The delayed potassium rectifier current, IKs, is composed of KCNQ1 and KCNE1 subunits and plays an important role in cardiac action potential repolarization. During β-adrenergic stimulation, 3′-5′-cyclic adenosine monophosphate (cAMP)-dependent protein kinase A (PKA) phosphorylates KCNQ1, producing an increase in IKs current and a shortening of the action potential. Here, using cell-attached macropatches and single-channel recordings, we investigate the microscopic mechanisms underlying the cAMP-dependent increase in IKs current. A membrane-permeable cAMP analog, 8-(4-chlorophenylthio)-cAMP (8-CPT-cAMP), causes a marked leftward shift of the conductance–voltage relation in macropatches, with or without an increase in current size. Single channels exhibit fewer silent sweeps, reduced first latency to opening (control, 1.61 ± 0.13 s; cAMP, 1.06 ± 0.11 s), and increased higher-subconductance-level occupancy in the presence of cAMP. The E160R/R237E and S209F KCNQ1 mutants, which show fixed and enhanced voltage sensor activation, respectively, largely abolish the effect of cAMP. The phosphomimetic KCNQ1 mutations, S27D and S27D/S92D, are much less and not at all responsive, respectively, to the effects of PKA phosphorylation (first latency of S27D + KCNE1 channels: control, 1.81 ± 0.1 s; 8-CPT-cAMP, 1.44 ± 0.1 s, P < 0.05; latency of S27D/S92D + KCNE1: control, 1.62 ± 0.1 s; cAMP, 1.43 ± 0.1 s, nonsignificant). Using total internal reflection fluorescence microscopy, we find no overall increase in surface expression of the channel during exposure to 8-CPT-cAMP. Our data suggest that the cAMP-dependent increase in IKs current is caused by an increase in the likelihood of channel opening, combined with faster openings and greater occupancy of higher subconductance levels, and is mediated by enhanced voltage sensor activation.
The repolarization phase of the cardiac action potential is dominated by the activity of two K+ currents, IKs and IKr (Sanguinetti and Jurkiewicz, 1990). At normal heart rates, IKs plays the lesser role, but at high heart rates and during stress, the current is up-regulated and the rate of deactivation is slowed (Terrenoire et al., 2005). This increase in IKs leads to a repolarization reserve, which shortens the action potential duration and allows for adequate ventricular filling (Stengl et al., 2003; Jost et al., 2005; Silva and Rudy, 2005).
IKs is the product of the coassembly of the Kv7.1 voltage-gated potassium channel (KCNQ1 [Q1]) with the KCNE1 (E1) β-subunit. The coassembly of E1 with Q1 causes notable changes in channel kinetics, converting a rapidly activating current into one with very slow activation and deactivation kinetics, and in which inactivation is altogether abolished. In addition, overall current amplitude is increased upon E1 coassembly (Takumi et al., 1988; Barhanin et al., 1996; Sanguinetti et al., 1996; Tristani-Firouzi and Sanguinetti, 1998). Mutations in Q1 or E1 can cause cardiac arrhythmias such as long QT and short QT syndromes and familial atrial fibrillation (Moss et al., 1991; Chen et al., 2003; Bellocq et al., 2004). Long QT mutations lead to a lengthening of the action potential because the amount of repolarizing IKs is reduced (Wang et al., 1996; Splawski et al., 2000). Because of the importance of IKs at high heart rates, many individuals with these mutations display symptoms when their heart rates are elevated—for example, while exercising or when under stress (Wit et al., 1975).
Response to stressful situations—for example, fight or flight—involves sympathetic nervous system activation via β-adrenergic receptors (β-ARs). This triggers a signaling cascade, which leads to phosphorylation of Q1 and an increase in IKs current. The β-ARs are coupled to heterotrimeric G-proteins that release GTP-bound α-subunits to activate the downstream effector, adenylyl cyclase 9 (Cumbay and Watts, 2004; Piggott et al., 2008; Dessauer, 2009). Activating adenylyl cyclase 9 increases the level of intracellular cAMP, which in turn activates cAMP-dependent protein kinase A (PKA). PKA is brought into the macromolecular complex and in close proximity to Q1 by Yotiao (A-kinase anchoring protein 9 [AKAP-9]), which allows PKA to phosphorylate the residue Ser27 (Fig. 1; Chen et al., 2005; Piggott et al., 2008; Li et al., 2012). Yotiao also anchors protein phosphatase 1 (PP1), which is key for regulation of β-AR stimulation of IKs (Fig. 1; Marx et al., 2002).
The full range of mechanisms behind the increase in IKs current after β-adrenergic stimulation is not fully understood. Phosphorylation of channels is known to cause a hyperpolarizing shift of the half-activation potential (V1/2), where the IKs channels open at more negative membrane potentials (Dilly et al., 2004; Terrenoire et al., 2005). Along with this is an increase in the rate of activation and a decrease in the rate of deactivation (Terrenoire et al., 2005), which increases IKs by allowing a buildup of open channels during successive depolarizations. As well, increases in current could be caused by a change in the number of channels at the cell surface. This has been seen to be the case for other ion transporters, such as the Na+/K+-ATPase pump, which shows increased translocation to the plasma membrane during cAMP stimulation (Gonin et al., 2001).
Here, we aimed to study the mechanisms by which β-adrenergic stimulation increases the IKs current at the microscopic ion channel level. From our prior work, we now understand that IKs channels do not occupy a single open state but transition through five or six open levels during activation of the channel complex, and only reach an open probability (Po) of ∼0.15–0.2 at 60 mV, even during prolonged depolarizations (Werry et al., 2013; Eldstrom et al., 2015; Murray et al., 2016). Once current reaches a stable level, channel activity is characterized by preferential occupancy of two or three relatively higher subconductance states while the channel pore opens in long bursts with frequent brief closings. By using a membrane-permeant cAMP analog, 8-CPT-cAMP, we can look for modulation of the single-channel kinetics in cell-attached patches. Up-regulation of voltage sensor domain (VSD) function is expected to cause changes in the first latency to opening or an increased Po that would underlie reported whole-cell findings such as the hyperpolarizing shift of the conductance–voltage (G-V) relationship. In addition, we hypothesize that PKA phosphorylation can facilitate single-channel gating and induce changes in substate occupancy that further increase single-channel currents.
