# Long-chain acylcarnitines regulate the hERG channel.

Fabio Ferro, Aude Ouillé, Truong-An Tran, Pierre Fontanaud, Patrick Bois, Dominique Babuty, François Labarthe, Jean-Yves Le Guennec

<figure><img src="image_1.png" /></figure>

## To cite this version:

Fabio Ferro, Aude Ouillé, Truong-An Tran, Pierre Fontanaud, Patrick Bois, et al., Long-chain acylcarnitines regulate the hERG channel.. PLoS ONE, 2012, 7 (7), pp.e41686. 10.1371/journal.pone.0041686. hal-00991850

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<figure><img src="image_2.png" /></figure>
# Long-Chain Acylcarnitines Regulate the hERG Channel

Fabio Ferro¹,*, Aude Ouillé²*,³, Truong-An Tran¹, Pierre Fontanaud³, Patrick Bois⁴, Dominique Babuty⁵, François Labarthe¹, Jean-Yves Le Guennec²

¹INSERM U921, Université François-Rabelais, Tours, France, ²INSERM U1046, Université Montpellier-1, Université Montpellier-2, Montpellier, France, ³IGF-CNRS INSERM 661, Université Montpellier-1, Université Montpellier-2, Montpellier, France, ⁴IPBC, UMR 6187, CNRS, Université de Poitiers, Poitiers, France, ⁵CHRU Tours, Hôpital Trousseau, Service de cardiologie B, Tours, France

## Abstract

**Background and purpose:** In some pathological conditions carnitine concentration is high while in othersitis low. In bothcases, cardiac arrhythmiascan occur and lead to sudden cardiac death. It has been proposed that in ischaemia, acylcarnitine (acyl-CAR), but not carnitine, is involved in arrhythmiastrough modulation of ionic currents. We studied the effects of acyl-CARs on hERG, $K_{IR}$2.1 and $K_v$7.1/minKchannels (channels responsible for $I_{KR}$, $I_{K1}$ and $I_{KS}$ respectively).

**Experimental approach:** HEK293 cells stably expressing hERG, $K_{IR}$2.1 or Kv7.1/minK were studied using the patch clamp technique. Free carnitine (CAR) and acyl-CAR derivatives from medium- (C8 and C10) and long-chain (C16 and C18:1) fatty acids were applied intra- and extracellularly at different concentrations. Forstudies onhERG, C16 and C18:1 free fatty acid were also used.

**Key results:** Extracellular long-chain (LCAC), but not medium-chain, acyl-CAR, induced an increase of $I_{hERG}$ amplitude associated with a dose-dependent speeding of deactivation kinetics. They had no effect on $K_{IR}$2.1 or Kv7.1/minK currents. Computer simulations of these effects wereconsistent with changes in action potential profile.

**Conclusions and applications:** Extracellular LCAC tonically regulates $I_{hERG}$ amplitude and kineticsunder physiological conditions. This modulation maycontribute to the changes in action potential duration thatprecede cardiac arrhythmias in ischaemia, diabetes and primary systemic carnitine deficiency.

**Citation:** Ferro F, Ouillé A, Tran T-A, Fontanaud P, Bois P, et al. (2012) Long-Chain Acylcarnitines Regulate the hERG Channel. PLoS ONE 7(7): e41686. doi:10.1371/journal.pone.0041686

**Editor:** Alexander G. Obukhov, Indiana University School of Medicine, United States of America

**Received** January 30, 2012; **Accepted** June 25, 2012; **Published** July 25, 2012

**Copyright:** © 2012 Ferro et al. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.

**Funding:** This work was financially supported by Boston Scientific and the conseil Régional du Centre. The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.

**Competing Interests:** The authors have read the Journal's policy and have the following conflicts: They have received funding from Boston Scientific. There are no patents, products in development or marketed products to declare. This does not alter the authors' adherence to all the PLoS ONE policies on sharing data and materials.

## Introduction

Fatty acids are the primary substrate used by the heart to generate ATP [1]. The initial steps involved in ATP production via β-oxidation include the formation of essential intermediates that facilitate the transport of fatty acids into the mitochondrial matrix where the β-oxidation enzymes are located. More specifically, after their entry into the cell, fatty acids are activated in the cytosol via the formation of acyl-CoA derivatives, which are either incorporated into intracellular lipid pools or enter mitochondria for β-oxidation. Carnitine (CAR) is the essential co-factor needed for mitochondrial fatty acid oxidation. It operates by shuttling long-chain fatty acids as acylcarnitinesesters (acyl-CAR) from the cytoplasm across the inner mitochondrial membrane into the mitochondrial matrix. After their entry into the mitochondria, long-chain acyl-CAR(LCAC) are converted back to long-chain acyl-CoAsesters, which are then β-oxidized into acyl-CoA of progressively shorter chain lengths (i.e. long-, medium-, short-chain acyl-CoA, and ultimately acetyl-CoA). Free carnitineis then recycled [2]. In contrast to acyl-CoA, acyl-CARs diffuse easily through the mitochondrial and plasma membranes.

