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Volume 17, Number 1, Issue of January 1, 1997 pp. 32-44
Copyright ©1997 Society for Neuroscience

A Novel Subunit for Shal K+ Channels Radically Alters Activation and Inactivation

Timothy Jegla and Lawrence Salkoff

Department of Anatomy and Neurobiology, Washington University School of Medicine, St. Louis, Missouri 63110

ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
DISCUSSION
FOOTNOTES
REFERENCES


ABSTRACT

Shal (Kv4) potassium channel genes encode classical subthreshold A-currents, and their regulation may be a key factor in determining neuronal firing frequency. The inactivation rate of Shal channels is increased by a presently unidentified class of proteins in both Drosophila and mammals. We have cloned a novel Shal channel subunit (jShalgamma 1) from the jellyfish Polyorchis penicillatus that alters Shal currents from both invertebrates and vertebrates. When co-expressed with the conserved jellyfish Shal homolog jShal1, jShalgamma 1 dramatically changes both the rate of inactivation and voltage range of activation and steady-state inactivation. jShalgamma 1 provides fast inactivation by a classic N-type mechanism, which is independent of its effects on voltage dependence. jShalgamma 1 forms functional channels only as a heteromultimer, and jShalgamma 1 + jShal1 heteromultimers are functional only in a 2:2 subunit stoichiometry.

Key words: K+ channel; Shal; inactivation; Polyorchis; a-current; heteromultimer; jellyfish; diploblast; gamma -subunit


INTRODUCTION

Transient K+ currents that are active at subthreshold potentials (A-currents) (Connor and Stevens, 1971a) are a dominant K+ conductance during the interspike interval and have a major influence on the firing frequency of neurons (Connor and Stevens, 1971b). Of the four subfamilies of genes that encode the channel-forming alpha -subunits of voltage-gated K+ channels (Shaker, Shab, Shal, and Shaw), the Shal (Kv4) subfamily most closely matches the description of the classical subthreshold A-current. The importance of subthreshold A-currents is underscored by the fact that Shal is the most highly conserved voltage-gated K+ channel subfamily in higher triploblastic metazoans (Salkoff et al., 1992).

Recent genetic and molecular evidence supports the idea that Shal channels underlie classical subthreshold A-currents in neurons of both vertebrates and invertebrates. Serodio et al. (1994) have shown that the major subthreshold A-current expressed in the rat brain is likely to be encoded by Shal genes. Shal channels in the mammalian brain are located primarily on the dendrites and cell bodies of neurons (Sheng et al., 1992), where their placement might influence spiking behavior. Using mutant analysis, Tsunoda and Salkoff (1995a,b) also found Shal currents in cell bodies of neurons from the fruit fly Drosophila, suggesting that the intracellular location and function of these channels is conserved across species.

Shal inactivation rate is regulated by an unknown mechanism in both vertebrates and Drosophila. Shal currents vary almost 50-fold in inactivation rate in Drosophila embryonic neurons. Most in vivo Shal currents inactivate far more rapidly than currents expressed when Shal cRNA is injected into Xenopus oocytes (Pak et al., 1991). In mammals, the inactivation rates of Shal currents can be increased by co-expression in Xenopus oocytes with low molecular weight fractions of mRNA from rodent brain (Chabala et al., 1993; Serodio et al., 1994). Both results suggest a mechanism for increasing the rate of inactivation in Shal channels that is not intrinsic to Shal alpha -subunits. Because Shal currents influence the duration of the interspike interval (Connor and Stevens, 1971b), their inactivation rates may determine neuronal firing patterns. Thus, understanding the mechanism controlling Shal inactivation rates may be important for understanding how neuronal firing patterns are generated.

We have explored the evolutionary origins of Shal channels in a primitive metazoan and have discovered a molecular mechanism for regulating the inactivation rate of Shal currents. We show here that Shal is highly conserved in the jellyfish Polyorchis penicillatus, a diploblastic coelenterate. Because diploblasts are the most primitive metazoans to have nervous systems, our results show that Shal currents were present in the first neurons that evolved in the last common ancestors of diploblasts and triploblasts, ~700 million to 1 billion years ago (Morris, 1993). One Polyorchis Shal homolog, jShalgamma 1, appears to function only as a heteromultimer in concert with a Shal alpha -subunit. Compared with homomultimeric Shal channels consisting of Shal alpha -subunits alone, Shalalpha  + Shalgamma heteromultimers produced currents that inactivate far more rapidly. In contrast to the cytosolic beta -subunits that provide rapid inactivation in mammalian Shaker K+ channels (Rettig et al., 1994), jShalgamma 1 is homologous to the alpha -subunits of voltage-gated K+ channels.


MATERIALS AND METHODS

Cloning. Amplification and isolation of fragments of jShal1 and jShalgamma 1 from Polyorchis penicillatus genomic DNA was performed as described in Jegla and Salkoff (1995) and Jegla et al. (1995). Briefly, the degenerate primers 5'-TCGGAATTCTATGACTACTGTTGGNTAYGGNGA-3' and 5'-ACCTCTAGAGGTAGTGCTATTRYNAGNACNCC-3', which are derived from the consensus amino acid sequences of the P-domain (MTTVGYGD) and the S6 domain (GVL(T/V)TIAL) of voltage-gated K+ channels, were used to amplify initial fragments. These were size-selected, reamplified using overlapping nondegenerate primers, and then subcloned to allow for isolation of individual fragments.

A complete jShal1 genomic clone was obtained using the initial jShal1 fragment to probe a Polyorchis genomic library (provided by Dr. Warren Gallin, University of Alberta) under high-stringency conditions (Butler et al., 1989) and sequenced. The coding region of jShal1 consists of three exons, as indicated in Figure 1. Two exons encoding the N-terminal, S1-S6, and neighboring C-terminal cytoplasmic regions were predicted based on their high homology to dShal and mShal. The third exon encoding the poorly conserved distal C-terminal region was identified by amplification from an oligo dT-primed Polyorchis cDNA library using a jShal1-specific sense primer in the S6 region (5'-CCTGGTAAACTA-GTTGGTAGTATTTGCTCA-3') and an antisense primer corresponding to the library vector sequence (5'-TCCGGTCGACGTAGAGGG-GAATAAATCGCCATA-3'). Construction of the Polyorchis genomic library and of cDNA libraries from neuronally enriched Polyorchis penicillatus tissue samples have been described previously (Gallin, 1991).


