Abstract
Mitochondria must maintain tight control over the electrochemical gradient across their inner membrane to allow ATP synthesis while maintaining a redox-balanced electron transport chain and avoiding excessive reactive oxygen species production. However, there is a scarcity of knowledge about the ion transporters in the inner mitochondrial membrane that contribute to control of membrane potential. We show that loss of MSL1, a member of a family of mechanosensitive ion channels related to the bacterial channel MscS, leads to increased membrane potential of Arabidopsis mitochondria under specific bioenergetic states. We demonstrate that MSL1 localises to the inner mitochondrial membrane. When expressed in E. coli, MSL1 forms a stretch-activated ion channel with a slight preference for anions and provides protection against hypo-osmotic shock. In contrast, loss of MSL1 in Arabidopsis did not prevent swelling of isolated mitochondria in hypo-osmotic conditions. Instead, our data suggest that ion transport by MSL1 leads to dissipation of mitochondrial membrane potential when it becomes too high. The importance of MSL1 function was demonstrated by the observation of a higher oxidation state of the mitochondrial glutathione pool in msl1-1 mutants under moderate heat- and heavy-metal-stress. Furthermore, we show that MSL1 function is not directly implicated in mitochondrial membrane potential pulsing but is complementary and appears to be important under similar conditions.
INTRODUCTION
The bioenergetic function of mitochondria is crucially dependent on the impermeable nature of their inner membrane to protons such that an electrochemical gradient can be established by the proton-pumping activity of the respiratory chain. This provides the proton motive force (Δp) that powers the F1F0ATP synthase. In plant mitochondria, the presence of an active K+/H+ exchange across the inner membrane (Hensley and Hanson, 1975; Zotova et al., 2010) means that ΔpH is a relatively minor component of Δp in plant mitochondria (Mitchell and Moyle, 1969; Nicholls, 1974; Santo-Domingo and Demaurex, 2012). In addition to K+/H+ exchange, it has long been apparent that plant mitochondrial membranes are permeable to other cations and anions (Moore and Wilson, 1977; Huber and Moreland, 1979; Jung and Brierley, 1979). However, the transporter proteins responsible for these ion fluxes are largely unknown and the purpose of these other ion-transport capabilities has not been established. One possibility is that ion transporters lead to a net transfer of charge from the intermembrane space to the matrix that serves to dissipate mitochondrial membrane potential (ΔΨM) and results in the endogenous inner membrane ‘leak’ observed in energised mitochondria. This is apparent as continued electron transport (oxygen consumption) in the absence dissipation of ΔpH by F1F0ATP synthase and can be stimulated by metals such as cadmium (Kesseler and Brand, 1994b, a, c). While membrane leak is disadvantageous in terms of ATP production it would be beneficial in situations where there is an imbalance between the rate of electron transport/proton pumping and F1F0ATP synthase activity, leading to a very high electrochemical potential across the inner membrane. Such an imbalance leads to increased production of damaging reactive oxygen species (ROS) because the large electrochemical gradient makes it harder for the respiratory chain complexes to pump protons against that gradient. Because redox cycling of complexes I, III and IV is coupled to proton pumping, this has the effect of reducing the rate of electron transport in the respiratory chain. As a result, the respiratory complexes become highly reduced which increases the propensity for ROS production by transfer of single electrons to molecular oxygen (Møller, 2001). Ion transport events that reduce the electrochemical gradient would therefore help prevent ROS production by easing the restriction on respiratory chain electron transport.
One established mechanism in which ion transport process functions in this way is mediated by uncoupling protein (UCP; (Vercesi et al., 2006)) that allows movement of protons from the intermembrane space to the matrix, most likely via an indirect mechanism involving transport of anionic fatty acids (Jezek et al., 1997). UCP is activated under conditions of bioenergetic imbalance (Smith et al., 2004) and has been demonstrated to reduce the production of mitochondrial ROS and to protect against oxidative stress (Barreto et al., 2014). Although activation of UCP is rapid, inactivation probably involves the turnover of the protein (Azzu et al., 2010) and thus UCP can be considered a medium timescale response to persistent mitochondrial imbalance caused by environmental stress. However, to maintain homeostasis there must also be mechanisms that can operate on a short timescale. Rapid, short term dissipation of ΔΨM has been observed in plant mitochondria with transients (pulses) lasting less than a minute (Schwarzländer et al., 2012). This appears to involve selective cation transport although the transporter or channel responsible has not been identified. Although the first molecular details of regulated cation transport in plant mitochondria are beginning to emerge with the identification of proteins involved in mitochondrial Ca2+ transport (Wagner et al., 2015; Wagner et al 2016, it is not yet clear if these proteins are involved in bioenergetic balancing. More work needs to be done to fully understand the mechanisms of ion transport in plant mitochondria and the biochemical and physiological roles of the transport events.
To this end, we searched for putative mitochondrial transporter proteins in Arabidopsis based on sequence analysis (identification of a mitochondrial targeting peptide and presence of extensive hydrophobic domains of sufficient length to be membrane spanning). One of the proteins we identified is a member of the MscS-Like (MSL) family of mechanosensitive ion channels (At4g00290; MSL1 (Hamilton et al., 2015a)). This ten-member gene family was initially identified in Arabidopsis based on homology with the bacterial mechanosensitive ion channel of small conductance MscS (Pivetti et al., 2003). The MSL proteins have different subcellular locations and have been identified or predicted to localise to the plasma membrane, ER and plastid, with MSL1 being the only member with a putative mitochondrial localisation (Hamilton et al., 2015a). Like their bacterial homologs, the MSL proteins characterized to date can be stretch-activated ion channels and show a slight preference for anions (Maksaev and Haswell, 2012; Hamilton et al., 2015b). In bacteria, stretch-activation of MscS promotes survival of hypo-osmotic shock: opening of the channel following cell swelling leads to the release of ions, reducing the cell’s osmotic potential (Levina et al., 1999). A similar hypo-osmotic shock protection role within plastids and during pollen germination has been demonstrated for specific Arabidopsis MSL family members (Veley et al., 2012; Hamilton et al., 2015b). Nevertheless, MSL proteins also appear to have other functions in plants including control of plastid division (Haswell and Meyerowitz, 2006; Wilson et al., 2011) and activation of programmed cell death by the plasma membrane-localised MSL10 (Veley et al., 2014). In this paper, we present a characterisation of the localisation and electrophysiological properties of MSL1 and investigate the conditions under which it is important for bioenergetics homeostasis.
