- Open Access
High glutamate permeability and distal localization of Best1 channel in CA1 hippocampal astrocyte
- Hyungju Park†1,
- Kyung-Seok Han†1, 2,
- Soo-Jin Oh1,
- Seonmi Jo1, 4,
- Junsung Woo1, 2,
- Bo-Eun Yoon1, 5 and
- C Justin Lee1, 2, 3Email author
© Park et al.; licensee BioMed Central Ltd. 2013
Received: 17 August 2013
Accepted: 4 December 2013
Published: 9 December 2013
Glutamate is the major neurotransmitter that mediates a principal form of excitatory synaptic transmission in the brain. From the presynaptic terminals of neurons, glutamate is released upon exocytosis of the glutamate-packaged vesicles. In recent years, astrocytes are also known to release glutamate via various routes to modulate synaptic transmission. In particular, we have characterized a glutamate-permeable Ca2+-activated anion channel encoded by Bestrophin 1 gene (Best1) that is responsible for Ca2+-dependent, channel-mediated glutamate release in astrocyte. Best1 channel contains a large pore that is readily permeable to large molecules such as glutamate and GABA. In those studies we obtained permeability ratio of glutamate to Cl- in heterologously expressed mouse Best1 in HEK293T cells and in endogenously expressed mouse Best1 in cultured astrocytes. However, up to now, glutamate permeability of the native Best1 channel in vivo has not been reported.
In whole-cell recordings of CA1 hippocampal astrocytes, we found that opening of Best1 channel upon activation of a Gq-coupled GPCR, protease-activated receptor 1 (PAR1) generated the anion current carried by glutamate via Ca2+ increase. This Ca2+-evoked glutamate-mediated anion current was unaffected by pretreatment of the inhibitors for a gap junction hemi-channel or Ca2+-activated K+ conductance. This astrocytic anion conductance carried by glutamate was mediated by Best1 channel expression in CA1 hippocampal astrocytes, because Best1 knock-down by shRNA expression eliminated astrocytic glutamate conductance by PAR-1 activation. However, we found that these astrocytes showed a deviation in reversal potential of Best1-mediated current from the predicted value. By performing dual patch recording, we concluded that the deviation of reversal potential is due to incomplete space clamping arising from extremely leaky membrane (input resistance ranging 1–3 MΩ), very low length constant of astrocytic processes, and the localization of Best1 channel in distal microdomains near synapses. Based on the relative shift of reversal potentials by ion substitutions, we estimated the permeability ratio of glutamate and Cl- (Pglutamate/PCl) as 0.53.
Our study shows that Best1, located at the microdomains near the synaptic junctions, has a significantly high permeability to glutamate in vivo, serving as the prominent glutamate-releasing channel in astrocytes, mediating the release of various gliotransmitters in the brain, and playing an important role in modulating synaptic transmission.
Astrocytes modulate neuronal function by releasing glutamate in response to neuronal activity [1, 2]. Astrocytically released glutamate has been shown to activate neighboring neuronal glutamate receptors such as N-methyl-D-aspartic acid receptor (NMDAR) which is a critical player for diverse neuronal function [3–5]. Thus, delineation of underlying mechanisms of glutamate release from astrocytes has received much attention.
Recently, it has been reported that astrocytic glutamate is released through glutamate-permeable channels, such as Ca2+-activated anion channel, Best1 and TREK-1 containing two pore potassium channel [4, 5]. In particular, Best1 is responsible for the Ca2+-dependent, channel-mediated glutamate release from astrocytes . Due to the preferential subcellular localization of Best1 at the microdomain near neuronal synaptic sites , it is believed that glutamate released through Best1 specifically targets postsynaptically localized neuronal NMDA receptors  and plays a critical role in modulating synaptic function .
The unique property of Best1 in mediating channel-mediated glutamate release originates from its pore that allows large ions and molecules to pass through [6, 7]. Best1 has been shown to be permeable to large ions and molecules with a significant permeability ratio of anion to Cl- (Px/PCl): GABA (0.19) , isothionate (0.47) , bicarbonate (0.44) , gluconate (0.4) . Despite the strong evidence for functional expression, physiological importance, and unique biophysical property of Best1, there has been no description or estimation of glutamate permeability of Best1 in vivo[4, 7]. To address this issue, we performed an electrophysiological measurement of whole-cell anion conductance from astrocytes in acute hippocampal slice to identify a Ca2+-dependent glutamate conductance mediated by Best1.
