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1 Department of Physiology and Biophysics, State University of New York, Stony Brook, New York 11794; and 2 Section of Hematology/Oncology, Department of Pediatrics, University of Chicago, Chicago, Illinois 60637-1470
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ABSTRACT |
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Many cardiovascular cells coexpress multiple connexins (Cx), leading to the potential formation of mixed (heteromeric) gap junction hemichannels whose biophysical properties may differ from homomeric channels containing only one connexin type. We examined the potential interaction of connexin Cx43 and Cx40 in HeLa cells sequentially stably transfected with these two connexins. Immunoblots verified the production of comparable amounts of both connexins, cross-linking showed that both connexins formed oligomers, and immunofluorescence showed extensive colocalization. Moreover, Cx40 copurified with (His)6-tagged Cx43 by affinity chromatography of detergent-solubilized connexons, demonstrating the presence of both connexins in some hemichannels. The dual whole cell patch-clamp method was used to compare the gating properties of gap junctions in HeLa Cx43/Cx40 cells with homotypic (Cx40-Cx40 and Cx43-Cx43) and heterotypic (Cx40-Cx43) gap junctions. Many of the observed single channel conductances resembled those of homotypic or heterotypic channels. The steady-state junctional conductance (gj,ss) in coexpressing cell pairs showed a reduced sensitivity to the voltage between cells (Vj) compared with homotypic gap junctions and/or an asymmetrical Vj dependence reminiscent of heterotypic gap junctions. These gating properties could be fit using a combination of homotypic and heterotypic channel properties. Thus, whereas our biochemical evidence suggests that Cx40 and Cx43 form heteromeric connexons, we conclude that they are functionally insignificant with regard to voltage-dependent gating.
heteromeric channel; intercellular communication; ion channel; electrophysiology
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INTRODUCTION |
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GAP JUNCTION CHANNELS are critical for the passage of current between cells in the working myocardium and specialized conducting tissues of the heart. Gap junctions are also present and implicated in the function of other cardiovascular cell types including endothelial cells and vascular smooth muscle cells. A gap junction channel is formed by the meeting of two hemichannels (connexons) located in the plasma membranes of apposed cells. A hemichannel is composed of six subunit proteins [connexins (Cx)]. Several different connexins are expressed in cardiovascular cells, including connexin Cx37, Cx40, Cx43, and Cx45. Each of these connexins can form functional gap junctions by themselves (homomeric/homotypic channels). However, many cells coexpress more than one connexin, suggesting that they might participate in the formation of mixed channels. One specialized mixed channel (a heterotypic channel) could be formed by the pairing of two hemichannels that contain different connexins. A more complicated type of mixing would occur if multiple connexins mixed within the same hemichannel (a heteromeric channel).
Biochemical studies have demonstrated the formation of heteromeric gap junction channels in expression systems and in various mature tissues. Stauffer (35) expressed recombinant Cx32 and Cx26 in insect cells and used gel filtration to detect mixing in detergent-solubilized connexons, whereas Jiang and Goodenough (21) used coimmunoprecipitation to show mixing of Cx46 and Cx50 in the lens. Bevans et al. (4) found heteromeric mixing of Cx26 and Cx32 in the rodent liver when Cx26 was coisolated with Cx32 by affinity chromatography on an anti-Cx32 column. He et al. (18) showed coimmunoprecipitation of Cx40 with Cx43 in A7r5 cells.
The observation of heteromeric forms has lead to speculation that some or all of the biophysical properties of the resultant gap junction channels might be different from homomeric gap junction hemichannels containing only one connexin type. We (5) previously utilized electrophysiological studies of Cx37 and Cx43 cotransfected into N2A cells to show the existence of a population of heteromeric Cx37-Cx43 channels. Dual whole cell patch-clamp analysis of coexpressing cells demonstrated that the voltage dependence was weaker and the range of single channel conductances was broader than could be explained as arising from conventional homotypic or heterotypic gap junction channels. Other studies have suggested that Cx43 and Cx40 can also make heteromeric channels. In A7r5 rat vascular smooth muscle cells, which normally coexpress Cx40 and Cx43, the macroscopic voltage dependence was weaker than that of either homotypic form, and some of the single channel conductances could not be explained easily as homotypic Cx43 or Cx40 forms (18). These authors concluded that the single channel data provided evidence for putative heteromeric Cx40-Cx43 gap junction channels. However, they did not consider heterotypic Cx40-Cx43 channels, whose existence has been subsequently established (37).
A tempting hypothesis is that the disparate properties of heteromeric channels relative to homotypic and/or heterotypic channels could affect multicellular function. For example, in excitable cells (such as the myocytes found in cardiac conducting and pacemaker regions), the type of gap junction channel (homotypic, heterotypic, or heteromeric) could potentially have a profound influence on action potential propagation (22, 34, 37).
The purpose of the current study was to examine biochemically the possible heteromeric mixing of Cx40 with Cx43 and to analyze the electrophysiological properties of gap junction channels formed between cells coexpressing these two connexins. We studied these two connexins because they are abundantly coexpressed in various cells (including atrial myocytes and some endothelial and smooth muscle cells). Double whole cell patch-clamp methods were used to compare the gating properties of channels formed between cells coexpressing Cx40 and Cx43 with those of homotypic Cx40 (Cx40-Cx40) and Cx43 (Cx43-Cx43) and heterotypic Cx43-Cx40 forms.