Materials and methods
To activate PKA inside cells, membrane-permeable cAMP was used in the form of 8-(4-chlorophenylthio)adenosine 3′,5′-cyclic monophosphate sodium salt (Sigma-Aldrich). To maintain activation of PKA after stimulation, okadaic acid (OA) was used to inhibit PP1 and PP2A phosphatases (EMD Millipore). To ensure that channels under study were indeed IKs, chromanol 293B was used as a selective blocker (Tocris Bioscience).
KCNQ1 and KCNE1 constructs were bought from OriGene. Throughout the article, Q1 and E1 are used as abbreviations for KCNQ1 and KCNE1, respectively. Q1 S209F was constructed from the KCNQ1 gene using a two-step PCR reaction (Eldstrom et al., 2010). Q1 S27D was a gift from the laboratory of N. Schmitt of the University of Copenhagen (Copenhagen, Denmark). Yotiao (AKAP-9) was a gift of R. Kass of Columbia University (New York, NY) and was inserted into a pcDNA3 vector. The E160R/R237E (E1R/R4E) and S27D/S92D KCNQ1 mutants were gifts from J. Cui of Washington University (St. Louis, MO). The EQ construct forces a 4:4 KCNQ1:KCNE1 stoichiometry to IKs and was constructed by tethering the C terminus FLAG tag on KCNE1 and a V5 epitope on KCNQ1, plus an additional 21 aa (SRGGSGGSGGSGGSGGSGGRS) after the FLAG-tag sequence (Murray et al., 2016). Sequencing confirmed all mutations.
Cell culture and transfections
For single-channel recordings, Itk– mouse fibroblast (LM) cells were used. They were plated to a confluence of 10–20% on sterile glass coverslips. These cells were transfected using Lipofectamine 2000 (Thermo Fisher Scientific) and with DNA ratios of 1:3:1.5:1 of KCNQ1, KCNQ1-S209F, KCNQ1-S27D, or KCNQ1-S27D/S92D:KCNE1:AKAP-9:GFP. For some experiments, E1-GFP was used to reduce the number of transfected plasmids. The cells were grown in MEM with 10% FBS (Gibco) and incubated in air/5% CO2 at 37°C. All recordings were done at room temperature, 24–48 h posttransfection.
For total internal reflection fluorescence (TIRF) microscopy, Chinese hamster ovary (CHO) cells were grown in DMEM/F12 (Thermo Fisher Scientific) supplemented with 10% FBS, 100 IU/ml penicillin, and 100 µg/ml streptomycin (Thermo Fisher Scientific). Cells were cultured at 37°C in an air/5% CO2 incubator. 1 d before transfection, cells were rinsed with 1× PBS (Thermo Fisher Scientific), lifted via 3-min exposure to trypsin-EDTA (Thermo Fisher Scientific), and replated on 35-mm2 glass-bottom microdishes (Ibidi). The cells were transiently transfected using Lipofectamine 2000 according to the manufacturer’s protocol. KCNE1-mCherry was coexpressed with KCNQ1-GFP and AKAP-9 in a 4:1:1 ratio. Cells were imaged 24–48 h after transfection.
Methods for single-channel recordings were previously published (Werry et al., 2013; Eldstrom et al., 2015). Whole-cell recordings were performed and patch electrodes were fabricated as previously described (Murray et al., 2016). Data were collected and analyzed using Axopatch hardware and pCLAMP 10.5 software (Molecular Devices).
IKs channels in CHO cells were visualized at ∼27°C with TIRF microscopy as described previously (Boycott et al., 2013). Cells were imaged for 15 or 30 min, with 200 µM 8-CPT-cAMP added to the bath after 5 or 15 min, respectively.
For single-channel recordings, the solution in the bath contained 135 mM KCl, 1 mM MgCl2, 1 mM CaCl2, and 10 mM Hepes and was adjusted to pH 7.4 with KOH. The solution in the patch pipette contained 6 mM NaCl, 129 mM MES, 1 mM MgCl2, 10 mM Hepes, 5 mM KCl, and 1 mM CaCl2 and was adjusted to pH 7.4 with NaOH. For whole-cell recordings, the solution in the bath contained 135 mM NaCl, 5 mM KCl, 1 mM MgCl2, 2.8 mM NaAcetate, and 10 mM Hepes, pH adjusted to 7.4 with NaOH. The solution in the pipette contained 130 mM KCl, 5 mM EGTA, 1 mM MgCl2, 4 mM Na2-ATP, 0.1 mM GTP, and 10 mM Hepes, pH adjusted to 7.2 with KOH. For TIRF microscopy, the external solution contained 135 mM NaCl, 4 mM KCl, 2 mM MgCl2, 2.5 mM Na-pyruvate, 1 mM Na2HPO4, 20 mM d-glucose, and 10 mM Hepes, pH adjusted to 7.4 with NaOH.
For TIRF microscopy imaging, overall fluorescence intensity of the cells was measured using Xcellence software (Olympus). Fluorescence of specific regions of interest (ROIs) was quantified using ImageJ with the Time Series Analyzer v3 plugin (National Institutes of Health).