Fig. 1. jShal1 and jShalgamma 1 amino acid sequences. Jellyfish Shal homologs jShal1 and jShalgamma 1 are compared with Shal channels from Drosophila (dShal; Wei et al., 1990) and mouse (mShal, Kv4.1; Pak et al., 1991). Identical residues are shown in reversed lettering (white on black). Predicted transmembrane domains (S1-S6) and a K+ channel pore motif (P-domain; Hartmann et al., 1991; Yool and Schwarz, 1991) are underlined. Also underlined is the cytoplasmic N-terminal domain (T1), which is believed to mediate subfamily-specific assembly of voltage-gated K+ channel subunits (Li et al., 1992; Shen et al., 1993; Shen and Pfaffinger, 1995). Large italic letters and plus symbols mark five evenly spaced positively charged residues found in S4 voltage sensor (Papazian et al., 1991) and seven positively charged residues near the N terminal of jShalgamma 1 that are part of a motif similar to N-terminal inactivation ball motifs (Murrell-Lagnado and Aldrich, 1993). The positions of two introns conserved in jShal1, dShal, and mShal are marked with arrows. Of these two, only the intron position in the P-domain motif is also found in jShalgamma 1. A third jShalgamma 1-specific intron near S6 is labeled with an arrow bracketed by asterisks. Residue numbers are shown on the right. Asterisks by the residue numbers at the end of the dShal and mShal sequences indicate that they are incomplete. The GenBank accession numbers for jShal1 and jShalgamma 1 are U78642[GenBank] and U78641[GenBank], respectively.
[View Larger Version of this Image (95K GIF file)]

The jShalgamma 1 genomic sequence was obtained in two sequential rounds of inverse PCR (Ochman et al., 1988). The genomic DNA used for inverse PCR was prepared by first cutting with a desired restriction enzyme and then ligating at concentrations of 2 ng/µl or less to promote self-circularization. In the first round of inverse PCR, a 1.4 kb fragment of jShalgamma 1 was amplified from DNA prepared with BglII using sense (5'-CAAGTCTAGATGATAGGCTCTATGTGTTGCTTGAT-3') and antisense (5'-AACTAAGCTTGGATGGTAACAGGAACAACATC-3') primers derived from the original P-domain-S6 jShalgamma 1 fragment. Sequencing revealed that the fragment included a BglII site at the beginning of S2 and extended through the 3' end of the open reading frame. Inverse PCR was also performed on genomic DNA prepared with HindII using jShalgamma 1-specific primers (5'-CAGTTGTTTAGTTATAACCCTCTCC-3') and (5'-GCCAAAGAAAAGGTGGGGTCTTCAC-3') located 5' of a HindII site in S3. A 900 bp fragment obtained in this screen was found to extend through the 5' end of jShalgamma 1 coding sequence. The 3' coding region of jShalgamma 1 was confirmed by PCR amplification from a Polyorchis cDNA bank by the same method as for jShal1, but with the jShalgamma 1-specific sense primer used in the first round of inverse PCR. A stop codon was found just 3' of S6 in two cDNAs and is also present in the genomic sequence. The 5' coding region was not found in any cDNA clones but was instead determined from genomic sequence. Our analysis, based on several observations, indicated that no introns interrupt coding in this region. First, no consensus sequences for acceptor or donor splice junctions were found in this region. Second, the codons used in this predicted 5' region of jShalgamma 1 match the coding bias we have observed for six Polyorchis K+ channel genes (data not shown). Finally, this region has an A/T content of 64%, which falls within the range we have observed for Polyorchis coding sequence (60-65%), but well below the range we have observed for Polyorchis introns (72-76%).

Alignments and phylogenetic trees. The amino acid alignment (see Fig. 1) was generated using Microgenie (Beckman, Palo Alto, CA) and optimized by eye. Phylogenetic trees were constructed from these alignments by maximum parsimony, as implemented in the PAUP computer program (Swofford, 1993). Only sections of the T1 region and membrane spanning core (S1-S6) that have relatively conserved lengths (and thus certain alignment) among the Shaker, Shal, Shab, and Shaw subfamilies were used for tree building. Tree lengths were calculated using a step matrix that weighted changes between amino acids according to the minimum number of nucleotide changes that were necessary to achieve the change. A heuristic search for optimal trees was performed using random addition to generate initial trees. Tree bisection and reconnection were then used to optimize the trees. The consensus maximum parsimony tree (see Fig. 2) was constructed from the 18 shortest trees found in this search.


Fig. 2. Phylogenetic analysis places jShal1 and jShalgamma 1 in the Shal subfamily. A consensus maximum parsimony tree of jShal1, jShalgamma 1, and 15 voltage-gated K+ channel genes representing the Shaker, Shab, Shal, and Shaw subfamilies is derived from the 18 most parsimonious trees found in a heuristic search. Numbers indicate the percentage of times a particular branch point was observed in these trees. For the unresolved branchings seen in the Shaker subfamily, no single pattern was observed in >50% of the trees from which the consensus is derived. Branches defining each subfamily are bracketed at the right edge of the figure. Shaker homologs are from rat (rKv1.1, X12589; Baumann et al., 1988), Drosophila (dShak, M17211; Papazian et al., 1987), Aplysia (aShak, M95914; Pfaffinger et al., 1991), a platyhelminth (pShak, L26968; Kim et al., 1995), and the jellyfish Polyorchis (jShak1 and jShak2, U32922 and U32923; Jegla et al., 1995). Shab subfamily members are from rat [rKv2.1, X16476, Frech et al. (1989); IK8 and K13, M81783 and M81784, Drewe et al. (1992)], Drosophila (dShab, M32659, Butler et al., 1989), and Aplysia (aShab, S68356, Quattrocki et al., 1994). The Shaw subfamily is represented by rKv3.1 [rat, M68880, Rettig et al. (1992)] and dShaw [Drosophila, M32661, Butler et al. (1989)]. The Shal subfamily includes sequences from mouse [mKv4.1, M64226, Pak et al. (1991)] and Drosophila [dShal, M32660, Wei et al. (1990)] as well as jShal1 and jShalgamma 1.
[View Larger Version of this Image (24K GIF file)]

Expression vector construction. The complete open reading frame of jShal1 was united by removing the two introns from the genomic clone. The 3' intron was removed from jShal1 in two subcloning steps. First, the C-terminal cDNA fragment (which spanned from S6 to the C terminal) was subcloned into Bluescript II SK+ (Stratagene, La Jolla, CA) using an SpeI site in S6 and an EcoRI site from the cDNA library vector. Second, a genomic fragment spanning from an XbaI site 5' of the initiator methionine to the SpeI site in S6 was cloned into the SpeI site of this cDNA subclone. The P-domain intron was removed using overlap extension PCR off this template (Ho et al., 1989). The final overlap extension product was produced using a sense primer (5'-TTACGAATTCG-<UNL>CCACCATG</UNL>AAT GGTGACATAGGCGCTT-3') that adds a consensus translation initiation sequence (underlined) (Kozak, 1987) surrounding the jShal1 initiator methionine and an antisense primer from the Bluescript vector. This product was cut with EcoRI and cloned into the EcoRI site of the Xenopus oocyte expression vector pBSMXT (Wei et al., 1994). The coding region was then sequenced and compared with the jShal1 genomic clone to confirm that no PCR-introduced mutations existed.