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MATERIALS AND METHODS |
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Cells and culture conditions. Experiments were carried out using HeLa cells transfected with DNA coding for rat Cx40, rat Cx43, or mouse Cx45. Cx40 or Cx43 DNA was subcloned into the eukaryotic expression plasmid pcDNA3.1/hygro (Invitrogen) or pSFFV-neo (15). Constructs containing a (His)6 tag appended to the Cx43 COOH-terminal were obtained using PCR methods. Cells were stably transfected with linearized DNA using lipofectin (Life Technologies) as described earlier (39). Cells that stably expressed both Cx43 and Cx40 were generated by sequential transfection with the two different expression plasmids. HeLa cells were grown in minimal essential medium supplemented with 10% fetal bovine serum, 0.1 mM nonessential amino acids, 2 mM L-glutamine, 100 U/ml penicillin, and 100 µg/ml streptomycin (Life Technologies). Stable clones were selected by culturing in medium containing 500 µg/ml G418 (Life Technologies) and/or 150 µg/ml hygromycin (Calbiochem). Clones were screened for Cx40 or Cx43 expression by immunofluorescence and immunoblotting. Selected clones were maintained in the medium described above but supplemented with G418 (250 µg/ml) and/or hygromycin (75 µg/ml). For later identification, some cultures were tagged with cell tracker green (5-chloromethyl-fluorescein diacetate; Molecular Probes) (37). Tagged cells expressing one type of connexin and nontagged cells expressing the other type of connexin were mixed and seeded onto sterile glass coverslips placed in multiwell culture dishes (~104 cells/cm2). Electrophysiological measurements were carried out on cells cultured for 1-3 days.
Anti-connexin antibodies. Commercially available mouse monoclonal antibody (Chemicon) directed against amino acids 252-270 of rat Cx43 was used at a dilution of 1:2,000 for immunoblots. Rabbit anti-Cx43 antiserum directed against a bacterially expressed Cx43 fusion protein (29) was used at a dilution of 1:200 for immunofluorescence. Rabbit anti-Cx40 antiserum directed against a bacterially expressed Cx40 carboxyl tail fusion protein (27) was used at a dilution of 1:4,000 for immunoblots. Rabbit polyclonal antibodies directed against a synthetic peptide immunogen corresponding to residues 316-329 of dog Cx40 were affinity purified as described earlier (23) and were used at a dilution of 1:200 for immunofluorescence.
Immunoblot analysis. Protein extracts from cells were prepared as described by Laing and Beyer (28). Aliquots containing 10 µg of protein were separated by SDS-PAGE on 12% polyacrylamide gels and blotted onto Immobilon-P membranes (Millipore). Immunoblots were developed with ECL (or ECL Plus) chemiluminiscence reagents (Amersham Pharmacia Biotech) following the manufacturer's procedures. Peroxidase-conjugated goat anti-rabbit IgG (1:5,000 dilution) or donkey anti-mouse IgG (1:4,000 dilution; Jackson ImmunoResearch Laboratories) was used as the secondary antibody. Rainbow molecular weight marker standards (Amersham Pharmacia Biotech) were used to calibrate the gels.
The abundance of connexin protein in cellular extracts was determined by comparison of the intensity of the reaction product generated from a 10-µg cell sample to a standard curve generated by immunoblotting bacterially expressed fusion proteins containing the carboxyl terminal tail domains of Cx40 or Cx43 linked to His6. The ECL Plus reaction was quantitated using a STORM Phosphorimager. The production of these fusion proteins has been described previously (27, 29). The minimum linear levels of detection were 5 and 20 ng for the Cx40 and Cx43 fusion proteins, respectively (data not shown).Chemical cross-linking. Cross-linking of connexins in unfractionated HeLa cell lysates was performed as described by Musil and Goodenough (32). Cells were lysed in 1% Triton X-100 in PBS at 4°C and then centrifuged at 100,000 g for 30 min at 4°C. Supernatants containing connexons (hexamers) were reacted with 2 mM disuccinimidyl suberate (DSS; Pierce) or DMSO for 30 min. Samples were quenched with 50 mM Tris (pH 7.5) for 15 min at 4°C, run on 7% SDS-polyacrylamide gels, and then blotted as described above.
Purification of His6-tagged proteins. His6-tagged proteins were purified from Triton X-100-solubilized supernatants using nickel-nitrilotriacetic acid (Ni-NTA) resin (Qiagen) as described by the company in the protocol for batch purification under native conditions with the following few modifications. To reduce nonspecific binding, the Ni-NTA resin was blocked for 15 min with 2.5% bovine serum albumin in lysis buffer; the concentration of imidazole in the lysis buffer was reduced to 1 mM, and all buffers contained 1% Triton X-100. Triton-extracted protein samples were incubated with resin for 2 h at 4°C. For protein analysis, 4-15% gradient SDS-polyacrylamide gels were run and immunoblotted as described above.
Immunofluorescent labeling of cells. Cells cultured on multiwell slides were stained as described earlier (30). CY3-conjugated goat anti-mouse or anti-rabbit IgG antibodies (Jackson ImmunoResearch Laboratories) were used as secondary antibodies. In double-labeling experiments, cells were incubated simultaneously with both anti-Cx43 monoclonal antibody and anti-Cx40 polyclonal antibody and then with secondary antibodies consisting of fluorescein-conjugated goat anti-mouse IgG (1:50 dilution) and CY3-conjugated anti-rabbit IgG (1:800 dilution) as described earlier (30).