RESULTS
MSL1 is an integral membrane protein in the mitochondrion
Among the ten MSL genes that harbour a conserved MscS domain in Arabidopsis, only MSL1 has a consensus mitochondrial class II (-3 R) cleavage site at Phe-79 (RAF↓SS; (Huang et al., 2009)). It is also the MSL family member that has been identified by previous proteomic analyses in either mitochondria- or plastid-enriched fractions (Froehlich et al., 2003; Zybailov et al., 2008; Ferro et al., 2010; Klodmann et al., 2011; Nikolovski et al., 2012), raising the possibility that MSL1 may be dual-targeted. To clarify the subcellular localization of MSL1, a C-terminal MSL1-GFP fusion was expressed under the control of the 35S promoter in transgenic Arabidopsis plants. Confocal laser scanning microscope (CLSM) imaging of leaf epidermal cells in this transgenic line revealed that MSL1-GFP localized to subcellular structures resembling mitochondria (Figure 1A). MSL1-GFP co-localized with the mitochondrial marker MitoTracker Red in root hair cells (Figure 1B), confirming a mitochondrial localization. To further verify MSL1 localization, an in vitro import assay was carried out by incubating radiolabelled precursor MSL1 with isolated mitochondria under conditions that support import (Figure 1C). MSL1 was imported into a proteinase K-resistant location inside mitochondria. Import required a negative mitochondrial membrane potential, as evidenced by the lack of proteinase K-protected mature MSL1 in the presence of valinomycin (Figure 1C). The presence of a processing intermediate and a mature protein indicate that MSL1 is most likely imported via a two-step process common to the import of inner membrane proteins that contain a cleavable pre-sequence (Murcha et al., 2004). In contrast, MSL1 is not imported into chloroplasts in vitro (Supplementary Figure 1), providing additional evidence that MSL1 is exclusively localized to mitochondria.
MSL1 is reported to be uniformly expressed across tissue types and developmental stages, as well as under most biotic and abiotic treatments (Genevestigator and AtGenExpress Visualization Tool analysis). To analyse the physiological and functional relevance of MSL1 in plant, we isolated a homozygous T-DNA insertion line (msl1-1) that carries a T-DNA insertion in the first exon leading to an absence of MSL1 transcript (Supplementary Figure 2A, B). A homozygous msl1-1 line complemented with a construct containing the genomic version of MSL1 controlled by its native promoter was also generated (msl1-1/gMSL1; Supplementary Figure 2B, C). Both transgenic lines show similar growth and morphology to wild type plants under standard growth conditions on agar plates and on soil (Supplementary Figure 2D). Using these genetic resources we confirmed that a peptide antibody raised against the C-terminal end of MSL1 was specific for this protein (Supplementary Figure 2C). We then further used this antibody to assess the precise intra-mitochondrial localization and orientation of MSL1. Based on the consensus TM prediction algorithms in ARAMEMNON (Schwacke et al., 2003), MSL1 is probably comprised of five transmembrane helices. When isolated mitochondrial membranes were fractionated into carbonate-soluble (peripheral) and -insoluble (integral) membrane proteins and analysed by Blue-Native PAGE and immunoblotting, MSL1 could only be found in the integral membrane fraction and migrated as a large ~350 kDa oligomeric complex (after correction by a factor of 0.7 for digitonin and Coomassie binding (Wittig et al., 2010)) (Figure 1D). The immuno-reactive protein band on Blue-Native PAGE was confirmed to be MSL1 by analysis of trypsin-digest-peptides using mass spectrometry (Supplementary Data 1). Furthermore, no trypsin-cleavable peptide fragments preceding Ser-83 (i.e. the mitochondrial targeting sequence) were detected (Supplementary Data 1), suggesting that MSL1 is imported into the mitochondrial matrix where its pre-sequence is cleaved before it is inserted, most likely, into the inner membrane. To test this, we assessed the accessibility of MSL1 to degradation by proteinase K in inner membrane vesicles lacking the outer membrane (mitoplasts) by immuno-blotting of MSL1 and marker proteins. Successful preparation of outer membrane-free mitoplasts was confirmed by the absence of the voltage-dependent anion channel (VDAC, outer membrane) and the sensitivity of cytochrome c (intermembrane space) to degradation by proteinase K (Figure 1E). Both an MSL1-containing complex and the inner membrane protein SLP2 (Gehl et al., 2014) were detected in the mitoplast fraction treated with proteinase K (Figure 1E). The detection of MSL1 band by anti-MSL1 antibodies, which recognize a short hydrophilic peptide sequence near the C-terminal end of MSL1 (see Materials and Methods), indicates that this region of the protein is in the matrix and is not accessible to proteinase K. In summary, MSL1 is an integral inner membrane protein of mitochondria with the C-terminus orientated towards the matrix.
MSL1 activity is a stretch-activated ion channel
To establish if MSL1 forms a mechanosensitive (MS) ion channel we used single-channel patch clamp electrophysiology. An N-terminal 6xHis-AtMSL1 construct was expressed in an E. coli strain that lacks all seven known mechanosensitive ion channels (MJF641, Δ7, (Edwards et al., 2012)) to provide an electrophysiologically-silent background. When expressed in E. coli, the 6xHis-tagged mature MSL1 (lacking its predicted mitochondrial targeting peptide) can be found in the total soluble fraction (Supplementary Figure 3A) and forms a large complex with a similar oligomeric size to the mitochondrial MSL1 (Supplementary Figure 3B; Figure 1D). Giant E. coli spheroplasts expressing mature MSL1 produced ion channel activity in response to increased lateral membrane tension, applied as suction—or negative pressure—through the patch pipette (Figure 2A).
The current/voltage plot for MSL1 gated by tension between +40 to −180 mV (Figure 2B) reveals that at negative membrane potentials, MSL1 has a single channel conductance of 1.2 nS. This is the same single channel conductance observed for E. coli MscS in the same system (Booth et al., 2011; Kung et al., 2010). However, MSL1 activity in E. coli spheroplasts was less stable than MscS, alternating more frequently between conducting and non-conducting states. MSL1 is likely to be oriented in the E. coli plasma membrane the same way as MscS, with the C-terminus facing the cytoplasm (Miller et al., 2003). MSL1 is similarly oriented in the inner membrane of mitochondria, with the C-terminus in the matrix (Figure 1). Both the E. coli plasma membrane and the mitochondrial inner membrane have strongly negative membrane potentials, indicating that MSL1 is likely to have high conductance in mitochondria once it is gated by membrane tension. Even in the absence of applied tension, we routinely observed noisy activity that may represent MSL1 channel opening at strongly negative membrane potentials (−160 mV or higher, double asterisk in Figure 2C). However, the membranes of E. coli giant spheroplasts deteriorate under such high membrane potentials, and it is therefore formally possible that this activity represents current fluctuation associated with imminent patch rupture (arrow, Figure 2C). We occasionally (in about 20% of patches) observed more easily identified opening and closing events without added tension at moderate membrane potentials (−60 to −100 mV, single asterisk, Figure 2C), suggesting that MSL1 may be voltage-gated, although it remains possible that this activity may be a response to transient fluctuations in patch tension. At positive membrane potentials, which are not physiologically relevant for E. coli or for the inner mitochondrial membrane, MSL1 channel activity was reduced and unstable (Supplementary Figure 4).
