Background: In skeletal muscle, DHPR cytoplasmic domains are thought to couple membrane depolarization to Ca2+ release via RyR1.
Results: The presence of RyR1 alters FRET between donor/acceptor pairs in cytoplasmic domains of the DHPR α1S subunit.
Conclusion: Interaction with RyR1 causes rearrangement of α1S cytoplasmic domains.
Significance: Multiple cytoplasmic domains of α1S may be involved in the interaction with RyR1.
Keywords: Calcium Channels, Excitation-Contraction Coupling, Fluorescence Resonance Energy Transfer (FRET), Ryanodine Receptor, Skeletal Muscle, Dihydropyridine Receptor, L-type Calcium Channel
Abstract
The skeletal muscle dihydropyridine receptor (DHPR) in the t-tubular membrane serves as the Ca2+ channel and voltage sensor for excitation-contraction (EC) coupling, triggering Ca2+ release via the type 1 ryanodine receptor (RyR1) in the sarcoplasmic reticulum (SR). The two proteins appear to be physically linked, and both the α1S and β1a subunits of the DHPR are essential for EC coupling. Within α1S, cytoplasmic domains of importance include the I-II loop (to which β1a binds), the II-III and III-IV loops, and the C terminus. However, the spatial relationship of these domains to one another has not been established. Here, we have taken the approach of measuring FRET between fluorescent proteins inserted into pairs of α1S cytoplasmic domains. Expression of these constructs in dyspedic (RyR1 null) and dysgenic (α1S null) myotubes was used to test for function and targeting to plasma membrane/SR junctions and to test whether the presence of RyR1 caused altered FRET. We found that in the absence of RyR1, measureable FRET occurred between the N terminus and C terminus (residue 1636), and between the II-III loop (residue 626) and both the N and C termini; the I-II loop (residue 406) showed weak FRET with the II-III loop but not with the N terminus. Association with RyR1 caused II-III loop FRET to decrease with the C terminus and increase with the N terminus and caused I-II loop FRET to increase with both the II-III loop and N terminus. Overall, RyR1 appears to cause a substantial reorientation of the cytoplasmic α1S domains consistent with their becoming more closely packed.
Introduction
In skeletal muscle, excitation-contraction (EC)2 coupling depends upon junctions between the plasma membrane and sarcoplasmic reticulum (SR) (1). At these junctions, dihydropyridine receptors (DHPRs), which are heteromeric proteins, serve as voltage sensors that respond to depolarization by triggering the release of Ca2+ from the SR via the type 1 ryanodine receptor (RyR1), a homotetrameric protein (2–4). In the junctional membrane, DHPRs are arrayed in groups of four (“tetrads”) as a consequence of physical links with RyR1 (5, 6). The existence of these links and the fact that skeletal-type EC coupling does not require the entry of external Ca2+ have led to the idea that conformational changes of the linking regions are responsible for the activation of RyR1 (7, 8). However, the identity of the linking regions has remained obscure in large measure because the interaction takes place between two separate membrane systems and depends upon voltage across the plasma membrane.
A variety of approaches has been used to try to identify the sites of linkage between the DHPR and RyR1, including binding assays in vitro and functional analysis of muscle cells after expression of proteins having altered sequence in specific regions. In the case of RyR1, this approach has shown that skeletal-type EC coupling depends on multiple regions far separated in the primary sequence (9, 10). However, these studies have been hampered by the relative lack of information about the tertiary structure of RyR1. There has been somewhat more progress for the DHPR because of its smaller size and its better understood domain structure. The principle subunit, α1S, has four homology repeats, which form the voltage-sensing and ion permeation structures. The N and C termini and the loops linking the repeats are all cytoplasmic (11). Two loops of particular importance are the I-II loop, which is known to bind the auxiliary β1a subunit (12), and the II-III loop, which is critical for both tetrad formation (13) and skeletal-type EC coupling (14–17). The β1a subunit is a soluble protein which binds to α1S and promotes its membrane trafficking (18). Moreover, β1a is co-equal in importance with the α1S II-III loop for tetrad formation (19) and skeletal EC coupling (20, 21). Among the possible explanations for these results is that β1a and/or the II-III loop bind to RyR1, perhaps in close proximity to one another. There is also evidence suggestive of binding interactions between other DHPR cytoplasmic domains and RyR1. These include the α1S III-IV loop, which is known to modulate EC coupling (22, 23), and the C terminus, a segment of which binds to RyR1 in vitro (24), and which becomes partially occluded in the presence of RyR1 in vivo (25, 26).
The evidence that multiple cytoplasmic domains of the DHPR may interact with RyR1 makes it important to determine the spatial interrelationships between these cytoplasmic domains within living muscle cells and whether these interrelationships are altered by the presence of RyR1. In the current study, we have investigated this issue by constructing cDNAs encoding α1S subunits doubly tagged with fluorescent proteins, in which a FRET donor (CyPet) was placed at one cytoplasmic site and a FRET acceptor (YPet) was situated at a second site. These constructs were expressed in skeletal myotubes produced from dyspedic (RyR1 null) and dysgenic (α1S null) mice. After expression in dyspedic myotubes, energy transfer indicated proximity (<10 nm separation) between N- and C termini and between the II-III loop and both termini. By contrast, the I-II loop produced weak FRET with the II-III loop and none with the N or C termini. After expression in dysgenic myotubes, the presence of RyR1 appeared to cause a substantial reorientation of the domains, including a shift of the II-III loop toward the C terminus and a shift of the I-II loop toward both the II-III loop and N terminus. Because the I-II loop is associated with β1a, the decreased proximity between the I-II and II-III loops may indicate that β1a and the II-III loop form a unified structure that interacts with RyR1 to promote tetrad formation and skeletal-type EC coupling.