Results and discussions
Characterization of Best1-mediated glutamate conductance from hippocampal CA1 astrocytes
We next tested whether this astrocytic glutamate conductance is mediated by Best1. In our previous report, we demonstrated that over 90% of GFAP positive astrocytes in stratum radiatum of CA1 hippocampus express functional Best1, and this Best1 mediates the TFLLR-induced CAAC . Thus, it is plausible to hypothesize that Best1 is also responsible for glutamate-mediated conductance elicited by PAR-1 activation. To reduce the Best1 expression in the astrocytes, we utilized the Best1-sensitive short hairpin RNA (shRNA) . A whole-cell patch clamp was made onto the astrocytes expressing scrambled- or Best1-shRNA (identified by co-staining of SR-101 and GFP (co-expressed with shRNA)) using the pipette solution containing glutamate as a main anion (Figure 1E). We found that TFLLR-induced anion conductance in Best1-shRNA expressing astrocytes was almost completely eliminated, compared to scrambled-shRNA expressing astrocytes (Figure 1E, F). The effect on TFLLR-induced glutamate efflux was quantified by measuring current magnitude at -100 mV: glutamate efflux at this potential was significantly smaller in astrocytes from mice injected with Best1-shRNA than with scrambled-shRNA or from naïve mice (Figure 1F). Taken together, our data indicate that Best1 in hippocampal astrocytes is required for generating TFLLR-induce anion conductance carried by glutamate.
Astrocytic glutamate conductance is unaffected by gap junction hemichannel or Ca2+-activated K+ channel
Dual patch-clamp recording from a single astrocyte reveals voltage error
We then performed dual patch-clamp recording to isolate the CAAC current induced directly by Ca2+ in the patch pipette solution and by using the blocker, 5-Nitro-2-(3-phenylpropylamino)benzoic acid (NPPB) to obtain the NPPB-sensitive CAAC current under symmetrical Cl- condition from a single astrocyte (Figure 5). This allowed us to isolate Best1-mediated conductance during the dual patch clamp recording and to confirm whether NPPB-sensitive current in this condition is same with the one recorded in Figure 1A. We isolated NPPB-sensitive current using voltage ramp protocol from +100 mV to -100 mV (Figure 5C) and plotted as an I-V relationship (Figure 5D). Instead of using the command voltage for the plot, we used the recorded actual voltage for the I-V relationship to bypass the voltage error due to access resistance (Figure 5D). The I-V relationship of Best1-medaited, NPPB-sensitive current showed a reversal potential of around -40 mV (Figure 5D), which was similar to the deviation that we observed with the reversal potential of TFLLR-induced CAAC current in Figure 1B (-34.8 mV).