Solutions. During experiments, the cells were superfused with bath solution containing (in mmol/l) 110 CsCl, 5 KCl, 2 CaCl2, 1 MgCl2, and 10 HEPES (pH 7.4). The patch pipettes were filled with saline containing (mmol/l) 110 CsCl, 0.1 MgCl2, 0.1 CaCl2, 3 EGTA, and 10 HEPES (pH 7.2).
Electrical measurements.
Glass coverslips with adherent cells were transferred to an
experimental chamber perfused with bath solution at room temperature (21-23°C). The chamber was mounted on the stage of an inverted microscope (Olympus IMT2). Patch pipettes were pulled from glass capillaries (code 7052, A-M Systems) with a horizontal puller (Sutter
Instruments). The resistance of the filled pipettes measured 1-1.5
M
. Experiments were carried out on mixed cell pairs. A dual
voltage-clamp method and whole cell recording were used to control the
membrane potential of both cells and to measure currents (6,
36). Each cell was attached to a patch pipette connected to a
separate micromanipulator (WR-88, Narishige Scientific Instruments) and
amplifier (Axopatch 200). Initially, the membrane potentials of
cell 1 and cell 2 were clamped to the same value:
the voltage of cell 1 (V1) = the
voltage of cell 2 (V2).
V2 was then changed to establish a
transjunctional voltage (Vj) = V2
V1. Currents recorded from cell 2 represent the sum of two components,
the junctional current (Ij) and the membrane
current of cell 2; the current obtained from cell
1 corresponds to Ij. To measure
Ij, both cells were held at the same holding
potential (Vh), i.e., Vh = 0 mV. The voltage of one of the cells
was then stepped to different levels (37). A bipolar pulse
protocol was used as described previously (5, 33). The
amplitudes of Ij were determined at the
beginning [instantaneous Ij
(Ij,inst)] and at the end of each pulse
[steady-state Ij
(Ij,ss)] to estimate the instantaneous and
steady-state conductances (gj,inst and
gj,ss, respectively). Because the "apparent
instantaneous" current rapidly decays with larger
Vj, gj,inst and
gj,ss were normalized with respect to a 10-mV
prepulse conductance (constant with time). We used this as our standard
for gj,inst and gj,ss
normalization. We used Ij,ss or
gjss to indicate junctional current or
conductance at the 400-ms or 10-s time points, where
gjss represents an approximation of the steady state.
Signal recording and analysis. Voltage and current signals were recorded on chart paper (Gould RS 2400, Gould Instruments) and videotape (Neurocorder DR-384, Neuro Data Instruments). For off-line analysis, the current signals were filtered at 1 kHz (low-pass filter), digitized with a 12-bit analog-to-digital converter (DT21EZ, Data Translation), and stored with a personal computer. Data acquisition and analysis were performed with custom-made software (6, 25). Curve fitting and statistical analysis were performed using SigmaPlot and SigmaStat (Jandel Scientific), respectively. Macroscopic conductances were compared using the Mann-Whitney rank sum test. Unless otherwise noted, data are presented as means ± SE. Single channel currents were studied in low-conductance cell pairs as previously described (5, 6, 12, 36, 37). The single channel data were fit using the analytical approach of Kullman (26).
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RESULTS |
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Double expression of Cx40 and Cx43 in HeLa transfectants. The properties of channels formed by cloned connexins can be examined by their exogenous expression in transfected HeLa cells, because these cells are virtually communication deficient. To examine the properties of Cx40 and Cx43 channels alone and after potential mixing with each other, we generated HeLa cell lines that were stably transfected with Cx40 or Cx43 alone (HeLa Cx40 and HeLa Cx43) or with both Cx43 and Cx40 (HeLa Cx43/Cx40) with the use of two different selectable markers. To facilitate isolation of expressed connexins, we also prepared a Cx43 construct in which a His6 tag was appended to the carboxyl terminus. We isolated HeLa clones expressing the His6-tagged Cx43 alone [HeLa Cx43(His)] or with Cx40 [HeLa Cx43(His)/Cx40].
The production of the transfected connexins was confirmed immunologically. As expected from previous studies (17, 20, 37), immunofluorescent staining of the parental HeLa cells showed no reaction with anti-Cx40 or anti-Cx43 antibodies (data not shown). In contrast, anti-Cx40 antibodies localized to appositional membranes (as expected for gap junctions) and perinuclear regions (likely within the protein synthesis/export pathway) in both HeLa Cx40 cells (Fig. 1A) and HeLa Cx43/Cx40 cells (Fig. 1, C and E). Anti-Cx43 antibodies showed a very similar staining pattern in HeLa Cx43 cells (Fig. 1B), HeLa Cx43(His) cells (data not shown), and HeLa Cx43/Cx40 cells (Fig. 1, D and F). Cx40 and Cx43 showed virtually identical intercellular and gap junctional distributions with double-label immunofluorescence in the coexpressing cells (Fig. 1, E and F).
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Voltage dependence of Cx43/Cx40 gap junction currents. Homotypic Cx40 or Cx43 channels have been characterized in primary cell cultures (36) and in transfected cells (1, 6, 8, 37). The formation of heterotypic channels containing Cx40 and Cx43 has been more recently demonstrated and analyzed (37).