EXPERIMENTAL PROCEDURES
DNA Constructs for the Expression of Fluorescently Labeled α1S
The backbone of the mammalian expression vectors pECFP and pEYFP (Clontech, Palo Alto, CA) was used to design plasmids for expression of fluorescently tagged rabbit α1S (GenBankTM accession no. M23919). Site-directed mutagenesis (Stratagene, La Jolla, CA) was used to generate unique restriction sites at defined positions within the α1S cDNA sequence, which were used to introduce the sequences encoding the FRET-optimized fluorescent proteins CyPet and/or YPet (27). The labeling positions were as follows.
CyPet-α1S-YPet and YPet-α1S-CyPet
One fluorescent protein was attached to the first residue of the α1S N terminus, separated by the 12-residue linker RSRAQASNSAVD. The second fluorescent protein was attached to the last residue of α1S truncated at residue 1636, separated by the four-residue linker PVAT.
CyPet or YPet within the α1S I-II Loop
The fluorescent protein was inserted with its N terminus immediately after residue 406 of the α1S I-II loop, and its C terminus connected via the 3-residue linker RLN to α1S residues 407–1860.
CyPet or YPet within the α1S II-III Loop
The fluorescent protein sequence was inserted into the II-III loop between α1S residues 726 and 727, connected via a four-residue linker (PVAT) and 18-residue linker (RSRAQASNSAVDGTAGPV), respectively.
CyPet or YPet within the α1S III-IV Loop
The fluorescent protein sequence was inserted into the III-IV loop between α1S residues 1096 and 1097 via a single leucine and a three-residue linker (SAR), respectively.
YPet-α1S-α1S-CyPet (α1S tandem)
The first α1S was attached via its C terminus, which had been truncated at residue 1636, to a three-residue linker (GVD), which was attached to the N terminus of the second α1S, which was C-terminally truncated at residue 1636. YPet was attached to the N terminus of the first α1S via a 12-residue linker (SRAQASNSAVD) and CyPet was attached to the C terminus of the second α1S via a four-residue linker (PVAT).
Primary Skeletal Muscle Cell Culture and Transfection
Myoblasts were prepared from newborn dysgenic mice, homozygous for absence of α1S (28), or newborn dyspedic mice, homozygous for absence of RyR1 (29) as described (30). The myoblasts were grown for 6–7 days in a humidified 37 °C incubator with 5% CO2 in Dulbecco's modified eagle medium (E15-009, PAA, Coelbe, Germany), supplemented with 10% fetal bovine serum/10% horse serum (Biochrom, Berlin, Germany). This medium was then replaced with differentiation medium (DMEM supplemented with 2% horse serum). Two to four days following the shift to differentiation medium, single nuclei were microinjected with plasmid cDNA (100 ng/μl in water).
Microscopy and Measurements of FRET
An important consideration for the studies reported here is that fluorescently tagged α1S constructs expressed in myotubes are concentrated in numerous discrete foci of small size (≤1 μm). Thus, methods for analysis of FRET, which require multiple scans, have the drawback that the measurements will be compromised if movement of the foci occurs in the time interval between the initial and final scans, an interval that can be substantial. For example, the acceptor photobleaching method requires the measurement of cyan fluorescence before after the bleaching of yellow and typically requires several seconds or more. Thus, we selected to employ a method in which an index of FRET could be obtained without multiple scans. Specifically, myotubes were examined 24–48 h after microinjection using a FV1000 confocal laser-scanning microscope (Olympus) under 60× magnification. For the measurement of FRET, an area of 512 × 512 pixels was selected to include both a part of the myotube to be analyzed and an adjacent region, which was cell-free. Excitation was at 440 nm, and emission was measured simultaneously via two photomultipliers, one of which was equipped with a 465–495 nm band pass filter (cyan channel, intensity IC), and the other photomultiplier was equipped with a 535–565 nm band pass filter (yellow channel, intensity IY). The photomultiplier gains, offsets, and pinhole diameters were kept the same for all experiments. Even when both YPet and CyPet are present, only CyPet contributes to IC because YPet does not emit in the 465–495 nm range. However, IY contains three contributions, emission from CyPet in the 535–565 nm range (IY(Cy)), emission from YPet, which is directly excited by 440 nm (IY(Y)), and YPet emission, which occurs as a consequence of FRET (IY(FRET)).
Correction for IY(Cy) is straightforward because the magnitude of IY(Cy) is a constant fraction of IC. To determine this fraction, we measured IC and IY(Cy) in cells expressing α1S labeled only with a single CyPet and excited at 440 nm. This yielded IY(Cy)/IC = 0.28 ± 0.02 (n = 25). Thus, for constructs labeled with both CyPet and YPet, we calculated the following in Equation 2.
In principle, it would also have been possible to have corrected for IY(Y) (emission from YPet excited at 440 nm) by scanning each cell twice, once with 440 nm excitation and once with 515 nm excitation (which does not excite CyPet). However, because 440 nm is near the absorption minimum for YPet, we chose for simplicity to calculate Equation 3 as an indication of FRET.
The calculation of IY*/IC was restricted to the punctate foci to which labeled α1S constructs localize in myotubes. First, the background intensity measured in a cell-free region was subtracted from all pixels of the respective scan. Then, by means of a custom made Microsoft Excel macro, the image was “masked” with an adjustable threshold, such that all areas below this threshold were excluded from analysis, and only areas exceeding the threshold (including the punctate foci) were included. The macro iteratively incremented the cut-off intensity, resulting in a successively decreasing number of included pixels. For each value of the threshold, the macro calculated IY* = IY − 0.28·IC and the ratio IY*/IC. During this iterative process, IY*/IC approached a quasi-constant level as the threshold was increased and the contribution of regions outside the punctate foci was reduced. Subsequently, IY*/IC abruptly became unstable when the cut-off threshold became so high that the small size of the analyzed areas caused large inhomogeneities in pixel levels between the cyan and yellow channels. The values of IY*/IC reported under “Results” (see Figs. 3 and 4) are from the approximately constant-level phase as revealed by the analysis macro. All data are reported as mean ± S.D. The unpaired Student's t test was used to compare the IY*/IC ratios calculated for a given construct expressed in dyspedic or dysgenic myotubes.