G-V relations were acquired from normalized tail current amplitudes. Fitting the data from each cell with a Boltzmann sigmoidal function allowed us to obtain the V1/2 values. Data analysis was done using Prism 7 (GraphPad Software). Single-channel current records were acquired at 2 kHz and digitized using Digidata 1440A hardware (Molecular Devices). For presentation and for all-points histograms (unless otherwise stated), data were filtered at 200 Hz. To compile events lists, data were filtered at 500 Hz and idealized using the Single-Channel Search function in Clampfit. Cursors were set between capacity transients at the beginning and end of the test pulse. Levels were set to 0, 0.145, 0.22, 0.33, 0.5, and 0.75 pA, and the “update level automatically” function was disabled. The program automatically detects each event and is then added to the events worksheet from which idealized amplitudes can be extracted. The final mean amplitudes of events at each sublevel are returned by the program (see legend to Fig. 5). Only events longer than 1.5 ms in duration were used in the analysis. A short section of current idealization shown in Fig. S8 B.
Results reported here are expressed as mean ± SE and represent data from at least three independent experiments. The median value and 95% confidence intervals are also reported for first-latency data. To compare control and cAMP-treated cells, nonparametric Mann–Whitney test was used (GraphPad Software). The statistically significant threshold was set at 0.05 or less. Gaussian fits and single-channel analysis were performed using Clampfit. Nonlinear regressions were used on G-V relations using the Boltzmann sigmoidal function in Prism 7.
Online supplemental material
Figs. S1 and S2 show Q1 + E1 single-channel data before and after cAMP. Fig. S3 shows V1/2 changes in macropatches before and after cAMP of EQ and S27D + E1. Figs. S4 and S5 show a detailed subconductance and kinetic analysis of S27D + E1. Fig. S6 shows whole-cell data of S209F + E1 before and after cAMP. Fig. S7 shows further analysis of the TIRF data focusing on ROIs and how those change after cAMP addition. Fig. S8 shows a snapshot of the idealization process used for subconductance analysis in Fig. 5 and Fig. S4.
The 8-CPT-cAMP–induced increase in
IKs current is seen at room temperature
It is not possible to resolve the kinetics of single-channel IKs currents at 37°C because of the rapid shifts between subconductance levels and the need to keep noise levels extremely low. Thus, experiments were done at room temperature (20–22°C). To confirm that the expected β-adrenergic modulation of IKs was still present at these temperatures in our hands, we first used whole-cell recording to look at the effect of 8-CPT-cAMP on macroscopic IKs currents.
Q1 was transiently transfected with E1 and Yotiao into a mouse fibroblast cell line, and whole-cell currents were recorded (Fig. 2). Representative currents during a 4-s pulse to 60 mV before (control) and after 200 µM 8-CPT-cAMP (Fig. 2 A) show that IKs increased significantly even at room temperature. The time course of the increase in peak current is illustrated in the diary plot (Fig. 2 B). There was an initial decrease in current as the 8-CPT-cAMP was added to the bath, and then a delayed onset as it permeated across the membrane, followed by a progressive increase in current amplitude.
The characteristic sigmoidal shape of IKs current activation is shown in the representative traces in Fig. 2. Apart from the increased current size apparent in the current–voltage (I-V) relationship (Fig. 2 C), the mean G-V curve (Fig. 2 D), obtained from analysis of the tail currents, hyperpolarized after the addition of 8-CPT-cAMP (V1/2 changed from 28 to 10.5 mV; Fig. 2 D). Saturation of current activation occurred at less-depolarized voltages in the presence of 8-CPT-cAMP compared with control (Fig. 2 D). This indicates that a major action of 8-CPT-cAMP phosphorylation is to increase the macroscopic channel Po at more negative membrane potentials. These results also show that, at room temperature, we are still able to see the classic effect of 8-CPT-cAMP on the IKs current.
IKs to cAMP in cell-attached recordings
In cell-attached recordings, an EQ tandem construct was used to force a 4:4 KCNQ1:KCNE1 IKs stoichiometry and ensure that the channel complex was fully saturated with E1. This construct has been previously characterized by Murray et al. (2016); in the present experiments, single channels were found to be modulated by 8-CPT-cAMP in the same manner as Q1+E1 expressed separately (Figs. S1 and S2). Cell-attached macropatch recordings were made from multiple channels under the pipette tip. 8-CPT-cAMP addition caused a hyperpolarizing shift in the V1/2 of activation for EQ and E1+Q1 (Fig. 3 A and Fig. S2 A), also seen at the whole-cell level with Q1+E1 (Fig. 2 D). This shift increased with longer exposure to 8-CPT-cAMP, with a mean hyperpolarizing shift of −25 ± 8.5 mV in the V1/2 of activation (Fig. S3 A). Deactivation appears to also be affected by the addition of 8-CPT-cAMP, as the macropatch tail currents decay more slowly (Fig. 3 A, insets). Of six macropatches for EQ and Q1+E1, two showed an increase in the amplitude of cell-attached macropatch currents.
IKs single-channel kinetics in the presence of 8-CPT-cAMP
8-CPT-cAMP stimulation affected single-channel properties of IKs in a number of ways, as illustrated in Figs. 3 and 4. Characteristically, in control, IKs single-channel currents have a long first latency, and once they appear, channels flicker rapidly in bursts with infrequent longer closings (Figs. 3 B and 4 A). After 200-Hz filtering, single-channel openings peak at less than 0.5 pA with only one active channel present. The all-points histogram of amplitude events from 21 active of 100 sweeps peaked at 0.38 pA with evidence of only a single channel present despite tens of thousands of opening events (Fig. 3 C, left). Similar results were seen in 100 control sweeps from a second patch (single sweep histogram shown in Fig. 4 B). However, after the administration of 8-CPT-cAMP, an increase in the current amplitude was observed from just under 0.5 pA to 1.5 pA (Fig. 3 B) and up to 2.5 pA in Fig. 4 B (bottom). An additional event peak was seen in the histogram of the 47 active 8-CPT-cAMP sweeps at 0.75 pA, and the range of the histogram included events at 1.5–2.0 pA, suggesting that there were now two to three channels active in the patch (Fig. 3 C, right). Data from the patch shown in Fig. 4 suggest that there were now approximately six channels active after addition of 8-CPT-cAMP (Fig. 4 B, bottom). In the presence of the selective blocker chromanol 293B, this increased current was almost abolished, suggesting that it arose from the presence of more active IKs channels. In the bottom panel of Fig. 3 B, ensemble averages are shown of the current in all 100 control, 79 8-CPT-cAMP, and 38 chromanol 293B sweeps. The mean current was much greater when 8-CPT-cAMP was present and least when chromanol 293B was added. Overall, in 20 initially single-channel EQ or E1+Q1 patches in control, there was an increase in the apparent number of active channels in nine exposed to 8-CPT-cAMP.