The anion preference of MSL1 was found to be very mild (Figure 2D), with a reversal potential (Erev) of 10.2 mV and a preference for anions over cations (PCl: PK) by a factor of ~2.2. These characteristics closely resemble those reported previously for EcMscS under the same experimental conditions in giant spheroplasts (Erev = 9.5 mV, (Edwards et al., 2008), Erev = 12 mV, (Li et al., 2002)) and when EcMscS was reconstituted into the liposomes (PCl: PK = 1.5, (Sukharev, 2002)), PCl: PK = 2.7 (Cox et al., 2013)). These results indicate that MSL1 is essentially non-selective and when open allows the passage of small anions and cations with similar efficiency.
MSL1 can provide modest protection against hypo-osmotic shock in E. coli but not in plant mitochondria
In bacteria, MscS protects against hypo-osmotic shock; the increased membrane tension due to cell swelling causes stretch-activated opening of the channel and release of ions, reducing the osmotic potential of the cell (Naismith and Booth, 2012). To determine if MSL1 was similarly capable of protecting bacterial cells from hypo-osmotic shock, MSL was expressed in the E. coli strain MJF465 that lacks three key mechanosensitive ion channels, MscS, MscL, and MscK (Levina et al., 1999). As expected, MJF465 cells do not survive severe hypo-osmotic shock, but this sensitivity could be fully rescued by expressing MscS from an IPTG-inducible plasmid (Figure 3A). Inducible expression of MSL1 resulted in partial rescue (40% of wild type survival) of the MJF465 osmotic shock sensitivity. Similar results were previously obtained for MSL3, a plastid-localized MscS homolog also from Arabidopsis (Haswell and Meyerowitz, 2006). To establish if MSL1 fulfils a similar osmotic-shock protection role in plant mitochondria, we examined the hypo-osmotic swelling behaviour of mitochondria isolated from WT and msl1-1 seedlings. After labelling with the membrane-potential-independent dye MitoTracker Green (MTG), mitochondria were subjected to hypo-osmotic shock and were visualized under CLSM (Figure 3B). Mitochondrial volumes were calculated from Z-stacks (Figure 3C) and it is apparent that as the concentration of osmoticum decreases, the mitochondria swell. However, the degree of swelling was not significantly different between WT and msl1-1. When osmoticum was completely omitted, the majority of mitochondria appeared ruptured, but the number of intact mitochondria that remained was the same in msl1-1 and WT mitochondria. These data demonstrate that MSL1 does not provide substantial protection against rupture from hypo-osmotic shock in isolated mitochondria.
Loss of MSL1 leads to increased membrane potential in isolated mitochondria when F1F0ATPsynthase is inactive
Given that MSL1 is essentially non-selective with respect to ion species (Figure 2D) and that these channels are not known to exclude H+ or K+ (Naismith and Booth, 2012; Maksaev and Haswell, 2012; Cox et al., 2013; Hamilton et al., 2015b) opening of MSL1 would be expected to lead to partial dissipation of the mitochondrial membrane potential (ΔΨM). We therefore sought to determine the effect of MSL1 on ΔΨM of isolated mitochondria and to use this readout to explore the conditions under which MSL1 is active. Isolated mitochondria from WT and msl1-1 and the complemented line, msl1-1/gMSL1, were energized with respiratory substrates and labelled with MTG and the cationic lipophilic fluorescent molecule tetramethyl rhodamine methyl ester (TMRM). The use of these two fluorescent probes provides a ratiometric estimation of membrane potential given that accumulation of TMRM in mitochondria is ΔΨM-dependent, while MTG accumulates in a ΔΨM-independent manner, providing a reference control. TMRM and MTG fluorescence were quantified by CLSM imaging (Figure 4A). When mitochondria were energised with succinate, a significantly higher proportion of msl1-1 mitochondria had a higher TMRM:MTG fluorescence ratio than WT and the complemented line (Figure 4B), demonstrating that loss of MSL1 leads to higher ΔΨM in the presence of respiratory substrate but no ADP. Similar results were obtained when malate and pyruvate were used as respiratory substrates (Figure 4C), suggesting that under state II conditions when the F1F0 ATP synthase is inactive due to lack of ADP and the ΔΨM is thus high, the MSL1 channel is active in WT and complemented lines. This would serve to limit the maximum membrane potential that can be reached.
To establish whether the bioenergetic state of the mitochondrion influences MSL1 function, we repeated the analysis with mitochondria in state III (supplied with succinate and ADP). As expected, the activation of the F1F0 ATP synthase caused a decrease in ΔΨM measured as a decrease in the TMRM:MTG fluorescence ratio. Additionally, it was apparent that there was no longer a difference in TMRM:MTG ratio between the genotypes (Figure 4D). To confirm that the genotype response under state III conditions was due to ATP synthase activity, oligomycin was added to inhibit ATP synthase and this restored the difference in TMRM:MTG ratio between genotypes (Figure 4E). Hence, loss of MSL1 leads to an increased ΔΨM compared to WT, but only under state II conditions when F1F0 ATP synthase is inactive. Given that opening of a non-selective ion channel such as MSL1 would dissipate ΔΨM, this is likely a direct consequence of the absence of MSL1, although an indirect or secondary effect cannot be ruled out.
