Bestrophin calcium-activated chloride channels (CaCCs) regulate the flow of chloride and other monovalent anions across cellular membranes in response to intracellular calcium (Ca2+) levels. Mutations in bestrophin 1 (BEST1) cause certain eye diseases. Here we present X-ray structures of chicken BEST1–Fab complexes, at 2.85 Å resolution, with permeant anions and Ca2+. Representing, to our knowledge, the first structure of a CaCC, the eukaryotic BEST1 channel, which recapitulates CaCC function in liposomes, is formed from a pentameric assembly of subunits. Ca2+ binds to the channel’s large cytosolic region. A single ion pore, approximately 95 Å in length, is located along the central axis and contains at least 15 binding sites for anions. A hydrophobic neck within the pore probably forms the gate. Phenylalanine residues within it may coordinate permeating anions via anion–π interactions. Conformational changes observed near the ‘Ca2+ clasp’ hint at the mechanism of Ca2+-dependent gating. Disease-causing mutations are prevalent within the gating apparatus.
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We acknowledge the staff at beamlines X25 and X29 of the National Synchrotron Light Source, beamline 24-ID-C of the Advanced Photon Source, and F. Weis-Garcia and the Monoclonal Antibody Facility at MSKCC. We thank C. Lima, M. Long, N. Pavletich, V. Ruta and members of the laboratory for discussions. S.B.L. is a recipient of a Burroughs Wellcome Career Award in the Biomedical Sciences.
The authors declare no competing financial interests.
Extended data figures and tables
The amino acid sequences of the crystallized chicken (Gallus gallus) BEST1 construct (amino acids 2–405) and human BEST1 are aligned and coloured according to the ClustalW convention. The secondary structure is indicated with cylinders representing α-helices, solid lines representing structured loop regions, and dashed lines representing disordered regions. Grey bars (labelled ‘in’ and ‘out’) indicate approximate boundaries of transmembrane regions.
The binding of the Fab to BEST1cryst was assayed by determining the amount of free Fab as a function of the concentration of BEST1cryst in the presence of either 10 μM Ca2+ or 5 mM EGTA (zero Ca2+) (Methods). The fraction of Fab bound is plotted with respect to the concentration of BEST1cryst. The curves correspond to fits of: fraction of Fab bound = [BEST1]h/(Kdh + [BEST1]h), where Kd is the equilibrium dissociation constant, h is the Hill coefficient, and [BEST1] is the BEST1cryst concentration. Derived parameters are: Kd = 15 nM in the presence of Ca2+ (h = 1.3) and Kd = 350 nM in the absence of Ca2+ (h = 1.3).
a, 2Fo − Fc electron density is shown, in stereo, for an area surrounding one of the five identical Ca2+ binding sites. The density was calculated from 40 to 2.85 Å resolution and contoured at 1.5σ (blue mesh) and 7σ (orange mesh) in the context of the final atomic model, which is shown as sticks and spheres (cyan sphere, calcium; red sphere, water). b, Electron density for the C-terminal tail. 2Fo − Fc electron density (blue mesh, calculated from 40 to 2.85 Å, and contoured at 1.5σ) is shown for the C-terminal tail of the yellow coloured subunit. c, Expanded view highlighting the electron density near Ser 358. Consistent with the electron density, mass spectrometry analysis of tryptic peptides of purified BEST1cryst detected only peptides containing Ser 358 that were not phosphorylated (Supplementary Discussion).
a, Structure of the BEST1cryst–Fab complex in the P21 crystal form, viewed from the extracellular side. Fab molecules are grey and BEST1 subunits are coloured individually with α-helices depicted as cylinders. b, Orthogonal view showing approximate boundaries of the membrane. For clarity, two Fabs are drawn. c, C2 crystal form. Overall structures of the two BEST1cryst–Fab complexes in the asymmetric unit of the C2 crystal form are depicted in cartoon representation. BEST1 subunits are coloured individually and Fabs are grey.