Thus their blood concentration reflects the fluxesof various mitochondrial β-oxidation steps. This process is also suspected to be protective againstthe accumulation of potentially toxic acyl-CoA derivatives in mitochondria and to preserve free CoA availability for energy metabolism [3].

In normal myocardium, the concentration of acyl-CARs is low, around 2–3 µM, because the transformation of cytosolic acyl-CoA into acyl-CAR is tightly coupled to myocardial energy demand [4–6]. Acyl-CARs are synthesized in the celland they can easily diffuse through the cell membrane and reach the cytosol.

Free fatty acid and acyl-CAR concentrations can increase in some pathological conditionssuch as myocardialischaemia [7], diabetes [8], [9] and genetic fatty acid disorders [10]. The arrhythmias observed in these conditions could be due to a perturbation of cardiomyocyte repolarisation by carnitine or its derivatives.

In pathological conditions such as primary systemic carnitine deficiency or ischaemia, acyl-CARs can either decrease to immeasurably low levels [2] or increase to 30 µM [11] respectively. It has been found that long chain acyl-CARs

<figure><img src="image_3.png" /></figure>

<footnote>* E-mail: aude.ouille@inserm.fr</footnote>

<footnote>‡ These authors contributed equally to the work.</footnote>
modulate the activity of certain calcium and sodium channels at a concentration of 5–10 µM [12–13]. However, the effects of acyl-CARs on outward currents participating in repolarization (hERG, Kv7.1/minK and Kir2.1 channels) have not been studied. Changes in the activity of these potassium channels are known to be associated with ventricular fibrillation and sudden death [14–15]. These arrhythmias could be either due to K⁺ channel blockade, by drugs or loss-of-function by mutations (long QT syndrome), or due to their activation by hyperkalemia, acidosis, digitalis toxicity, hyperthermia [16], or gain-of-function mutations [17].

The purpose of this study was to evaluate the effects of different concentrations of medium- and long-chain acyl-CARson these repolarising potassium channels. A physiological concentration of 3 µM acyl-CAR [5–6], [18], was compared to very low and high acyl-CAR concentrations, applied either intra- or extracellularly.

## Methods

### Cell Culture

HEK293 cells expressing Kv11.1 (hERG channel) were a kind gift from Drs Zhou and January (Madison, USA) [19]. HEK293(LGC Promochem, France) expressing K₅.7.1 associated with minK subunit (KCNE1/gene) and Kir2.1 channel (KCNJ2 gene, IK₁) were made inhouse. Cells were seeded in 25 cm² cell-culture flasks at 37°C and 10% CO₂ and grown in DMEM Dulbecco's modified Eagle's medium supplemented with 10% (v/v) Fetal Bovine Serum (Cambrex Bio Science Verviers, Belgium).- HEK-hERG medium was supplemented with 0.4 mg/ml geneticin (Gibco, Invitrogen Corporation, UK). Culture medium was changed every 2–3 days. Within 7 days, cells were at approximately 80% of confluence. The cells were then harvested using a Dulbecco Phosphate Buffered Saline without calcium and magnesium (DPBS, Cambrex Bio Science Verviers, Belgium)and trypsin (Lonza, Belgium) and seeded in a new culture flask (60000 cells/flask) for following week. Cells were also seeded in 35 mm Petri dishes to obtain a confluence of about 50%on the day of experimentation. Cells were mycoplama negative.

### Whole-cell patch-clamp Recording

Cells were placed on the stage of an inverted microscope (Nikon TE2000-U, Japan). Patch-clamp techniques have been described in detail elsewhere [20]. Currents were recorded by whole-cell voltage clamp with a Biologic RK-400 amplifier (Biologic, Grenoble, France) and an Axopatch 200 B (Axon Instrument, La Jolla, USA). Currents were filtered at 3 kHz (Axopatch) or 2 kHz (Biologic)and sampled at 5 kHz. Borosilicate glass electrodes (GC150F-15, Harvard Apparatus, UK) with tip resistances of 3.5–5 MΩ when filled with the internal solution for IK₄ and IK₁ channel. This solution contained (in mM): KCl 130, MgCl₂ 1, Mg-ATP 5, EGTA 5, HEPES 10, adjusted to pH 7.2 with KOH. The internal solution for studying IK₅ was (in mM): KCl 130, MgCl₂ 1, NaCl 10, CaCl₂ 1, HEPES 5, adjusted to pH 7.2 with KOH. The external physiological saline solution (PSS) contained (in mM): NaCl 137, KCl 4, MgCl₂ 1, CaCl₂ 1.8, D-Glucose 10, and HEPES 10, adjusted to pH 7.4 with NaOH. For HEK-IK₅ experiments we used the perforated-patch configuration which was obtained with 0.250 mg/ml nystatin (Sigma-Aldrich, St Quentin Fallavier, France). Experiments were conducted at 23±1°C. Junction potentials were zeroed before formation of the membrane-pipette seal. Series resistance and capacitance were compensated. Current amplitudes were normalized to cell capacitance and expressed as current density (pA/pF). Cell capacitance ranged between 10 to 20pF. The cell under study

was positioned at the tip of a conical microcapillary that received the outlet of six microcapillaries connected to 10 ml syringes. Superfusion was gravity-driven at 0.4 ml/min.