A similar overlap extension protocol was used to remove both introns from the open reading frame of jShalgamma 1. The final product was made with a sense primer (5'-ATATGGAT<UNL>CCACCATG</UNL>TATTCGGTTACTTC-CACTGCAAC-3') that introduced a consensus translation initiation sequence (underlined) to the jShalgamma 1 initiator methionine and an antisense primer (5'-CTTATCTAGATCAATCTTCTTCGCTAGCCTTCA- TTTGAATTATTGGGACAGG-3') that includes the jShalgamma 1 stop codon and spans coding sequence on both sides of the 3' intron. It was cut at flanking BamHI and XbaI sites introduced in the primers and subcloned into the pOX expression vector. Four individually amplified clones were sequenced and compared with each other as well as with the original inverse PCR-generated jShalgamma 1 clones, allowing PCR-introduced mutations to be identified. A jShalgamma 1 expression vector clone containing two silent mutations was used in all physiological experiments. The pOX vector was constructed by inserting Xenopus beta -globin 5' and 3' untranslated sequences contained in pBSMXT (Wei et al., 1994) into new restriction sites in pBluescript II KS+ (Stratagene). Briefly, the Xenopus beta -globin 5' untranslated and an NheI site was inserted between the KpnI and SalI sites of the vector, while an XhoI site and the Xenopus beta -globin 3' untranslated were inserted between the XbaI and NotI sites.

Expression and electrophysiology. Capped cRNAs were prepared by run-off transcription with T3 RNA polymerase using the mMessage mMachine kit (Ambion, Austin, TX) and diluted in RNase-free ddH2O to desired concentrations before injection. Mature stage IV Xenopus oocytes were prepared for injection as described in Wei et al., 1990. Oocytes were injected with 50 nl of cRNA and incubated at 18°C for 1-5 d in ND96 containing (in mM): 96 NaCl, 2 KCl, 1.8 CaCl2, 1 MgCl2, 5 HEPES-NaOH, pH 7.5, supplemented with 100 U/ml penicillin, 100 µg/ml streptomycin, and 2.5 mM sodium pyruvate. Recording methods used were as published previously in Covarrubias et al., 1991. Briefly, whole-cell recordings were made 1-5 d after injection at room temperature (~22°C) by conventional two-microelectrode voltage-clamp techniques. Electrodes ranged from 0.2 to 0.5 MOmega in resistance and were filled with 3 M KCl. The standard recording solution consisted of ND96 with 1 mM 4,4'-diisothiocyanatostilbene-2,2' disulfonic acid to block native oocyte chloride currents. Currents were digitally acquired with CCURRENT using linear leak subtraction, filtered at 1 kHz with an eight-pole Bessel filter and analyzed with CQUANT. Capacitative transients were removed by leak subtraction or clipped out.

Stoichiometry calculations. Time constants (see Fig. 7) were calculated by least-squares fits of double-exponential functions to traces like those shown in the insets. Because the slowly inactivating jShal1 current could be inactivated by a prepulse to -90 mV, such a prepulse was often used to help isolate the fast components produced by jShal1 + jShalgamma 1 heteromultimers in oocytes expressing both currents. The free-mixing curve shown in Figure 7 assumes a binomial distribution of channels containing zero to four jShalgamma 1 inactivation balls. If p equals the fraction of jShal1 subunits and q equals the fraction of jShalgamma 1-subunits, then the distribution of channel types is as follows: p4 (0 balls) + p3q (1 ball) + p2q2 (2 balls) + pq3 (3 balls) + q4 (4 balls). The fractional size of the slowly inactivating current (jShal1 homomultimers, 0 balls) represents p4 and could thus be used to predict the fraction of each type of channel. The predicted fast-inactivation time constants were obtained by adjusting the inactivation rate constant calculated for these currents to the average number of inactivation balls per channel predicted from the binomial distribution of channel types. Only those channels containing one to three balls were included in the calculations of the fast-inactivation time constants, because channels with four balls (jShalgamma 1 homomultimers) are nonfunctional. Thus, if free mixing occurs, the fastest inactivation time constants observed in jShalgamma 1-biased currents with no jShal1 homomultimeric fraction (2.69 msec) should be produced primarily by channels with three inactivation balls. Thus, the time constant of fast N-type inactivation should approach three times this value as the proportion of jShal1 is increased. The equations for calculating inactivation rate constants from the time constants of inactivation and recovery and for calculating the free mixing curve are from MacKinnon et al., 1993.


Fig. 7. jShal1 and jShalgamma 1 form functional channels in a single stoichiometry. 1 and 2 show current traces (normalized in amplitude) for oocytes expressing jShal1 + jShalgamma 1 in a jShalgamma 1-biased mix (1) or a jShal1-biased mix (2). The large, slowly inactivating component in 2 has the properties of a jShal1 homomultimer current. On the right, the fast-inactivating components of 1 and 2 have been normalized to the same amplitude and plotted together, showing nearly identical inactivation rates. The graph shows a plot of the fast-inactivation time constant versus fraction of the total current with slow inactivation (jShal1 homomultimeric current) for individual experiments in which oocytes were injected with varying ratios of jShal1 and jShalgamma 1 (solid circles). The time constants are normalized to the mean fast-inactivation time constant calculated from the leftmost group of data points (2.69 msec), representing jShalgamma 1-biased mixes in which virtually no slowly inactivating current is seen. Inactivation rate was not increased by further biasing the ratio toward jShalgamma 1. The straight line (Fixed Stoichiometry) indicates the predicted relationship between the fast-inactivation time constant and the fraction of current with slow inactivation if only a single stoichiometry of heteromultimer is functional. The curve (Free Mixing) represents the prediction of fast-inactivation time constant if jShal1 and jShalgamma 1 form functional channels in all possible stoichiometries.
[View Larger Version of this Image (17K GIF file)]