Macroscopic intercellular currents (Ij) were examined in 32 pairs of HeLa cells double transfected with Cx43 and Cx40 (HeLa Cx43/Cx40). In 27 preparations, the cells were coupled by gap junctions (see Table 1). Analysis of these cell pairs yielded a gap junction conductance (gj) of 14.3 ± 1.1 nS. The remaining five cell pairs contained cytoplasmic bridges. To distinguish between gap junctions and cytoplasmic bridges, the preparations were uncoupled by exposure to CO2 (10). The average junctional conductance of coexpressing HeLa Cx43/Cx40-HeLa Cx43/Cx40 cell pairs was less than that of either homotypic form (14.3 vs. 24.8 or 20.5 nS for HeLa Cx43-HeLa Cx43 and HeLa Cx40-HeLa Cx40, respectively) despite the similar abundances of Cx40 and Cx43 in the cotransfected cells relative to the singly transfected cells (Fig. 3). The heterotypic Cx40-Cx43 junctional conductance determined by Valiunas et al. (37) was 6.8 nS, which is a similar value to our new data obtained for HeLa Cx43/Cx40-HeLa Cx40 and HeLa Cx43/Cx40-HeLa Cx43 pairs (Table 1).
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83/72 mV, voltage-insensitive
component of gj
(gj,min) = 0.33/0.28, and gating charge
(z) =1.5/1.6, for negative/positive
Vj, respectively. For the longer
duration data (5 preparations), Boltzmann fits (continuous dashed line
in Fig. 6E) yielded the following values: Vj,0 =
72/66 mV,
gj,min = 0.28/0.23, and z = 1.7/1.8, for negative/positive Vj, respectively.
When compared with the respective homotypic Cx40-Cx40 and Cx43-Cx43
channels under the same conditions (400-ms pulse protocol), the gap
junctions from pairs of doubly transfected (HeLa Cx43/Cx40) cells
exhibited a broader voltage sensitivity
(Vj,0 = 56 and 66 mV for Cx40-Cx40 and
Cx43-Cx43, respectively) (37).
Plots from three asymmetrical cases obtained using the short pulse
protocol are shown in Fig. 6F. The
gj,ss declined in a sigmoidal fashion to a
quasistable level at a Vj of ~150 mV when Vj was made negative, and, in contrast, it
decreased gradually without reaching a plateau at positive
Vj. The continuous curves in Fig. 6F
at negative values of Vj represent the best fit
of the data to the Boltzmann equation using the following parameters: Vj,0 =
104 mV,
gj,min = 0.29, maximum
gj (gj,max) = 1.02, and z = 1.7. In the case of the long pulse protocol, a
Boltzmann fit (continuous dashed line in Fig. 6F) yielded
the following parameters: Vj,0 =
76 mV,
gj,min = 0.27, gj,max = 1.0, and z = 2.5. The pronounced asymmetry of the gj,ss = f(Vj ) relationship implies the
existence of more than one population of channels distributed between
cell pairs. The currents and the relationship between
Vj and gj from asymmetrical cases resembled heterotypic Cx40-Cx43 channel currents and
their gj-Vj relationship
(37).
From the data shown here, we conclude that the 400-ms step duration and
10-s step duration give qualitatively similar results: symmetric or
asymmetric current-voltage relationships. We refrained from assuming
the 400-ms data are representative of the steady state, but rather we
used the same pulse duration to compare the behavior of the different
channel types.
Voltage dependence of Cx43/Cx40-Cx40 and Cx43/Cx40-Cx43 gap junction currents. We cocultured cotransfected cells (HeLa Cx43/Cx40) with singly transfected cells (HeLa Cx40 or HeLa Cx43). This strategy allowed us to observe channels in which one hemichannel potentially contained two connexin types but the other contained only a single connexin (was homomeric) to determine whether this configuration would distinguish heteromeric forms from homotypic or heterotypic channnels.
Like the pairs of double-transfected HeLa Cx43/Cx40 cells, recordings from these mixed cell pairs consisting of one HeLa Cx43/Cx40 cell and one HeLa Cx40 or HeLa Cx43 cell revealed quasisymmetrical and asymmetrical gap junction currents. Figure 7, A and B, shows data obtained from mixed pairs of HeLa Cx43/Cx40 and HeLa Cx40 cells. Figure 7A, top, illustrates an example with quasisymmetrical Ij, and Fig. 7B, top, shows asymmetrical Ij. In the former case, the gj,ss = f(Vj) relationship was nearly bell shaped and tended to symmetry. In the latter case, it was strongly asymmetrical.
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71/92
mV; gj,min = 0.39/0.28, gj,max = 1.01/1.06, and z = 2.2/0.7, for negative/positive Vj, respectively.
In this case, negative Vj indicates positive
potential inside the HeLa Cx40 cell.
The three most pronounced asymmetrical cases are summarized Fig.
7B, bottom. It shows the normalized relationships
gj,inst versus
f(Vj) and
gj,ss versus
f(Vj). Both plots were strongly asymmetrical. The gj,inst increased when the
cell expressing Cx40 was made positive inside and decreased when it was
made negative. The increase in gj,inst peaked at
~1.29 at Vj =
150 mV. The decrease in
gj,inst reached a value of ~0.94 at
Vj = 150 mV. In contrast, the
gj,ss declined when the Cx40 cell was made
positive. It decreased in a sigmoidal fashion to a quasistable level at
a Vj of ~
150 mV. When the HeLa Cx40 cell was
made negative, gj,ss decreased moderate without
reaching a plateau, i.e., it closely followed gj,inst. The continuous curves in Fig.
7B at negative values of Vj represent
the best fit of the data to the Boltzmann equation using the following
parameters: Vj,0 =
103 mV,
gj,min = 0.33, gj,max = 1.03, and z = 2.2.