MSL1 is not responsible for ΔΨM pulsing, but loss of MSL1 creates conditions that increase pulsing
Some of the frequency distribution histograms of the TMRM:MTG fluorescence ratio in individual isolated mitochondria taken at single time-points (Fig. 4) appear bimodal. One possible cause of bimodal populations of ΔΨM is membrane potential pulsing which is prevalent in isolated mitochondria in state II (Schwarzländer et al., 2012). These ΔΨM pulses are frequent in state II (on a time scale of seconds to minutes) and rather irregular in frequency and amplitude (Schwarzländer et al., 2012). Hence in a snapshot of a population of mitochondria (as shown in Fig. 4), some mitochondria will be between pulses (higher ΔΨM) and some will be in a pulse (lower ΔΨM), leading to two peaks in the TMRM:MTG frequency distribution histograms. Moreover, the state II bioenergetic condition that promotes pulsing is the same condition under which loss of MSL1 affects ΔΨM, raising the possibility that transient opening of MSL1 could be responsible for pulsing. To investigate this further, we quantified ΔΨM (from TMRM fluorescence) over a timecourse in multiple individual isolated state II mitochondria from WT and msl1-1 and the complemented line (Figure 5). As expected, State II WT mitochondria showed frequent ΔΨM pulses (Figure 5A). However, frequent ΔΨM pulsing was also apparent in state II msl1-1 mitochondria meaning that MSL1 is not the channel responsible for pulsing. Frequency distribution histograms of the complete set of these timecourse data were plotted for populations of mitochondria from WT, the msl1-1 knockout and the complemented line (Figure 5B) and, as in the single time point snapshots of Figure 4, a bimodal distribution was apparent that could be fitted with a two-component Gaussian mixture model. The same analysis was done for mitochondria from the three genotypes under state III (in the presence of ADP). As expected this dramatically reduced the extent of pulsing in all genotypes (Figure 5C) and decreased ΔΨM (Figure 5D). We previously established that the best statistical measure of the amount of pulsing is given by the coefficient of variation (CV) of ΔΨM over time for each mitochondrion (Schwarzlander et al., 2012). The mean CV from multiple mitochondria revealed that the amount of pulsing was significantly greater in the msl1-1 mutant (Figure 5E). Additionally, the proportion of the population of mitochondria that was pulsing (given by the area under the left-hand peak in the TMRM:MTG frequency distribution histogram with decreased ΔΨM) was also significantly greater in the msl1-1 mutant (Figure 5G), suggesting a greater frequency or duration of pulsing. Finally, to provide a robust measure of the resting ΔΨM (i.e. between pulses) and to confirm the apparent increase in ΔΨM in the msl1-1 line in state II mitochondria shown in Figure 4, we determined the mean TMRM:MTG value of the right-hand peak of the frequency distribution corresponding to the higher ΔΨM that occurs between pulses. This confirmed a significant increase in ΔΨM in the msl1-1 mutant in comparison to the WT and complemented line (Figure 5G) consistent with the data from single time-points (Figure 4). In summary, we infer that MSL1 is not directly responsible for ΔΨM pulsing but that loss of MSL1 does increase pulsing frequency and amplitude. The most likely role of MSL1 is thus to help to limit build-up of excessive membrane potential during temporary bioenergetic imbalance. Likewise, loss of MSL1 may exacerbate, the bioenergetic conditions that cause pulsing (high membrane potential and ROS production).
The effect of MSL1 on ΔΨM in isolated mitochondria is moderated by ROS scavengers and antioxidants
When mitochondria are energised by respiratory substrate but ATP synthase is not active (state II), the respiratory chain becomes highly-reduced and the rate of mitochondrial ROS production increases (Møller, 2001). This phenomenon and the changes in pulsing (Figure 5) raise the possibility that MSL1 channel function is influenced by the redox status of mitochondria. To test this, we incubated state II mitochondria with a range of different antioxidants, free radical scavengers and lipid peroxidation inhibitors (Figure 6). If MSL1 is directly activated by the ROS produced in state II mitochondria, then we would expect the addition of ROS scavengers to increase WT membrane potential to mutant values, i.e. the prevention of ROS-activation of MSL1 under state II conditions, would mean that it no longer serves to dissipate ΔΨM. Thus, by preventing activation of MSL1 by ROS, the WT could be expected to phenocopy the knockout mutant. This behaviour is what was observed when the matrix-accumulating antioxidant MitoTEMPOL was added. However, a less clear picture emerged when other ROS-ameliorating agents were used. For example, addition of MitoQ which specifically prevents inner membrane lipid peroxidation (Kelso et al., 2001; Murphy and Smith, 2007), abolished the difference in ΔΨM between msl1-1 and WT, but not by increasing WT ΔΨM to the level expected in the msl1-1 mutant, but by reducing ΔΨM in the msl1-1 mutant to WT levels. This was not the result of a non-specific uncoupling effect of MitoQ because the control analogue decyl triphenylphosphonium (dTPP) which lacks antioxidant activity did not alter ΔΨM in the msl1-1 mutant. The antioxidant, ascorbate, also had a similar effect to MitoQ whereas the matrix-accumulating superoxide dismutase mimetic MnTMPyP had no effect. These data suggest that alterations in mitochondrial ROS can affect MSL1 activation state but there is also evidence that loss of MSL1 alters the sensitivity of mitochondria to the antioxidants MitoQ and ascorbate. The interaction between MSL1, ROS and ΔΨM is complex, and appears to depend on the local origin and type of ROS produced. At this stage we do not have a clear understanding of the mechanism behind these interacting indirect effects.
MSL1 is crucial for regulating mitochondrial redox status during abiotic stress
So far we have demonstrated that the presence of MSL1 is important under bioenergetic conditions in which the respiratory chain is likely to become highly reduced and the rate of mitochondrial ROS production would increase. This bioenergetic state can often be triggered by abiotic stresses due to disruption of normal electron transport or general alterations in redox and energy balance (Møller, 2001). To establish whether MSL1 is important during abiotic stress we monitored the in vivo mitochondrial redox status of WT and msl1-1 roots expressing a mitochondria-targeted roGFP2 that reports on the redox poise of the mitochondrial glutathione pool (mito-roGFP2) (Schwarzländer et al., 2015) subjected to various pharmacological treatments and stresses (Figure 7). Figure 7A shows false-coloured images of the ratio of mito-roGFP2 fluorescence collected with 405 and 488nm excitation wavelengths. An increase in this ratio corresponds to greater oxidation of the roGFP2 probe and indicates greater oxidation state of the glutathione pool in the mitochondrial matrix (Schwarzländer et al., 2015). As expected, incubation of roots with oligomycin to inhibit mitochondrial ATP synthase increased the oxidation of mito-roGFP2 in WT mitochondria (Figure 7A, B), because the reduced ATP synthase activity leads to over-reduction of respiratory chain complexes and subsequent ROS production in the mitochondrial inner membrane. The increase in roGFP2 oxidation in response to oligomycin treatment was substantially greater in the msl1-1 mutant than in WT, demonstrating that loss of MSL1 compromises the ability of mitochondria to maintain redox homeostasis in vivo. The involvement of mitochondrial bioenergetic imbalance was confirmed by the addition of a membrane uncoupler, carbonyl cyanide m-chlorophenyl hydrazone (CCCP) which restored mito-roGFP2 oxidation state to WT values (Figure 7B). The involvement of ROS was confirmed by the restoration of msl1-1 mito-roGFP2 oxidation state to WT values by the addition of ascorbate (Figure 7B). Addition of antimycin A, which is known to raise mitochondrial membrane potential and generate mitochondrial ROS by inhibition of the Q cycle in complex III (Quinlan et al., 2011) also caused an increase of mito-roGFP2 oxidation state in msl1-1, but rotenone, an inhibitor of complex I, had no effect (Figure 7B). In contrast, addition of propranolol, which prevents the uptake of inorganic anions as well as di- and tricarboxylates by the plant inner mitochondrial membrane anion channel (PIMAC; Beavis, 1992; Laus et al., 2008), reduced the roGFP2 oxidation state to a similar degree in WT and msl1-1.
