Abstract
Pulmonary hypertension is a complex disorder characterized by pulmonary vascular remodeling and right ventricular hypertrophy, leading to right heart failure. The mechanisms underlying this process are not well understood. We hypothesize that the structural remodeling occurring in the cardiomyocytes of the right ventricle affects the cytosolic Ca2+ handling leading to arrhythmias. After 12 days of monocrotaline-induced pulmonary hypertension in rats epicardial mapping showed electrical remodeling in both ventricles. In myocytes isolated from the hypertensive rats, a combination of high-speed camera and confocal line-scan documented a prolongation of Ca2+ transients along with a higher local Ca2+-release activity. These Ca2+ transients were less synchronous than in controls, likely due to disorganized transverse-axial tubular system. In fact, following pulmonary hypertension, hypertrophied right ventricle myocytes showed significantly reduced number of transverse tubules and increased number of axial tubules; however, STED microscopy demonstrated that the co-localization of L-type Ca2+ channels and RyR2 remained unchanged. Finally, STED microscopy and super resolution scanning patch-clamp analysis uncovered a decrease in the density of active L-type Ca2+ channels in RV myocytes with an elevated open probability of the T-tubule anchored channels. This may represent a general mechanism of how nanoscale structural changes at the early stage of pulmonary hypertension impact on the development of the end stage failing phenotype in the right ventricle.
Keywords: right ventricle, cardiomyocytes, electrical remodeling, T-tubule, Ca2+ sparks, L-type Ca2+ channels
Subject codes: Pulmonary hypertension, Hypertrophy, Calcium Cycling, Excitation-Contraction Coupling, Ion Channels/Membrane Transport
Graphical Abstract

INTRODUCTION
Pulmonary arterial hypertension (PAH) is a vascular disease induced by increased proliferation of cells in the pulmonary vasculature, leading to progressive narrowing of the vascular lumen and increased workload of the right ventricle (RV).1 PAH patient survival is largely determined by the ability of the RV to adapt to the pressure overload.2 In PAH, the RV undergoes structural3 and electrical remodeling.4,5 Even though the PAH-induced changes in the RV are known, so far there is no specific RV targeted treatment. While treatments effective for the left ventricular (LV) hypertrophy have been proposed for the RV dysfunction1, the differences in the biological origin and working conditions of the two chambers6 raise questions about the suitability of such approach. A better understanding of the mechanisms of RV remodeling in PAH is clearly needed.
RV hypertrophy has been studied by different groups using a monocrotaline induced model of pulmonary hypertension (PH) in rats.7–9 This model reproduces several important aspects of the cellular and molecular remodeling linked to human PAH pathogenesis.10 At the level of Ca2+ handling some discrepancies have been found, with some groups finding smaller and slower Ca2+ transients,9,11 and others observing an increase in Ca2+ transients and more intensive contractions in myocytes.7,8 Furthermore, alterations in Ca2+ transients have been linked to structural changes in the transverse-axial tubular system (TATS).9,12 Specifically, in PH RV myocytes, it has been shown that the increase in spontaneous Ca2+ releases could be due to a reduction of SERCA2a pump expression and activity.7 Interestingly, considering the importance of L-type Ca2+ channels (LTCC) in the Ca2+ handling process, no alteration in expression or whole cell current was reported in PH RV myocytes.7,13
These described changes in Ca2+ signaling could be due to the reorganization in the microdomains. Recently we reported that microdomain remodeling in the failing human and rat LV myocytes could produce the arrhythmogenic triggers that lead to reentrant arrhythmias.14 Microdomain organization in ventricular myocytes is maintained by the elaborate organization of TATS, bringing LTCCs close to ryanodine receptors (RyR2) and establishing an excitation-contraction coupling. The loss of TATS in heart failure (HF) has been associated with the redistribution of functional LTCCs from T-tubule to sarcolemma membrane14 and with the uncoupling of sarcoplasmic reticulum from the sarcolemma membrane.15 The redistribution of the LTCCs is accompanied by an increased open probability,14,16 likely due to the channel hyperphosphorylation of the channels. Although this is well described in LV myocytes, little is known about the microdomain organization of RV myocytes and their changes during RV failure. We hypothesized that RV myocytes have less complex organization of the excitation-contraction coupling microdomains compared to LV myocytes due to the lower workload of the chamber, and that in PH the microdomain remodeling leads to relocation and hyperactivation of LTCCs.