Both the relationships gj,inst = f(Vj) and
gj,ss = f(Vj) for the asymmetric cases were
similar to those obtained from heterotypic Cx40-Cx43 gap junctional
channels (37). The kinetics of current inactivation and
Vj polarity dependence were also reminiscent of
heterotypic Cx40-Cx43 channels.
Figure 7D summarizes the results of 12 experiments where
Ij was symmetric for the HeLa Cx43/Cx40-HeLa
Cx43 cell pair configuration. The continuous curve in Fig.
7D corresponds to the best fit of the data to the Boltzmann
equation using the following values: Vj,0 =
82/87 mV; gj,min = 0.26/0.42,
gj,max = 1.04/1.05, and z = 1.3/1.0, for negative/positive Vj, respectively.
When the HeLa Cx43 cell was negative inside (negative
Vj), gj was 0.26; in
contrast, stepping the inside of the HeLa Cx43 cell to positive yielded
a gj of 0.42.
Time- and conductance-dependent transition from asymmetric to
symmetric voltage dependence.
The total gap junction conductance between cell pairs often declined
with time. As already indicated, the degree of asymmetry of
Ij was variable and dependent on total gap
junction conductance. In some cases, the changes of total gap junction
conductance between cell pairs led to transformation from asymmetrical
currents to symmetrical ones. This was observed for all cell types
investigated (i.e., HeLa Cx43/Cx40-HeLa Cx43/Cx40, HeLa Cx43/Cx40-HeLa
Cx40, and HeLa Cx43/Cx40-HeLa Cx43). Figure
8, A and B,
illustrates an example of a mixed HeLa Cx43/Cx40-HeLa Cx40 cell pair.
At the beginning of the measurements, the total conductance of the cell pair was ~3 nS (Fig. 8A, top). Stepping
Vj to make the inside of the HeLa Cx40 cell
positive resulted in a large Ij,inst with pronounced inactivation. Conversely, stepping Vj
to make the inside of the HeLa-Cx40 cell negative led to a smaller
Ij,inst with marginal or no inactivation. When
spontaneous total conductance dropped to ~2 nS,
Ij became more symmetrical (Fig. 8A,
bottom).
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Properties of Cx43/Cx40-Cx45 gap junction currents. The gating properties of heteromeric Cx43/Cx40 channels were difficult to distinguish from homotypic forms of Cx40 or Cx43 and heterotypic Cx40-Cx43. This prompted us to try to unmask heteromeric gating by pairing Cx45-expressing HeLa cells with HeLa Cx43/Cx40 cells. The bipolar pulse protocol was used to study multichannel currents from a HeLa Cx43/Cx40-HeLa Cx45 cell pair (Fig. 8C). Stepping Vj to make the inside of the HeLa Cx45 cell negative or the inside of the HeLa Cx43/Cx40 cell positive resulted in an Ij,inst with pronounced inactivation. Conversely, stepping Vj to make the inside of the HeLa Cx45 cell positive and the inside of the HeLa Cx43/Cx40 cell negative led to an Ij,inst with distinct activation.
Figure 8D shows the results from five cell pairs. The plots represent the normalized relationships gj,inst versus Vj and gj,ss versus Vj. The gj,inst decreased slightly when the cell expressing Cx45 was made negative. The gj,ss increased when the HeLaCx45 cell was made positive inside and decreased when it was made negative. Note that gj was far from steady state at the end of the 400-ms pulse applied (see Fig. 8C). The continuous curves in Fig. 8C at positive values of Vj represent the best fit of data to the Boltzmann equation using the following parameters: Vj,0 =
59 mV,
gj,min = 0.05, gj,max = 1.01, and z = 2.9.
The currents and conductances of the HeLa Cx43/Cx40-HeLa Cx45 cell
pairs behaved similarly to HeLa Cx40-HeLa Cx45 and HeLa Cx43-HeLa Cx45
cell pairs [see Valiunas et al. (37)] with regard to
Vj dependence, gating polarity, current
patterns, kinetics of inactivation, and the presence of activation of
Ij. The data shown here support the conclusion
of Valiunas et al. (37): that Cx45 gates negatively.
Simulation of macroscopic gap junction conductance involving Cx40 and Cx43 channels. We modeled our data to examine whether the gj = f(Vj) relationship for cells cotransfected with Cx40 and Cx43 could be explained under some conditions where only heterotypic and homotypic channels were present.
In Fig. 9A, we attempted to fit the averaged steady-state symmetric data (shown in Fig. 6C) assuming different proportions of homotypic Cx43 and Cx40 channels and heterotypic Cx40-Cx43 channels. In Fig. 9A, the solid line represents a smooth curve fit to the actual data obtained from symmetrically behaving HeLa Cx43/Cx40 cell pairs. The other curves in Fig. 9A represent the predicted results [using actual data from Valiunas et al. (37)] where the percentages of homotypic and heterotypic channels were varied. For the heterotypic population, we assumed that the two possible polarities (Cx43-Cx40 and Cx40-Cx43) always existed in equal amounts. The dashed dotted line in Fig. 9A (with the closest fit to our data) represents the results predicted by the case where 70% of the channels were heterotypic (35% of each polarity) and 15% were homotypic Cx43-Cx43 and 15% were homotypic Cx40-Cx40. The short dashed line in Fig. 9A represents the results predicted by the case where 30% of the channels were heterotypic (15% of each polarity) and 35% were homotypic Cx43-Cx43 and 35% were homotypic Cx40-Cx40. The two extremes shown represent the cases where 100% of the channels were heterotypic (50% of each polarity, long dashed line in Fig. 9A) or 100% were homotypic (50% Cx40 and 50% Cx43, dotted line in Fig. 9A).