The amplitude of single-channel openings appeared unchanged in the presence of 8-CPT-cAMP. For EQ, the mean single-channel conductance in control was 2.9 pS and unchanged after cAMP. For E1+Q1, the mean single-channel conductance in control was 2.7 pS and 2.8 pS after 8-CPT-cAMP. These values are close to the single-channel conductance of 3.2 pS reported by Werry et al. (2013). Ensemble average (93 sweeps) currents at 60 mV from a single-channel patch before and after cAMP are shown in Fig. 4 C. There is an increase in peak ensemble current from 0.04 to 0.12 pA in the presence of 8-CPT-cAMP, which corresponds to an increase in Po from 0.12 to 0.27 in this patch, and agrees quite well with the ∼2.5-fold increase in whole-cell current at 60 mV shown in Fig. 2 C.
A consistent increase in the number of active sweeps occurred in the presence of 8-CPT-cAMP and is clearly seen in the latency histogram (Fig. 4 D). In control, 43 of 367 sweeps were active (black line), whereas in 8-CPT-cAMP, 69 sweeps of 345 were active (red line). The mean first latency of EQ IKs channels was measured from patches in which only a single channel was found to be present, even after exposure to 8-CPT-cAMP, and was 1.61 ± 0.13 s in control. It was significantly shortened upon 8-CPT-cAMP addition to 1.06 ± 0.11 s (Fig. 4 D and Table 1; P = 0.0005, n = 3). These numbers correlate well with the first latency of E1 and Q1 expressed separately (Fig. S1 C; and Table 1) and favorably with changes in the activation time course of EQ macropatches. The time to half-activation at 60 mV was reduced from 1.04 to 0.65 s (n = 4) with 8-CPT-cAMP, a 37% reduction, compared with the 34.2% decrease in first latency for EQ after 8-CPT-cAMP addition (Table 1).
Changes in substate occupancy in the presence of 8-CPT-cAMP are primarily VSD activation effects
In patches with no increase in the number of active channels, we analyzed the occupancy of the subconductance levels of the single channel present in control and after 8-CPT-cAMP addition. During the idealization process (Materials and methods and Fig. S8), we assumed that 8-CPT-cAMP did not change the subconductance amplitude levels reached in control, just the occupancy of these levels. The computer-defined event amplitudes usually clustered closely around these preset levels. The results of this analysis on sweeps from two different EQ patches are shown in Fig. 5, 26 active sweeps before, and 25 sweeps after the addition of 8-CPT-cAMP. The results illustrate the occupancy of five defined EQ IKs substate levels (0.145–0.75 pA). In Fig. 5 A, the raw all-points histograms for control (blue) and 8-CPT-cAMP (red) are overlaid. The initial peak, or level 0, is the closed state (0 pA). It can already be clearly seen that the area of the envelope to the right of the 0 pA peak, corresponding to channel openings, is greater after exposure to 8-CPT-cAMP (red) than control (blue).
The idealized histograms of the subconductance analysis for control (blue) and 8-CPT-cAMP (red) show the grouping of opening events into the five subconductance levels (Fig. 5 B). We have already established that the 0.29- and 0.44-pA sublevels when data are filtered at 0.2 kHz are the most frequently occupied upper open levels (Werry et al., 2013). The present data were filtered at 0.5 kHz, and in Fig. 5 (B and C), the 0.33- and 0.5-pA levels are the most frequently visited upper open levels, accounting for 2.6% and 3.1% of the total dwell time, respectively. In the presence of 8-CPT-cAMP, there is a clear shift of occupancy away from the closed state to the higher subconductance opening levels. For example, 2.6% of events occurred at the 0.33-pA sublevel in control, but after 8-CPT-cAMP addition, this almost doubled to 4.5%. The 0.5-pA level also saw an increase in the number and doubling in the proportion of events from 3.1 to 7.6%, and the 0.75-pA sublevel increased from 0.8 to 1.7%. The first latencies to opening of each of the six sublevels before and after 8-CPT-cAMP also showed a trend to shorter times to reach each of the levels in the presence of 8-CPT-cAMP, although it was not statistically significant. Similar results were seen in two other EQ or Q1+E1 patches, indicating that phosphorylation of IKs leads to more frequent high-subconductance-state occupancy, consistent with the increased current levels observed at the microscopic and macroscopic levels.
An analysis of EQ burst kinetics in controls and in the presence of 8-CPT-cAMP is shown in Fig. 6. Bursts of channel openings such as those shown in Fig. 4 and Fig. S1 are largely outside the VSD-driven activation pathway (Werry et al., 2013) and allow us to examine the effects of 8-CPT-cAMP on pore kinetics of EQ. After idealization of 26 control and 25 8-CPT-cAMP 4-s sweeps, we found two resolvable closed states for EQ with similar time constants to those we reported previously in Werry et al. (2013). In the presence of cAMP, there is no change in the mean closed time for the vast majority of events. For the longer closed time, there was an increase, but there are few events for this fit (Fig. 6 A). Interestingly, the closed dwell times of EQ in 8-CPT-cAMP are very close to those reported for S209F + E1 in Eldstrom et al. (2015). A probability plot of the closed dwell time distribution shows clearly how the burst closing kinetics are unaffected by 8-CPT-cAMP (Fig. 6 B). Peaks of the closed dwell time distribution at ∼2 and 10 ms are very similar in both control and 8-CPT-cAMP.