Electrically Evoked Contractions
The ability of fluorescently labeled α1S constructs to support EC coupling was tested by determining whether myotubes expressing the construct and bathed in rodent Ringer's (146 mm NaCl, 5 mm KCl, 2 mm CaCl2, 1 mm MgCl2, 10 mm HEPES, 11 mm glucose, pH 7.40, with NaOH) contracted in response to a 10-ms, 100-V pulse applied via an extracellular pipette filled with 150 mm NaCl.
Measurement of L-type Currents
The whole cell patch clamp method was used to measure macroscopic Ca2+ currents (31). Borosilicate glass pipettes were polished to a final resistance of ∼2.0–3.0 MΩ when filled with intracellular solution containing the following: 140 mm CsAsp, 5 mm MgCl2, 10 mm Cs2EGTA, 10 mm HEPES, pH 7.4, with CsOH. The external bath solution contained the following: 10 mm CaCl2, 145 mm tetraethylammonium-Cl, 0.003 mm tetrodotoxin, 0.1 mm N-benzyl-p-toluene sulfonamide, 10 mm HEPES, pH 7.4 with tetraethylammonium-OH. To isolate L-type currents, voltage was stepped from the holding potential (−80 mV) to −20 mV for 1 s to inactivate endogenous T-type current and then repolarized to −50 mV for 50 ms, depolarized to varying test potentials for 200–400 ms, repolarized to −50 mV for 100 ms, and then returned to the holding potential. Test currents were corrected for linear components of leak and capacitive current by digitally scaling and subtracting the average of 11 control currents elicited by a hyperpolarizing step from −80 to −110 mV. Cell capacitance was determined by integration of a transient from −80 to −70 mV and was used to normalize current amplitudes (pA/pF). Peak currents as a function of test potential were fitted according to Equation 4,
where I is the peak inward Ca2+ current measured at the potential V, Vrev is the reversal potential, and kG is a slope factor.
RESULTS
Sites within α1S Cytoplasmic Domains Suitable for Labeling with Fluorescent Protein
The goal of this study was to determine whether association with RyR1 causes rearrangement of the cytoplasmic domains of α1S, as indicated by altered FRET between donor/acceptor pairs inserted at various cytoplasmic sites. A necessary requirement for these constructs was that they target to plasma membrane/SR junctions in both dyspedic (RyR1 null) and dysgenic (α1S null) myotubes and that they function as both L-type Ca2+ channels and voltage sensors for EC coupling after expression in dysgenic myotubes. Correct targeting was assessed by the presence of discrete, fluorescent foci (∼0.3–1 μm in diameter) located close to or at the cell surface. Focal extracellular stimulation was used to test for contractions as an indicator of EC coupling, and whole-cell voltage clamp measurements were used to test for L-type Ca2+ current.
As a first step toward double labeling α1S with fluorescent proteins, we tested constructs with single additions to the cytoplasmic domains. As expected from previous work (25), a construct in which the fluorescent protein was attached to the N terminus, produced fluorescent puncta in both dyspedic and dysgenic myotubes, and was able to produce L-type Ca2+ current and support EC coupling in dysgenic myotubes (Fig. 1a). The effects of insertion into the I-II loop depended on whether this was upstream or downstream of the AID (residues 357–374), at which high affinity binding of β1a occurs (32). A construct with upstream insertion (between residues 350 and 351) failed to target in dyspedic myotubes and did not restore Ca2+ channel and EC coupling functions in dysgenic myotubes, although targeting in dysgenic myotubes still appeared to occur (Fig. 1b). Insertion downstream of the AID, between residues 406 and 407, did not interfere with either targeting or function (Fig. 1c). Previous work (33) had shown targeting to be unaffected, and function to be only partially reduced, after expression in dysgenic myotubes of a construct in which a single fluorescent protein had been inserted into the II-III loop between residues 726 and 727, which is near the N terminus of a domain (residues 720–765) known to be critical for EC coupling (16). Here, we also found that targeting and function in dysgenic myotubes were preserved after insertion of fluorescent protein between residues 726 and 727, and additionally observed that constructs with this insertion displayed junctional targeting in dyspedic myotubes (Fig. 1d). We did not test insertions further downstream in the II-III loop because the previous work had shown that signaling interactions with RyR1 were ablated by insertions either between residues 760 and 761, or between residues 785 and 786 (33). In the III-IV loop, we found that insertion at a point near the middle (between residues 1096 and 1097) abolished targeting in both dyspedic and dysgenic myotubes and also eliminated EC coupling (Fig. 1e). Given the relatively short length of the III-IV loop (53 residues), we did not test other insertion sites. Based on the results illustrated in Fig. 1, the N terminus, the I-II loop downstream of the AID, and the II-III loop at the beginning of the domain critical for EC coupling were identified as potential sites for double labeling of α1S.
Previous work had shown that attachment of either a CFP-YFP tandem (25), or the biotin acceptor domain (26), to a C-terminally truncated α1S (at residue 1667) did not interfere with function after expression in dysgenic myotubes, and we found similar results for truncation and attachment of YPet at residue 1666 (data not shown). Additionally, we observed that constructs C-terminally tagged with YPet at residue 1666 and N-terminally tagged with CyPet (CyPet-α1S1666-YPet) produced co-localized cyan and yellow puncta after expression in dysgenic myotubes (Fig. 2a, upper row). Co-localized puncta were also observed after expression of CyPet-α1S1666-YPet in dyspedic myotubes, but this was superimposed on a substantial background of diffuse yellow fluorescence (Fig. 2a, bottom row). Because post-translational cleavage of full-length α1S (1873 residues) has been reported to occur at residue 1664 (34), this diffuse yellow fluorescence could have been a consequence of the proteolytic liberation of YPet from a fraction of the CyPet-α1S1666-YPet molecules. Thus, we tested the construct CyPet-α1S1636-YPet in which YPet had been attached to the C terminus truncated at residue 1636, upstream of the putative cleavage site. This construct produced co-localized cyan and yellow foci in both dysgenic and dyspedic myotubes (Fig. 2b). On the basis of these results, all the C-terminally tagged α1S constructs used for the FRET measurements in this study were truncated at residue 1636. All other α1S constructs did not have this truncation and their sequence ended at residue 1860 (25).
