Copyright © 2006, European Society of Cardiology
The role of angiotensin receptor-1 blockade on electromechanical changes induced by left ventricular hypertrophy and its regression
aDepartment of Medicine, University College London, 48 Riding House St, London W1P 7PN, UK
bAcademic Cardiology Unit, Imperial College School of Medicine, St Mary's Hospital, London W2 1NY, UK
* Corresponding author. Clinical and Academic Department of Cardiovascular Medicine, Whittington Hospital, Highgate Hill, London N19 5NF, UK. Tel.: +44 20 7288 5292; fax: +44 20 7288 5010. Email address: rosaire.gray{at}whittington.nhs.uk
Received 21 April 2006; revised 3 November 2006; accepted 7 November 2006
| Abstract |
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Objective: The aims of this study were to: i) investigate the role of angiotensin in mediating changes to myocardial electromechanical properties during the development and regression of left ventricular hypertrophy (LVH) generated by constriction of the thoracic aorta; ii) identify any role of angiotensin-1 receptor blockade on ameliorating changes to these electromechanical properties.
Methods: LVH was induced in guinea-pigs by constricting the ascending aorta (AC groups). After 42±3 days, the constriction was either removed or left in place. Following the second operation animals were fed losartan (10 mg·kg–1·day–1) or saline for 42±3 days. Sham-operated animals served as controls. In other groups, LVH was generated by subcutaneous angiotensin II (200 ng·kg–1·min–1) infusion for 42±3 days with or without losartan administration (AT groups), and compared to animals undergoing aortic constriction for a similar period. Electromechanical changes were recorded in isolated left ventricular myocardial preparations.
Results: Wet and dry heart-to-body weight ratios (HBR) increased significantly in the AC and AT models compared to control. Losartan prevented the increase of HBR in the AT group. Removal of the constriction allowed LVH to regress to control. The force–frequency relationship was reduced in both models and recovered fully on regression. However, the two models generated different electrophysiological changes: in the AC group, longitudinal conduction velocity was reduced and transverse conduction increased, with a consequent reduction of the anisotropic conduction ratio. On regression recovery was only partial; action potential duration was prolonged and did not recover. In the AT group, electrophysiological changes were limited: only an increase of transverse conduction and a reduction of the anisotropic conduction ratio were observed. Losartan had no effect on HBR or electromechanical variables in the aortic constricted animals, nor did it affect the extent of recovery in animals with regression of LVH.
Conclusions: The electromechanical changes to hypertrophied myocardium are different in these two models of LVH. Moreover, losartan was ineffective in modulating the consequences of hypertrophy induced by constriction of the thoracic aorta.
KEYWORDS Hypertrophy; Ventricular function; Arrhythmia; Angiotensin-receptor blockade; Conduction
| 1. Introduction |
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Left ventricular hypertrophy (LVH) is a significant predictor of cardiovascular mortality and morbidity arising from both ventricular arrhythmias and myocardial failure [1,2]. Electrophysiological changes occur during hypertrophy, in particular to action potential (AP) duration, and to conduction due to alterations of the active and passive electrical properties of the myocardium [3–5], and these are likely to contribute to the risk of re-entrant arrhythmias and sudden death.
Regression of LVH by pharmacological and surgical procedures has been shown in animal models of hypertrophy [6,7] and in humans with aortic stenosis and hypertension [8,9]. However, this is not always accompanied by normalisation of the associated pathophysiology, in particular electrophysiological abnormalities [6], and indeed the prognosis associated with previous LVH remains poor [10]. Furthermore, it is difficult to separate out the effects of drug-induced regression of LVH from the action of the drugs themselves or the reduction of blood pressure.
The renin–angiotensin system has been implicated in the development of some models of hypertrophy [11], but its involvement in the changes to the physiological properties of myocardium that occur during hypertrophy has not been investigated. Although systemic increases of angiotensin (AT) have not been observed in hypertrophy induced by constriction of the thoracic aorta [12] it remains possible that AT may mediate some of the functional changes. The purpose of this study was twofold: to investigate the potential role of AT in this context, by comparing the electromechanical changes induced in hypertrophied myocardium by aortic constriction or infusion of AT; and to determine the role that blockade of angiotensin-1 receptors may play in ameliorating the consequences of hypertrophy and reversal of changes on regression of hypertrophy.