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Conductances of single channels.
To study single channel currents, we selected cell pairs with one or
two to three operational channels. The pulse protocol adopted involved
an inversion of the Vj polarity. Figure
10 illustrates experiments in weakly
coupled pairs or in normally coupled pairs after advanced spontaneous
uncoupling. Figure 10, A-C, shows data from HeLa
Cx43/Cx40-HeLa Cx40 cell pairs, and Fig. 10, D-F, shows data from HeLa Cx43/Cx40-HeLa Cx43/Cx40 cell pairs.
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j,main and
j,residual of 109 and 18 pS, respectively. These
data are similar to what we observed for heterotypic Cx40-Cx43
channels, which exhibit a unitary channel conductance of 100 pS for the
main state (
j,main) and 14-20 pS for the residual
state (
j,residual) when the Cx40 side is negative
(37).
Figure 10D shows single channel activity during short (400 ms) biphasic Vj of 110 mV. The current analysis
revealed the following conductances (arrows in Fig. 10D):
inward current, 143, 106, and 45 pS; and outward current, 60 and 62 pS.
These conductances may be interpreted as follows: 143 pS, Cx40
homotypic; 106 pS, Cx40-Cx43 heterotypic; 45 pS, heteromeric, substate,
or endogenous; and 60 and 62 pS, Cx40-Cx43 heterotypic.
Figure 10, E and F, shows single channel records
obtained from Cx40/Cx43 cell pairs at a maintained
Vj of 50 and 60 mV, respectively. In the former
case, current histograms revealed conductance states corresponding to
44 and 105 pS; these may correspond to a heterotypic Cx40-Cx43 channel
(105 pS) and an unknown channel (endogenous/possibly heteromeric). In
Fig. 10F, histograms revealed peaks yielding conductance levels of 32, 49, and 78 pS; these values could be interpreted as
follows: 78 pS, homotypic Cx43-Cx43 channel; 49 pS, unknown homotypic
channel (homomeric or heteromeric, because there is no
Vj polarity dependence, characteristic of
heterotypic channels); and 32 pS, substate, endogenous or heteromeric.
The data shown in Fig. 10 represent the spectrum of conductive states
observed from HeLa Cx43/Cx40-HeLa Cx43/Cx40 cotransfectant pairs and
partial heterotypic HeLa Cx43/Cx40-HeLa Cx40 pairs. Data were collected
from many records, because in each individual single channel recording,
the likelihood of observing multiple conductance states was low. The
conductance values obtained from single channel records were sampled in
5-pS bins and plotted as frequency histograms. Figure
11 shows the histograms for HeLa
Cx43/Cx40-HeLa Cx43/Cx40 pairs (Fig. 11A, 6 cell pairs) and
heterotypic HeLa Cx43/Cx40-HeLa Cx40 cell pairs (Fig. 11B, 5 cell pairs). The single channel data yielded a complex distribution in
both cases. In the case of cotransfected HeLa Cx43/Cx40-HeLa Cx43/Cx40
pairs, the data were best fitted by five Gaussians using the analytical
approach of Kullmann (26) with the following conductances:
37 ± 6, 59 ± 6, 75 ± 4, 98 ± 7, and 128 ± 8 pS. Fitting of the data from the partial heterotypic HeLa
Cx43/Cx40-HeLa Cx40 cell pairs yielded four Gaussians. The four
conductive states were as follows: 33 ± 5, 58 ± 8, 102 ± 8, and 131 ± 5 pS. Thus the histogram from HeLa Cx43/Cx40-
HeLa Cx43/Cx40 cotransfectants (Fig. 11A) contains one more
peak than the data from HeLa Cx43/Cx40-HeLa Cx40 cell pairs (Fig.
11B). The missing conductive state in Fig. 11B is
~75 pS, which is similar to homotypic Cx43 in our experimental
conditions (pipette solution, 110 mM CsCl; temperature, 22°C).
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DISCUSSION |
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The potential physiological consequences of formation of mixed channels by Cx40 and Cx43 may have importance for understanding cardiovascular function, because these two proteins are coexpressed in a number of cell types. Conflicting data have been published regarding the heterotypic and heteromeric interactions of these proteins. The initial electrophysiological observations suggested that Cx40 and Cx43 did not interact to form heterotypic channels in Xenopus oocytes (7, 41). Other studies performed in HeLa cell transfectants utilized dye injection (14) or the induction of channels in approximated cells (17). Unfortunately, these approaches may not have allowed detection of heterotypic channel formation, because later studies by Valiunas et al. (37) revealed that Cx40 and Cx43 do form functioning heterotypic gap junction channels in transfected HeLa and RIN cells.
Recently, He et al. (18) have argued for functional mixing of Cx40 and Cx43. They studied A7r5 rat vascular smooth muscle cells, which normally coexpress Cx40 and Cx43. The macroscopic voltage dependence that they detected in these cells was weaker than that produced by either homotypic form, and some of the observed single channel conductances could not be readily explained as homotypic Cx43 or Cx40 forms. These authors concluded that their data provided evidence for heteromeric Cx40/Cx43 gap junction channels. However, they did not consider the possible existence of heterotypic Cx40-Cx43 channels, which we (37) recently detected and studied.