In this study we evaluated in an early stage of PH, the functional and structural changes in RV and LV myocytes at nanoscale level that could be responsible for the altered cardiac electrophysiology seen in pre-clinical models of PH. We have identified prominent cytoarchitectural changes at the single cell level, from the TATS regularity to the surface topography. Our approach allowed us to distinct two subpopulations of LTCC and RyR2 in RV cardiomyocytes; one located close to the T-tubules and one away from them. Hyperactivation of T-tubular LTCC in conjunction with SR RyR2 coupling could be responsible for the high spontaneous Ca2+ releases, desynchronization of Ca2+ transients and appearance of alternans in PH hearts.
METHODS
The data supporting the results presented in this article is available from the corresponding authors upon reasonable request. Detailed descriptions of animal procedures, cell isolation, and other methodologies are available in the Online Supplement (please see http://hyper.ahajournals.org). This work was approved by the Animal Welfare and Ethics Review Board (AWERB) of Imperial College London. It is guided by United Kingdom Home Office guidelines (ASPA 1986 and EU Directive 2010/83). The monocrotaline model of PH was generated in male Sprague-Dawley rats by 60 mg/kg intraperitoneal injection,17 with the experiments performed on days 10–12 after injection. Epicardial mapping with 11×11 multielectrode grid was applied to analyze electrical properties of the tissue.18 Standard procedures were applied to measure the conduction velocity (CV), excitability, refractoriness, and mean parameters of ECG.19,20 Cell isolation was performed using a modified Landendorf perfusion protocol.21 Data analysis was performed using GraphPad prism 6. Normality was assessed by the Kolmogorov–Smirnov test. In cases where data failed the normality test, the nonparametric Kruskal-Wallis analysis of variance (ANOVA) with Dunn’s post-hoc analysis was used instead of the two-way ANOVA test with Bonferroni post-hoc comparison. Fisher exact test was used for the occurrence analysis of extrasystole, Ca2+ transient alternans and the analysis of LTCC density. All data were expressed as mean ± standard error of mean (SEM). A value of p<0.05 was considered statistically significant.
RESULTS
Early stage PH rat characterization, RV hypertrophy with conduction abnormalities
PH monocrotaline (MCT) treated rats showed a significant increase in the mean pulmonary artery pressure within 12 days of MCT injection (Figure 1B), which was accompanied by a higher lung weight (Figure S1B) and muscularization (Figure S1C and S1D). RV hypertrophy was indicated by a markedly increased ratio of RV to LV/septum weight in PH rats (Figure 1C), as previously reported in this model.7,8
Figure 1. Characterization of control and PH rats.
A) Elastic van Gieson (EVG) representative staining of peripheral arteries in control and MCT treated animals. Scale bar, 100 μm. B) Mean pulmonary arterial pressure measured in control and MCT treated rats. C) Proportion of RV weight to LV+septum weight in control and MCT treated animals (N=7–12 rats, **p<0.01, ***p<0.001). D) Anisotropy ratio averages of conduction velocity (CV-l/CV-t). E) Effective refractory period measures. F) The percentage of the RV and LV showing extrasystole appearance (N=7 rats, * p<0.05, ** p<0.01).
The electrophysiological properties of RV and LV control and PH rats were studied by epicardial multiple lead recording. The multielectrode grid and representative isochrone maps measured in RV and LV are presented in Figures S2 and S3A, respectively. PH led to a decrease in conduction velocity along epicardial fiber direction longitudinally (CV-l) in both ventricles, but only statistically significant in LV tissue (p<0.05, Figure S3B). We found no changes in conduction velocity across epicardial fiber direction transversally (CV-t) in both RV and LV after PH (Figure S3C). Interestingly, when the CV-l/CV-t was calculated to measure the anisotropy ratio of conduction velocity (Figure 1D), it showed a lower value in PH rats and only statistically significant in RV (p<0.05). The refractoriness of the tissue was assessed with the analysis of the effective refractory period (ERP). In control animals, the ERP in RV was significantly shorter than in LV (p<0.01, Figure 1E). PH led to a prolongation of ERP both in the RV (p<0.01) and the LV (p<0.05). The basic electrocardiogram parameters were also evaluated (Figure S4). We found longer QT intervals in the LV compared with the RV (p<0.001) and the RV in PH showed prolonged QT with respect to that in control RV (p<0.05, Figure S4C).