| 2. Methods |
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2.1. Induction of left ventricular hypertrophy (LVH) and regression from LVH
Ten groups of adult male Dunkin–Hartley guinea-pigs (600–800 g) were used to study the pathophysiology of LVH, seven by constriction of the ascending aorta (including sham-operated controls), and three by angiotensin infusion: the protocols are shown in Fig. 1. The basic treatment block was 42 or 84 days, as in this model these periods generate LVH without development of heart failure [3,6]. In groups 2, 3, 4, 5 and 7 LVH was induced by placing a high-density plastic clip (internal diameter 2.0 mm) around the ascending aorta. Animals were anaesthetised with Na pentobarbitone (0.12 mg Sagatal, Rhone Merieux Ltd, Harlow) and 0.1 mg diazepam for injection (Phoenix Pharma Ltd, Gloucester), followed by inhalation of a 49%/49%/2%, N2O/O2/halothane mixture. Animals were intubated and ventilated at 100 cycles per minute, with an O2 flow of 0.4 l·min–1 and the aorta exposed via a left thoracotomy, as previously described [13]. Groups 1 and 6 were sham-operated controls that underwent the same procedures, without clip placement. After 42±3 days, animals in groups 6 and 7 were killed, and the hearts removed rapidly for in vitro experiments. Animals in groups 1–5 at this time underwent a right thoracotomy and the plastic clip was either left in place (age-matched LVH, groups 2 and 3), removed (de-banded groups 4 and 5), or had a second sham-operation (group 1). After this second procedure, animals in groups 2–5 were daily given an oral gavage containing losartan in 1 ml isotonic saline (10 mg·kg–1, Merck, Sharp and Dohme [14], groups 3 and 5), or saline alone (groups 2 and 4).
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With group 9 guinea-pigs, LVH was induced by infusion of angiotensin II for 42±3 days (200 ng·kg–1·min–1, Sigma; [15]), by subcutaneous osmotic mini-pumps inserted under anaesthesia: group 8 animals received saline infusion. Finally, group 10 animals also received 42 days of angiotensin infusion, with losartan also administered as described above.
All procedures conformed to The Guide for the Care and Use of Laboratory Animals (National Institute of Health (NIH) Publication No. 85-23, revised 1996) and UK Guidelines in The Operation of Animals (Scientific Procedures) Act, 1986.
2.2. Isolated preparations
Animals were weighed, sacrificed by cervical dislocation and the hearts rapidly removed and weighed. Heart-to-body weight ratio (HBR) was used to assess the extent of hypertrophy and regression. Lung-to-body weight ratio was used to assess a lack of heart failure if the value was similar in experimental and sham-operated groups. Parallel cohorts of animals for groups 1, 2, 4, 6, 7, 8 and 9 were prepared to measure the dry weight of the left ventricle to test the hypothesis that and increase of HBR was due to a greater tissue mass rather than accumulation of oedema. The left and right ventricles were separately weighed, placed in an oven at 80 °C and dried for 48 h.
Left ventricular papillary muscles were isolated from experimental hearts, mounted in a superfusion bath, secured at one end to a fixed hook and at the other end to an isometric tension transducer, and superfused with Tyrodes's solution at 4 ml·min–1, at 37 °C. Tyrode's contained (mM): NaCl 118, KCl 4.0, NaHCO3 24, MgCl2 1.0, CaCl2 1.8, NaH2PO4 0.4, glucose 6.1, Na pyruvate 5.0, pH 7.40±0.2, gassed with 95% O2 and 5% CO2. Muscles were up to 6 mm long, <2 mm wide, and <1 mm thick to minimize hypoxic damage to the tissue.
The force–frequency relationship was quantified as the ratio of peak isometric tensions generated at 1.6 and 0.8 Hz stimulation frequencies (T1.6/0.8). Field-stimulated action potentials were recorded with 10 M
, 3 M KCl-filled microelectrodes at 1 Hz. AP duration was the time from the upstroke to 95% repolarisation (APD95). Conduction velocity along the longitudinal axis (
L) was measured by stimulating the muscle at one end via insulated Ag–AgCl electrodes, with pulses at 1.5x threshold to minimize extracellular current spread, and recording APs at distances, d, more than 1 mm from the stimulation site. The distance d was measured with a Vernier scale on the microelectrode micromanipulator, and checked with an eyepiece graticule under x40 magnification, both methods were accurate to 100 µm.
L was calculated as the distance:delay ratio over several values of d. Transverse conduction velocity,
T, was measured using large extracellular stimulating electrodes parallel to the muscle axis, and restricting the extracellular volume, under these conditions AP conduction is transverse to the axis [16]. We have shown previously [4,5] that these stimulating conditions provide one-dimensional, planar conduction in the axis of interest, with an error of <5% in other dimensions. The time constant of the action potential base or foot,
ap, was calculated from a semilogarithmic plot of the initial 10–12 mV depolarisation of the conducted AP.