The table in Fig. 5 C shows a measure of the mean dwell times at each sublevel; they were relatively unchanged in the presence of 8-CPT-cAMP, with some dwell times increasing and some decreasing. The data give an indication of the time the channel spent bursting at a particular sublevel before moving to a higher or lower subconductance level. A more formal analysis of overall open burst durations was performed using a burst termination criterion of pore closing for >2 ms. The event histograms were fitted as the sum of two decay exponentials, the faster of which accounted for >90% of bursts and had time constants of 2.9 ± 0.07 ms in control and 2.5 ± 0.09 ms in 8-CPT-cAMP. The burst duration probability functions are shown together in Fig. 6 C and appear unaffected by cAMP addition (Fig. 6 C). In fact, there is a small but significant decrease in the number of bursts at intermediate dwell times in the presence of 8-CPT-CAMP. Overall, these data suggest that 8-CPT-cAMP has only minor effects, both positive and negative, on channel pore kinetics.
8-CPT-cAMP effects on
IKs mutants described as having fixed and activated VSDs
E160R/R237E (E1R/R4E) KCNQ1, a charge reversal mutant suggested to lock the voltage sensors in an upward position and stabilize the position of the VSD (Wu et al., 2010; Zaydman et al., 2014), was used to further test the action of 8-CPT-cAMP by isolating VSD-induced changes in the channel complex and allowing a direct test on pore kinetics. In controls, when E1R/R4E is coexpressed with KCNE1 (Fig. 7, A–C, left), at 40 mV channels opened without any latency and burst throughout 4-s sweeps, as well as during repolarization to −40 and −80 mV. The ensemble average current (Fig. 7 A, middle) was time-independent compared with WT IKs (Fig. 3 B) and unaffected by 8-CPT-cAMP, but still sensitive to chromanol 293B (Fig. 7 A, bottom).
All-points histograms reveal a distribution of openings with the major event peak at ∼0.35 pA at this potential. The mean single channel conductance was 3.2 pS and was unchanged in the presence of 8-CPT-cAMP (n = 5). These values may be compared with a conductance of 2.9 pS in EQ channels before and after exposure to cAMP (see Fig. 4 legend). The histograms show that the effect of cAMP in the same single-channel patch was to decrease the closed-state occupancy without significantly changing numbers of events at the higher-subconductance-occupancy levels shown in Fig. 7 C at ∼0.55 pA. As a result, there was little effect on the ensemble current (Fig. 7 A, middle). These changes are in contrast to the shortened latency to opening and occupancy of higher sublevels seen in EQ channels (Figs. 4 and 5) and increased EQ and E1+Q1 ensemble currents (Fig. 4 C and Fig. S2 B) during exposure to 8-CPT-cAMP. Similar results have been observed in four other E1R/R4E patches.
KCNQ1 S209F is a gain-of-function mutation found in the S3 domain of the VSD (Eldstrom et al., 2010) and is like E1R/R4E in that it has a saturated Po over a wide potential range. S209F+E1 has been previously characterized as having a much higher open probability than that of WT IKs, (Po = 0.6 compared with 0.15 in WT after 4 s at 60 mV; Werry et al., 2013; Eldstrom et al., 2015), with dominant residency in higher subconducting open states. At room temperature, whole-cell experiments on S209F revealed that it possesses almost voltage-independent gating when expressed with E1 (Fig. S6 A). Currents are fairly time independent, and the Po shows only a small decrease negative to −50 mV (Fig. S6 B). No effect of 8-CPT-cAMP on G-V relationships or current amplitude was seen at the whole-cell level (Fig. S6, B and C).
Because this mutant already has activated and equilibrated VSD gating, it can provide a good test of cAMP on pore kinetics at positive potentials. Data in Fig. 8 A show single sweeps of S209F+E1 at 60 mV. From these representative traces, it can be seen that the channel opens with little latency but still sometimes occupies lower sublevels before reaching higher subconductance states. The single-channel currents for S209F before and after 8-CPT-cAMP appear to be very similar and show that the time the channel is open is greatly increased compared with that of EQ (Figs. 3 B and 4 A), but perhaps less than E1R/R4E, as judged by the relative number of closed events in the all-points histograms (Fig. 8 B).
The active peaks of the raw histograms higher than 0.4 pA enclose a much larger number of events than the closed events peak (compare with EQ or WT Q1+E1; Fig. 3 C and Fig. S1 B). There is not much difference in the numbers of closed events before and after cAMP, but there is a shift of open events from lower to higher open subconductance levels in S209F in the presence of cAMP and an increase in the amplitude corresponding to the event peak of the histogram. Before addition of 8-CPT-cAMP, the event peak amplitude was 0.38 pA, and after, 0.42 pA (Fig. 8 B). As in whole-cell data, there was no change in ensemble average single-channel currents at 60 mV (Fig. 8 C) and 0 mV (not depicted) after exposure to 8-CPT-cAMP, with a calculated Po of 0.71 at 60 mV (control) and 0.74 (8-CPT-cAMP; Fig. 8 C). S209F first latency was markedly reduced compared with that of WT Q1+E1. In S209F patches in control, first latency was 0.16 ± 0.05 s, and upon 8-CPT-cAMP addition, actually lengthened to 0.18 ± 0.056 s, although the median value declined (Fig. 8 D; and Table 1). There was also no increase in the number of active sweeps and no recruitment of new or silent channels upon 8-CPT-cAMP administration, such as that seen with EQ or WT Q1+E1 (Figs. 3 B and 4 B and Fig. S2 C).
Both E1R/R4E and S209F are mutations described as having fixed and activated VSDs, and our data indicate that their overall gating is relatively unaffected by 8-CPT-cAMP, which suggests that the actions of 8-CPT-cAMP on the channel complex are mediated principally via the voltage sensor domains.