The arrhythmogenicity of the tissue was assessed by the occurrence of extrasystoles. We recorded a higher number of animals with extrasystoles in the PH group, 5 out of 7 animals, versus 3 out of 7 animals in the control group, but this difference was not statistically significant (Figure 1F).
Increased local Ca2+ transients in PH RV cardiomyocytes promotes Ca2+ alternans.
To evaluate Ca2+ handling in PH rat myocytes, we analyzed the spontaneous Ca2+ waves by optical mapping according to 22. Two types of waves were examined, local and propagated through the entire cell, as shown in Figure 2A. The frequency of local waves was significantly elevated in PH RV myocytes (p<0.05, Figure 2C) without changes in the frequency of propagated waves (Figure S5). Local Ca2+ releases were then analyzed using the line mode of the confocal microscope.23 A representative Ca2+ spark image is shown in Figure 2B. In the control group, RV myocytes showed a similar frequency of Ca2+ sparks as LV myocytes (Figure 2D), but spark mass was lower in RV myocytes (Figure 2E). In the PH group, RV myocytes exhibited a significant increase in Ca2+ spark frequency (Figure 2E) and mass (Figure S5B) as compared to the control group. These properties of Ca2+ sparks were preserved in PH LV myocytes. Elevated rate of Ca2+ sparks could be associated with elevated SR Ca2+ load or abnormal SERCA2a Ca2+ reuptake. However, caffeine–induced Ca2+ release experiments did not show significant changes in fractional Ca2+ release and SERCA2a activity (Figure S6).
Figure 2. Pulmonary hypertension induced high spontaneous Ca2+ activity in RV but not in LV myocytes.
A) Representative traces of spontaneous Ca2+ activity measured in isolated ventricular myocytes. Cells were electrically paced at 4 Hz for 1 min to enhance sarcoplasmic reticulum Ca2+ loading. Local and propagated Ca2+ waves were recorded during a 16-s rest period after cessation of pacing. On the left, optical traces showing changes in [Ca2+] from 3 different points (1–3) selected in a single cardiomyocyte, on the right. B) Average frequency of local Ca2+ waves (n=25–45 cells, N=5–9 rats, *p<0.05). C) Representative confocal line scans of LV (top) and RV (bottom) myocytes loaded with Fluo4-AM. Recordings were performed during 2 s rest period after 1 min of pacing. D) Average Ca2+ sparks frequency in control and PH myocytes (n=30–67 cells, N=4–5 rats), E) Representative traces of Ca2+ transients with and without alternans at 4 Hz stimulation, F) The percentage of cells showing Ca2+ transients alternans in control and PH myocytes (n=30–67 cells, N=5–6 rats, *p<0.05, **p<0.01).
Abnormal Ca2+ cycling has been shown to be associated with the appearance of Ca2+ transients alternans.24 When single cardiomyocytes were paced at 4 Hz, the proportion of cardiomyocytes showing Ca2+ transient alternans in PH RV myocytes were significantly higher than in control RV myocytes (Figure 2E).
To examine the effects of the increased spontaneous local Ca2+ activity in PH RV myocytes, we performed analysis of the electrically evoked Ca2+ transients (Figures 3A and S7). Ca2+ transients of significantly slower time to peak were observed in PH RV myocytes (Figure 3B). Next, the spatial variability of time to reach half-maximal fluorescence (TTF50) across the cell was analyzed. Histograms of TTF50 in LV myocytes have a peak around 10 ms, whereas for RV myocytes the peak is lower and the distribution is wider (Figures S8A and S8B). A ‘dyssynhcrony index’ defined as the standard deviation of TTF50,25 showed a significantly higher value in PH RV myocytes as compared to control RV myocytes (Figure 3C).
Figure 3. PH – induced desynchronization of Ca2+ transients.
A) Representative images of Ca2+ transients recorded in LV and RV myocytes paced at 1 Hz. B) Time to peak of the Ca2+ transients measured in LV and RV myocytes from control and PH rats paced at 1Hz (n=14–20 cells, N=4 rats, *p<0.05, **p<0.01). C) Average of ‘dyssynchrony’ index (n=24–38 cells, N=4–5 rats, *p<0.05, *p<0.05, ***p<0.001). D) Duration of early and delayed Ca2+ sparks measured in control RV and PH RV myocytes. (n=34–41 cells, N=4–5 rats, *p<0.05, **p<0.01).