**I<sub>HERG</sub> protocols.** Cells were held at a membrane potential of –70 mV. After control data were obtained, the superfusion was switched to the chosen acyl-CAR-containing solution, fatty-acid-containing-solution, or E4031-containing solution. Currents were elicited by 5 s test pulses to –10 mV applied every 18 s until steady-state was obtained. Steady-state current-voltage relationships (IV) were obtained by stepping the membrane voltage for 5 s to voltages between –80 and +50 mV by 10 mV increments. Deactivating tail currents were recorded at –55 mV. The activation curves were obtained from the tail current amplitude measured at its peak value. The availability curves were obtained from the maximum current amplitude measured at a test pulse to +40 mV, applied after a two-pulse protocol that consisted of a 1 s depolarizing pulse to +40 mV followed by a second 25 ms pulse to different membrane potentials between –120 and +10 mV. At the end of each experiment, the cellunder study was perfused with E-4031 30 nM (a hERG blocker) (Alomone Labs, Jerusalem, Israel).

**IK₁ protocol.** Cells were held at a membrane potential of –90 mV. A voltage ramp protocol of 1 s duration, from –120 to +40 mV was applied each 11 s. We measured the peak inward current, in the presence or absence of acyl-CAR. At the end of each experiment, the cell under study was perfused with BaCl₂ 150 µM (an IK₁ blocker) (Sigma-Aldrich, St Quentin Fallavier, France).

**IK₅ protocols.** Cells were held at a membrane potential of –70 mV. Steady-state current-voltage relationships (IV) were obtained by stepping the membrane voltage for 3.5 s between –60 and +40 mV in 10 mV increments. Deactivating tail currents were recorded at –30 mV. The activation curves were obtained from the peak tail current amplitude. At the end of each experiment, the cell under study was perfused with Chromanol 293 B15 µM (an IK₅ blocker) (Sigma-Aldrich, St Quentin Fallavier, France).

Command potentials, data acquisition and analysis were generated using Clampex 8.2 (Axon Instrument, Forster City, CA, USA).

Deactivating currents were best described by two exponentials using the following equation:

<table><caption>**Table 1.** Effect of application of intra- or extracellular acyl-CARs on I<sub>HERG</sub> deactivation time constants. The hERG current was fitted to a two exponential function (see Methods for details).</caption><thead><tr><th>Treatment</th><th></th><th>Tau 1<br>Mean ± SEM</th><th>Tau 2<br>Mean ± SEM</th><th>n</th></tr></thead><tbody><tr><td>Control</td><td></td><td>1663±118.5</td><td>314.4±26.5</td><td>12</td></tr><tr><td rowspan="4">Intracellular</td><td>3 µM C8-CAR</td><td>1378.6±75.1</td><td>263.3±12.1</td><td>8</td></tr><tr><td>3 µM C10-CAR</td><td>1467.6±64.5</td><td>306.6±10.6</td><td>7</td></tr><tr><td>3 µM C16-CAR</td><td>1658.4±105.8</td><td>323.5±15.8</td><td>12</td></tr><tr><td>3 µM C18-CAR</td><td>1440.4±120.6</td><td>288.8±26.6</td><td>9</td></tr><tr><td rowspan="4">Extracellular</td><td>3 µM C8-CAR</td><td>1488.6±87.1</td><td>275.8±11.8</td><td>8</td></tr><tr><td>3 µM C10-CAR</td><td>1667.9±101.1</td><td>301.5±17.8</td><td>7</td></tr><tr><td>3 µM C16-CAR</td><td>1077.1±139.7**</td><td>222.2* ±21.3</td><td>7</td></tr><tr><td>3 µM C18-CAR</td><td>1059.4±88.7**</td><td>212.6* ±18.9</td><td>8</td></tr></tbody></table>

The values of tau1 and tau2 are given in ms. Values were obtained when the membrane potential returned to –55 mV after stepping to –10 mV for 5s.
*p<0.05, ** p<0.01.
doi:10.1371/journal.pone.0041686.t001

<figure><img src="image_4.png" /></figure>
$$I = A_0 + A_1 \cdot \exp(-t/\tau_1) + A_2 \cdot \exp(-t/\tau_2).$$

where $τ₁$ and $τ₂$ are the time constants, $A₁$ and $A₂$ are the amplitude of the 1st and 2nd component of the exponential respectively and $A₀$ the amplitude of the remaining current.

Half-maximal voltages ($V_{1/2}$) of activation and availability were determined by fitting data with a Boltzmann equation:

$$I/Imax = 1/\{1 + \exp[-(E - V_{1/2})/s]\}.$$

where $I/Imax$ represents the normalized current, $V_{1/2}$ the half-maximal voltages of activation or availability and $s$ the slope factor. These analyses were performed using Origin 7 (Microcal Software, Northampton, MA, USA).