Effect of 8-CPT-cAMP on the pseudo-phosphorylated
IKs channel mutants S27D and S27D-S92D
The Ser27 residue in Q1 is a phosphorylation site known to be important in the response of IKs to β-AR stimulation (Fig. 1; Kurokawa et al., 2003), and S27D is a phosphomimetic mutant that recapitulates most of the effects seen with phosphorylation of IKs. However, the S27D+E1 macropatch data still showed a hyperpolarizing shift in the V1/2 of activation after 8-CPT-cAMP addition, as shown in Fig. 9 A (−15.4 mV). The mean hyperpolarization in S27D macropatches in the presence of 8-CPT-cAMP was from 13.1 to −1.1 mV (−14.3 mV, n = 3; Fig. S3 B), compared with a hyperpolarization from 27.0 to 2.1 mV (−24.9 mV) for EQ (n = 4; Fig. S3 A). Deactivation also appeared to be slowed when 8-CPT-cAMP was added (Fig. 9 A, insets). The single-channel recordings are shown in Fig. 9 B, and there were more subtle changes in the kinetics with 8-CPT-cAMP than seen in EQ channels. The all-points histograms showed a relative reduction of closed-state occupancy and a small shift of open events to higher subconductance amplitudes (Fig. 9 C). The amplitude of the single-channel events peak was unchanged though, as all-point histograms of 11 active control and 11 active 8-CPT-cAMP sweeps were fitted with an event peak at 0.365 pA in control and 0.361 pA with 8-CPT-cAMP/OA (Fig. 9 C). As might be expected from the all-points histograms, there was little change in ensemble average currents at 60 mV (Fig. 9 D) in S27D after exposure to 8-CPT-cAMP, with a calculated Po of ∼0.33 in control and 8-CPT-cAMP.
The detailed changes in subconductance occupancy were analyzed after data idealization, and results are shown in Figs. S4 and S5. It is of note that the closed dwell time in S27D as a proportion of the total in control (78%) is very similar to that seen in EQ after exposure to 8-CPT-cAMP (78.8%; Fig. 5 C). However, there is a reduction of closed-state occupancy and a shift of subconductance occupancy to all the higher sublevels after cAMP/OA exposure. The first latency was also still significantly shortened by the addition of 8-CPT-cAMP (Fig. 9 E), from 1.81 ± 0.13 to 1.44 ± 0.11 s (Table 1; P = 0.032), and overall, these changes after cAMP are very similar to those seen in EQ and E1+Q1 channels but are attenuated as expected in this mutant. There were few changes in the burst kinetics in the S27D mutant after exposure to 8-CPT-cAMP (Fig. S5).
Ser92 is also a potential phosphorylation site in the N terminus of KCNQ1 (Lopes et al., 2007) that has been shown to increase IKs current (Lundby et al., 2013), and thus we were prompted to test the effects of 8-CPT-cAMP/OA on the double-mutant S27D/S92D-Q1 channel (Fig. 10). Surprisingly, the G-V relationship was slightly depolarized from the WT IKs relationship, rather than hyperpolarized, but there was no further change upon exposure to 8-CPT-cAMP. There was no change in peak whole-cell currents with cAMP, and no change in single-channel peak event amplitudes or latency kinetics, although we did not perform a subconductance analysis (Fig. 10, C and D). The mean first latency in control was 1.62 ± 0.08 s and was not significantly different in the presence of 8-CPT-cAMP, at 1.43 ± 0.13 s (Table 1; P = 0.332). These results suggest that almost all of the kinetic effects of 8-CPT-CAMP on IKs channels are mediated via phosphorylation of these two residues, Ser27 and Ser92.
Effect of 8-CPT-cAMP on the surface expression of WT
To investigate whether the recruitment of WT IKs channels in the single-channel patches and whether an increased current density at the whole-cell level could be in part because of an increase in channels present at the cell surface, total internal reflection fluorescence (TIRF) microscopy was used to allow visualization of channels within 80 nm of the surface of the cell and monitor channel trafficking (Schwarzer et al., 2013; Yamamura et al., 2015).
CHO cells transfected with WT KCNQ1-GFP and WT KCNE1-mCherry were recorded for a period of 15–30 min, and 200 µM 8-CPT-cAMP was added at 5 min. TIRF images of KCNQ1-GFP and KCNE1-mCherry at 0 and 15 min, respectively, are shown in Fig. 11 (A and C); 8-CPT-cAMP was added at 5 min. After measuring the fluorescence intensity of the whole cell, there does not appear to be an increase in the overall surface expression of KCNQ1-GFP or KCNE1-mCherry after the addition of 8-CPT-cAMP (Fig. 11, B and D). This indicates that addition of cAMP does not increase the net trafficking of IKs to the cell surface.
It was clear from observation of the KCNQ1-GFP fluorescence signals over the time frame of 15–30 min that the channels are highly mobile in both the presence and absence of 200 µM 8-CPT-cAMP (Fig. S7 A). Some ROIs did show a decrease or an increase (Figs. S7, A and B) in fluorescence intensity with cAMP exposure, indicating that channels had internalized or been inserted at these locations during the experiment. In Fig. S7 A, a cell with three chosen ROIs is shown before (0 or 15 min) and after (30 min) addition of 8-CPT-cAMP. ROI 1 shows a decline in fluorescence intensity immediately after addition of 8-CPT-cAMP (Fig. S7 B, left). Before addition of 8-CPT-cAMP, the fluorescence at 15 min was 385 a.u.; after addition of 8-CPT-cAMP, at 30 min, it had dropped to 354 a.u. (Fig. S7 B, left). In ROI 2, the number of KCNQ1-GFP channels increased shortly after 8-CPT-cAMP was added (Fig. S7 B, middle). The fluorescence intensity went from a stable baseline at 215 a.u. to 230 a.u. (Fig. S7 B, middle). Finally, the largest increase is seen in ROI 3, in which the fluorescence intensity increases from 270 to 350 a.u. after addition of 8-CPT-cAMP (Fig. S7 B, right). However, when analysis was expanded to 54–61 ROIs from the border region of the cell and 52–64 ROIs from the cell center of 11 cells before and after 2-, 5-, and 10-min exposure to 8-CPT-cAMP (Fig. S7 C), the mean fluorescence intensities of ROIs did not change significantly from those in the center to those in the border over the 10 min analyzed, in control conditions (Fig. S7 C, left) or during exposure to 8-CPT-cAMP (Fig. S7 C, right). This supports the conclusion that addition of cAMP does not lead to any organized redistribution of the channel or increase in net trafficking to the surface.