We used the approach of Heinzel et al26 and Biesmans et al27 to divide Ca2+ release points into early and late ones according to their TTF50 (Figure S8C). We used 50% of the cumulative histogram as a threshold value for this division (Figure S8D). Ca2+ sparks occurring in early or delayed areas were analyzed separately. In PH RV myocytes, Ca2+ spark duration and time to peak in delayed areas were significantly prolonged (Figures 3D and S9G). Ca2+ sparks from delayed areas had a higher frequency and amplitude in PH RV myocytes but not in PH LV myocytes (Figure S9A-S9F).
Structural regularity is reduced in PH RV myocytes.
It has been shown previously that the reorganization of membrane structure affects the Ca2+ handling and synchronization in the LV myocytes.25,28,29 To study the organization of the sarcolemma membrane, TATS and surface topography of RV and LV myocytes were visualized by Di-8-ANEPPS membrane staining and SICM, respectively. Representative images are shown in Figure 4A. In analyzing the cardiomyocytes shape the length to width ratio was decreased in PH RV myocytes (p<0.01, Figure 4B). RV myocytes from PH rats had a reduced length (Figure S10A) and increased width (Figure S10B) compared to control ones, while LV myocytes became thinner in PH (Figure S10B).
Figure 4. Reorganization of sarcolemma membrane in PH rat model.
A) Representative images of TATS and SICM scans of LV and RV myocytes from control and PH rats; scale bar, 10 μm. B) Summary graph of cell length to width ratio (n=37–55 cells. N=4 rats, *p<0.05, **p<0.01). C) Average Z-groove ratio of control and PH myocytes (n=23–30 cells, N=3–5 rats, *p<0.05, ***p<0.001). D) Power of TATS regularity measured in RV and LV from control and PH myocytes (n=25–40 cells, N=3–5 rats, *p<0.05). E) Directionality histograms for the TATS of control and PH RV myocytes and F) summary of the axial tubules and transverse tubules in LV and RV myocytes after PH (n=20–73, N=4–5rats, **p<0.01, ***p<0.001).
In the analysis of SICM images, we used the z-groove ratio as an index of surface regularity30 and found a significant z-groove index reduction in RV myocytes in PH (Figure 4C) as compared to control. However, despite this reduction, the number of T-tubule openings on the surface of PH myocytes was unaffected (Figure S10C).
Although the total density of the TATS was preserved in PH rats (Figure S10D), the average TATS regularity was reduced in PH RV cardiomyocytes (Figure 4D). The directional analysis of TATS31 showed a re-arrangement of tubules from the transversal to the axial direction in PH, which could explain the differences in the regularity (Figure 4E). The average fraction of the axial tubules was significantly higher in PH RV myocytes as compared to control (Figure 4F), whereas the average fraction of transverse tubules was significantly lower (Figure 4F).
RV cardiomyocytes exhibit smaller Cav1.2 density
We hypothesized that remodeling of the TATS in PH leads to dissociation of LTCC from RyR2, which could be the cause for the Ca2+ handling changes mentioned above. It has been shown that in HF, orphaned RyR2 are the source of increased spontaneous Ca2+ activity.32 To determine the amount of LTCC co-localized with RyR2, we performed Stimulation Emission Depletion (STED) imaging on fixed myocytes. Figure 5A illustrates representative STED images of RV and LV myocytes stained with antibodies against Cav1.2 (magenta) and RyR2 (cyan). There were no differences in Cav1.2 and RyR2 signal densities between control RV and LV myocytes (Figure 5B and 5C). PH promoted a reduction of Cav1.2 signal density in RV myocytes, but not in LV ones (Figure 5B). No alterations in signal density of RyR2 staining were found in PH (Figure 5C). These results were supported by Western blot analysis (Figure S11). While a trend towards a reduction of Cav1.2 protein expression in RV tissue after PH (Figure S11B), no changes were observed in the levels of RyR2 protein expression in RV tissue after PH (Figure S11D).
Figure 5. Co-localization of Cav1.2 and RyR2 in PH rat model.