2.3. Statistical analyses
Results are expressed as mean±SD, or when several separate measurements were made from the same preparation as SE. Comparison between groups was assessed using ANOVA with Bonferroni post hoc tests. The null hypothesis was rejected when p<0.05.
| 3. Results |
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3.1. Development of cardiac hypertrophy and regression from hypertrophy
The magnitude of cardiac hypertrophy was assessed in two ways: the wet heart-to-body weight ratio (HBR); and the dried left ventricular-to-body weight ratio (DLVBR). Table 1 shows that both variables increased after constriction for 42 days (group 7) and 84 days (group 2), with respect to their respective age-matched controls (groups 6 and 1, respectively). Furthermore, in the group that was de-banded after 42 days constriction (group 4) HBR and DLVBR decreased significantly to values not different from the age-matched control. HBR and DLVBR after 42 and 84 days constriction were not significantly different. Thus, the effect of the debanding procedure after 42 days could be measured after ventricular hypertrophy had developed to a steady level. Table 1 also shows that angiotensin, compared to saline, infusion for 42 days (groups 8 and 9) also increased HBR and DLVBR, to values similar to the time-matched aortic constriction groups. Thus, with respect to generation of hypertrophy the methods of thoracic aortic constriction and angiotensin infusion produced comparable results.
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The lung-to-body weight ratio in the combined control groups (sham constriction and saline infusion, groups 1, 6 and 8) was 4.44±0.65 g·kg–1; values in all remaining groups were not significantly different from this value.
3.2. Electromechanical changes during hypertrophy and its regression
Table 2 summarises the electromechanical properties of myocardium after 84 days aortic constriction, and also after 42 days of constriction and 42 days of de-banding, compared to 84-day sham-operated controls. Some data is in confirmation of previous findings [4–6]. It should be noted that the changes to the 84-day constricted group were quantitatively similar to changes after 42 days constriction (for the latter see AC data in Fig. 2B). Preparations from control animals showed a positive staircase, as evidenced by values for T1.6/0.8 greater than 1.0. This variable was significantly reduced in the hypertrophied hearts but recovered completely in the regressed hearts. Absolute twitch strength at 1 Hz, time-to-peak tension and twitch duration were similar in all experimental groups (sham-operated values were respectively: 2.15±1.40 mN·mm–2; 132±3.7 ms; 289±8.1 ms).
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However, electrophysiological changes associated with LVH showed less complete reversibility. Table 2 shows that APD95 was prolonged in hypertrophy and remained so after LVH regression. Action potential conduction velocity in the longitudinal axis of the preparation,
L, was reduced in LVH, but was increased in the transverse axis,
T, resulting in a reduction of the anisotropic conduction ratio,
L/
T. Regression of hypertrophy only partially ameliorated these conduction changes; thus
L only partially recovered to an intermediate value, although transverse conduction,
T, returned to control. The anisotropy ratio also returned to a value not significantly different from the control value. By contrast, the resting membrane potential, Em, was unaffected by LVH and its regression. The maximum rate of action potential (AP) depolarisation (dV/dtmax), and the time constant of the action potential foot,
ap – factors importantly determined by the magnitude of the Na+ current – were also unaltered in LVH and its regression. dV/dtmax and
ap were measured from action potentials conducting in the longitudinal (L) or transverse (T) axes. In groups shown in Table 2, and in all other experimental groups, these values were greater in the transverse compared to the longitudinal axis; this significance will be considered in the Discussion. Fig. 2A illustrates the rising phases of longitudinally and transversely conducting action potentials. The thicker lines (arrowed) drawn over the subthreshold regions of the rising phase indicate the regions used to calculate
ap. The delay, d, between the start of the stimulus artefact and the peak of differential response (lower traces) was used to calculate conduction velocity – see also figure legend). All further interventions had no effect on the values of membrane potential, dV/dtmax or
ap so their values are not further reported.
3.3. Effects of angiotensin II infusion
Table 1 shows that angiotensin II infusion (n=7) also increased significantly HBR and DLVBR. Fig. 2B shows the electromechanical properties with angiotensin infusion and compares these with aortic constriction for 42 days. It shows that the changes accompanying myocardial hypertrophy were different in the two models. The T1.6/0.8 ratio was reduced from 1.55±0.02 to 1.24±0.02, similar to that in the aortic constriction group. However, the prolongation of the action potential, and reduction of longitudinal conduction velocity were absent in the angiotensin group, although there was a similar increase of transverse conduction velocity and a consequent reduction, albeit smaller, of the anisotropic conduction ratio. Control data from sham-operated (group 6) and saline-infused (group 8) animals were identical; for clarity only the latter control data are shown in Fig. 2. Fig. 2C shows sample action potentials from the control, aortic-constricted and angiotensin-infused groups.