The mechanism behind the increase in IKs current after cAMP administration has not been fully defined. It is well understood at the whole-cell level that there is a hyperpolarization of the G-V relationship and that there must be effects on the channel complex Po, but these have not been studied before at the single-channel level. The underlying mechanisms for the cAMP-induced increase in current were an increased likelihood of channels to open at all during 4-s depolarizations, the ability of the channels to open sooner during a depolarizing test pulse than in control, and to occupy higher subconducting states more frequently. The studies with the E1R/R4E and S209F KCNQ1 mutants indicated that these dominant effects of cAMP were mediated preferentially via effects on voltage sensor domain kinetics rather than changes in pore kinetics. Our experiments also revealed that the effects of 8-CPT-cAMP on IKs single-channel kinetics could largely be mimicked by Asp substitution at Ser27 and Ser92.
We have proposed that there may be an increase in the number of IKs channels at the cell surface that could increase overall current. Indeed, in cell-attached single-channel and macropatch recordings, we could often see an increase in the number of active channels after the addition of the cAMP analog. However, our TIRF results showed that there is no net increase in the number of channels present and active on the surface of cells, and although the data do support a constant redistribution of channels across the cell surface, this was not significantly changed by cAMP administration.
Single channel studies of
The fusion construct EQ is composed of one E1 and one Q1 subunit attached together by a linker as characterized in (Murray et al., 2016). The response to 8-CPT-cAMP was tested on independently expressed Q1 and E1 subunits, and they responded similarly to the tandem EQ construct (Figs. S1 and S2). Half the time, both constructs also showed an increase in the number of channels in the patch after cAMP addition. Single-channel recordings of both EQ and Q1+E1 show the characteristic long latencies to the initial opening of the channel, and their properties are similar to those previously reported for these constructs when AKAP-9 was not transfected (Murray et al., 2016). However, once the cAMP analog was added, this first latency was significantly decreased (Fig. 4 D; and Table 1) and the channel opened more quickly upon depolarization (Fig. 2 C). The number of active sweeps also increased by ∼70% upon 8-CPT-cAMP stimulation (Fig. 4 D).
IKs has a number of discernible subconducting levels (Fig. S8) that are transitioned through rapidly to produce its characteristic flickering single-channel behavior. Because β-adrenergic stimulation increases the amount of current, our hypothesis was that in the presence of 8-CPT-cAMP, occupancy of the higher sublevels would be favored. The time spent at each of these subconducting states was different before and after PKA activation, and in the presence of 8-CPT-cAMP, more time was spent at the higher sublevels without any change in subconductance amplitudes (Fig. 5). We also did not see the appearance of new, larger sublevels in the presence of cAMP (Figs. 3, 4, and 5). The shift of occupancy toward the higher subconducting levels mediated by PKA was accompanied by a 10% decrease in the time spent closed, and together they translate into the well-known increase in macroscopic channel current seen during cAMP administration or β-adrenergic activation. In contrast to the marked effects on latency and subconductance state occupancy, the effects on pore kinetics were minor, with channel closed times and burst kinetics remaining relatively unaffected by 8-CPT-cAMP (Figs. 5 B and 6).
The molecular mechanisms behind the PKA-dependent changes in IKs current kinetics that we have described are not fully understood. However, it has been suggested that the distance between the Q1 N and C termini shortens once the channel opens (Haitin et al., 2009). Residue Ser27 is located in the N terminus, and PKA is bound to a complex in the C terminus. Shortening the distance between the N and C termini is thought to be necessary for this phosphorylation to occur (Haitin et al., 2009). How this affects IKs gating is not understood (Liin et al., 2015), but in the present experiments it appears that most of the effects on the single channels can be explained through actions on the VSD.
Effects of cAMP on the E1R/R4E and S209F channels with augmented VSD function
The E1R/R4E mutant is suggested to possess voltage-independent gating, as the Q1 voltage sensors are suggested to be locked in an upward position (Wu et al., 2010; Zaydman et al., 2014). The S209F KCNQ1 mutant is a VSD gain-of-function mutation that opens at highly hyperpolarized potentials compared with WT, but with much slower or absent deactivation at −80 mV. The increase in Po of S209F compared with WT has been previously reported by Werry et al. (2013), as has a much slower rate of deactivation. These properties are similar to those described for other Q1 gain-of-function mutations (Restier et al., 2008). These mutants allowed us to separate the potential actions of cAMP on pore kinetics from any effects on the VSD, which would already be maximally activated in these mutants. As anticipated, we did not observe a decrease in the number of silent 4-s sweeps, significant decreases in the first latency, or increases in E1R/R4E or S209F channel current amplitudes after 8-CPT-cAMP addition (Figs. 7 and 8). Interestingly, we did still see minor subconductance effects of cAMP on S209F (which presumably retains some ability to show VSD gating), but not on E1R/R4E. It is worth noting that in neither of these mutant channels did we observe an increased appearance of channels in cell-attached patches exposed to cAMP. Perhaps this is caused by trafficking deficiencies between these mutant channels and WT (Eldstrom et al., 2015).
Effects of cAMP on phosphomimetic mutants
Although the main target of phosphorylation for Q1 is Ser27, other phosphorylation sites are also important. Mutating Ser27 from a serine to aspartic acid using site-directed mutagenesis recreates the effects of phosphorylation, but to a lesser degree (Kurokawa et al., 2003). As described by Kurokawa et al. (2003), S27D+ E1 current densities were twofold higher than WT, and S27D had a slower rate of deactivation when cAMP was present. The V1/2 of activation (23.2 ± 4.2 mV in S27D) was hyperpolarized compared with WT (34 mV), but less than with cAMP (V1/2 = 4.1 ± 4.3 mV), suggesting that this mutation does not completely recapitulate the hyperpolarizing shift of the V1/2 seen in WT.