A) Representative STED confocal images of RV and LV myocytes labelled with antibodies against Cav1.2 (magenta) and RyR2 (cyan). Overview scale bars: 10 μm. Magnified area scale bars: 2 μm. B) Average density of Cav1.2 signal and C) RyR2 signal from LV and RV myocytes from control and PH rats (n=10–16 cells, N=3–4 rats, ***p<0.001). D) Percentage of Cav1.2 clusters colocalized with RyR2 and E) Percentage of RyR2 clusters colocalized with Cav1.2. (n=10–16, N=3–4 rats).
Co-localization of Cav1.2 and RyR2 was determined using two methods: by defining the percentage of overlap between the two stainings and by calculating Manders’ coefficients.33,34 The colocalization analysis did not show any significant changes in both parameters: percentages of overlapped Cav1.2 or RyR2 (Figure 5D and 5E) and Manders coefficients (Figure S12).
Open probability of L-type Ca2+ channels in the T-tubules of RV cardiomyocytes is increased in PH.
Finally, to understand the localization and distribution of functionally active LTCC in RV myocytes in the context of functional changes in the PH heart, we used super resolution patch clamp method (Figure 6). LTCC membrane density is calculated by normalizing the total number of channels observed in TT or crest to the patched area.35,36 It has been shown that in LV myocytes LTCCs predominantly localize in T-tubules and not in the crest area.28,37 However, in RV myocytes LTCCs were observed at almost equal density in both locations; only a slightly (not significant) higher channel density was found in T-tubule versus crest microdomains (Figure 6C). Inlet in Figure 6C shows that PH RV myocytes have a reduced density of functional LTCCs, however no significant changes were found regarding LTCCs in T-tubules or crests. To maximize the chance of recording LTCC current, we applied the LTCC agonist BayK8644 in the next set of experiments (Figure 6B). In the presence of BAYK8644 in control myocytes the average density of LTCC in control and PH myocytes remained equal (Figure 6D).
Figure 6. Analysis of L-type Ca2+ channels distribution and function in RV myocytes after PH.
A) Representative single channel traces showing LTCC current recorded at −6.7 mV in T-tubule and crests of RV myocytes in normal solution and B) in presence of BayK8644. C) LTCC density observed in normal solution and D) with the agonist in T-tubule and crests of RV myocytes from control and PH rats. The number in each column represents the total number of successful seals in each group. Inlets show total LTCC density analysis from both T-tubules and crests together, from control versus PH RV myocytes. E) LTCC open probability (Po) at −6.7 mV in control and PH RV myocytes at physiological conditions or with the agonist BayK8644. (n=6–19 channels, 40–100 cells, 6–10 rats, *p<0.05).
We then calculated the open probability of LTCC in all the groups. In control RV myocytes, the open probability (Po) of LTCC was significantly lower in the T-tubules as compared to the crest (Figure 6E). In PH RV myocytes, the LTCCs located in T-tubules exhibited a significantly elevated Po in respect to control T-tubules (p<0.05), with the crest subpopulation of LTCCs having preserved Po after PH. In the presence of BayK8644, the mean LTCC Po was preserved (Figure S13).
DISCUSSION
This study provides evidence of the nanoscale microdomain-related disruptions in Ca2+ handling that occur in PH, which could affect electrical conductance in the heart. We conclude that during PH development, the increased workload of RV due to the high pulmonary artery pressure causes structural remodeling of TATS and surface topography in RV myocytes. This structural remodeling promotes local alterations in the Po of LTCC and in the frequency and duration of delayed Ca2+ sparks, which in turn could be responsible for the desynchronization of Ca2+ transients and the appearance of Ca2+ transient alternans observed. The increase in local spontaneous Ca2+ activity and the appearance of Ca2+ transient alternans could serve as trigger for arrhythmias in the settings of substantial tissue remodeling.38 However, our in vivo experiments showed that the remodeling is not sufficient to evoke a significant arrhythmic activity, as reported at the more severe stages of disease.7 In LV myocytes, PH leads to prolongation of Ca2+ transients but this occurs without changes in TATS organization.