We also examined the mito-roGFP2 oxidation state in roots exposed to a range of stress conditions, namely salt-, osmotic-, heavy- metal- and high-temperature-stress (Figure 7C). As found previously (Schwarzländer et al., 2012), salt stress did not affect the oxidation of a mitochondria-targeted roGFP2 in WT roots and there was no significant difference between WT and msl1-1. Similarly, there was no effect of absence of MSL1 on mito-roGFP2 following hyper-osmotic stress (150 mM and 300 mM mannitol treatments), with both a slight decrease in mito-roGFP2 oxidation in both WT and msl1-1 roots. This corroborates the osmotic-shock assays on isolated mitochondria (Figure 3). In contrast, high temperature (44°C for 10 min) caused a significant increase in mito-roGFP2 oxidation in WT roots (Figure 7C) and this was significantly exacerbated in msl1-1 roots. At a more extreme temperature (48°C for 5 min) roGFP2 became more oxidised (around 60% oxidised) and the difference between msl1-1 and WT disappeared (Figure 7C). There was also a significant increase in mito-roGFP2 oxidation in msl1-1 compared to WT roots treated with 3 or 5 mM Cd2+. Collectively, these data demonstrate that loss of MSL1 exacerbates mitochondrial glutathione pool oxidation under specific abiotic stresses and suggest that MSL1 may provide a mechanism for maintenance of mitochondrial redox status under stress.
DISCUSSION
Our data demonstrate that MSL1 is a stretch-activated non-selective ion channel (Figure 2). Stretch activation provides a regulatory mechanism that allows the channel to respond to cell/organellar swelling due to hypo-osmotic stress. The resultant release of ions reduces osmotic potential and can protect against hypo-osmotic shock, which is thought to be an important function of MscS homologues in E. coli and in Arabidopsis plastids and pollen grains. And although E. coli expressing MSL1 show enhanced tolerance of hypo-osmotic shock, we did not find strong evidence that MSL1 fulfils this role in Arabidopsis mitochondria (Figure 3). In isolated mitochondria, reduction of the osmotic potential of the incubating medium had only a minor effect on WT mitochondrial volume indicating a robust mechanism for volume homeostasis. Absence of MSL1 had no significant effect on this response because the osmotic shock we administered was too severe or too rapid for MSL1 to have an effect, or possibly due to redundant osmoregulatory mechanisms, as in E. coli (Levina et al., 1999). In chloroplasts, osmotic pressure and ion homeostasis are controlled not only by MSL2 and MSL3 (Valey et al., 2012), but also by a family of K+/H+ antiporters (KEA) that work cooperatively with other cation channels (Kunz et al., 2014). A similar K+/H+ antiporter (KHE) also exists in plant mitochondria, although its molecular identity remains unknown to date (Hensley and Hanson, 1975; Diolez and Moreau, 1985; Trono et al., 2015). Nevertheless, it is also notable that treatment of WT and msl1-1 roots with hyper-osmotic concentrations of mannitol did not cause a significant increase in oxidation of the mitochondrial glutathione pool (Figure 7C), suggesting that MSL1 is not a major part of the mechanism that maintains mitochondrial redox poise under this stress condition. Instead, our data point to MSL1 being important under conditions of bioenergetic imbalance characterised by high ΔΨM and a potential high-reduction state of the respiratory chain leading to ROS production (Figure 4 and 5). The increased impact of high temperature and Cd2+ treatments on the oxidation state of mitochondrially-targeted roGFP2 in roots of msl1-1 knockout mutants (Figure 7C) demonstrates that MSL1 is an important component of the molecular machinery that maintains mitochondrial redox status under these specific stresses. Both of these stresses are known to cause bioenergetic imbalances in mitochondria (Lin and Markhart, 1990; Kesseler and Brand, 1994b, a, c; Atkin et al., 2002) and also stimulate mitochondrial pulsing (Schwarzlander et al., 2012). Indeed, in isolated mitochondria, MSL1 functions in the same bioenergetic conditions that lead to pronounced pulsing, whilst a lack of MSL1 enhances the extent of pulsing, suggesting that the two mechanisms are complementary. Given that opening of MSL1 would cause dissipation of ΔΨM it is likely that, similar to pulsing, MSL1 acts as a release valve to avoid over-reduction of the respiratory chain and ROS production due to the build-up of a very high ΔΨM.
Clearly, an important feature of such an uncoupling ion channel would be that it selectively opens only when the mitochondria are in this unbalanced bioenergetic state. One possibility is that the channel is gated or modulated by high negative transmembrane voltage. Although we saw some evidence of this in patched-clamped E. coli spheroplasts expressing MSL1, the instability of spheroplast membranes at high negative voltages made it impossible to characterise this behaviour in more detail. An alternative possibility is that high ΔΨM leads to changes in membrane tension and this leads to activation of MSL1. This could be mediated by damage to membrane lipids by ROS, leading to altered conformation and tension of the membrane. A final possibility is that the MSL1 channel could be directly activated by ROS via oxidation of amino acid side groups in such a way that alters the membrane tension threshold for channel opening (Ridone et al., 2015). We explored the effect of reducing ROS in vivo using mitochondrially-targeted antioxidants (Figure 6). In one case (MitoTEMPOL), we found effects consistent with ROS activation of MSL1 in that MitoTEMPOL increased ΔΨM in WT mitochondria to levels observed in the msl1-1 mutant. Other antioxidants also abolished the differences in state II mitochondrial membrane potential between WT and the msl1-1 mutant, but via unexplained indirect effects that operated in the msl1-1 mutant background rather than in WT plants with functional MSL1. These differences could be related to the different mode of action of the antioxidant reagents used. MitoTEMPOL consists of an antioxidant piperidine nitroxide group conjugated to the lipophilic cation trimethylphosphonium that delivers the nitroxide group to the matrix face of the inner membrane in a membrane-potential-dependent fashion (Murphy and Smith, 2007). The nitroxide group can catalyse the dismutation of superoxide and detoxify Fe2+ ions (Samuni et al., 1990; Bar-On et al., 1999; Trnka et al., 2009) thereby preventing Fenton chemistry that leads to hydroxyl radical formation. In contrast, MitoQ delivers the antioxidant ubiquinone into the hydrophobic core of the inner membrane preventing lipid peroxidation (Murphy and Smith, 2007), while ascorbate detoxifies hydrogen peroxide via matrix-localised ascorbate peroxidase activity. The contrasting effects of these antioxidants may suggest that a direct oxidation of the MSL1 protein by hydroxyl radicals may be a potential activating mechanism rather than alteration of membrane tension via lipid peroxidation, but more detailed studies would be required to establish this.