Acyl-CARs(except oleylcarnitine) were purchased from Drten Brink (Amsterdam, Netherland). Oleylcarnitine and chemicals were purchased from Sigma-Aldrich (St Quentin Fallavier, France). Two medium-chain acyl-CAR derivatives were used: octanoylcarnitine (C8-CAR) and decanoylcarnitine (C10-CAR) and two long-chain palmitoylcarnitine (C16-CAR) and oleylcarnitine (C18-CAR).

To simplify the terminology, we indicate the number of carbon atoms in the aliphatic chain. We used C18:1-CAR rather than C18:0-CAR because the C18:1 carnitine derivative is more abundant in the myocardium than C18:0, in both physiological and pathophysiological conditions [18]. A stock solution of 30 mM Acyl-CARs, dissolved in water, was diluted to experimental concentrations between 1 and 30 µM.

## Mathematical Modelling

The model used in this study is the human endocardial ventricular cell model described by Ten Tusscher & Panvilov [21] in which we replaced the Hodgkin-Huxley equation for $I_{KR}$ by a Markov equation. Following Fink et al. [22] we chose to describe $I_{KR}$ using the following Markov chain which had 3 closed states, one open state and one inactivated state:

$$C1 \underset{k21}{\overset{k12}{\rightleftharpoons}} C2 \underset{k32}{\overset{k23}{\rightleftharpoons}} C3 \underset{k43}{\overset{k34}{\rightleftharpoons}} O \underset{k54}{\overset{k45}{\rightleftharpoons}} I$$

The simplex method was used to fit the experimental data using JSim software.

<figure><img src="image_5.png" /><figcaption>**Figure 1. Effect of extracellular acyl-CARs on $I_{HERG}$. $I_{HERG}$-V relationships, in all graphs, the filled squares represent the current in the absence of acyl-CAR in the pipette (control, n = 12 cells). Aa, effect of 3 µM C8-CAR (empty circles, n = 8 cells) or 3 µM C10-acyl-CAR (filled circles, n = 7 cells); Ab, typical example of C8-CAR (red) compared with PSS (black). Ba, effect of 3 µM C18-CAR (filled circles, n = 9 cells) on $I_{HERG}$-V relationship. The inset shows the effect of 3 µM C18-CAR on end-pulse hERG current elicited by a depolarisation to -10 mV from a holding voltage of -70 mV, obtained on a representative cell (the arrows indicate the current obtained at -10 mV during an IV protocol, see Methods), ***, p<0.001. **, p<0.01. Bb, typical example of C18-CAR (red) compared with PSS (black). doi:10.1371/journal.pone.0041686.g001</figcaption></figure>

<figure><img src="image_6.png" /></figure>
The reaction constants were:

k12 = 0.01507341.exp(0.001459408.V) in PSS and
k12 = 0.02007341.exp(0.07865593.V) in the presence of C16-CAR.

k21 = 0.05364064.exp(-0.19822938.V) in PSS and
k21 = 0.2364064.exp(-0.00011822938.V) in the presence of C16-CAR.

k23 = 0.08927204 in PSS and k23 = 0.02927204 in the presence of C16-CAR.

k32 = 15686841 in PSS and k32 = 0.01686841 in the presence of C16-CAR.

k34 = 0.01066403.exp(0.00131023.V) in PSS and
k34 = 0.15066403.exp(0.0231023.V) in the presence of C16-CAR.

k43 = 0.0005743.exp(-0.0006156.V) in PSS and
k43 = 0.00037433.exp(-0.04078603.V) in the presence of C16-CAR.

k45 = 0.05042237.exp(0.00854485.(V+18)) in PSS and
k45 = 0.16042237.exp(0.01554485.(V+4.5)) in the presence of C16-CAR.

k54 = 0.01731608.exp(-0.04090733.(V+18)) in PSS and
k54 = 0.03731608.exp(-0.05090733.(V+4.5)) in the presence of C16-CAR.

## Statistics

Data are described as mean ± standard error of the mean (n = number of cells). Two-way repeated measures ANOVA followed

A

<figure><img src="image_7.png" /></figure>

B

<figure><img src="image_8.png" /></figure>

C

<figure><img src="image_9.png" /></figure>

D

<figure><img src="image_10.png" /></figure>

**Figure 2.** Effect of extracellular long-chain acyl-CARs on the activation and availability of the hERG current. A, effect of 3 µM C16-CAR on the activation curve. In the absence of C16-CAR (filled squares, n=6 cells), the V₁/₂ is -17.4±0.2 mV while in the presence of 3 µM acyl-CAR (empty squares) the V₁/₂ is -26.5±0.5 mV. B, effect of 3 µM C16-CAR on availability. In the absence of C16-CAR (empty squares, n=6 cells), the V₁/₂ is -35.4±1.4 mV while in the presence of 3 µM acyl-CAR (filled squares) the V₁/₂ is -37.4±0.5 mV. C, effect of 3 µM C18-CAR on activation. In the absence of C18-CAR (filled squares, n=7 cells), the V₁/₂ is -21.0±0.1 mV while in the presence of 3 µM acyl-CAR (empty squares) the V₁/₂ is -23.0±0.2 mV. D, effect of 3 µM C18-CAR on availability. In the absence of C18-CAR (filled squares, n=7 cells) the V₁/₂ is -42.9±1.0 mV while in the presence of 3 µM acyl-CAR (empty squares) the V₁/₂ is -27.0±1.0 mV. *: p<0.01.
doi:10.1371/journal.pone.0041686.g002

