Statistical analysis (Student's unpaired t test) was applied to the resulting data from at least 5 different measurements. Significant differences compared to WT alpha1G: *P < 0.05, **P < 0.01.

Calcium-dependent inactivation cannot be transferred from alpha1C to alpha1G

Inactivation properties of wild-type alpha1G in 20 mM Ba2+ and 20 mM Ca2+ are compared in Fig. 7. Figure 7A represents the peak I-V relation curves showing a small shift to more positive potentials for Ba2+. Current amplitudes in Ba2+ were smaller than Ca2+ currents. Time constants of inactivation (Fig. 7B) were the same in Ba2+ and Ca2+, except at positive test potentials where inactivation was slightly faster in Ba2+ than in Ca2+. Steady-state inactivation curves, as depicted in Fig. 7D, were obtained from peak current amplitudes during steps to -20 mV following long-lasting steps to various potentials, an example of which is shown in Fig. 7C for Ca2+ and Ba2+. The inactivation curve for Ba2+ (Vinact = -57.4 ± 1.0 mV; sinact = 4.9 ± 0.4 mV; tauinact = 14.1 ± 1.6 ms) was shifted 12 mV to the right compared to Ca2+ (Vinact = -69.6 ± 0.8 mV; sinact = 4.2 ± 0.3 mV; tauinact = 15.8 ± 1.8 ms), which is consistent with the observed shift of the peak I-V relations shown in Fig. 7A.

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    Figure 7 Inactivation properties of alpha1G in Ca2+ compared to Ba2+

    A, current-voltage relationships of alpha1G in 20 mM Ba2+ (fullcir) and 20 mM Ca2+ (cir). B, time constants of inactivation (tauinact) at different test potentials in Ca2+ and Ba2+. Statistical analysis (Student's unpaired t test) was applied to the resulting data from at least 6 different measurements. C, representative inactivation current traces in Ca2+ and Ba2+ for alpha1G. The currents resulted from a protocol that consists of an 80 ms test pulse at -20 mV, following variable 5120 ms pre-pulses from -100 to -25 mV in steps of 5 mV. The holding potential was -100 mV. The interval between different episodes was 2 s. D, the average steady-state inactivation curves of alpha1G in Ba2+ (fullcir) and Ca2+ (cir). Statistical analysis (Student's unpaired t test) was applied to the resulting data from at least 6 different measurements.

Figure 8 compares the slopes of the steady-state inactivation curves, sinact, and time constants of inactivation at -20 mV, tauinact, for WT alpha1G and all C-terminal chimeras. Mean values for both Ba2+ and Ca2+ are compared to the mean value of alpha1G for Ca2+ (*). The mean of each chimera for Ba2+ is also compared to the mean of alpha1G for Ba2+ (+). For alpha1G and each chimera separately, a comparison of the mean values for Ba2+ and the mean for Ca2+ is shown (cir). The presence or absence of the IQ motif and EF hand is indicated on the left. sinact for GCDeltaC1 (+IQ/+EF) and GCDeltaC5 (+IQ/+EF) in the presence of either Ba2+ or Ca2+ was significantly higher than for alpha1G in the presence of Ca2+, whereas GCDeltaC4 (+IQ/-EF) only differed from alpha1G if Ba2+ was the charge carrier. The slope parameter of GCDeltaC5 (+IQ/+EF) was significantly larger than that of alpha1G in the presence of Ba2+. GCDeltaC2 (-IQ/-EF) and GCDeltaC4 (+IQ/-EF) were the only chimeras that showed a significantly different increase in the slope of steady-state inactivation between Ca2+ and Ba2+.

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    Figure 8 Comparison of sinact and tauinact in Ca2+ and Ba2+ for alpha1G and C-terminal chimeras

    The figure shows the slopes of the steady-state inactivation curves, sinact, and the time constants of inactivation for a test pulse at -20 mV, tauinact, for WT alpha1G and all chimeras. The presence (+) or absence (-) of the IQ or EF motifs is shown on the left side. Asterisks (*) indicate significant differences between the means of chimeras in Ba2+ or Ca2+, and the mean of alpha1G in Ca2+. Crosses (+) indicate significant differences between the mean of each chimera for Ba2+ and the mean of alpha1G for Ba2+. For alpha1G and each chimera separately, a significant difference between the mean for Ba2+ and the mean for Ca2+ is shown as an open circle (cir). Single symbols are used for P < 0.05 and double symbols for P < 0.01.

Compared to alpha1G with Ca2+, tauinact for GCDeltaC1 (+IQ/+EF) was increased with both Ba2+ and Ca2+. Also tauinact of GCDeltaC5 (+IQ/+EF) was increased for Ca2+, while inactivation was slower for GCDeltaC4 (+IQ/-EF) with Ba2+. Compared to alpha1G in Ba2+, GCDeltaC1 (+IQ/+EF) and GCDeltaC5 (+IQ/+EF) showed a slower inactivation if Ba2+ was the charge carrier, while GCDeltaC4 (+IQ/-EF) was much faster. In contrast with alpha1G, chimeras GCDeltaC1 (+IQ/+EF), GCDeltaC2 (-IQ/-EF), GCDeltaC4 (+IQ/-EF) and GCDeltaC5 (+IQ/+EF) inactivated faster with Ba2+compared to Ca2+, while no difference was seen for GCDeltaC3 (-IQ/-EF).