3.4. Effects of the angiotensin II type-1 receptor (AT1) antagonist, losartan, on electromechanical changes during hypertrophy
Forty-two days after initiating aortic constriction, two groups of animals were fed losartan: during the continued presence of the constriction (group 3); after removal of the constriction (group 5). The objective was to determine if AT1-receptor antagonism influenced changes to myocardial electromechanical properties during these periods. To determine if the losartan dose, and route of administration, were adequate, a control series of experiments was carried out whereby losartan was administered during angiotensin infusion via osmotic mini-pumps. In three separate experiments losartan administration alone had no effect on HBR (2.66±0.24 vs 2.44±0.18 g·kg–1, saline vs losartan) or any electromechanical variable (data not shown).
Fig. 3A shows that losartan prevented the increase of HBR induced by angiotensin infusion (group 10 vs group 9 animals); the value of 2.93±0.41 g·kg–1 was significantly less than the angiotensin group, and not different from the saline-infusion group. Furthermore, losartan prevented the angiotensin-mediated changes to electromechanical properties reported above, i.e. the T1.6/0.8 ratio (1.59±0.08 vs 1.24±0.04, p<0.05, with and without losartan respectively). It may be concluded that the administration of losartan effectively antagonised the effect of infused angiotensin on cardiac growth and functional myocardial properties.
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The possible involvement of angiotensin, through a losartan-sensitive mechanism, in altering electromechanical function during LVH maintained by aortic constriction was therefore examined. Fig. 3B shows that 42-day administration of losartan did not reduce HBR. Furthermore, Fig. 4 shows that treatment with losartan had no effect on the variables altered during aortic constriction. Thus, the T1.6/0.8 ratio was attenuated, APD95 was prolonged, longitudinal conduction velocity was reduced, transverse conduction increased, and the anisotropic conduction ratio decreased: all to similar extents to those without losartan.
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3.5. Effects of losartan on electromechanical changes during regression
Fig. 3C shows that 42-day oral administration of losartan after removal of the aortic constriction had no influence on the return of HBR to the control value. Fig. 5 also shows that losartan also had no effect on the complete recovery of T1.6/0.8 after regression of LVH, and that the action potential also remained prolonged. For reference, the data for the maintained-LVH group are also shown. Equally, longitudinal conduction velocity,
L, only partially recovered in the deconstricted group, with or without losartan; the values in both groups were significantly different from both the sham-operated and the maintained-LVH groups. The transverse conduction, and hence the computed conduction anisotropy data were not completely comparable between the de-banded groups with and without losartan. With losartan the mean value of transverse conduction velocity did reduce after de-banding, but the recovery was statistically incomplete.
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It may be concluded that losartan was able to prevent the generation of cardiac hypertrophy induced by angiotensin infusion, along with the limited number of electromechanical changes observed in this model of cardiac hypertrophy. However, losartan had no effect on ameliorating the magnitude of hypertrophy, and the associated electromechanical changes, after aortic constriction. Furthermore, losartan, at least over 42-day administration, had no effect on the regression process, in particular the electrophysiological changes that persisted after cardiac size had normalised were unaffected by treatment with losartan.
| 4. Discussion |
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4.1. Alterations to electromechanical function in LVH and its regression
In confirmation of previous work [4,6], constriction of the guinea-pig ascending aorta for about 42 days generated cardiac growth as evidenced by a larger heart-to-body weight ratio (HBR) and an increase of dry heart weight. This was completely reversible on removal of the constriction, after a period comparable to the constriction phase. Morphological regression was accompanied by recovery of contractile function, as evidenced by the staircase response; however, several electrophysiological changes either remained (APD) or recovered only partially (conduction velocity). Whether these variables would eventually normalise after a longer period of de-banding is unclear and requires further study. The risk of arrhythmias in humans is not always reduced with regression of LVH [17], which may in part be due to incomplete recovery of electrophysiological function. Our study concords with a canine model of volume-overload hypertrophy, which showed that despite regression of hypertrophy QT interval remained prolonged [18]. In contrast, a feline model of pressure-overload hypertrophy showed that with regression of wall thickness, ventricular fibrillation thresholds and the ease of induction of ventricular arrhythmias reverted to control levels [19].