<figure><img src="image_11.png" /></figure>
<figure><img src="image_12.png" /><figcaption>**Figure 3.** Concentration-dependent acceleration of $I_{hERG}$ inactivation induced by C18-CAR. The records were obtained in 3 different cells. The current obtained in presence of C18-CAR is shown in red. doi:10.1371/journal.pone.0041686.g003</figcaption></figure>

by a Student–Newmann–Keuls test were used to compare current densities. To compare the effects of acyl-CARs on the kinetics of deactivation, we performed unpaired (intracellular) and paired (extracellular) Student's t-test. Differences were considered as statistically significant when $p<0.05$.

## Results

### Acylcarnitines have no impact on $I_{hERG}$ when applied intracellularly

We compared $I_{hERG}$ in the absence or presence of intracellular free carnitine, medium-chain acyl-CARs (e.g. C8-

<figure><img src="image_13.png" /><figcaption>**Figure 4.** Effect of extracellular C18-CAR on hERG activation and availability. A. Activation curve in PSS (squares): $V_{1/2} = -20.3 \pm 0.1$ mV (n = 10); in the presence of 1 µM C18-CAR (circles): $-22.8 \pm 0.1$ mV (n = 8); in the presence of 3 µM C18-CAR (diamonds): $-30.0 \pm 0.3$ mV (n = 8) and in the presence of 10 µM C18-CAR (triangles): $-31.9 \pm 0.9$ mV (n = 4). B. Availability curve in PSS (squares): $V_{1/2} = -40.9 \pm 2.3$ mV (n = 8); in the presence of 1 µM C18-CAR (circles): $V_{1/2} = -36.2 \pm 3.1$ mV (n = 8); in the presence of 3 µM C18-CAR (diamonds): $V_{1/2} = -34.8 \pm 1.4$ mV (n = 8) and in the presence of 10 µM C18-CAR (triangles): $V_{1/2} = -35.6 \pm 2.1$ mV. doi:10.1371/journal.pone.0041686.g004</figcaption></figure>

<figure><img src="image_14.png" /></figure>
<table><caption>**Table 2.** Effect of different concentrations of extracellular C18-CAR on I<sub>hERG</sub> deactivation time constants.</caption><thead><tr><th rowspan="2">Treatment</th><th colspan="2">Tau1</th><th colspan="2">Tau2</th></tr><tr><th>Mean ± SEM</th><th>n</th><th>Mean ± SEM</th><th>n</th></tr></thead><tbody><tr><td>PSS</td><td>2331±160</td><td>13</td><td>469±37</td><td>13</td></tr><tr><td>C18-CAR 1 µM</td><td>2289±154</td><td>8</td><td>431±18</td><td>8</td></tr><tr><td>C18-CAR 3 µM</td><td>1659±360**</td><td>4</td><td>326±72*</td><td>4</td></tr><tr><td>C18-CAR 10 µM</td><td>772±82***</td><td>3</td><td>191±14**</td><td>3</td></tr><tr><td>C18-CAR 30 µM</td><td>638±98***</td><td>4</td><td>176±15***</td><td>6</td></tr></tbody></table>

Values obtained when the membrane potential returned to -55 mV after stepping to -10 mV for 5 s. *p<0.05, **P<0.01, ***P<0.001. doi:10.1371/journal.pone.0041686.t002

CAR and C10-CAR), or long-chain acyl-CARs(e.g. C16-CAR and C18-CAR). Compared to the physiological concentration (3 µM), absence of acyl-CAR in the pipette had no impact on I<sub>hERG</sub> (data not shown). Raising the concentration of the various acyl-CARs from 3 µM to 30 µM had no effect on the amplitude of the current (data not shown). Similarly, the kinetics of deactivation of the current were not affected by the various acyl-CARs, whatever their chain length (Table 1). We concluded that CAR and acyl-CAR had no impact on I<sub>hERG</sub> when applied intracellularly.

## Long-chain Acylcarnitines Increase I<sub>hERG</sub> Amplitude and Accelerate Deactivation when Applied Extracellularly

Acyl-CARs of various chain lengths were applied extracellularly. Free CARs (data not shown) or medium-chain acyl-CARs had no impact on the amplitude of I<sub>hERG</sub> (fig.1A). In contrast, 3 µM C18-CAR increased the amplitude of the end-pulse current. This effect took about 2 minutes to be complete and occurred at almost

all voltages (fig. 1B). Similar results were obtained with 3 µM C16-CAR, another LCAC derivative (data not shown). External application of 3 µM C16-CAR for about 4 minutes led to a significant leftward shift of the activation curve without any effect on the availability properties (fig. 2A and 2B). Conversely, C18-CAR did not affect the activation properties while the availability curve was shifted to the right (fig. 2C and 2D). We concluded from these experiments that extracellularly-applied long-chain acyl-CAR increased I<sub>hERG</sub> amplitude in a manner, dependent on their chain length.