The time constants (see Fig. 8) were determined by triple exponential fits to current traces like those shown in the insets, because two time constants of slow inactivation (from jShal1 + jShalgamma 1(T) heteromultimers) contributed to the accuracy of the fit. The curve for the prediction ofchannels containing three jShalgamma 1-subunits assumes that four types exist, all heteromultimers with three jShalgamma 1-based-subunits and one jShal1-subunit, but with zero to three inactivation balls. Because of the high ratio of jShalgamma 1 and jShalgamma 1(T) to jShal1 used in these experiments, few jShal1 homomultimers are predicted to exist, allowing these channels to be excluded from the calculations. If p equals the fraction of jShalgamma 1(T)-subunits and q equals the fraction of jShalgamma 1-subunits, then the distribution of channel types is: p3 (0 balls) + p2q (1 ball) + pq2 (2 balls) + q3 (3 balls). The fraction of slowly inactivating current (p3) was used to calculate the fraction of each channel type. For the prediction of two jShalgamma 1-subunits in each channel, the distribution is simplified to three possible channel types: p2 (0 balls) + pq (1 ball) + q2 (2 balls). In this case, the slowly inactivating current fraction equals p2. For the prediction of a single jShalgamma 1-subunit, just two channel types will exist, p and q, and the slowly inactivating current fraction equals p. The curves were again calculated by the method of MacKinnon et al. (1993) but with the binomial distributions explained above.


Fig. 8. Functional jShal1-jShalgamma 1 heteromultimers have a 2:2 stoichiometry. 1 and 2 show currents (normalized in amplitude) from an oocyte expressing only jShal1 + jShalgamma 1 (1) and an oocyte expressing jShal1 + jShalgamma 1 + jShalgamma 1(T) (2) [jShalgamma 1 and jShalgamma 1(T) are in a 1:1 ratio]. The slowly inactivating current fraction is almost completely produced by jShal1 + jShalgamma 1(T) heteromultimers. jShal1 homomultimers contribute little to this slow current, because cRNA mixes were biased toward jShalgamma 1 + jShalgamma 1(T). Therefore, the inactivation time constants and steady-state inactivation curves for slowly inactivating fractions closely matched the inactivation time constants of jShal1 + jShalgamma 1(T) heteromultimers. The traces on the right show a comparison of the fast-inactivating fractions of 1 and 2 normalized to the same amplitude. This shows that adding jShalgamma 1(T) slows N-type inactivation. The graph shows predictions of the fast-inactivation time constant versus fraction of slowly inactivating current, in which the functional heteromultimeric channels contain either 1, 2, or 3 jShalgamma 1-based-subunits. Solid circles represent data from individual experiments; the fit assumes two jShalgamma 1-subunits in the functional heteromultimers.
[View Larger Version of this Image (20K GIF file)]


RESULTS

Cloning and conservation

A previous study of the evolutionary origins of voltage-gated K+ channels showed that homologs of mammalian channels are present in the jellyfish Polyorchis penicillatus, which is among the simplest extant metazoans to have an organized nervous system (Jegla et al., 1995). We infer from this result that a similar set of voltage-gated K+ channels play an indispensable role in the nervous systems of all metazoans. Shal is the most conserved among these channels in the higher triploblastic metazoa, and here we describe highly conserved Polyorchis Shal homologs, jShal1 and jShalgamma 1. Because regulation of Shal channels may be a key element in the generation of patterned neuronal output, we have now focused attention on the mechanism of this regulation, which may be conserved as well.

jShal1 and jShalgamma 1 gene fragments were initially isolated by a PCR screen of Polyorchis penicillatus genomic DNA. Degenerate primers for this screen were based on regions of the P-domain (MTTVGYGD) and S6 transmembrane domain (GVL(T/V)IAL) that are highly conserved among voltage-gated K+ channels. The P-domain-S6 fragments of jShal1 and jShalgamma 1 were used to isolate complete coding sequences for these genes both by hybridization and PCR techniques, as described in Materials and Methods. Figure 1 shows the deduced amino acid sequences of the jShal1 and jShalgamma 1 proteins compared with the sequences of Shal proteins from the fruit fly Drosophila (dShal) and mouse (mShal, Kv4.1). Each contains the characteristic structural features of voltage-gated K+ channel alpha -subunits.

jShal1 is very clearly a direct homolog of triploblastic Shal genes, because the jShal1 protein shares high conservation to triploblastic Shal alpha -subunits over virtually its entire length. It is ~65% identical to dShal and mShal across the membrane-spanning channel core (Table 1). Interspecies homologs of specific voltage-gated K+ channel genes typically share at least 50% amino acid identity over this region, and jellyfish and triploblastic Shaker homologs share only this 50% amino acid identity (Jegla et al., 1995). The higher level of conservation in jShal1 is consistent with previous observations that Shal is the most highly conserved subfamily of voltage-gated K+ channels (Salkoff, 1992). Conservation is nearly as high in the T1 domain, which mediates subfamily-specific channel assembly (Li et al., 1992; Shen et al., 1993; Shen and Pfaffinger, 1995). jShal1 also has a conserved genomic structure; the positions of two introns, one in the P-domain motif and one in the C-terminal cytoplasmic domain, are perfectly conserved among jShal1, dShal, and mShal (Fig. 1, arrows).

Table 1. Percent amino acid identity shared between jellyfish Shal homologs, triploblastic Shal homologs, and a jellyfish Shaker homolog


jShal1 jShalgamma 1 dShal mShal jShak1

jShal1 - 41 (52) 66 (64) 65 (51) 40 (37)
jShalgamma 1 41 (52) - 42 (51) 44 (51) 33 (32)
dShal 66 (64) 42 (51) - 83 (67) 43 (36)

Percent amino acid identities are shown for pairwise alignments between jShal1, jShalgamma 1, the Drosophila Shal homolog dShal (Wei et al., 1990), the mouse Shal homolog mShal or Kv4.1 (Pak et al., 1991), and the jellyfish Shaker homolog jShak1 (Jegla and Salkoff, 1995). Identities are measured from the first residue of S1 to the last residue of S6 and for the most highly conserved regions surrounding the T1 domain corresponding to amino acids 39-133 of jShal1 (shown in parentheses).

In contrast, jShalgamma 1 is less well conserved and shares barely >40% amino acid identity from S1 to S6 (Table 1). Despite this lower conservation, several lines of evidence lead us to put jShalgamma 1 in the Shal K+ channel subfamily. As with all Shal alpha -subunits, jShalgamma 1 contains an intron at the "Shal-specific" site in the P domain. Introns are not found at this position in genes from the Shaker, Shab, or Shaw subfamilies. Secondly, Shal-specific conservation is high (>50%) in the T1 subfamily-specific assembly domain. Finally, phylogenetic analysis of jShal1, jShalgamma 1, and 15 other voltage-gated K+ channel proteins representing the Shaker, Shab, Shal, and Shaw subfamilies unequivocally places jShalgamma 1 within the Shal subfamily. A consensus of the 18 shortest trees found in a heuristic search using maximum parsimony (PAUP, Swofford, 1993) is shown in Figure 2. jShalgamma 1 is placed within the Shal subfamily in all of these trees. The order of branching between channel subfamilies shown in Figure 2 is not consistent in these 18 trees and should not be taken to indicate the evolutionary relationships of these subfamilies.