A rise of the intracellular [Na+] is an early characteristic of LVH and we have postulated that this is partly responsible for electromechanical changes by indirectly affecting gap junction conductance [3,20]. However, this cannot be the sole explanation, because of the heterogenous changes to conduction velocity. Our data are consistent with a change also to gap junction redistribution around the myocyte, as observed in other models of LVH [21]. However, we do not know the rate and extent of recovery of these cellular and morphological changes during regression of LVH.
Of note was a lack of change to the AP upstroke (dV/dtmax), or the time constant of the AP foot (
ap) associated with any of the interventions. However, both were hastened in transverse conduction pathways, indicative of discontinuous conduction in the myocardial syncitium [22]. Its significance is that reduction of longitudinal conduction velocity in LVH, and the failure to normalise completely on regression of LVH, would emphasise the low safety factor in this axis (i.e. increase the likelihood of conduction failure), and increase the possibility of re-entrant arrhythmias [23]. Both dV/dtmax and
ap are importantly determined by the magnitude and/or kinetics of the Na+ inward current, and implies these did not alter significantly during any intervention. We propose that the persistent changes to conduction in LVH result mainly from alterations to unit gap junction conductance and their redistribution around the myocyte. Moreover it is important to identify conditions that may ameliorate the effect of LVH on altered electrophysiological variables, and if recovery during regression could be hastened. For this reason we investigated the role of angiotensin and AT1 receptor blockade by losartan.
4.2. The pathology associated with LVH and the role of angiotensin
Changes to myocardial function in humans are also associated with an increase of afterload, e.g. with aortic stenosis. In the intact heart this can be manifested as increased QT dispersion [24], and in isolated tissues as prolongation of the action potential and slowed conduction [25]. Furthermore, regression of hypertrophy reduced the electrophysiological changes, but incompletely [24,26], and thus mirror results with our guinea-pig model. Many animal models of hypertrophy are associated with upregulation of the renin–angiotensin system, with an increase of systemic angiotensin-II (AII) and aldosterone levels [27]. The evidence from this study is that angiotensin does not play a prominent role in the changes to electromechanical function associated with thoracic aortic constriction (AC). Firstly, the changes occurring with angiotensin-induced hypertrophy were quite different from those evoked by AC. Secondly losartan had no effect, at the dose used (10 mg·kg–1·day–1) on changes evoked by AC, although it prevented completely the changes induced by angiotensin infusion.
Most studies using AT1 receptor antagonists and ACE inhibitors have focused on regression of hypertrophy itself, and fewer on their ability to reverse associated electromechanical changes. In keeping with our conclusions, other observations have shown that losartan did not regress LVH associated with thoracic AC, nor improve contractile function [28,29]. Concerning other models of hypertrophy AT1 receptor blockade did not reverse electrophysiological changes, nor prevent the development of arrhythmias [30] or improve survival [31].
Whether ACE inhibitors affect regression of LVH in this model requires further study. In rats the ACE inhibitor perindropril prevented the age-related increase in HBR independent of its antihypertensive effects, but did not prevent APD prolongation [32]. However, chronic treatment of SHR rats with capropril restored APD with regression of hypertrophy [33]. Studies in other models of cardiac hypertrophy and failure have shown differential effects of ACE inhibition and AT1 receptor antagonism [34,35]. One possibility is that ACE inhibitors, but not AT1 receptor antagonists, inhibit degradation of bradykinin into non-active metabolites, as bradykinin itself can inhibit progression of hypertrophy [36].
However, in hypertrophy generated by renovascular hypertension both AT1 receptor antagonists and ACE inhibitors normalise ventricular electrophysiology assessed by ventricular fibrillation thresholds, action potential duration and effective refractory periods [37–40]. This model is more similar to our angiotensin-infusion model, but it should be stressed that the electromechanical properties that we described above were not identical to those in this pressure-overload hypertrophy.
In conclusion, induction of LVH by different methods generates variable electromechanical changes to myocardium. Regression of cardiac growth is not accompanied by complete recovery of function, and in particular electrophysiological changes that could predispose the heart to arrhythmias remain altered. Losartan, at a dose sufficient to prevent angiotensin-induced LVH, had no effect on regressing hypertrophy induced by thoracic aortic constriction, nor did it facilitate recovery of function during natural regression of cardiac growth. Further studies may reveal if higher doses, or longer treatment periods with AT1 receptor blockers, ACE inhibitors or direct aldosterone blockers, affect electromechanical changes with aortic constriction.
| Acknowledgements |
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We thank the British Heart Foundation for financial assistance and Merck, Sharp and Dohme for supplying the Losartan.
| Notes |
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Time for primary review 31 days
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p<0.05 with respect to AC values. Mean data±SD.