Doubly Labeled α1S Constructs
On the basis of the results illustrated in Figs. 1 and 2, there were potentially six constructs of α1S that could be doubly tagged; these are illustrated in Fig. 3, a–f. Surprisingly, all six of the doubly tagged constructs produced, in both dyspedic and dysgenic myotubes, co-localized cyan and yellow foci near/at the cell surface, indicative of successful targeting. In addition to these punctate foci, there was a low level of diffuse/reticular fluorescence in dyspedic myotubes after expression of the three constructs labeled with YPet at position 406 of the I-II loop (asterisks, Fig. 3, a, d, and e). For these constructs, a corresponding diffuse/reticular distribution was also observed for the cyan fluorescence, which differs from dyspedic myotubes expressing CyPet-α1S1666-YPet, in which diffuse fluorescence was observed only for the C-terminal tag (Fig. 2a) and could be attributed to the freeing of YPet by proteolytic cleavage. Areas of colocalized cyan and yellow fluorescence that were diffuse/reticular were omitted from the analysis of FRET (see “Experimental Procedures”). In addition to the constructs in which two tags were introduced into a single α1S, we also expressed an α1S-α1S tandem labeled on the N terminus with YPet and on the C terminus with CyPet (YPet-α1S-α1S-CyPet). As well as displaying junctional targeting, all of the constructs illustrated in Fig. 3 were able to restore L-type Ca2+ current and electrically evoked contractions in dysgenic myotubes, although the fraction of contracting cells was lower than reported for α1S constructs tagged only on the C terminus (33). Based on the previous work in which both electrically evoked contractions and whole-cell Ca2+ transients were measured (cf. Table 2 of Ref. 33), this indicates that these doubly labeled constructs restored excitation-contraction coupling of reduced efficiency, with the result that the amount of released Ca2+ was subthreshold for movement in a significant fraction of the expressing myotubes. Thus, all cells in which the doubly tagged constructs produced discrete fluorescent foci were analyzed for FRET.
The Presence of RyR1 Alters FRET between α1S Cytoplasmic Domains
Both functional and structural evidence strongly support the idea that α1S and RyR1 are linked to one another either directly or via intervening proteins. On first principles, one would expect that these functional and structural interactions would involve cytoplasmic domains of α1S. Thus, as already stated, the main goal of the current work was to test whether the presence of RyR1 causes spatial reorganization of the cytoplasmic domains as indicated by altered FRET between fluorescent probes attached to these domains. For this, we calculated the FRET index IY*/IC for each of the doubly tagged constructs both in dyspedic myotubes, where RyR1 is absent, and in dysgenic myotubes where RyR1 is present (Fig. 3). To determine the value of IY*/IC that corresponds to the absence of FRET, we used the construct YPet-α1S-α1S-CyPet, on the assumption that the N- and C termini of adjacent DHPRs would be separated by too great a distance to support FRET. If this is correct, then the IY*/IC ratios calculated for the α1S tandem, which were 0.24 ± 0.03 (n = 35) and 0.26 ± 0.03 (n = 40) for dyspedic and dysgenic myotubes, respectively, should correspond to the absence of FRET for a 1:1 CyPet-YPet stoichiometry. As an experimental test for the absence of FRET, we applied the method of acceptor photobleaching to YPet-α1S-α1S-CyPet expressed in dysgenic myotubes (25). The intensity of CyPet emission (excitation at 440 nm) was the same before and after the photobleaching of YPet by full-power excitation at 515 nm, which supports the assumption that FRET does not occur between the N terminus of the first α1S in the tandem and the C terminus of the second α1S, and that IY*/IC ≈ 0.25 represents the absence of FRET.
Fig. 4 presents a graphical comparison of the IY*/IC values, illustrates how these values depend on the cytoplasmic locations of the donor and acceptor fluorophores, and how they depend on the absence or presence of RyR1. The major results are as follows. First, there was substantial FRET between the N terminus and C terminus (residue 1636), and this did not differ between dyspedic and dysgenic myotubes (Fig. 4c). Thus, the presence of RyR1 did not appear to alter the spatial disposition of the N and C termini with respect to one another and they can thus be considered as “anchor points” to which reorientation of other cytoplasmic domains can be related. Second, there is no detectable FRET between the I-II loop (residue 406) and C terminus in either dyspedic or dysgenic myotubes (Fig. 4e) in that the IY*/IC values differed little from those of YPet-α1S-α1S-CyPet (indicated by the dashed, horizontal line). Third, RyR1 caused the emergence of FRET between the I-II loop and N terminus (Fig. 4a) and caused increased FRET between the II-III loop and N terminus (Fig. 4b). Fourth, RyR1 caused increased FRET between the I-II and II-III loops (Fig. 4d) and decreased FRET between the II-III loop and C terminus (Fig. 4f). Overall, these results suggest that the presence of RyR1 causes an appreciable rearrangement of the α1S cytoplasmic domains.