PH induced RV hypertrophy and electrical remodeling
It was previously shown that PH leads to RV hypertrophy formation of arrhythmogenic substrates at the last stages of disease.7 Here we studied the preceding changes in electrical remodeling. The increase of CV anisotropic ratio was linked to the generation of unidirectional conduction block and sink to source mismatch.39 Our data shows that that early PH leads to the reduction in the anisotropy ratio in RV but not in LV (Figure 1D). It has also been known that structural remodeling of the tissue influences CV.40 However, it has been already shown previously that no significant increases in fibrosis, apoptosis or infiltration of the inflammatory cells occur in the heart tissue after 2 weeks of MCT treatment.41 On the other hand, RV myocytes in PH become significantly hypertrophied (Figure 4B) and redistribution of gap junction occurs40 on the surface of PH RV myocytes; these changes can produce alteration of the passive electrical properties of the ventricle and change the balance between longitudinal and transverse conductions.
We also observed longer ERP in both RV and LV following PH (Figure 1E), which could be related to the prolonged Ca2+ transient duration (Figure 3B and Figure S7). Increasing the ERP can precipitate torsades de pointes, a type of ventricular tachycardia caused by early or delayed afterdepolarizations.42 We did not see a significant increase in occurrence of extrasystole in the PH RV as compared to the control RV, so we could assume this stage of the disease is not severe enough for the development of a pro-arrhythmogenic substrate.
The observed remodeling of LV electrophysiology and cell dimensions could be induced by neurohormonal activation in PH hearts43 or due to mechanical interdependence of the two ventricles.44
PH increased spontaneous Ca2+ activity in RV myocytes
PH led to an increase in spontaneous local Ca2+ waves and Ca2+ sparks frequency in RV but not LV myocytes. Interestingly, the preserved SR Ca2+ load and SERCA activity in PH myocytes suggest the remodeling happens mostly in RyR2 activity. We observed a significantly slower time to peak of Ca2+ transients in PH RV myocytes (Figure 3B), with an increased Ca2+ transient dyssynchronization (Figure 3C). Dyssynchronization of Ca2+ transients found in PH RV myocytes could be related to the rearrangement of TATS.
We defined the early and delayed Ca2+ release points of Ca2+ transients according to their TTF50 (Figure S9). Early release regions of Ca2+ transients were shown to arise from areas with higher TAT density while delayed ones arose from areas with lower TATS density.26 Assigning of Ca2+ sparks to early or delayed areas were performed according to their position on the scan line. RV myocytes showed a significantly higher frequency of early sparks versus delayed ones (Figure S9). Higher frequency of sparks located close to the T-tubule has been shown in myocytes from different species.27,45 It has been proposed that the higher local Ca2+ concentration close to the T-tubule produces Ca2+ sparks more frequently. PH significantly increased the frequency and prolonged the duration of delayed but not the early Ca2+ sparks in RV myocytes. This could be due to rearrangement of the TATS microdomains or alterations of RyR2 clustering. Kolstad et al46 showed that in failing LV myocytes RyR2 undergo significant dispersion and that large RyR2 clusters produce slower Ca2+ sparks and, consequently, a desynchronization of Ca2+ transients.
Ca2+ transient alternans observed in PH RV myocytes could be related to the abnormal Ca2+ release or Ca2+ reuptake (Figure 2F). As we did not find any reduction in SERCA activity in PH (Figure S6), the appearance of Ca2+ alternans could be associated with the abnormal RyR2 activity.47 Ca2+ transient alternans have been shown to produce action potential duration alternans, reentrant activity and contractile impairment,24 however, our in vivo data indicates that the remodeling was still not sufficient for the formation of a pro-arrhythmic substrate (Figure 1).