Deviation of reversal potential due to specific localization of Best1 in microdomain
What is the source of -40 mV deviation in the reversal potential of both NPPB sensitive current and TFLLR-induced CAAC current? The distortion of voltage-gated currents due to incomplete space-clamp in neuronal dendrites under patch-clamp technique has been extensively reported [18–25]. Unlike neurons, astrocytes are known to exhibit high expression of background potassium channels, which results in very low membrane resistance in a unit length, Rm. In addition, astrocytes contain elaborate processes with a small diameter of around 1 μm, which should result in high axial resistance per unit length, Ri. The combination of these two factors affects the length constant by the relationship, λ = , which governs the degree of voltage error (ΔV) due to an incomplete space clamp in voltage clamping experiments by the relationship, ΔV(χ) = Vmax (e-χ/λ), where χ represents the distance from the recording electrode. The length constant λ can be rewritten as, λ = , where ρ is the specific resistivity of astrocytic process and a is the diameter of astrocytic process. In case of hippocampal astrocytes, λ should be very low due to low Rm and high Ri and therefore the voltage error, ΔV should be significantly high. Similar to an axon of mammalian neuron, the diameter of each astrocytic process is estimated to be around 1 μm . Best1 is reported to be expressed mostly in the distal microdomains of astrocytes, near synaptic junctions, as shown in our previous study  as well as in Figure 4A. Thus, the average distance of Best1 from the recording electrode, χ, should be around 50 μm (Figure 4B). Under symmetrical Cl- condition, the expected voltage at the microdomain when the Best1 is fully open should be around 0 mV. Thus, the Vmax can be estimated to be around -80 mV (Vmax = -80 mV – 0 mV), based on the fact that the resting membrane potential at soma around the recording electrode is around -80 mV. Using the observed voltage error of -40 mV for ΔV(χ) at 50 μm, we can now estimate the length constant λ for astrocytic processes to be 72.1 μm (or 0.0721 mm) (Figure 4G), which is much lower (44 fold less) than the reported length constant for neuronal dendrite (λ = 3.16 mm, ). Unlike hippocampal astrocytes, Bergmann glial cells express Best1 in the cell body as well as main processes (Figure 4D) . Therefore, the voltage error is minimal due to minimal distance between the locations of Best1 to the recording electrode. This is most likely the reason for the consistency between the observed reversal potential and the predicted value in Bergmann glial cells (Figure 4D). Taken together, we concluded that the I-V relationships in Figure 1B are deviated by about -40 mV due to voltage error arising from incomplete space-clamp, which originates from the very low length constant of the astrocytic processes. These results and estimations strongly support the idea that functional Best1 channel is mostly expressed in distal microdomains of hippocampal astrocytes, as predicted by the immunohistochemical and electrophysiological evidence.
Calculation of glutamate permeability ratio
The relative shift in the reversal potential might underestimate the true permeability ratio due to the evident voltage error. Nevertheless, we found a shift in reversal potential for each anion in accord with anion substitution in the pipette solution (Figure 1B). Based on the shift in reversal potential, it was possible to calculate a relative permeability of each anion to Cl- anion according to the Goldman-Hodgkin-Kats equation (see Materials and Methods). The estimated permeability ratio of glutamate to Cl- was Pglutamate/PCl = 0.53, which was in the range of the reported values between 0.47 for cultured astrocytes  and 0.67 for heterologously expressed Best1 channels in HEK293T cells . The calculated glutamate permeability ratio of Best1 was much higher than the reported GABA permeability ratio, PGABA/PCl = 0.19, of the Best1 in Bergmann glial cells of the cerebellum .
In conclusion, our results indicate that Best1 in CA1 hippocampal astrocytes shows a relatively high permeability to glutamate. In addition, its specific localization at microdomain near synaptic junctions is further evidenced by the deviation of the reversal potential of Best1-mediated CAAC current. This unique biophysical property of Best1 makes this channel a prominent molecule responsible for channel-mediated release of important gliotransmitters such as glutamate and GABA. It is possible that Best1 channel is also permeable to many other important gliotransmitters such as D-serine, aspartate and taurine. Future studies will provide these intriguing possibilities of their roles in channel-mediated gliotransmitter release and in synaptic functions.
Cell culture and electrophysiology
HEK293T cell culture was performed as previously described . For measuring SK1 conductance, HEK293 cells were transfected with human SK1-containing plasmid pcDNA3.1-hSK1 using Effectene (Qiagen, Valencia, CA, USA) at 1 mg of DNA per 35-mm culture dish. Transfected HEK293 cells were recorded using a conventional whole-cell patch-clamp within 48 hrs. Fire-polished borosilicate glass patch pipettes were 3 ~ 5 MΩ. Experiments were conducted at room temperature (20 ~ 25°C). Current–voltage curves were established by applying 500 ms duration voltage ramps from -100 to +100 mV (Vh = -70 mV). Data were acquired with an Axopatch 200A amplifier controlled by Clampex 10.0 software via a Digidata 1322A data acquisition system (Molecular Devices, Sunnyvale, CA, USA). The extracellular solution is composed of (mM) 150 NaCl, 10 HEPES, 3 KCl, 2 CaCl2, 2 MgCl2, and 5.5 glucose at pH 7.3 adjusted with NaOH (300 ~320 mOsm). Internal pipette solution is composed of (mM) 106 CsCl or KCl, 20 TEA-Cl, 10 BAPTA, 8.7 CaCl2, 0.5 MgCl2, and 5 HEPES (500 nM free Ca2+).