DISCUSSION
In this work, we have described measurements of FRET on intact muscle expressing α1S constructs in which the fluorescent proteins CyPet and YPet were attached to pairs of cytoplasmic domains. We found that junctional targeting, L-type Ca2+ current, and EC coupling were all preserved for doubly labeled constructs with the fluorescent proteins attached at the N terminus, I-II loop (residue 406, 33 residues downstream of the AID), II-III loop at residue 726 (i.e. within the domain that spans residues 720–765 and is critical for EC coupling), and the C terminus truncated at residue 1636 (Figs. 1–3). When these constructs were expressed in dyspedic myotubes, which lack RyR1, appreciable FRET occurred between the N and C termini, and from the II-III loop to the N terminus, the C terminus, and (to a lesser extent) the I-II loop (Fig. 4). After expression in dysgenic myotubes, in which RyR1 is present, FRET from the N to C terminus was unchanged, from the II-III loop was increased to the N terminus and decreased to the C terminus; for the I-II loop, FRET became measureable to the N terminus and increased to the II-III loop (Fig. 4). Thus, the presence of RyR1 appeared to cause a widespread rearrangement of the cytoplasmic domains of α1S.
Although the changes in FRET are strongly suggestive that the presence of RyR1 causes a reorientation of the α1S cytoplasmic domains, a more specific interpretation in terms of interdomain distances depends upon a number of assumptions that are difficult to test directly. For example, FRET depends not only on distance but also on the donor:acceptor ratio (CyPet:YPet), which we have assumed to be 1:1 for our constructs. However, the “effective” stoichiometry depends upon the extent of maturation (35) of each of the fluorophores and on their local environment (e.g. dielectric constant), which could be differentially affected by the presence or absence of RyR1 and thus affect measured FRET. The presence of RyR1 could also alter FRET by affecting the orientation of the donor and acceptor dipoles with respect to one another (36). In addition to these “generic” concerns, which apply to most studies employing FRET, an issue of specific importance for our studies is the extent to which intermolecular FRET, between neighboring DHPRs, might have contributed to the measured FRET values. It seems likely that the FRET measured in the absence of RyR1 was only intramolecular because DHPRs appear to be randomly oriented in dyspedic myotubes (37). In the presence of RyR1, however, the ordered array of DHPR tetrads (37, 38) could have resulted in an additional, intermolecular component that would have increased total FRET. In principle, this might account for the RyR1-associated increase in FRET between the I-II loop and both the N terminus (Fig. 4a) and II-III loop (Fig. 4b). Relevant to this issue, earlier experiments examined the spatial interrelationships of β1a subunits in DHPR tetrad arrays by analyzing constructs expressed in α1 null myotubes. These experiments failed to detect either intermolecular FRET (39) or bimolecular fluorescence complementation (40) between β1a subunits in adjacent DHPRs. Thus, it was suggested that the adjacent β1a subunits were separated from one another by >10 nm (see Fig. 8 in Ref. 40). If this suggested arrangement is correct, then the I-II loops of α1S also would likely be positioned at a distance >10 nm from the α1S cytoplasmic domains of adjacent DHPRs.
Under the assumption that the FRET we measured was produced intramolecularly and is an indication of proximity, our results can be summarized by the diagram in Fig. 5, which represents a cytoplasmic view of α1S. Because the practical limit for measurable FRET is a donor-acceptor distance of ∼100 Å (36), the diagram illustrates each of the labeled domains surrounded by an ∼50 Å circle and the extent of FRET between any two domains is indicated by the overlap between the circles surrounding those domains. In the absence of RyR1 (overlapping areas indicated in red), the N and C termini are close enough to one another to produce an IY*/IC ratio of 0.54, and, to a slightly lesser degree, the II-III loop is close to both the N and C terminus (IY*/IC ratios of 0.47 and 0.50, respectively). There is less proximity between the I-II and II-III loops (IY*/IC = 0.33, where 0.25 corresponds to the absence of FRET), and the I-II loop is sufficiently far from both the N and C terminus that there was no detectable FRET. The presence of RyR1 causes a significant rearrangement of both the I-II and II-III loops (Fig. 5, overlapping areas indicated in blue). In particular, the II-III loop appears to move away from the C terminus (IY*/IC decreases to 0.39) and toward the N terminus (IY*/IC increases to 0.60), and the I-II loop moves toward both the II-III loop and the N terminus (IY*/IC increases to 0.48 with respect to both). Thus, the overall consequence is that the cytoplasmic domains appear to assume a more compact arrangement when RyR1 is present.
Obviously, Fig. 5 presents an extremely simplified view of the cytoplasmic domains because each of them spans many residues (N terminus, residues 1–51; I-II loop, residues 335–432; II-III loop, residues 662–799; full-length C terminus, residues 1382–1873). Virtually nothing is known about the folding of these domains, but their dimensions would be substantial even if they were folded as compact globular structures (diameters from ∼20 to ∼50 Å). Thus, one would expect that the interdomain distances inferred from FRET would be strongly dependent on the sites of placement of the donor and acceptor fluorophores. Nonetheless, it seems useful to relate the interdomain relationships inferred from FRET with the results of previous studies bearing on these domains and their possible interactions with other junctional proteins.
It remains unknown whether, in vivo, the DHPR and RyR1 contact one another directly, or indirectly via intervening proteins. However, the evidence is compelling that there are structural (5, 6) and functional (7, 8) interactions linking the two. Thus, independent of whether the contacts are direct or indirect, it is valuable to compare our results on RyR1-dependent rearrangements of DHPR cytoplasmic domains with previous work on structural/functional links between the DHPR and RyR1. From this work, it seems unlikely that the N terminus, the smallest domain, interacts structurally or functionally with RyR1 because removal of ∼70% (residues 2–37) has essentially no effect on function (41). In the case of the C terminus, the largest domain, it has been reported that residues 1393–1527 bind to a segment of RyR1 in vitro (24). However, it is unclear whether such binding to RyR1 also occurs in vivo. Specifically, this C-terminal segment is highly conserved in α1C, which appears not bind to RyR1 in vivo because tetrads are not observed after expression of α1C in dysgenic myotubes (13). A second role that has been described for the C terminus is in targeting. In particular, C-terminal residues 1607–1661 (42) have been reported to be important for the targeting of α1S to the junctional membrane, and the mutation V1642D in this region was reported to impair targeting (43). However, we found that targeting of α1S could still occur when a fluorescent protein was attached to the C terminus truncated at 1636. Certainly, some targeting can occur in constructs entirely lacking this region because some restoration of EC coupling, which depends on junctional targeting, was reported to occur for α1S truncated at residue 1542 (43). In any event, it seems unlikely that junctional targeting is a result of the binding of DHPR cytoplasmic domains to RyR1, because α1S targets to junctions in muscle cells null for RyR1 (44). The idea that neither the C terminus (proximal to residue 1636) nor the N terminus bind to RyR1 appears to be consistent with our observation that FRET between the N and C terminus (residue 1636) was not affected by the presence or absence of RyR1 (Fig. 4c).