TATS reorganization in PH
TATS organization largely impacts on the intracellular Ca2+ cycling.25 We observed a reduction of TATS power of regularity in RV PH myocytes due to the lower amount of transverse tubules and a higher number of axial tubules in PH (Figure 4). The recent study by Shobesberger et al48 documented higher frequency of axial (longitudinal) tubules during hypertrophic state of the myocardial infarction. The role of axial elements in the excitation-contraction coupling is still not fully understood, although recent studies of Ashari et al49 and Swift et al50 showed that axial tubules can be fully functional with LTCC coupled to SR and RyR2 clusters. Thus, the increase in the number of axial tubules was proposed to be the first compensatory mechanism in maintaining high working load and secure Ca2+ influx to support contractions.50
Analysis of the membrane topography by SICM showed a reduction in z-groove index in RV but not in LV myocytes in PH (Figure 4C). Studies of LV myocytes from rat and human failing hearts have shown that this reduction is accompanied by an increase of Ca2+ waves and sparks.14,28 The disruption of surface topography could be linked with the weakening of sarcomeres and myocardial stretch, which results in opening of stretch-activated channels,8 and/or altered Ca2+– troponin interaction at different sarcomere lengths.51
RV Cav1.2 re-arrangement in PH
Our results on PH rats showed that RyR2 protein expression and RyR2 STED signal densities are unchanged when compared to control (Figure S11 and 5C). In agreement with this, research into HF and PH has demonstrated that RyR2 arrangement and expression is preserved in failing myocytes.8,9 RyR2 activation depends on the Ca2+ entry through LTCC. Interestingly, we observed the distribution of LTCC between T-tubule and crest in RV is more similar to atrial myocytes than LV myocytes.14,22,37 Taking into account differences observed in early and delayed Ca2+ sparks parameters between control RV and LV myocytes, these findings suggest an altered organization of Ca2+ handling microdomains between both ventricles.
Following PH, we found a reduction of Cav1.2 STED signal density (Figure 5B) and a reduction in the number of functional LTCCs in RV myocytes (Figure 6C). The analysis of Cav1.2 protein expression from tissue after PH (Figure S11) and the LTCC density in presence of agonist (Figure 6D), however, did not show a significant change. Also, co-localization between RyR2 and Cav1.2 in both RV and LV myocytes was not affected by PH (Figure 5D). This evidence suggests that the expression of Cav1.2 protein remains unaffected at this early stage of the disease, but a functional remodeling of LTCC is already happening. This is supported by other groups that found no changes of the pore-forming Cav1.2 protein expression in the early hypertrophic stage of the disease.7,13 Although a down-regulation of Cav1.2 protein expression has been observed in the late stages of PH.9,52 In terms of whole-cell Ca2+ current, which density in PH RV myocytes is preserved,7 we suggest that the silencing of functional LTCCs is partially compensated by the increase of the Po in T-tubular LTCC. This increased Po of LTCC in T-tubules could be caused by phosphorylation of the channels by PKA or CaMKII.14,16 In fact, Fowler et al12 found an increased β-adrenergic stimulation in PH rats, which will activate PKA and consequently, LTCCs. Although this activation could work as a compensatory mechanism to keep the contraction requirements, it could also be the substrate of the increased Ca2+ activity observed in this work. Overall, our findings underscore the role of nanoscale organization of Ca2+ handling within myocytes in the pathophysiology of the heart, particularly during development of a disease such as PH.
Perspectives
Our study shows that during development of PH RV cardiomyocytes undergo structural remodeling that induces functional alterations of intracellular Ca2+ behavior and could affect the electrical properties of the whole heart. However, the arrhythmogenic activity in the RV, reported at the later stages of PH, was not found. This suggests that the changes observed at the cellular level could precede development of arrhythmias. Our findings provide new mechanistic insights into right ventricular dysfunction, which could help identify novel therapeutic approaches for RV failure in PH.
Supplementary Material
Novelty and Significance.
What Is New?
We observed that at an early stage of pulmonary hypertension, myocytes of right ventricle develop local nanoscale changes in L-type calcium channel and Ca2+ spark properties which could encourage dysregulation of Ca2+ transients which in turn could form a pro-arrhythmic substrate in the whole heart.
What Is Relevant?
We found alterations in transverse and axial tubular network and surface topography of myocytes, leading to changes in local L-type calcium channel activity and Ca2+ spark properties, which occurred before a significant arrhythmogenic remodeling in the whole heart.
Summary
Right ventricle myocytes of the heart have a distinct ultrastructure and functional behavior as compared to left ventricle myocytes. Pulmonary hypertension induces membrane remodeling in right ventricle myocytes and alteration of the local properties of L-type calcium channels and Ca2+ sparks, producing significantly altered Ca2+ transients and prolonged refractoriness on the whole heart level. Left ventricle at this stage of the disease is mostly preserved in terms of its structure and function, but we cannot exclude its involvement at later stages.
Acknowledgments
We thank Peter O’Gara for myocyte isolation.
Sources of funding
This work was supported by British Heart Foundation grants (RG/17/13/33173 to JG and PG/15/69/31719 to B.W.-S) and NIH grant (ROI-HL 126802 to NT and JG).
Footnotes
Disclosures
None.
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