  DISCUSSION
Top
Abstract
Introduction
Methods
Results
Discussion
References

We have studied a number of chimeras of T- and L-type Ca2+ channels in order to investigate the inactivation mechanism of the T-type Ca2+ channel alpha1G at the molecular level. This is important for several reasons. (1) The inactivation mechanism of T-type channels seems to be different from that of other voltage-dependent channels. It has indeed been shown that the macroscopic time constant of inactivation is closely correlated with the latency time of channel opening in single-channel recordings, suggesting that macroscopic inactivation may reflect delayed microscopic activation rather than a channel transition to an absorbing closed state (Droogmans & Nilius, 1989; Chen & Hess, 1990; Serrano et al. 1999). (2) In contrast with L-type channels, T-type calcium channels lack Ca2+-dependent inactivation (Bossu et al. 1985; Chen & Hess, 1990; Randall & Tsien, 1996). (3) Some channel properties, which may be related to the mechanism of inactivation, are essential for several biological functions, e.g. role in pace-making (Nilius, 1986; Droogmans & Nilius, 1989; Chen & Hess, 1990; Randall & Tsien, 1996) and Ca2+ entry during repolarization (Tseng & Boyden, 1989; Lei et al. 1996).

As to current inactivation, it is obvious that the substitution of the III-IV linker region (GCDeltaL) affects the inactivation properties of alpha1G. Vinact and tauinact are changed significantly. This is not an unexpected finding, since this structure is responsible for fast inactivation of voltage-gated Na+ channels, which have a structure analogous to that of alpha1G, although the III-IV linker of alpha1G does not contain the IFM motif, necessary for fast inactivation of the sodium channel (Stühmer et al. 1989; Patton et al. 1993; Catterall, 1999). This indicates that the III-IV linker influences alpha1G inactivation via another mechanism.

On the other hand, the cytoplasmic C-terminal end seems to play a key role in inactivation, since the removal of a region of 161 amino acids at the amino side of this C-terminus slowed down inactivation for GCDeltaC5 by a factor of 2-3. However, if only the first 23 amino acids of the C-terminus were conserved in GCDeltaC4, the rate of inactivation was similar to alpha1G. This relatively small region contains 10 glutamate residues forming a negatively charged stretch adjacent to the intracellular part of the channel pore. The protein sequence of this region is also highly conserved in alpha1H (Cribbs et al. 1998) and alpha1I (Lee et al. 1999). An intriguing tentative mechanism could be a 'ball-and-chain'-type inactivation process as described for K+ channels (Armstrong & Bezanilla, 1977; Hoshi et al. 1990; Zagotta & Aldrich, 1990) whereby the proximal part of the C-terminus functions as a negatively charged acceptor region for a ball located in another intracellular part of the channel. An involvement of the intracellular N-terminus, as observed for K+ channels, can be ruled out since inactivation was not affected in GCDeltaN. The faster inactivation of GCDeltaL, in which all 77 amino acids of the III-IV linker are replaced by the shorter linker of alpha1C (containing only 49 residues), could be due to an improved accessibility of the C-terminal acceptor region for some attracted ball during inactivation. The shift of the potential of half-maximal steady-state current inactivation, Vinact, towards less negative potentials for GCDeltaC2, GCDeltaC3 and GCDeltaC4 resulting from the replacement of respectively 272, 126 and 410 amino acids from the alpha1G C-terminus by the corresponding alpha1C region containing respectively 477, 237 and 627 amino acids may indicate that movement of the chimerical C-terminus during a putative ball-acceptor interaction requires more energy. For the slowly inactivating chimeras GCDeltaC1 and GCDeltaC5, this positive shift of Vinact was not observed when the C-terminal acceptor region was replaced and this may cause a lower impact of the C-terminus on the remaining inactivation process.

We were not able to transfer the calcium dependency of inactivation from alpha1C to alpha1G. Chimeras GCDeltaC1 and GCDeltaC5, both containing the EF hand as well as the IQ motif, even showed a slower inactivation in Ca2+ compared to WT alpha1G. In fact, inactivation was slower in Ca2+ than in Ba2+ for those chimeras. These results confirm the hypothesis that other amino acid sequences, outside the C-terminus of alpha1C, could be involved in Ca2+-dependent inactivation of alpha1C, like a binding region for constitutive, Ca2+-independent tethering of calmodulin to the channel (Peterson et al. 1999, 2000). Obviously, alpha1G does not have a proper site for constitutive calmodulin binding which could allow the C-terminal chimeras containing the IQ motif and EF hand (GCDeltaC1 and GCDeltaC5) to inactivate in a Ca2+-dependent way.

Further investigation including measurements at the single channel level is necessary to localise the critical domains for inactivation more precisely and to unravel the possible interactions between different regions of the alpha1G channel.

  REFERENCES
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Abstract
Introduction
Methods
Results
Discussion
References

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Acknowledgements

We thank Drs J. Eggermont, K. H. Suh, J. Papassotiriou and R. Vennekens for helpful discussions. The expert technical assistance of M. Crabbé, H. Van Weijenbergh and M. Schuermans is greatly acknowledged. This work was supported by the Belgian Federal Government, the Flemish Government and the Onderzoeksraad KU Leuven (GOA 99/07, F.W.O. G.0237.95, F.W.O. G.0214.99, F.W.O. G.0136.00; Interuniversity Poles of Attraction Program, Prime Ministers Office IUAP Nr.3P4/23, and C.O.F./96/22-A069), and by 'Levenslijn' (7.0021.99).

Corresponding author

B. Nilius: Laboratorium voor Fysiologie, KU Leuven, Campus Gasthuisberg, Herestraat 49, B-3000 Leuven, Belgium.

Email: bernd.nilius{at}med.kuleuven.ac.be




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