In the present study, we extensively analyzed the biochemical properties of HeLa cells coexpressing Cx40 and Cx43. Immunoblotting experiments showed that cells produced both Cx40 and Cx43 proteins, and quantitation of immunoblots showed that the cotransfected cells produced very similar amounts of the two proteins. Immunofluorescence microscopy showed that both Cx40 and Cx43 localized to virtually identical cell surface locations, consistent with their participation in the same gap junctions. Cotransfected cells were disrupted with Triton X-100 under conditions that solubilize connexons (hexameric hemichannels); chemical cross-linking of this material showed that both Cx40 and Cx43 formed oligomers in these cells. Finally, when the Triton X-100 extracts were affinity purified using Ni-NTA-Sepharose, Cx40 copurified with Cx43(His); this result implied that Cx43(His)-containing connexons also contained Cx40. Thus our cotransfected cells abundantly expressed both Cx40 and Cx43 and contained biochemically detectable heteromeric connexons. Our data extend the data of He et al. (18), who showed coimmunoprecipitation of Cx40 with Cx43 from A7r5 cells, and support their conclusion of heteromeric mixing. One caveat of both studies is that they are based on Triton X-100 solubilization, which has become a standard procedure to examine connexon assembly (3, 24, 32). However, this is not a quantitative procedure; moreover, as noted in earlier studies by Musil and Goodenough (31), some cellular connexin (including some material in gap junction plaques) is not solubilized by this procedure. Much of the Triton X-100-solubilized material may derive from connexons within the assembly/export pathway and from hemichannels and channels that have not been incorporated into plaques. An assumption is that the mixing of connexins to form heteromers is similar in the synthetic pathway and in the plasma membrane.
We also extensively analyzed the electrophysiological properties of HeLa cells coexpressing Cx40 and Cx43. Our double whole cell patch-clamp data are less striking than might have been anticipated in suggesting unique electrophysiological properties conferred by heteromeric mixing.
One of our findings was that in HeLa cell pairs with one or more member coexpressing Cx40 and Cx43, the junctional conductance was substantially less than in pairs where each cell was transfected with only a single connexin (Table 1). For example, the junctional conductance of the cotransfected HeLa Cx43/Cx40 cell pairs (14.3 nS) was only 56-66% of the conductance obtained in homotypic Cx40 or Cx43 cell pairs. These results are somewhat surprising compared with our connexin protein data. The HeLa Cx43/Cx40 cell pairs were prepared by transfecting Cx40 into the same HeLa Cx43 cell clone used for the homotypic studies. Thus the HeLa Cx43/Cx40 cells contain indistinguishable amounts of Cx43 compared with the HeLaCx43 cells plus the introduction of a similar amount of Cx40 (Fig. 3). We might have expected an increased (approximately doubled) conductance in the HeLa Cx43/Cx40 pairs. The observed reduction cannot be due to impaired trafficking of Cx43 produced by introduction of Cx40, because both connexins were detected in similar plasma membrane locations (Fig. 1). Therefore, it must be that some of the heteromeric Cx43/Cx40 connexons are nonfunctional as hemichannels or are unable to pair with other connexons to make functionally complete gap junctional channels.
We observed even further reduced conductances in the partial heterotypic cell pairs formed when HeLa Cx43/Cx40 cells were paired with cells expressing only Cx40 or Cx43 (14.3 vs. 7.6-8.0 nS; Table 1). These data suggest a reduced efficiency of channel formation/function for the heterotypic channel.
The single channel data are equivocal in terms of distinguishing between homotypic, heterotypic, and heteromeric forms. Many of the single channel events that we observed in pairs of HeLa Cx43/Cx40 cells were similar to ones that we detected in homotypic or heterotypic pairs of HeLa Cx40 and/or HeLa Cx43 cells; a relatively small number of events were unique. The conductances that are dissimilar from homotypic or heterotypic forms provide the strongest argument for heteromeric channel types, but interpretation of these data is unclear, because these events may also represent substates of any of the gap junction channels present or involvement of an endogenous connexin (such as Cx45). [In studies of cardiac myocytes, Elenes et al. (13) suggested that Cx45 might facilitate interactions of Cx40 and Cx43.] Thus the data do not unequivocally demonstrate unique conductances that can be defined as heteromeric Cx43/Cx40. Moreover, it is quite possible that heteromeric Cx43/Cx40 channels have similar or identical conductances to the homomeric/homotypic or homomeric/heterotypic forms, as speculated by Hopperstad et al. (19). These data differ from our previous observations of many different single channel events when Cx43 and Cx37 were coexpressed; this difference suggests the possibility that less functional heteromeric channels are formed between Cx40 and Cx43 than between Cx37 and Cx43.
Brink et al. (5) calculated that 196 different gap junction channel forms are potentially formed when two connexins are equally coexpressed and have similar affinities for each other. In contrast, the maximum number of conductive forms would be only 14 for a pair between a cell coexpressing two connexins and a partner cell expressing only a single connexin (and therefore containing only homomeric connexons). Therefore, one expectation might be that the event histogram of channel conductances for the cotransfectant cell pairs (HeLa Cx43/Cx40 paired with HeLa Cx43/Cx40) would show more conductive states than are detected between HeLa Cx43/Cx40 and HeLa Cx40 cells. The data shown in Fig. 11 qualitatively meet this criterion; however, in fact, there is only one additional conductive state demonstrable for the cotransfectant pairs relative to the HeLa Cx43/Cx40-HeLa Cx40 cell pairs. The conductive state missing in the HeLa Cx43/Cx40-HeLa Cx40 cell pairs is in the range of 75 pS, which is similar to homotypic Cx43 observed under our conditions (37). There are two alternative possible explanations for these data. First, it is possible that virtually all of the channels in the cotransfectants are heteromeric, but they function similarly to homotypic and heterotypic Cx43 and Cx40 channels. The conductances of the heteromers might not be distinguishable. Any of the peaks in the channel event histograms could represent multiple channel populations with similar or identical conductances but with very different connexin composition. Second, alternatively, it is possible that there is only a small population of heteromeric forms, which are not easily detected with our analysis; functional heteromer formation might be rare.