LCAC also affected deactivation kinetics when they are applied extracellularly, 3 µM C16-CAR and C18-CAR significantly increased deactivation kinetic (by about 30-35%), whereas medium-chain acyl-CAR had no effect on deactivation (fig. 3 and Table 1).

## The Effects of Long-chain Acylcarnitines are Dose-dependent

Increasing the concentration of C18-CAR from 1 to 30 µM caused an increase in I<sub>hERG</sub> amplitude (fig. 4) and deactivation kinetics (Table 2). Similar results were obtained with C16-CAR (data not shown).

## Accelerated Deactivation is not Due to Fatty Acid Alone

In order to understand the specificity of the effect of long-chain acyl-CAR on hERG channels, we investigated the effects of two long-chain free fatty acids with the same chain length. Extracellular application of 3 µM palmitoyl methyl ester (C16:0) or oleyl methyl ester (C18:1) caused a leftward shift of the activation curve with no change in the availability curve, reproducing increase of I<sub>hERG</sub> amplitude caused by long-chain acyl-CARs (data not shown). In contrast, long-chain fatty acids did not change the deactivation kinetics (Table 3 and fig. 5). This suggests that the effect of long-chain acyl-CARs on the deactivation of I<sub>hERG</sub> was specifically related to long-chain acyl-CAR derivatives.

<table><caption>**Table 3.** Effect of extracellular C16 free fatty acid either alone or in combination with C16-CAR on I<sub>hERG</sub> deactivation time constants.</caption><thead><tr><th colspan="7">Tau1</th></tr><tr><th rowspan="2">Voltage (mV)</th><th colspan="2">PSS</th><th colspan="2">C16</th><th colspan="2">C16+ C16-CAR</th></tr><tr><th>Mean ± SEM</th><th>n</th><th>Mean ± SEM</th><th>n</th><th>Mean ± SEM</th><th>n</th></tr></thead><tbody><tr><td>-30</td><td>2620.3±497.6</td><td>6</td><td>2780.7±220.7</td><td>5</td><td>2620.3±497.6</td><td>6</td></tr><tr><td>-20</td><td>2661.7±226.9</td><td>6</td><td>2131.7±148.9</td><td>5</td><td>2661.7±226.9</td><td>6</td></tr><tr><td>-10</td><td>2076.7±85.1</td><td>7</td><td>2012.8±122.1</td><td>7</td><td>2076.7±85.1</td><td>7</td></tr><tr><td>0</td><td>2070.5±133.4</td><td>7</td><td>1973.2±135.8</td><td>7</td><td>2070.5±133.4</td><td>7</td></tr><tr><td>10</td><td>2028.8±116.7</td><td>7</td><td>1927.7±113.4</td><td>7</td><td>2028.8±116.7</td><td>7</td></tr><tr><th colspan="7">Tau 2</th></tr><tr><td>-30</td><td>670.3±123.6</td><td>5</td><td>587.5±52.4</td><td>7</td><td>370.5±48.6*</td><td>7</td></tr><tr><td>-20</td><td>590.1±87.3</td><td>7</td><td>522.4±88.7</td><td>7</td><td>284.8±36.2***</td><td>7</td></tr><tr><td>-10</td><td>381.0±23.1</td><td>7</td><td>364.3±22.5</td><td>7</td><td>257.0±29.0***</td><td>7</td></tr><tr><td>0</td><td>349.3±24.2</td><td>7</td><td>337.9±25.4</td><td>7</td><td>242.0±27.3***</td><td>7</td></tr><tr><td>10</td><td>339.8±22.6</td><td>7</td><td>310.8±13.2</td><td>7</td><td>236.4±25.5***</td><td>7</td></tr></tbody></table>

Values obtained when the membrane potential returned to -55 mV after stepping to the voltage indicated in the left column in mV for 5 s. The current was fitted to a two exponential function (see Methods). The values of tau1 and tau2 are expressed in ms. *p<0.05, **P<0.01, ***P<0.001. doi:10.1371/journal.pone.0041686.t003

<figure><img src="image_15.png" /></figure>
<figure><img src="image_16.png" /><figcaption>**Figure 5.** The effect of extracellular C16 or C16-CAR on deactivation kinetics of I<sub>hERG</sub>, when membrane potential returned to −55 mV from a 5sto −10 mV. ** p<0.01.**
doi:10.1371/journal.pone.0041686.g005</figcaption></figure>

Acylcarnitines do not Affect K<sub>IR</sub>2.1or Kv7.1/minK
Channels

To evaluate a possible impact of extracellular acyl-CAR on the K<sub>IR</sub>2.1 channel, we compared the current in the absence or presence of long-chain acyl-CARs. At concentrations up to 10 µM, C16-CAR has no effect on I<sub>K1</sub>amplitude (fig. 6). Application of 3 µM C16-CAR had no effect on Kv7.1/minK channel amplitude (fig. 7) or kinetics (data not shown).