Our characterization of MSL1 means that it now sits alongside a growing cast of players that act to uncouple plant mitochondria. These include mitochondrial membrane potential pulsing (Schwarzländer et al., 2012), UCP (Vercesi et al., 2006), and alternative respiratory pathways generated by electron flow via the alternative NAD(P)H dehydrogenases (Rasmusson et al., 2004) and alternative oxidase (Moore et al., 2013). Moreover, it is clear that MSL1, pulsing and UCP all respond in various ways to mitochondrial ROS and/or mitochondrial membrane lipid peroxidation. The effect of activation of these three ion transport processes is the same – to dissipate ΔΨM – leading to the question of why more than one mechanism is necessary to achieve the same end. We show here that other uncoupling processes cannot completely compensate for a loss of MSL1: the mitochondrial glutathione pool (as indicated by the degree of mito-roGFP2 oxidation) is more oxidised in the msl1-1 mutant under specific abiotic stress conditions and when the mitochondrial bioenergetic state is directly manipulated with respiratory inhibitors (Figure 7B). This is despite the observation that loss of MSL1 causes an increase in pulsing (Figure 5). This suggests that MSL1, pulsing and UCP are non-redundant in planta.
Three reasons can be envisaged for multiple routes to mitochondrial uncoupling. Firstly, it is possible that different mechanisms could lead to activation at different levels of mitochondrial respiratory chain over-reduction. The second reason could be related to capacity in different cell types. The abundance of the transporters and channels responsible could be quite different leading to different capacities for uncoupling. Combined with different activation thresholds, this would allow a fine tuning of the response, which may be important to dampen bioenergetic imbalance while minimising the effect on ATP synthesis. Finally, it is evident that the different uncoupling mechanisms operate on different timescales and this could be important in allowing both short- and long-term homeostasis and adaptation to environment. In particular, the alternative respiratory pathways appear to be largely regulated at the transcriptional level (Escobar et al., 2004; Clifton et al., 2005), which means they allow relatively long-term adjustments to environmental stress. In contrast, pulsing operates on the timescale of less than one minute (Schwarzländer et al., 2012) and MSL1 function is also likely to be rapid given the timescale of its response to bioenergetic state changes in isolated mitochondria. It is possible that MSL1 may function to limit increases in mitochondrial membrane potential prior to the onset of pulsing.
In summary, we have shown that MSL1 is a stretch-activated ion channel with electrophysiological similarities to its homologues from E. coli and Arabidopsis. While mitochondrially-localised MSL1 can confer protection from osmotic shock onto E. coli lacking key bacterial mechanosensitive channels, it does not protect isolated mitochondria against lysis under hypo-osmotic shock. Instead, we demonstrate that MSL1 function is apparent when mitochondrial membrane potential is high, which is also a condition that leads to mitochondrial ROS production and lipid peroxidation. We also show that the absence of MSL1 loads a greater oxidative burden on mitochondria under abiotic stress, reflected in an increased oxidation of the mitochondrial glutathione pool.
METHODS
Plant Materials and Growth Conditions
Arabidopsis thaliana (ecotype Columbia-0) seedlings and plants were grown under a light intensity of 50 μmol m−2s−1 with a photoperiod of 16 h after seeds were stratified at 4°C in the dark for 2–3 days. The msl1-1 T-DNA insertion line was obtained directly from GABI-Kat (GK-844G07). Plants were grown on compost supplemented with Vermiculite. For the isolation of mitochondria, seeds were surface-sterilized and grown in Murashige and Skoog (MS) medium (½-strength MS medium, 2 mM MES pH 5.7) supplemented with 1% (w/v) sucrose and 0.1% (w/v) agar for 14–16 days with gentle agitation (40–60 rpm). For growth assays or in vivo confocal laser scanning microscopy (CLSM) of roots, seedlings were grown for 5–6 days on vertical plates containing ½-MS medium and 1.5% (w/v) agar.
Generation of MSL1 transgenic lines and mutant identification
Plants homozygous for a T-DNA insertion in the first exon of MSL1 were identified by PCR of genomic DNA using the following primer pairs: MSL1_F and MSL1_R; T-DNA_F and T-DNA_R (Supplementary Table 1). To visually confirm the absence of MSL1 transcript in the insertion line, cDNA was synthesized from DNase-treated total RNA as previously described (Birke et al., 2013) and semi-quantitative PCR was carried out with the primer pair MSL1_sqPCR_F and MSL1_sqPCR_R (Supplementary Table 1). Quantitative RT-PCR was performed in a Rotor-Gene Q cycler (Qiagen) using the Rotor-Gene SYBR Green PCR kit (Qiagen) according to the manufacturer’s instructions with the primers MSL1_qPCR_F and MSL1_qPCR_R (Supplementary Table 1). The amount of MSL1 protein in the transgenic lines was quantified by immunoblotting using a peptide antibody raised against the C-terminus of the MSL1 protein (see below).
The MSL1 genomic complementation transgene MSL1g was made by amplifying the entire MSL1 genomic region, including the promoter, 5′, and 3′ UTRs from wild-type Columbia DNA with oligos LHO710 and LHO817 (Supplementary Table 1). The resulting 3.6 kb fragment was cloned via the Gateway system into pENTR/D-TOPO and then into the destination binary vector pBGW. The complemented lines were generated by agrobacteria-mediated transformation of the pBGW-MSL1g construct. Primary transformants were screened for BASTA resistance and the presence of MSL1 transcript by RT-PCR. After two generations (T2), a segregation analysis was performed and the homozygous complemented line with approximately equal amount of MSL1 transcript as Col-0 was chosen for further analysis. For generating the MSL1-GFP construct, the MSL1 open reading frame was amplified from leaf cDNA with MSL1-GFP_F and MSL1-GFP_R (Supplementary Table 1) and cloned via the Gateway system into pENTR/D-TOPO and then into the destination binary vector pK7FWG2. This construct was then introduced into Col-0 by Agrobacterium-mediated transformation. To generate the msl1-1/roGFP2 line, the homozygous msl1-1 line was crossed with a transgenic line carrying a roGFP2 construct (Schwarzländer et al., 2008).