This is in agreement with our findings. The macropatch data (Fig. S3) show that S27D channels have a more negative V1/2 of activation than WT, and that there is still an effect, albeit attenuated, of 8-CPT-cAMP on them. The first latency of S27D is similar to EQ before the addition of cAMP, although the total closed time of S27D+E1 in control is similar to that of EQ plus cAMP. Once 8-CPT-cAMP was added, there was a significant shortening of the first latency (Fig. 9 E and Table 1), but this was proportionally far less (20%) than that observed for either EQ (34%) or Q1+E1 expressed separately (39%). Therefore, this phosphomimetic residue is responsible in part for the shortening of first latency seen when IKs is exposed to 8-CPT-cAMP, but an additional effect remains. This construct also shows a recruitment of channels upon 8-CPT-cAMP (unpublished data) similar to that of EQ and Q1+E1.
The S27D result suggests that there might be other relevant phosphorylation sites in KCNQ1, and Ser92 is another potential N-terminal site (Lopes et al., 2007) that has been shown to increase IKs current when phosphorylated (Lundby et al., 2013). In the double serine to aspartic acid mutant, S27D/S92D-Q1 channel, changes in macroscopic current amplitude or in the G-V relationship were no longer observed (Fig. 10). At the single-channel level, no significant changes were seen in latency or single-channel conductance, and no obvious differences were seen in subconductance distribution in the raw event histograms. Subconductance analysis of Q1 S27D+E1 patches showed that before 8-CPT-cAMP, this construct occupied the higher open sublevels, much like EQ and Q1+E1 after cAMP (Fig. S4). This suggests that phosphorylation of Ser27 is largely responsible for changes in channel Po once activated. However, when 8-CPT-cAMP is present, the time the channel spends closed is further reduced, so other sites like Ser92 may be involved in this response, as with the shift in V1/2 in macropatches, and the shortening of the first latency that was seen with S27D.
Other than phosphorylation sites in the N terminus of KCNQ1, Yotiao itself is phosphorylated by PKA at a residue in its N terminus, Ser43. Mutation of this serine residue to alanine prevents phosphorylation from occurring and reduces the response to cAMP (Chen et al., 2005). E1, although not a substrate for PKA phosphorylation, is also required for the effect of phosphorylation to occur. Q1 can still be phosphorylated if E1 is not present, but the functional response to phosphorylation is not apparent (Kurokawa et al., 2003). This highlights the importance of E1 in sympathetic regulation of IKs activity. The E1 C-terminal domain has been suggested to be partly responsible for the IKs response to phosphorylation. E1-D76N is a LQT-5 mutation in the C terminus that does not respond to cAMP (Kurokawa et al., 2003), and there are a number of other LQT-5 mutations that occur in this region (Splawski et al., 1997; Bianchi et al., 1999).
Trafficking and expression of
TIRF experiments were done to assess whether the increase in current after cAMP addition was at least in part the result of an increase in trafficking of the channels to the cell membrane. This, however, was not the case, as there appeared to be no overall change in expression levels of Q1 and E1 at the surface of the cell after cAMP exposure (Fig. 11). However, there were clearly areas of local rearrangement of channels (Fig. S7). There are regions from which the channels seem to exit, and areas where there is increased channel density, often where channels are moving toward the edges of the cells. This phenomenon did not seem to be dependent on cAMP, but rather the result of normal turnover of the channel in heterologous cells. This might explain, however, why during single-channel recordings after adding cAMP we sometimes see an increase in the number of channels (Figs. 3 and 4), or even a decrease/complete loss of channel activity (data not depicted).
Others have also shown no increase in Q1 movement to the cell surface upon isoproterenol exposure in COS-7 cells (Wang et al., 2013), although PKA activation is known to alter the rate of trafficking in several channels, such as the cystic fibrosis transmembrane conductance regulator and voltage-gated Na+ and K+ channels (Levin et al., 1995; Lehrich et al., 1998; Zhou et al., 2000). Kv1.1 channels are affected by PKA activation by two different mechanisms; one where an increase in channel synthesis occurs in response and the second where there is a redistribution of already synthesized channels to the membrane (Levin et al., 1995). It is also worth mentioning that other AKAPs, such as D-AKAP2, have been found to interact with Rab4 and Rab11 proteins and allow for protein recycling regulation (Eggers et al., 2009). In rats, cardiac Na+ channels have been shown to increase in number at the surface, not directly through PKA modulation, but via the G protein stimulatory α subunit (Lu et al., 1999). The remodeling effect may not be a direct effect on IKs but an effect on cytoskeleton remodeling that consequently causes relocalization of IKs channels.
The increase in IKs current after addition of cAMP is caused by phosphorylation of the VSD at Ser27 and other sites, which moves the VSD into more activated states and allows the channels to open more often, more quickly, and to higher sublevels. The direct effects on pore opening and closing are less significant. Our results also suggest that Ser27 and Ser92 are important phosphorylated residues in this response, but that others may also be of importance. The overall membrane surface expression of IKs is unchanged by cAMP stimulation, but local rearrangement may occur.
This work was supported by a grant from the Heart and Stroke Foundation of Canada (G-14-0006091), a grant from the Natural Sciences and Engineering Research Council of Canada (RGPIN-2016-05422 to D. Fedida), and a grant from the Fondation pour la Recherche Médicale to E. Balse. M. Westhoff is supported by a Graduate Research Scholarship from the University of British Columbia and was in receipt of a travel scholarship from Mitacs to perform TIRF experiments.
The authors declare no competing financial interests.
Kenton J. Swartz served as editor.