The lower conservation shared between jShalgamma 1 and Shal alpha -subunits is especially evident in the S4 voltage sensor (Papazian et al., 1991), which is perfectly conserved between dShal and mShal and has only two substitutions of 22 residues in jShal1. In contrast, there are 12 substitutions in the same 22 residues of jShalgamma 1 (Fig. 1). Interestingly, these S4 differences are found in the hydrophobic residues, whereas the string of positively charged residues characteristic of S4 is identical.

Two other key features distinguish jShalgamma 1 from jShal1 and other Shal homologs. One is that jShalgamma 1 has a group of seven positively charged residues at near its N terminal that is not found in other Shal homologs (Fig. 1). This motif is reminiscent of an inactivation "`ball," similar to those responsible for rapid inactivation in both triplobastic and diploblastic Shaker channels (Hoshi et al., 1990; Zagotta et al., 1990; Jegla et al., 1995). Later, we will show that these charges are indeed part of a functional inactivation ball in channels containing jShalgamma 1. The second feature is that after S6, jShalgamma 1 has a segment of just seven amino acids and thus lacks a long conserved C-terminal cytoplasmic segment found even in jShal1 (Fig. 1).

Expression

Shal1 expresses a rapidly activating transient current in Xenopus oocytes that resembles Shal currents from Drosophila and mammals. Figure 3 shows a comparison of the jShal1 current and the Drosophila Shal current dShal. The biophysical properties of these two currents are summarized in Table 2. Both currents share features of classic subthreshold A-currents that distinguish Shal currents from other voltage-dependent K+ currents. These include a hyperpolarized steady-state inactivation curve and an inactivation time course that is relatively insensitive to voltage. However, the jShal1 current differs in two important ways. First, its inactivation rate is severalfold slower than that of dShal. Whereas the fastest inactivation time constant is ~140 msec for jShal1 at +50 mV, it is ~40 msec for dShal. Second, jShal1's activation and steady-state inactivation curves are shifted to even more hyperpolarized voltages. The V50 for activation of jShal1 is approximately -35 mV more hyperpolarized than that of dShal (Fig. 3C). The V50 for steady-state inactivation for jShal1 is approximately -106 mV compared with -62 mV for dShal (Fig. 3D).
Fig. 3. Comparison of the jShal1 and dShal currents. Families of outward currents are shown for Xenopus oocytes expressing either jShal1 (A) or dShal (B). Currents were recorded in response to 1 sec test pulses from -90 mV to +50 mV in 20 mV increments. Five second prepulses to -140 mV (from a holding potential of -90 mV) preceded each test pulse to ensure complete recovery from inactivation. C, Conductance versus voltage curves are shown for jShal1 (solid circles) and dShal (open circles). Error bars indicate SEM, and solid curves represent Boltzmann fits of the data (G/Gmax = 1/(1 + exp(- (V - V50)/a), where G is the conductance at voltage V, Gmax is the maximal conductance, V50 is the voltage at which G = 0.5 × Gmax, and a is the slope factor. D, Steady-state inactivation curves for jShal1 and dShal. Currents were obtained by measuring the peak current during test pulses to +40 mV, after 10 sec prepulses to the voltage shown on the x-axis. Holding potentials were -90 mV with 5 sec prepulses to -140 mV preceding test pulses. The curves represent best fits of the data to the Boltzmann function I/Imax = 1/(1 + exp((V - V50)/a), where I is the peak current measured during the test pulse after a prepulse to voltage V, Imax is the maximal current measured, V50 is the prepulse voltage at which I = 0.5 × Imax, and a is the slope factor.
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Table 2. Summary of the biophysical properties of jellyfish and Drosophila Shal currents


Parameter dShal jShal1 jShal1 + jShalgamma 1 jShal1 + jShalgamma 1 (T)

Activation
V50 (mV)  -3.8  ± 0.1 (8)  -39.3  ± 0.1 (11)  -11.8  ± 0.9 (8)  -17.7  ± 0.7 (7)
Slope (mV/e-fold) 15.38  ± 0.07 (8) 22.4  ± 0.1 (11) 17.4  ± 0.1 (8) 17.5  ± 0.07 (7)
Inactivation
V50 (mV)  -60.6  ± 0.1 (8)  -106.1  ± 0.2 (11)  -71.5  ± 0.2 (8)  -64.4  ± 0.7 (7)
Slope (mV/e-fold) 6.3  ± 0.1 (8) 6.1  ± 0.15 (11) 4.9  ± 0.2 (8) 7.9  ± 0.2 (7)
 tau FAST (msec) 40.1  ± 2.1 (8) 137  ± 6.7 (4) 2.69  ± 0.04 (13) 24.3  ± 0.8 (8)
 tau SLOW (msec) 165  ± 8.4 (8) 889  ± 61 (4) 275  ± 12 (8)
% Fast 57  ± 3 (8) 41  ± 2 (4) 43  ± 2 (8)
Recovery
 tau R-F (msec) 505  ± 12.9 (9) 375  ± 25.4 (4)* 170  ± 5.7 (5) 9.76  ± 2.5 (7)
 tau R-S (msec) 3824  ± 813 (5)** 155  ± 17.2 (7)**

V50 and slope (in mV/e-fold change in conductance) of activation and steady-state inactivation are derived from the Boltzmann fits of the conductance/voltage and steady-state inactivation data shown in Figures 3, 4, 5. tau FAST and tau SLOW are the fast and slow time constants of inactivation and were determined at +50 mV. The percent of the current inactivating with tau FAST is also given. tau R-F and tau R-S are time constants of fast and slow components of recovery from inactivation determined at -100 mV for dShal and the heteromultimeric currents and at -120 mV for jShal1. If a single component to recovery was identified, it is given as tau R-F. Error values (±) are for SEs of curve fits and data points, and sample sizes are indicated in parentheses.
* A small (<= 15%), virtually instantaneous component to jShal1 recovery fit is not listed, because it is probably caused by channels that did not inactivate during the test pulse and did not close during the shortest recovery periods.
** These are the major recovery components for jShal1 + jShalgamma 1 and jShal1 + jShalgamma 1 (T) heteromultimers, at 87 and 64%, respectively.