Production of mBest1-shRNA containing lentivirus and delivery into mouse hippocampus
Scrambled shRNA and mBest1-shRNA were inserted into pSicoR lentiviral vector (provided by Dr. T. Jacks through Addgene Inc.)  as previously described . For shRNA expression into hippocampal CA1 region, lentivirus (produced by Macrogen, Korea) was delivered into hippocampal CA1 region of wild type C57BL/6 mice by a stereotaxic surgery method .
Slice preparation and electrophysiology
Horizontal or transverse mouse brain slices (300 ~ 400 μm) containing hippocampus were acutely prepared as previously described . SR-101 (Sigma; 1 μM) dye was loaded into acute brain slice as previously described . Prepared slices were left to recover for at least 1 h before recording in oxygenated (95% O2 and 5% CO2) artificial cerebrospinal fluid (ACSF; in mM, 130 NaCl, 24 NaHCO3, 3.5 KCl, 1.25 NaH2PO4, 1 CaCl2, 3 MgCl2 and 10 glucose, pH 7.4.; room temperature). The standard ACSF recording solution was composed of (mM): 130 NaCl, 24 NaHCO3, 3.5 KCl, 1.25 NaH2PO4, 1.5 CaCl2, 1.5 MgCl2 and 10 glucose saturated with 95% O2–5% CO2, at pH 7.4. To observe Ca2+-induced glutamate conductance in CA1 astrocytes, the pipette solution contained (in mM) 133 Cs-glutamate, 1 MgCl2, and 10 HEPES, at pH 7.3 adjusted with CsOH (~280 Osm). For Cl- or gluconate-based internal solution, Cs-glutamate was replaced with the same concentration of CsCl or Cs-gluconate. To block the effect of neuronal spontaneous activity on astrocytes, TTX (0.5 μM; Tocris) was added into ACSF. Experiments with a holding current more than -100 pA or a change in input resistance >30% of control were rejected. To induce CAAC activation from CA1 astrocytes, 30 μM of TFLLR was bath-treated. In one series of experiments, dual-patch recording from a single astrocyte was used to directly measure the voltage errors in whole-cell voltage clamp recording. The standard electrode solution contained the following (in mM): 140 KCl, 0.5 CaCl2, 1.0 MgCl2, 5 EGTA, 10 HEPES, 3 Mg-ATP, and 0.3 Na-GTP (pH 7.3). The pH was adjusted to 7.3 with KOH.
Length constant (λ) = (Rm is membrane resistance, and Ri is axial resistance.).
V(x) = Vmax(e-x/λ) (x is the distance from the start of the potential).
Rabbit polyclonal Best1 IgG was produced using antigen (Ab Frontier). Primary antibody was then applied at appropriate dilution [Chicken polyclonal GFP at 1:1000 (Abcam), Best1 IgG at 1:100] and incubated overnight at 4°C. After this, the sections were washed three times in 0.1 M PBS and incubated in secondary antibody [DyLight 488 donkey anti-chicken IgG at 1:200 (The Jackson Laboratory), Alexa 555 donkey anti-goat IgG at 1:200 (Invitrogen)] for 2 h. After three rinses in 0.1 M PBS and DAPI staining at 1:1000 (PIERCE), the sections were mounted on polysine microscopic slide glass (Thermo Scientific). Images were acquired using a Nikon A1R confocal microscope.
Statistical analysis was performed using Prism software (GraphPad software). Statistical significance between two groups was analyzed by using student t-test and among multiple groups at least three groups by using One-way ANOVA with Dunnett’s multiple comparison. All values are shown as mean ± s.e.m.
This work was supported by the World Class Institute (WCI 2009–003) of the National Research Foundation (NRF) funded by the Korean Ministry of Science and Technology (MEST), and National Agenda Project (NAP) of the Korea Research Council of Fundamental Science & Technology.
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