Based on a number of studies, it is clear that the functional and structural interactions between the DHPR and RyR1 depend on both the II-III loop of α1S and the β1a auxiliary subunit. For example, expression of chimeras containing various combinations of sequence from α1S, α1C, and α1M has shown that the presence of α1S sequence in the II-III loop (roughly, residues 720–765) is required both for skeletal-type EC coupling (16, 45) and for the formation of DHPR tetrads (13). Similarly, expression of different β isoforms in β1 null myotubes from mouse (46) and zebrafish (21) has shown that only β1a is able to restore full, skeletal type EC coupling. A possibility raised by these data is that the II-III loop and/or β1a bind to RyR1. Indeed, in vitro binding of II-III loop residues 720–765 to RyR1 residues 1837–2168 (47) and of β1a to RyR1 (48) have both been reported. As for other instances of in vitro binding of DHPR domains to RyR1, however, it is uncertain that this binding occurs in vivo. In particular, even though some α1S is present in the membrane of β1 null zebrafish muscle cells, it is not arrayed as tetrads (19), indicating that α1S does not bind to RyR1 in the absence of the β subunit. Conversely, in α1S null myotubes, fluorescently tagged β1a does not bind to RyR1 (18) and is freely diffusible (39). Thus, it appears that even though there must be protein-protein contacts linking the DHPR and RyR1, identifying these contacts may not be feasible using isolated components of the DHPR complex. For example, one could imagine that a high affinity interaction required the simultaneous binding of β1a and the α1S II-III loop to RyR1 domains, which form a single binding pocket in three dimensions. If so, it might explain why the FRET results suggest a decreased separation between the I-II loop (to which β1a is attached) and the II-III loop when RyR1 is present (Fig. 4). Interestingly, the larger separation between the I-II and II-III loops in the absence of RyR1 may be represented in the structure of the isolated DHPR determined by electron cryo-microscopy (49), in which β1a appears to be deflected laterally with respect to α1S.
The approach we have employed here, of measuring FRET for doubly tagged α1S constructs expressed in myotubes, is useful because it provides spatial information about functional DHPRs in plasma membrane/SR junctions. However, as already discussed above, this information is necessarily somewhat imprecise. Nonetheless, this information provides obvious directions for future experiments. For example, it will be important to determine whether the interdomain FRET changes in response to depolarization and whether such changes correlate with activation of Ca2+ release via RyR1. Similarly, it will be of interest to determine whether these FRET signals are altered by application of pharmacological agents (e.g. ryanodine, dihydropyridines) or by mutations of α1S and RyR1 that are associated with human muscular disorders.
Acknowledgment
We are indebted to Dr. P. S. Daugherty who provided us with the CyPet and Ypet expression plasmids.
This work was supported by Deutsche Forschungsgemeinschaft Grant PA 801/6-1 (to S. P.) and by National Institutes of Health Grants AR055104 and MDA 176448 (to K. G. B.).
- EC
- excitation-contraction
- DHPR
- dihydropyridine receptor
- RyR1
- type 1 ryanodine receptor
- SR
- sarcoplasmic reticulum
- AID
- α1S interaction domain.
REFERENCES
- 1. Franzini-Armstrong C. (1970) Studies of the triad. I. Structure of the junction in frog twitch fibers. J. Cell Biol. 47, 488–499 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 2. Schneider M. F., Chandler W. K. (1973) Voltage dependent charge movement of skeletal muscle: A possible step in excitation–contraction coupling. Nature 242, 244–246 [DOI] [PubMed] [Google Scholar]
- 3. Tanabe T., Beam K. G., Powell J. A., Numa S. (1988) Restoration of excitation-contraction coupling and slow calcium current in dysgenic muscle by dihydropyridine receptor complementary DNA. Nature 336, 134–139 [DOI] [PubMed] [Google Scholar]
- 4. Inui M., Saito A., Fleischer S. (1987) Purification of the ryanodine receptor and identity with feet structures of junctional terminal cisternae of sarcoplasmic reticulum from fast skeletal muscle. J. Biol. Chem. 262, 1740–1747 [PubMed] [Google Scholar]
- 5. Block B. A., Imagawa T., Campbell K. P., Franzini-Armstrong C. (1988) Structural evidence for direct interaction between the molecular components of the transverse tubule/sarcoplasmic reticulum junction in skeletal muscle. J. Cell Biol. 107, 2587–2600 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 6. Paolini C., Fessenden J. D., Pessah I. N., Franzini-Armstrong C. (2004) Evidence for conformational coupling between two calcium channels. Proc. Natl. Acad. Sci. U.S.A. 101, 12748–12752 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 7. Armstrong C. M., Bezanilla F. M., Horowicz P. (1972) Twitches in the presence of ethylene glycol bis(-aminoethyl ether)-N,N′-tetracetic acid. Biochim. Biophys. Acta 267, 605–608 [DOI] [PubMed] [Google Scholar]
- 8. Dirksen R. T. (2002) Bi-directional coupling between dihydropyridine receptors and ryanodine receptors. Front. Biosci. 7, d659–670 [DOI] [PubMed] [Google Scholar]