jShalgamma 1 is unlike an alpha -subunit in that it does not form functional voltage-dependent channels when expressed as a homomultimer in Xenopus oocytes (Fig. 4A). Instead, jShalgamma 1 functions only in combination with Shal alpha -subunits. Figure 4B shows currents resulting from its co-expression with jShal1 in Xenopus oocytes. Because this current is distinct from jShal1 currents, it is assumed that it results from the heteromultimeric assembly of jShalgamma 1 and jShal1. Relative to jShal1 homomultimers, jShal1 + jShalgamma 1 heteromultimers inactivate much more rapidly with a time constant of <3 msec at +50 mV. This represents a several hundredfold increase in the inactivation rate from jShal1 currents (Table 2). These heteromultimeric jellyfish Shal currents resemble the majority of Shal currents expressed in Drosophila embryonic neurons, which inactivate with time constants near 5 msec (Tsunoda and Salkoff, 1995a). A second major change produced by the co-expression of jShalgamma 1 with jShal1 is a large depolarizing shift in the activation and steady-state inactivation curves compared with jShal1 (~+30 mV for activation and ~+35 mV for steady-state inactivation) (Fig. 4C,D, Table 2). Unlike jShal1 homomultimers, these heteromeric channels are much more typical of Shal channels from triploblasts with regard to their voltage range of activation.


Fig. 4. jShalgamma 1 modifies the inactivation and activation range of jShal1. A, Currents recorded from a Xenopus oocyte expressing only jShalgamma 1. Test pulses (400 msec) from -70 mV to +50 mV were as described in Figure 3A. B, Rapidly inactivating outward currents recorded from an oocyte co-expressing jShalgamma 1 and jShal1. The same voltage protocol was used, except that test pulses were 100 msec in duration. The thin dotted line is a jShal1 homomultimeric current (+50 mV) scaled to the same amplitude for comparison of inactivation rate. C, Conductance versus voltage curves for jShal1 homomultimers (solid circles), dShal homomultimers (open circles), and jShal1 + jShalgamma 1 heteromultimers (solid triangles). D, Steady-state inactivation curves for jShal1, dShal, and jShal1 + jShalgamma 1 co-injection. Data collection, analysis, and curve fitting for C and D are as in Figure 3, C and D.
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An N-type inactivation mechanism in jShalgamma 1

Because jShalgamma 1 is unique among Shal homologs in containing a positively charged inactivation ball-like motif at its N terminal, we tested the possibility that jShalgamma 1 causes rapid inactivation in jShal1 currents by contributing an N-type inactivation mechanism. To investigate this, we removed the positively charged N terminal from jShalgamma 1; this truncated construct is referred to here as jShalgamma 1(T). This N-terminal truncation does indeed result in removal of fast inactivation from the heteromultimeric current (Fig. 5A, Table 2), providing the first clear example of rapid N- type inactivation in Shal channels. The mechanism of N-type inactivation conferred by jShalgamma 1 is independent of the shift in the voltage range of activation. Thus, the activation and steady-state inactivation curves of jShal1 + jShalgamma 1(T) heteromultimers resemble those of jShal1 + jShalgamma 1 heteromultimers; both have a depolarizing shift relative to that of jShal1 homomultimers (Fig. 5B,C). Hence, this depolarized voltage range is likely to be conferred by regions other than the N terminal such as the poorly conserved regions of the jShalgamma 1 core. For instance, it was demonstrated that changes in the hydrophobic residues of the S4 region of Shaker can cause large shifts in the activation range (Lopez et al., 1991). Although fast N-type inactivation is absent in jShal1 + jShalgamma 1(T) heteromultimers, slower inactivation remains that is accelerated with respect to the inactivation of jShal1 homomultimers (Fig. 5A, Table 2). The residues responsible for this increased rate of residual inactivation are not known. Because N-type inactivation has been removed from jShalgamma 1(T), the remaining inactivation may occur by a mechanism similar to C-type inactivation in Shaker channels, which depends on residues in the P-domain and S6 (Hoshi et al., 1991, Lopez-Barneo et al., 1993).
Fig. 5. jShalgamma 1 confers rapid inactivation by an N-type mechanism. An N-terminal truncated form of jShalgamma 1, jShalgamma 1(T), was constructed by replacing the N-terminal amino acids MYSVTSTATYFLTRKVKNRHRTNVTRNK with an initiator Met. Seven positively charge residues (bold) that distinguish jShalgamma 1 from Shal alpha -subunits were removed. A, Current traces from oocytes expressing jShal1, or jShal1 + jShalgamma 1, or jShal1 + jShalgamma 1(T) recorded in response to depolarizations to +50 mV. Traces are scaled to the same amplitude for comparison of inactivation rate. B, Conductance voltage curves for jShal1 (solid circles), jShal1 + jShalgamma 1 (solid triangles), and jShal1 + jShalgamma 1(T) (open triangles). C, Steady-state inactivation curves for jShal1, jShal1 + jShalgamma 1, and jShal1 + jShalgamma 1(T). D, Time course of recovery from inactivation for jShal1, jShal1 + jShalgamma 1, and jShal1 + jShalgamma 1(T). Recovery rates were determined by a double-pulse protocol in which test pulses to +40 mV were separated by a recovery pulse of increasing duration. Recovery was at either -100 mV or -120 mV (jShal1). Because the recovery rate of all Shal channels increases with increasing hyperpolarization (T. Jegla and L. Salkoff, unpublished observations), the difference in recovery rate between jShalgamma 1(T) heteromultimers and jShal1 homomultimers at an identical voltage is likely to be even greater than the difference we show here. Pulse series were preceded by 5 sec prepulses to -140 mV to ensure complete recovery from inactivation. Test pulse durations were 1 sec for jShal1 and jShal1 + jShalgamma 1(T) and 200 msec for jShal1 + jShalgamma 1. Curves were generated using the equation It = {a × (1 - exp(-t/tau 1))} + {b × (1 - exp(-t/tau 2))}, where It is the current amplitude of the second +40 mV pulse divided by the current amplitude of the first pulse, t is the interval of the recovery step at -100 mV, and a and b are the components of current recovering exponentially with time constants of tau 1 and tau 2, respectively.
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The highly charged N-terminal domain of jShalgamma 1 had a profound effect on recovery from inactivation as well as on the inactivation rate. Recovery from inactivation in jShal1 + jShalgamma 1 heteromultimers was measured and compared with recovery of jShal1 + jShalgamma 1(T) heteromultimers and jShal1 homomultimers (Fig. 5D). jShal1 + jShalgamma 1 heteromultimers recovered slowest, with a time constant of several seconds at -100 mV. However, in jShal1 + jShalgamma 1(T) heteromultimers, recovery is significantly more rapid and is complete within a few hundred milliseconds (Fig. 5D). Thus, the very slow phase of recovery from inactivation is attributable to fast N-type inactivation. On the other hand, recovery from slow "C-type" inactivation is actually faster in jShal1 + jShalgamma 1(T) heteromultimers than in jShal1 homomultimers (Fig. 5D). jShal1 recovery was measured at -120 mV instead of -100 mV because, as Figure 5C illustrates, most jShal1 channels are inactivated at -100 mV. jShal1 + jShalgamma 1 heteromultimers have a small but faster component to recovery, which may be caused by a few channels entering an alternative "C-type" inactivated state before N-type inactivation can occur. The very slow recovery from N-type inactivation indicates that the association between the jShalgamma 1 inactivation ball and its blocking site on jShal1 + jShalgamma 1 heteromultimers is very strong.