Interestingly, most, if not all, of the conductances in both histograms corresponded to conductances that are similar to the homotypic and heterotypic forms of Cx43 and Cx40. The least conductive peak in both histograms (33 and 37 pS) might represent channel activity of heteromeric forms. However, we cannot exclude involvement of subconductive states of either Cx40 or Cx43 channels or endogenous Cx45 channels.
Our new data regarding Vj dependence are consistent with previous reports (5, 18) utilizing cotransfected cell pairs in which the voltage dependence of coexpressing cells was shown to be broadened or less sensitive than the equivalent homotypic forms. We found that the junctional conductances observed in cells cotransfected with Cx40 and Cx43 showed weaker voltage dependence than their homotypic counterparts. A subset of cell pairs showed asymmetric voltage dependence similar to heterotypic Cx40-Cx43 channels. Similar observations were made in cell pairs where one hemichannel of the gap junction was homomeric (Cx40 or Cx43) and the other hemichannel was a cotransfected cell (HeLa Cx43/Cx40). Such cases with asymmetrical Vj dependence (as in Fig. 7, B and C) exhibited gating polarities corresponding to heterotypic Cx40-Cx43 channel gating polarities (37).
We tried to explain our data by fitting them with a combination of homotypic and heterotypic forms. The summarized data and fits shown in Fig. 9 do not distinguish between two possible situations where 1) the majority of the channels are heteromeric and behave like homotypic and/or heterotypic channels, or 2) there is only a small heteromeric channel population and the total junctional conductance is dominated by homotypic and heterotypic channel types. Such conclusions are also supported by the data from Cx45-Cx43/Cx40 gap junctions (Fig. 8, C and D). Interestingly, the macroscopic properties observed were indistinguishable from heterotypic/homomeric gap junction channels, i.e., the recorded currents, their Vj dependence, and gating polarities (Fig. 8, C and D) corresponded closely with those of heterotypic Cx40-Cx45 or Cx43-Cx45 gap junctions (37).
In terms of voltage gating, either the heteromeric hemichannel forms follow the behavior of their homomeric hemichannel counterparts or the heteromeric forms are functionally nonexistent.
It is possible that heteromeric mixing has a more profound influence on other properties of gap junction channels. For example, Gu et al. (16) presented data suggesting that the carboxyl tail of Cx43 can modulate the pH-dependent gating of Cx43 when the two connexins are coexpressed in Xenopus oocytes. Thus chemical gating is a potentially important physiological parameter with regard to heteromers. It is also possible that heteromeric Cx43/Cx40 channels might have altered permeability properties, because the two connexins individually form channels with some differences in permeability and selectivity (1, 2, 11, 38, 40), but a detailed characterization of these permeability/selectivity properties requires a full study of its own.
In summary, our data from expression of two major cardiac connexins (Cx40 and Cx43) in HeLa cells show biochemically that the two connexins can mix to form heteromeric connexons. However, reduced total conductances between pairs of coexpressing cells suggest that some heteromeric channels may be nonfunctional. Other electrophysiological analyses suggest that most properties of these cells can be understood based on the properties of homomeric and heterotypic channels. Single channel data revealed conductances that were consistent with the dominant channel forms being homomeric/homotypic or heterotypic-like. Moreover, studies of the cotransfected HeLa Cx43/Cx40 cells yielded gj,ss = f(Vj) relationships that could be explained on the basis of homotypic and heterotypic channels alone, although the qualifier is that a high percentage of heterotypic channel types (between 30% and 70%) would be necessary to approximate the data. A related point is our observation that junctional conductances were initially asymmetrically voltage dependent but became symmetrically dependent as junctional conductance was reduced (Fig. 8, A and B). This is consistent with the presence of at least two distinct populations of voltage-dependent channels, one symmetric and other asymmetric. Thus either 1) heteromeric forms are the most prevalent channel type and have gating properties similar to heterotypic and homotypic channels, or 2) the population of functional heteromeric channels is so low that their gating behavior cannot be detected apart from the combination of homotypic and heterotypic channels. In either case, the heteromeric channels do not make a distinguishable contribution to voltage-dependent gating.
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ACKNOWLEDGEMENTS |
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The authors acknowledge the expert technical assistance of Laima Valiuniene. The authors thank Dr. K. Willecke for the HeLa Cx45 cells.
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FOOTNOTES |
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This work was supported by National Institutes of Health Grants GM-55263 (to P. R. Brink), HL-59199 (to E. D. Beyer), and HL-45466 (to E. C. Beyer) and a grant from the Bear Necessities Pediatric Cancer Research Foundation (to J. Gemel).
V. Valiunas was on sabbatical from the Institute for Biomedical Research, Kaunas Medical University, Eiveniu 4, LT-3007 Kaunas, Lithuania
Address for reprint requests and other correspondence: E. C. Beyer, Sect. of Pediatric Hematology/Oncology, Univ. of Chicago MC4060, 5841 S. Maryland Ave., Chicago, IL 60637-1470 (E-mail: ebeyer{at}peds.bsd.uchicago.edu).
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
Received 12 March 2001; accepted in final form 28 June 2001.
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