Isolation and fractionation of mitochondria
Mitochondria were isolated from two-week-old Arabidopsis seedlings as described previously (Sweetlove et al., 2007). Fractionation of mitochondria into peripheral and integral membrane fractions was carried out according to Millar et al. (2001) with slight modifications. Briefly, 1 mg of mitochondrial proteins was resuspended in 100 μl of 20 mM TES (2-[(2-Hydroxy-1,1-bis(hydroxymethyl)ethyl)amino]ethanesulfonic acid) buffer (pH 7.5) and incubated for 10 min. Following three freeze-thaw cycles, the pellet containing membrane-associated proteins was collected by centrifugation at 20,000 × g for 25 min. It was then resuspended in 100 μl of 100 mM Na2CO3 (pH 11.5) and incubated on ice for 20 min. The resulting sample was centrifuged at 20,000 × g to collect the peripheral and integral membrane fractions in the supernatant and pellet respectively. The pellet was resuspended in blue-native solubilisation buffer containing digitonin before loading onto a blue native- or SDS-PAGE.
Mitoplasts were obtained by hypo-osmotic shock of mitochondria, using a method described previously (Murcha et al., 2003). To determine the topology of proteins, 750 μg of mitochondria or mitoplasts were treated with 24 μg/ml proteinase K (Sigma-Aldrich) or water on ice. Following 30 min incubation, 1 mM PMSF was added to the samples to stop the reaction. Mitochondria or mitoplasts were collected by sedimentation at 20,000 × g for 20 min. This step effectively removed unpelleted proteins in the intermembrane space in the mitoplast fraction. The pellet was resuspended in 75 μl of 100 mM Na2CO3 (pH 11.5) and integral membrane proteins were extracted as described above. In vitro import of MSL1 into isolated mitochondria and chloroplasts was carried as described previously (Duncan et al., 2015).
CLSM and data analysis
Freshly isolated mitochondria (in 1 mg/ml) were incubated in 500 nM MitoTracker Green in minimum medium (0.3 M sucrose, 10 mM TES and pH 7.2 (adjusted with NaOH)) for 30 min at 4°C. Mitochondria were then immobilized onto round glass cover slides by centrifugation in minimum medium at 2,000 × g for 5 min at 4°C with brake off. Immobilized mitochondria were energized by the addition of a minimum medium containing respiratory substrates and/or effectors (as stated in the text and in figure legends) and labelled with 25 nM TMRM for state II respiration or 100 nM TMRM for state III respiration. Microscopy was performed using a Zeiss LSM510 META confocal microscope (Carl Zeiss MicroImaging) equipped with laser lines for 488-and 543-nm excitation. Images were collected with a 60× lens (Zeiss 60× 1.4 N.A. Plan-Apochromat oil-immersion lens) for in multi-track mode with line switching between channels. Excitation/emission wavelengths were selected for different probes as follows: TMRM, 543/565–615 nm and MitoTracker Green, 488 nm/505–530 nm. The pinhole diameter was 1.2–1.4 airy units depending on the emission band-pass filter, but the optical slice was kept constant at 1.0 μm for all channels. All other imaging parameters, including laser power of both excitation channels, were kept constant throughout all measurements. CLSM z-stack (10× 0.2 μm) and time series data (3 s interval in the total of 2–3 min) of mitochondria were analysed using a custom Matlab program available from www.markfricker.org (Fricker, 2015). In brief, the mitochondria were automatically separated into unique domains using a watershed algorithm and individually segmented with a local intensity threshold set at the mid-point between each object and the background. This was required to ensure that objects with different intensity values were segmented correctly, which was not possible with a single, global intensity threshold. The average fluorescence intensity at each wavelength were measured for each mitochondrion, and the volume estimated from the projected area assuming spherical geometry.
CLSM imaging of MSL1-GFP seedlings was performed using a FLUOVIEW FV1000 (Olympus) and images were captured with FVIO-ASW software (Olympus). GFP signal was excited at 488 nm and emissions collected with a 505–520 nm bandpass filter. Mitotracker was excited at 543 nm and emissions collected with 560–620 BP filter. Chlorophyll autofluorescence was excited at 635 nm and emissions collected with a 655–755 nm BP filter.
For ratiometric in vivo imaging of 5–6 day old roGFP2-expressing seedlings, a Nikon A1Si confocal microscope equipped with laser lines 405- and 488-nm excitation and emission band-pass filter of 500–520 nm and controlled by a NIS-Elements AR software package (version 4.13.01, Build 916) was used. Images were acquired in the ‘2Ex 1Em’ mode using a 20× lens (Nikon CFI Plan Apo VC 20× 0.75 N.A.) with pinhole diameter of 2.5 airy units (corresponds to the optical slice of 4.37 μm). The 405/488-nm laser power ratio of 6:1 for imaging roGFP2 was kept constant for all treatments as indicated. The 405/488-nm fluorescence ratios and the degree of oxidation of roGFP2 were calculated using the same custom Matlab program described above (available from www.markfricker.org; Fricker, 2015). In brief, this approach finds the brightest voxel in z with excitation at 488nm, and then collects the equivalent voxel from the 405 and autofluorescence channels before background subtraction and ratioing (Fricker, 2015). Calibration of the roGFP2 probe was carried out using 10 mM DTT (full reduction) and 10 mM H2O2 (full oxidation) and the degree of oxidation of roGFP2 was calculated according to Schwarzländer et al. (2008).
Molecular cloning and expression of MSL1
The gene corresponding to the mature version of MSL1 (i.e. without the first 79 amino acid residues that constitute the mitochondrial targeting sequence) was amplified with the primer pair His-MSL1-m_F and His-MSL1-m_R (Supplementary Table 1). The PCR product was then subcloned into an entry vector using a pENTR/D-TOPO cloning kit. MSL1 was then cloned into a Champion pET300/NT-DEST vector (Life Technologies) by Gateway LR reaction, and the resulting construct was transformed into Escherichia coli Rosetta strain. Before induction, bacteria were inoculated in 40 ml LB medium containing 1% glucose, 200 μg/ml Ampicillin and 34 μg/ml chlorophenicol. Following overnight pre-induction, cells were collected by centrifugation (4,000 × g for 15 min), and the resulting pellet was resuspended in fresh LB-medium. Bacteria were added to 200 ml LB-medium containing 1% glucose and antibiotics to achieve the final OD550nm of at least 0.4. Induction was carried out overnight at 28°C after the addition of 1 mM IPTG. Cells were harvested by centrifugation (4,000 × g for 20 min) and the pellet was resuspended and clarified in 10 ml lysis buffer (50 mM phosphate buffer pH 8.0, 300 mM NaCl and 10 mM imidazole) containing 0.5% (v/v) Triton X-100. Following centrifugation to remove insoluble materials (e.g. inclusion bodies), proteins in the supernatant was separated overnight by a 4.5–16% BN-PAGE and the identity of the MSL1 band was confirmed by immunoblotting and mass spectrometry (see below).