jShalgamma 1 heteromultimerizes with dShal and mShal

jShalgamma 1 does not appear to form functional heteromultimers with alpha -subunits from subfamilies of voltage-gated K+ channels other than Shal. In co-expression experiments, we found no evidence that jShalgamma 1 alters any biophysical properties of channels formed by the Polyorchis Shaker homologs jShak1 and jShak2 (data not shown). However, the ability of jShalgamma 1 to form heteromultimers with Shal alpha -subunits from other species is conserved. Evidence for this is presented in Figure 6, which shows currents resulting from the co-expression of jShalgamma 1 with dShal or mShal. Inactivation rates are increased when dShal and mShal are co-expressed with jShalgamma 1 in Xenopus oocytes. However, co-expression of jShalgamma 1 with dShal and mShal has only minor effects on the activation range, probably because homomultimeric dShal and mShal channels already operate in the voltage range in which jShalgamma 1 biases activation (data not shown).
Fig. 6. Heteromultimerization of jShalgamma 1 with dShal and mShal. A, Current traces recorded in response to a test pulse to +50 mV for Xenopus oocytes expressing dShal, dShal + jShalgamma 1, and dShal + jShalgamma 1(T) are shown normalized in amplitude for comparison of inactivation rates. B, Similar traces for oocytes expressing mShal, mShal + jShalgamma 1, and mShal + jShalgamma 1(T). C, Comparison of currents produced by co-expression of jShalgamma 1 + jShal1, jShalgamma 1 + dShal, and jShalgamma 1 + mShal. Although jShalgamma 1(T) appears to have opposite effects on the inactivation rates of dShal and mShal relative to jShal1 (Fig. 5A), the absolute inactivation rates of all three heteromultimers are actually quite similar.
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Several observations suggest that the inactivation ball binding site on heteromultimers containing dShal or mShal has lower affinity for the jShalgamma 1 inactivation ball than the binding site on heteromultimers containing jShal1. The increase in inactivation rate in the interspecies heteromultimers is clearly caused by the N-terminal inactivation ball of jShalgamma 1, because inactivation is slowed if this N-terminal ball is removed (Fig. 6A,B). Nevertheless, N-type inactivation in these heteromultimers is not nearly as fast or complete as when jShalgamma 1 is mixed with jShal1 (Fig. 6C, Table 3). This shows that the Shal alpha -subunits, which do not have a high affinity inactivation ball themselves, contribute to the binding affinity of the jShalgamma 1 inactivation ball. This result is consistent with observations of the Drosophila Shaker channel showing that only one inactivation ball at a time is able to block the channel (MacKinnon et al., 1993). Taken together, these results suggest that N-type inactivation particles may bind to a single site formed by all four subunits (Murrell-Lagnado and Aldrich, 1993).

Table 3. Inactivation rates of different heteromultimers containing jShalgamma 1


Inactivation time constants (msec)
Fast Medium* Slow % Fast**

jShal1 + jShalgamma 1 2.69  ± 0.04 (13) Close to 100
dShal 40.1  ± 2.1 (8) 165  ± 8.4 (8) 57  ± 3 (8)
dShal1 + jShalgamma 1 20.2  ± 0.6 (8) 99.8  ± 5.8 (8) 59  ± 1 (8)
dShal1 + jShalgamma 1 (T) 44.2  ± 1.5 (7) 272  ± 8.1 (7) 44  ± 1 (7)
mShal 25.5  ± 1.0 (6) 109  ± 2.1 (6) 337  ± 13.7 (6) 19  ± 1 (6)
mShal + jShalgamma 1 12.3  ± 0.3 (8) 41.8  ± 1.4 (8) 228.7  ± 3.9 (8) 52  ± 2 (8)

Time constants for mShal + jShalgamma 1 (T) are not given because of insufficient data.
* The inactivation rate of mShal-based currents is best fit with three exponentials. The new time constant is given as "Medium."
** % Fast is the percentage of the current that inactivates with the "Fast" inactivation time constant.

Stoichiometry of jShal1 + jShalgamma 1 heteromultimers

We have exploited the presence of the N-terminal inactivation ball on jShalgamma 1 to estimate the subunit stoichiometry of jShal1 + jShalgamma 1 heteromultimers. Our strategy was based on two assumptions. (1) The functional mechanism of N-terminal inactivation provided by jShalgamma 1 is the same as in Shaker N-type inactivation (MacKinnon et al., 1993). (2) jShal1 and jShalgamma 1 form tetrameric channels. This latter assumption is based on the structural similarity of Shal alpha -subunits to Shaker alpha -subunits, which are known to form tetramers (MacKinnon, 1991). In Shaker, the inactivation ball contributed by each of the four subunits functions independently (MacKinnon et al., 1993). This independence results in a simple additive effect of each ball on the inactivation rate. Thus, the inactivation rate of channels that have only one inactivation ball would be roughly four times slower than the inactivation rate for channels containing four inactivation balls. This result was shown by mixing increasing proportions of Shaker subunits lacking an inactivation ball with Shaker subunits having an inactivation ball. In these experiments, the inactivation rate is progressively slowed, because the number of inactivation balls per channel is progressively reduced.