Discussion

Summary of Results

In this study we compare the effects of free carnitine and acyl-
CARon hERG, Kv7.1/minKand K<sub>IR</sub>2.1 channels. Acyl-CARs
with different aliphatic hydrocarbon tail lengths, were applied at
different concentrations to both intra- and extracellular sides of the
cell membrane. Palmitoyl-carnitine had no effect on K<sub>IR</sub>2.1 and
Kv1.7/minK at concentrations up to 10 µM but some effects were

observed on the hERG channel. These effects were specific to
extracellular LCAC. Intracellular application of free carnitine or
acyl-CARs had no effect on any current, irrespective of the acyl
chain length. At the extracellular side of the membrane, free
carnitine and medium-chain acyl-CAR up to 30 µM had no effect.
Only LCAC had some effects on hERG current.

When applied extracellularly, LCACs induced increased I<sub>hERG</sub>
probably due to the leftward shift of the activation for C16-CAR
and rightward shift of the availability for C18-CAR. This effect
began at 1 µM, a physiological concentration of LCAC, and
increased dose-dependently. Since other potassium channels
(K<sub>IR</sub>2.1 and K<sub>V</sub>7.1/mink) were not sensitive to LCAC, it is likely
that these are direct effects on the channel protein and not due to
any non-specific effects of the lipophilic compounds on the plasma
membrane. These results suggest a tonic regulatory role of
physiological concentrations of long-chain acyl-CAR on I<sub>KR</sub>.

<figure><img src="image_17.png" /></figure>

<figure><img src="image_18.png" /><figcaption>**Figure 6.** Effect of C16-CAR on I<sub>K1</sub>. A, mean current measured at −120 mV and normalized to the current in PSS (n = 7 cells). B, typical example of I<sub>K1</sub> elicited by a ramp of voltage between −120 and +40 mV, with (red) or without (black) 10µM C16-CAR.
doi:10.1371/journal.pone.0041686.g006</figcaption></figure>

<figure><img src="image_19.png" /></figure>
<figure><img src="image_20.png" /></figure>

<figure><img src="image_21.png" /></figure>

<figure><img src="image_22.png" /></figure>

<figure><img src="image_23.png" /></figure>

**Figure 7.** Effect of 3 µM C16-CAR on $I_{KS}$. A, $I_{KS}$-V curves of the current at the end of the pulse (Aa) and peak tail current (Ab). B, Typical examples of families of currents in the absence (Ba) and presence of C16-CAR (Bb). doi:10.1371/journal.pone.0041686.g007

## Effects of Long-chain Acylcarnitines on Other Ion Channels

The regulation of ion channels by acyl-CAR has been widely studied in recent years. In every case, the comparison was between high concentrations of LCAC (up to 30 µM) and no LCAC, two situations now known to be pathological. Most of these previous studies were focused on the specific effect of C16-CAR. Various effects have been described depending on whether the acyl-CAR was applied extra- or intracellularly and also depending on the technique used to study the currents. Wu and Corr [12] found that C16-CAR applied extra- or intracellularly led to an inhibition of the whole-cell L-type calcium current in guinea-pig ventricular myocytes. Conversely, Liu and Rosenberg [23] found that 1 µM C16-CAR increased the open probability of reconstituted cardiac L-type calcium channels in membrane bilayers. $I_{K,ATP}$ was blocked by micromolar concentrations of C16-CAR when applied to the internal face of the membrane in the inside-out configuration of the patch clamp technique [24]. Sato *et al.* [25] reported that this amphipathic molecule reduced $I_{K1}$ but only when it is applied at concentrations higher than 10 µM. Sato *et al.* reported a reversible blockade of the sodium current associated with a slowing of both activation and inactivation properties when 5 µM C16-CAR was applied extracellularly [26]. Rat cardiac ventricular $I_{TO}$ was inhibited by C16-CAR in a dose-dependent manner when present in the pipette solution, but had no effect

when superfused extracellularly [27]. In agreement with our results, these authors did not observe any effect on $I_{K1}$ whether the amphipathic molecule was applied intra- or extracellularly at concentrations up to 10 µM.

Surprisingly, there has been no previous study of the effects of LCAC on the hERG (or $I_{KR}$) and $I_{KS}$ even though these channels are considered to be the target of drugs which seek to prevent ventricular fibrillation and sudden cardiac death see [15].

## Effects of Long-chain Acylcarnitines on hERG Channel

From our experiments on HEK293 cells stably expressing hERG, we can infer that LCAC regulate hERG channel activity via an extracellular site. Indeed, long-chain acyl-CARs are associated with an increase in the speed of deactivation of the channel compared to the “pathological” condition where acyl-CAR is absent. This effect is dose-dependent, at least up to 30 µM. Both, C16-CAR and C18-CAR increase the amplitude of the current but the mechanism of increased current amplitude is different. C16-CAR induced a shift of the activation curve in the hyperpolarizing direction without any effect on the availability curve. C18-CAR has no effect on the activation curve but provoked a shift in the availability curve in the depolarizing direction. Interestingly, quite similar results were obtained by Wang *et al.* [28] with lysophosphatidylcholine (LPC) having a C16:0 or C18:1 as acyl groups. Changing the positively charged phosphatidylcholine with phosphatidylcholineglycerol was associ-