- 9. Protasi F., Paolini C., Nakai J., Beam K. G., Franzini-Armstrong C., Allen P. D. (2002) Multiple regions of RyR1 mediate functional and structural interactions with α(1S)-dihydropyridine receptors in skeletal muscle. Biophys. J. 83, 3230–3244 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 10. Sheridan D. C., Takekura H., Franzini-Armstrong C., Beam K. G., Allen P. D., Perez C. F. (2006) Bidirectional signaling between calcium channels of skeletal muscle requires multiple direct and indirect interactions. Proc. Natl. Acad. Sci. U.S.A. 103, 19760–19765 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 11. Tanabe T., Takeshima H., Mikami A., Flockerzi V., Takahashi H., Kangawa K., Kojima M., Matsuo H., Hirose T., Numa S. (1987) Primary structure of the receptor for calcium channel blockers from skeletal muscle. Nature 328, 313–318 [DOI] [PubMed] [Google Scholar]
- 12. Pragnell M., De Waard M., Mori Y., Tanabe T., Snutch T. P., Campbell K. P. (1994) Calcium channel β-subunit binds to a conserved motif in the I-II cytoplasmic linker of the α1-subunit. Nature 368, 67–70 [DOI] [PubMed] [Google Scholar]
- 13. Takekura H., Paolini C., Franzini-Armstrong C., Kugler G., Grabner M., Flucher B. E. (2004) Differential contribution of skeletal and cardiac II-III loop sequences to the assembly of dihydropyridine-receptor arrays in skeletal muscle. Mol. Biol. Cell 15, 5408–5419 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 14. Tanabe T., Beam K. G., Adams B. A., Niidome T., Numa S. (1990) Regions of the skeletal muscle dihydropyridine receptor critical for excitation-contraction coupling. Nature 346, 567–569 [DOI] [PubMed] [Google Scholar]
- 15. Lu X., Xu L., Meissner G. (1994) Activation of the skeletal muscle calcium release channel by a cytoplasmic loop of the dihydropyridine receptor. J. Biol. Chem. 269, 6511–6516 [PubMed] [Google Scholar]
- 16. Nakai J., Tanabe T., Konno T., Adams B., Beam K. G. (1998) Localization in the II-III loop of the dihydropyridine receptor of a sequence critical for excitation-contraction coupling. J. Biol. Chem. 273, 24983–24986 [DOI] [PubMed] [Google Scholar]
- 17. Grabner M., Dirksen R. T., Suda N., Beam K. G. (1999) The II-III loop of the skeletal muscle dihydropyridine receptor is responsible for the bi-directional coupling with the ryanodine receptor. J. Biol. Chem. 274, 21913–21919 [DOI] [PubMed] [Google Scholar]
- 18. Neuhuber B., Gerster U., Döring F., Glossmann H., Tanabe T., Flucher B. E. (1998) Association of calcium channel α1S and β1a subunits is required for the targeting of β1a but not of α1S into skeletal muscle triads. Proc. Natl. Acad. Sci. U.S.A. 95, 5015–5020 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 19. Schredelseker J., Di Biase V., Obermair G. J., Felder E. T., Flucher B. E., Franzini-Armstrong C., Grabner M. (2005) The β1a subunit is essential for the assembly of dihydropyridine-receptor arrays in skeletal muscle. Proc. Natl. Acad. Sci. U.S.A. 102, 17219–17224 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 20. Coronado R., Ahern C. A., Sheridan D. C., Cheng W., Carbonneau L., Bhattacharya D. (2004) Functional equivalence of dihydropyridine receptor alpha1S and beta1a subunits in triggering excitation-contraction coupling in skeletal muscle. Biol. Res. 37, 565–575 [DOI] [PubMed] [Google Scholar]
- 21. Schredelseker J., Dayal A., Schwerte T., Franzini-Armstrong C., Grabner M. (2009) Proper restoration of excitation-contraction coupling in the dihydropyridine receptor beta1-null zebrafish relaxed is an exclusive function of the beta1a subunit. J. Biol. Chem. 284, 1242–1251 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 22. Weiss R. G., O'Connell K. M., Flucher B. E., Allen P. D., Grabner M., Dirksen R. T. (2004) Functional analysis of the R1086H malignant hyperthermia mutation in the DHPR reveals an unexpected influence of the III-IV loop on skeletal muscle EC coupling. Am. J. Physiol. Cell Physiol. 287, C1094-C1102 [DOI] [PubMed] [Google Scholar]
- 23. Bannister R. A., Grabner M., Beam K. G. (2008) The α(1S) III-IV loop influences 1,4-dihydropyridine receptor gating but is not directly involved in excitation-contraction coupling interactions with the type 1 ryanodine receptor. J. Biol. Chem. 283, 23217–23223 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 24. Sencer S., Papineni R. V., Halling D. B., Pate P., Krol J., Zhang J. Z., Hamilton S. L. (2001) Coupling of RYR1 and L-type calcium channels via calmodulin binding domains. J. Biol. Chem. 276, 38237–38241 [DOI] [PubMed] [Google Scholar]
- 25. Papadopoulos S., Leuranguer V., Bannister R. A., Beam K. G. (2004) Mapping sites of potential proximity between the dihydropyridine receptor and RyR1 in muscle using a cyan fluorescent protein-yellow fluorescent protein tandem as a fluorescence resonance energy transfer probe. J. Biol. Chem. 279, 44046–44056 [DOI] [PubMed] [Google Scholar]
- 26. Lorenzon N. M., Beam K. G. (2007) Accessibility of targeted DHPR sites to streptavidin and functional effects of binding on EC coupling. J. Gen. Physiol. 130, 379–388 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 27. Nguyen A. W., Daugherty P. S. (2005) Evolutionary optimization of fluorescent proteins for intracellular FRET. Nat. Biotechnol. 23, 355–360 [DOI] [PubMed] [Google Scholar]