Inserts for pCTC-His6-MSL1 and pCTC-MSL1-FLAG were amplified from pET300-MSL1 using LHO2458 and LHO2459 or LHO2460 and LHO2462, respectively (Supplementary Table 1). PCR products were inserted into pCTC-FLAG (Sigma) digested with EcoRI and SalI using a Gibson Assembly Cloning Kit (NEB).
Polyacrylamide gel electrophoresis, immunoblotting and mass spectrometry
To produce a specific antibody against AtMSL1, a homology modelling was performed, using the known structure of E. coli MscS (Bass et al, 2002; Steinbacher et al., 2007) as a template, to determine the peptide sequence where it is exposed to the aqueous environment that allows recognition and binding by the epitopes. Antibodies against the peptide sequence QISNEIKEMLRSNTK were produced in rabbits (Eurogentec Inc.). Purified antibodies were used in 1:1000 for probing the native form of MSL1.
Separation of digitonin-solubilized mitochondrial proteins was carried out according to Eubel et al. (2003) using a 4.5%–16% gradient BN gel dimension and a two-step Tricine-SDS second dimension (8% and 12%). For western blotting, BN gels and PVDF membranes were equilibrated in a modified transfer buffer (48 mM tris, 15 mM bis-tris and 2.5 mM tricine at 4°C). Protein transfer was carried out using a semi-dry FastBlot B43 system (Biometra) at 0.5 mA per square centimetre of gel for 3 h at 4°C.
For Western blotting with 1D SDS-PAGE, 20 μg proteins were separated by SDS-PAGE using a Hoefer MiniEV systems and transferred to PVDF or nitrocellulose membranes for immunodetection by standard procedures using horseradish peroxidase-conjugated secondary antibody. Transferred proteins were probed with primary antibodies specifically targeted to MSL1 (1:1000), Porin (1:5000; (Lee et al., 2008)), SLP2 (1:5000, (Gehl et al., 2014)), cytochrome c (1:1000; Balk et al., 1999), and penta-His (Anti-His Antibody Selector Kit, Qiagen).
For protein identification, gel pieces were destained in 25 mM ammonium bicarbonate in 50% acetonitrile, reduced (10 mM DTT, 37 °C, 30 minutes) and alkylated (55 mM iodoacetamide, 25 ºC, one hour). Trypsin digest (200 ng (Promega) in 25 mM ammonium bicarbonate) was performed at 37 ºC overnight. Extracted peptides were concentrated in a SpeedVac (ThermoSavant). Samples were then processed for protein identification at the Central Proteomics Facility, Dunn School of Pathology, University of Oxford. Briefly, samples were resolved on a 25 cm by 75 μm diameter column in an Ultimate 3000 nanoRSLC system (Dionex) at 300 nl/min flow rate using a 125 minute gradient before detection in a Q Exactive mass spectrometer (Thermo). Sample Data were queried using Mascot Search Engine (version 2.4, MatrixScience, London) against UniProtCP_arath. Search criteria were trypsin with two missed cleavage sites allowed; fixed modification was carbamidomethyl (C), variable modification was oxidised (M). Precursor mass tolerance was +/− 20 ppm and fragment mass tolerance was +/− 0.02 Da.
Osmotic Shock Assays
Bacterial osmotic downshock assays were performed essentially as described in Bartlett et al. (2004). Cultures of bacteria (transformed either with a pCTC-FLAG, pCTC-His6-MSL1 or pCTC-MSL1-FLAG construct) were inoculated from newly transformed colonies and grown overnight at 37°C, then diluted 1:10 and grown until an OD600 of 0.1. IPTG induction was for 2 hours.
Electrophysiology
Giant spheroplasts were made essentially as described in Martinac et al. (2013), with the following modifications. E. coli cell cultures were treated with cephalexin for 1.5 hour and then induced with 1 mM IPTG for 2 hours. Spheroplasting was carried out at room temperature for 20 min. The resulting suspension was centrifuged through 7 mls of 1 M sucrose, resuspended in 1 M sucrose, and stored in aliquots at −20°C or −80°C.
Patch-clamp experiments were performed using a pipette buffer (200 mM KCl, 90 mM MgCl2, 5 mM CaCl2, 5 mM Hepes, pH 7.4) and a bath buffer (same as pipette with added 400 mM sucrose). Excised inside-out patches (using pipettes with bubble number ~4.5 (Schnorf et al. (1994)) from spheroplast membranes were treated with 5-second triangle pressure ramps of amplitudes from −40 mmHg to −200 mmHg. Data were collected using Axopatch 200B amplifier and Digidata 1440 digitizer (Molecular Devices) at 20 kHz and filtered at 5kHz. Data were analyzed with Clampfit 10.5 (pCLAMP 10 software suite, Molecular Devices).
The ion selectivity of MSL1 was probed under asymmetric buffer conditions. Inside-out patches were excised in symmetric buffer (200 mM KCl, 90 mM MgCl2, 5 mM CaCl2, 5 mM Hepes, pH 7.3). Then the bath was perfused with a high salt solution (600mM KCl, 90mM MgCl2, 5mM CaCl2, 5mM Hepes, pH 7.3). The value of reversal potential was calculated as the point of intersection of voltage axis with a line representing a linear fit of unitary current in the range between 40 mV and −50 mV membrane potential.
Supplementary Material
Acknowledgments
CPL was supported by a European Molecular Biology Organization (EMBO) long-term fellowship (ALTF 1140-2011). CPL also acknowledges support from the CellNetworks Excellence Cluster Postdoctoral Program (University of Heidelberg) to initiate this work.
AHM was support by the ARC (Australian Research Council) Centre of Excellence in Plant Energy Biology [grant numbers CE140100008; FT110100242]
ESH acknowledges the support of the NIH (National Institutes of Health) grant number 2R01GM084211-5A1.
We also acknowledge the Centre for Microscopy, Characterisation & Analysis (CMCA) at the University of Western Australia for the use of facilities and technical assistance.
Finally, we would like to thank Mike Murphy (Medical Research Council Mitochondrial Unit, Cambridge, UK) for providing MitoQ.
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