<figure><img src="image_24.png" /></figure>
<figure><img src="image_25.png" /><figcaption>**Figure 8.** Computer simulation of the effects of LCAC on $I_{KR}$ and the human ventricular action potential. A, families of currents mimicking $I_{KR}$ with or without acyl-CARs. B, action potential profile in the absence of acylcarnitine (black line) or the presence of a physiological concentration of 3 µM LCAC (red line). doi:10.1371/journal.pone.0041686.g008</figcaption></figure>

ated with substantial modifications of the effects underlying the important role played by this charged head. These authors concluded that the effects they observed were not due to membrane incorporation of the lipids or to any intracellular signalling pathways currently known to be related to these lipids. They proposed that there must be a direct interaction of the lysophospholipid molecules with the channel protein. However, they also proposed that these lipids could modify hERG activity *via* unidentified pathways. In the present work, we found that acyl-CARs had no effect on the hERG current, at concentrations up to 30 µM. So either these lipids do not incorporate into the membrane or their incorporation has no effect on the activity of the ion channel. In contrast, LCAC can incorporate into the plasma membrane and modify membrane fluidity. However, there is no effect of the fatty acids palmitate and stearate that can also integrate the membrane. Also, LCAC does not affect $K_{IR}$2.1 and $K_V$7.1/mink currents. Thus, the electrophysiological effects of LCAC on $I_{hERG}$ are dependent on the aliphatic hydrocarbon tail length but are unlikely to involve changes in plasma membrane properties. These results are in agreement with previously reported cases of cardiac arrhythmias associated with inherited fatty acid oxidation disorders in human. Indeed, Bonnet *et al*. [29] reported that cardiac arrhythmias and sudden death were usually observed in patients with genetic disorders of long-chain fatty acid oxidation

associated with long-chain acyl-CAR accumulation. In contrast, cardiac electrical disturbances were absent in patients with medium-chain fatty acid oxidation deficiency, a condition associated with a specific increase in medium-chain acyl-CAR but normal long-chain derivatives [28].

Our observations suggest that there is a dual interaction of the acyl group and the charged head of the LPC or LCAC with the channel. Since the physiological concentration of LCAC is between 1 and 3 µM [5–6], [18], there must be a tonic regulation of hERG channels by long-chain acyl-CAR under physiological conditions.

## Consequences of Extracellular Accumulation or Depletion of Long-chain Acylcarnitines under Pathological Conditions

Acyl-CAR concentration can reach 10 µM in some pathological conditions such as myocardial ischaemia [7], diabetes [8], [9], or genetic fatty acid disorders [10]. Conversely there is a drop in CAR and acyl-CAR cytosolic concentrations in primary systemic carnitine deficiency [2]. All these pathological situations are associated with cardiac arrhythmias and sudden cardiac death [29–32], [2]. Accordingly, hERG regulation by LCAC could play a

<figure><img src="image_26.png" /></figure>
role in the cardiac arrhythmias genesis observed in these
pathological conditions.

Consequences for the Action Potential?

An increase of I<sub>KR</sub>, the cardiac current encoded by hERG,
could lead to a reduction of the action potential duration.
However, it is known that this channel inactivates and reactivates
very rapidly leading to a higher current during the final
repolarisation phase than during the plateau phase of the action
potential. Since the deactivation of the current is accelerated, the
current during the action potential must be lower. Indeed, Clancy
and Rudy [33] reported a case of congenital long QT syndrome
due to a mutation of hERG leading to an acceleration of I<sub>KR</sub>
deactivation kinetics (see also Rudy and Silva [34]). This speeding
of deactivation could overcome the effect on the increased
amplitude. To investigate this point, we simulated hERG current
in the presence and absence of C16-CAR 3 µMusing Markov
equations (see methods). Introducing such a current in the human
endocardial ventricular cell model developed by TenTusscher and
Panfilov [21] showed that the regulation of the hERG by C16-
CAR could be responsible for a pronounced shortening of the

action potential. This indicates that with the absence of carnitine,
there must be an increased APD (fig. 8) while the opposite could
be induced with an accumulation of LCAC, both conditions being
potentially pro-arrhythmic.

Summary

The results of this study demonstrate that long-chain acyl-CARs
have regulatory properties on the hERG channel. These
electrophysiological effects were not observed with medium-chain
acyl-CARs. This emphasizes the relationship between long-chain
fatty acid metabolism and cardiac electrical activity that contribute
to cardiac arrhythmias associated with LCAC depletion or
accumulation occurring in some pathologies.

Author Contributions

Conceived and designed the experiments: FF AO TAT PF PB DB FL JYLG. Performed the experiments: FF AO TAT PF PB DB FL JYLG. Analyzed the data: FF AO TAT PF PB DB FL JYLG. Contributed reagents/materials/analysis tools: FF AO TAT PF PB DB FL JYLG. Wrote the paper: FF AO TAT PF PB DB FL JYLG.

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<figure><img src="image_27.png" /></figure>