Extended Data Figure 5 Ca2+-dependent activation of Best1cryst and permeability of the BEST1cryst–Fab complex.
a, Schematic of the fluorescence-based flux assay. Vesicles diluted into various test salts establish ion gradients. Anion influx through BEST1 produces a negative electric potential within the liposomes that drives the uptake of protons through an ionophore (CCCP) and quenches the fluorescence of a pH indicator (ACMA). b, Ca2+-dependent activation of BEST1cryst using NO3− as the permeant anion. The experimental setup was identical to that for Fig. 1a, except that NO3− was used as the permeant ion. Data presented here and in Fig. 1a were collected on the same day using the same batch of proteoliposomes and indicate the higher permeability of NO3− relative to Cl−. Free concentrations of Ca2+ are indicated. c, Ionic permeability of the BEST1cryst–Fab complex. The experiment setup is identical to that shown in Fig. 1b, except that it was performed using proteoliposomes reconstituted with the BEST1cryst–Fab complex. The Fab remained bound to the channel following reconstitution and excess Fab was maintained throughout (Methods). The slight differences in the shape of the curves for the BEST1cryst and BEST1cryst–Fab samples (for example, the lower rate of fluorescence decrease for Cl– compared with Fig. 1b) are in accord with variability observed among different liposome preparations.
a, The molecular surface of the channel is shown in the same orientation as Fig. 2a and coloured according to electrostatic potential (red, −10 kT e−1; grey, neutral; blue, +10 kT e−1). An asterisk marks the location of the acidic cluster in the foreground. Approximate boundaries for the membrane are indicated. b, Subunit topology. N-terminal ends of α-helices exposed to the pore are indicated by +. The colouring corresponds to that of Fig. 2b. c, Anion binding in the outer entryway. Extracellular cut-away view of the molecular surface of BEST1 (orthogonal representation of Fig. 4a), revealing the surface of the pore (coloured by electrostatic potential; red, −10 kT e−1; white, neutral; blue, +10 kT e−1) and anomalous difference electron density for Br− ions (magenta mesh; 45–5 Å, non-crystallographic symmetry averaged, 8σ contour) in sites 1 and 2.
a, b, Representations of the pore at Phe 80 (a) and Phe 84 (b) are shown as sticks. The distance (d) from the central axis of the pore (black sphere) to the centre of the face of the aromatic ring is shown. An angle θ is defined as the angle between this distance vector and the plane of the ring. The geometry indicated corresponds to the crystal obtained in cymal-6. For the cymal-6-NG crystal, the values are: d = 3.9 Å, θ = 45° (Phe 80) and d = 4.8 Å, θ = 44° (Phe 84). c, Space-filling CPK representation of the pore at Phe 80, showing a hypothetical Cl− (green) positioned in the centre. Standard radii were used for the figure (carbon = 1.7 Å; Cl− = 1.81 Å). δ+ and – represent partial charges on the edge of the aromatic rings and the charge on Cl−, respectively.
Extended Data Figure 8 Evidence for coupling between the Ca2+ clasp and the gate from crystals grown in different detergents.
Comparison among crystals grown using different detergents gives insight into the channel’s gate and it’s coupling to Ca2+. Well-diffracting crystals belonging to the P21 space group were obtained using either the detergent cymal-6 or the detergent cymal-6-NG. Electron density maps indicated the presence of ordered cymal-6-NG but not cymal-6 molecules bound to the S1a–S1b components of the Ca2+ clasps (a). In addition, difference Fourier electron density maps suggested a slight widening of the neck of the pore in the structure with cymal-6 (b). Accordingly, while refined structures superimpose with an overall root mean squared deviation of only 0.15 Å, the diameter of the pore in the hydrophobic neck is ∼0.5 Å wider at Phe 80 for crystals in cymal-6 than it is with cymal-6-NG. Differences on the order of 0.3 Å between the atomic models are localized to the region near the Ca2+ clasp and to the neck of the pore (a). The subtle effects are an indication that changes in or around the Ca2+ clasp induce changes in the neck of the pore and they may hint at the mechanism of gating. a, 2FO − FC electron density for cymal-6-NG detergent molecules, contoured at 1.2σ, is shown as blue mesh in the context of the channel. The channel, with α-helices depicted as cylinders, is coloured on a yellow-to-red spectrum according to the displacement of Cα atoms between the refined atomic models obtained from crystals grown in cymal-6 and cymal-6-NG. Yellow colour represents displacements less than 0.15 Å and red colour represents displacements greater than 0.3 Å. An arrow indicates the neck of the pore and teal spheres denote Ca2+. b, Conformational shift in the gate. Phe 80 and surrounding residues of the refined structures from crystals in cymal-6 and cymal-6-NG are shown as sticks (coloured cyan and yellow, respectively) and viewed along the channel’s axis of symmetry from the extracellular side. Superimposed on this is an Fcymal-6 − Fcymal-6-NG difference Fourier map, which is calculated from 25 Å to 3.5 Å resolution and contoured at −3.8σ (magenta mesh) and +3.8σ (blue mesh).
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Kane Dickson, V., Pedi, L. & Long, S. Structure and insights into the function of a Ca2+-activated Cl− channel. Nature 516, 213–218 (2014). https://doi.org/10.1038/nature13913
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