Similarly, if jShal1 and jShalgamma 1 mix freely to produce functional heteromultimers of several stoichiometries, then increasing the proportion of jShal1 in an oocyte will progressively reduce the average number of inactivation balls on each heteromultimeric channel. This should result in slower N-type inactivation. If, on the other hand, there is only a single functional stoichiometry of jShal1 + jShalgamma 1 heteromultimer, then the rate of N-type inactivation should remain constant as the proportion of jShal1 is increased (while the relative amount of slowly inactivating current increases). Figure 7 illustrates this unchanging rate of fast inactivation and suggests that there is only a single functional stoichiometry in jShal1 + jShalgamma 1 heteromultimers. As predicted, when the amount of jShal1 is increased relative to the amount of jShalgamma 1, the fast-inactivating component of the current is progressively reduced, leaving a larger slow component (corresponding to the jShal1 homomultimeric current). Significantly, the time constant of fast inactivation remains unchanged.

To further investigate the stoichiometry of jShal1 + jShalgamma 1 heteromultimers, we co-injected jShalgamma 1(T), which has the inactivation ball removed, with jShal1 and jShalgamma 1. Unlike the previous experiment, increasing proportions of jShalgamma 1(T) should progressively reduce the average number of inactivation balls per heteromultimeric channel, even if the functional stoichiometry of jShalgamma 1 + jShal1 heteromultimers is fixed. In contrast to the experiments shown in Figure 7, the fast-inactivation rate should progressively slow. Oocytes injected with jShalgamma 1(T), jShalgamma 1, and jShal1 again had both fast- and slow-inactivating current fractions (Fig. 8). Most importantly, the rate of fast N-type inactivation is slowed almost twofold by the addition of increasing amounts of jShalgamma 1(T). By analogy to the Shaker results, the twofold slowing of N-type inactivation suggests that the number of inactivation balls is reduced by half when jShalgamma 1(T) is added. These results can be explained by postulating three significant current components: a very fast component produced by channels with two jShal1 and two jShalgamma 1-subunits, a slower "fast" component produced by channels with two jShal1, one jShalgamma 1, and one jShalgamma 1(T)-subunits, and the slow component produced by channels with two jShal1 and two jShalgamma 1(T)-subunits. A second slow component produced by jShal1 homomultimers is of insignificant size in these mixes, because of the high ratio of jShalgamma 1 and jShalgamma 1(T) to jShal1. Thus, it appears that heteromultimers are limited to a single stoichiometry of two jShal1-subunits and two jShalgamma 1-subunits (Fig. 8). The fact that we can progressively reduce the number of inactivation balls without completely removing N-type inactivation strongly supports our initial assumption that the jShalgamma 1 inactivation balls function independently of each other, exactly like Shaker inactivation balls.


DISCUSSION

Significance of the conservation of Shal in diploblasts

Connor and Stevens (1971b) first recognized that subthreshold A-currents have the capacity to influence neuronal firing frequency because of their active role during interspike intervals. Patterned neural output from single neurons appears to be highly conserved among animals. Neurons of diploblastic coelenterates such as Polyorchis are capable of firing trains of action potentials or rhythmic bursts of action potentials that are virtually indistinguishable from those of vertebrates (Anderson, 1979; Przysiezniak and Spencer, 1989). The high conservation of Shal channels is likely to be part of the reason. The conservation of several additional classes of voltage-gated ion channels also contributes to this conservation of intrinsic electrical properties between diploblastic and triploblastic neurons (Anderson and McKay, 1987; Dunlap et al., 1987; Holman and Anderson, 1991; Przysiezniak and Spencer, 1992, 1994; Anderson et al., 1993; Meech and Mackie, 1993; Jegla et al., 1995). This growing set of channels known to be shared by diploblasts and triploblasts may represent an essential set for the patterning of signals in all nervous systems and suggests that the intrinsic electrical properties of neurons were optimized early in the evolution of the nervous system.

Regulation of Shal inactivation by jShalgamma 1

Our finding that jShalgamma 1, a functionally novel Shal-subunit, regulates the inactivation rate of Shal currents parallels the discovery that beta -subunits can induce rapid inactivation in Shaker currents (Rettig et al., 1994). In contrast to jShalgamma 1, these beta -subunits are cytosolic proteins homologous to members of the NAD(P)H-dependent oxidoreductase superfamily (McCormack and McCormack, 1994) and are not structurally homologous to voltage-gated K+ channel alpha -subunits. Although both jShalgamma 1 and Shaker beta -subunits cause rapid inactivation by N-type mechanisms, jShalgamma 1 has additional effects on the voltage range of channel activation. This is, perhaps, attributable to the fact that jShalgamma 1 forms an integral part of the voltage-sensing mechanism of the channel.

Although jShalgamma 1 is similar in structure to the alpha -subunits of Shal and other voltage-gated K+ channels, it is unique in that it does not form functional homomultimeric channels. Instead, it modifies the gating properties of Shal alpha -subunits, functioning only as a heteromultimer. This distinct functional role has led to an interesting pattern of conservation between Shal alpha -subunits and jShalgamma 1. Regions involved in subfamily-specific assembly (T1) and ion selectivity (pore region) are highly conserved, whereas regions involved in determining gating properties (N terminal, S1-S4) differ substantially.

The reason that jShalgamma 1 does not form functional homomultimers is not clear, but it is not exclusively attributable to constitutive inactivation resulting from the presence of four high-affinity inactivation balls. This is demonstrated by the fact that the N-terminal truncated construct jShalgamma 1(T) also fails to express a voltage-dependent current as a homomultimer. The unusually short C-terminal cytoplasmic domain is also unlikely to be responsible for the failure of homomultimer formation. This was shown by substituting the longer C-terminal domain of jShal1 for the shorter C-terminal domain of jShalgamma 1; expression of voltage-dependent currents was not recovered (data not shown). These experiments strongly imply that jShalgamma 1 is specifically designed to function only in a heteromultimeric configuration.

The restriction of functional jShal1 + jShalgamma 1 heteromultimers to a single 2:2 functional stoichiometry may be necessary to precisely fix the voltage range and inactivation rate of the current rather than to allow gradations of these properties. Because the jShalgamma 1 inactivation ball binding site appears to involve both the jShal1 and jShalgamma 1-subunits, a precise arrangement of these two types of subunits may be necessary to produce a high-affinity binding site. If so, only one of two possible arrangements of the two jShalgamma 1-subunits within the 2:2 heteromultimers (side by side or opposite) may produce functional fast-inactivating channels. It may be possible to address this question in the future by using tandem constructs of jShalgamma 1 and jShal1. If both arrangements are functional, fast-inactivating heteromultimers should be obtained by expression of jShalgamma 1 + jShal1 dimers (opposite arrangement) as well as by co-expression of jShalgamma 1 + jShalgamma 1 and jShal1 + jShal1 dimers (side by side arrangement). We do not know whether 3:1 and 1:3 stoichiometries of jShal1 + jShalgamma 1 heteromultimers assemble but are nonfunctional or simply do not