- 28. Knudson C. M., Chaudhari N., Sharp A. H., Powell J. A., Beam K. G., Campbell K. P. (1989) Specific absence of the α1 subunit of the dihydropyridine receptor in mice with muscular dysgenesis. J. Biol. Chem. 264, 1345–1348 [PubMed] [Google Scholar]
- 29. Buck E. D., Nguyen H. T., Pessah I. N., Allen P. D. (1997) Dyspedic mouse skeletal muscle expresses major elements of the triadic junction but lacks detectable ryanodine receptor protein and function. J. Biol. Chem. 272, 7360–7367 [DOI] [PubMed] [Google Scholar]
- 30. Beam K. G., Franzini-Armstrong C. (1997) Functional and structural approaches to the study of excitation-contraction coupling. Methods Cell Biol. 52, 283–306 [DOI] [PubMed] [Google Scholar]
- 31. Hamill O. P., Marty A., Neher E., Sakmann B., Sigworth F. J. (1981) Improved patch-clamp techniques for high-resolution current recording from cells and cell-free membrane patches. Pflugers Arch. 391, 85–100 [DOI] [PubMed] [Google Scholar]
- 32. De Waard M., Witcher D. R., Pragnell M., Liu H., Campbell K. P. (1995) Properties of the α1-β anchoring site in voltage-dependent Ca2+ channels. J. Biol. Chem. 270, 12056–12064 [DOI] [PubMed] [Google Scholar]
- 33. Bannister R. A., Papadopoulos S., Haarmann C. S., Beam K. G. (2009) Effects of inserting fluorescent proteins into the alpha1S II-III loop: insights into excitation-contraction coupling. J. Gen. Physiol. 134, 35–51 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 34. Hulme J. T., Konoki K., Lin T. W., Gritsenko M. A., Camp D. G., 2nd, Bigelow D. J., Catterall W. A. (2005) Sites of proteolytic processing and noncovalent association of the distal C-terminal domain of CaV1.1 channels in skeletal muscle. Proc. Natl. Acad. Sci. U.S.A. 102, 5274–5279 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 35. Tsien R. Y. (1998) The green fluorescent protein. Annu. Rev. Biochem. 67, 509–544 [DOI] [PubMed] [Google Scholar]
- 36. dos Remedios C. G., Moens P. D. (1995) Fluorescence resonance energy transfer spectroscopy is a reliable “ruler” for measuring structural changes in proteins. Dispelling the problem of the unknown orientation factor. J. Struct. Biol. 115, 175–185 [DOI] [PubMed] [Google Scholar]
- 37. Protasi F., Franzini-Armstrong C., Allen P. D. (1998) Role of ryanodine receptors in the assembly of calcium release units in skeletal muscle. J. Cell Biol. 140, 831–842 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 38. Sun X. H., Protasi F., Takahashi M., Takeshima H., Ferguson D. G., Franzini-Armstrong C. (1995) Molecular architecture of membranes involved in excitation-contraction coupling of cardiac muscle. J. Cell Biol. 129, 659–671 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 39. Leuranguer V., Papadopoulos S., Beam K. G. (2006) Organization of calcium channel β1a subunits in triad junctions in skeletal muscle. J. Biol. Chem. 281, 3521–3527 [DOI] [PubMed] [Google Scholar]
- 40. Sheridan D. C., Moua O., Lorenzon N. M., Beam K. G. (2012) Bimolecular fluorescence complementation and targeted biotinylation provide insight into the topology of the skeletal muscle Ca2+ channel β1a subunit. Channels 6, 26–40 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 41. Bannister R. A., Beam K. G. (2005) The α1S N-terminus is not essential for bi-directional coupling with RyR1. Biochem. Biophys. Res. Commun. 336, 134–141 [DOI] [PubMed] [Google Scholar]
- 42. Flucher B. E., Kasielke N., Grabner M. (2000) The triad targeting signal of the skeletal muscle calcium channel is localized in the COOH terminus of the α(1S) subunit. J. Cell Biol. 151, 467–478 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 43. Proenza C., Wilkens C., Lorenzon N. M., Beam K. G. (2000) A carboxyl-terminal region important for the expression and targeting of the skeletal muscle dihydropyridine receptor. J. Biol. Chem. 275, 23169–23174 [DOI] [PubMed] [Google Scholar]
- 44. Takekura H., Franzini-Armstrong C. (1999) Correct targeting of dihydropyridine receptors and triadin in dyspedic mouse skeletal muscle in vivo. Dev. Dyn. 214, 372–380 [DOI] [PubMed] [Google Scholar]
- 45. Kugler G., Weiss R. G., Flucher B. E., Grabner M. (2004) Structural requirements of the dihydropyridine receptor α1S II-III loop for skeletal-type excitation-contraction coupling. J. Biol. Chem. 279, 4721–4728 [DOI] [PubMed] [Google Scholar]
- 46. Beurg M., Sukhareva M., Ahern C. A., Conklin M. W., Perez-Reyes E., Powers P. A., Gregg R. G., Coronado R. (1999) Differential regulation of skeletal muscle L-type Ca2+ current and excitation-contraction coupling by the dihydropyridine receptor β subunit. Biophys. J. 76, 1744–1756 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 47. Proenza C., O'Brien J., Nakai J., Mukherjee S., Allen P. D., Beam K. G. (2002) Identification of a region of RyR1 that participates in allosteric coupling with the α1S (CaV1.1) II-III loop. J. Biol. Chem. 277, 6530–6535 [DOI] [PubMed] [Google Scholar]
- 48. Cheng W., Altafaj X., Ronjat M., Coronado R. (2005) Interaction between the dihydropyridine receptor Ca2+ channel β-subunit and ryanodine receptor type 1 strengthens excitation-contraction coupling. Proc. Natl. Acad. Sci. U.S.A. 102, 19225–19230 [DOI] [PMC free article] [PubMed] [Google Scholar]
- 49. Wolf M., Eberhart A., Glossmann H., Striessnig J., Grigorieff N. (2003) Visualization of the domain structure of an L-type Ca2+ channel using electron cryo-microscopy. J. Mol. Biol. 332, 171–182 [DOI] [PubMed] [Google Scholar]