Introduction

The human voltage-gated proton channel (hH_v1) is a membrane protein that forms a proton selective channel (1, 2). Despite its physiological importance, its molecular mechanisms are still poorly understood, including the precise structural identity of the permeation pathway and the gating mechanism of voltage (3, 4), pH gradients (3, 5), membrane stretch (6), and ligands such as the classical inhibitor Zn²⁺ (7, 8). Understanding these processes requires connecting the functional properties to the hH_v1 structure.

Each monomer of hH_v1 dimers includes an intracellular N-terminal domain of unknown function, a transmembrane voltage-sensor domain (VSD), and an intracellular coiled-coil (CC), which forms the primary intersubunit interface (9, 10). Current structural models, however, have been obtained from truncated or chimeric channel constructs (11, 12), and thus, it is not clear whether they correspond to physiological or functional conformations. Moreover, the multiple kinetic components of H_v1 gating currents suggest that the protein’s resting state comprises an ensemble of conformations (4, 5), which is consistent with the conformational flexibility inferred from structural approaches (12–14). Because protein function arises from this distribution of conformational states (15), approaches to directly measure structural heterogeneity in the full-length hH_v1 are needed.

An attractive approach to interrogate the structural heterogeneity of hH_v1 is fluorescence spectroscopy, which offers high sensitivity at nanomolar protein concentrations and compatibility with near-physiological conditions. Fluorescence can report on local environment and accessibility changes, as well as quantify distance changes through Förster resonance energy transfer (FRET) (16). Importantly, time-resolved FRET measured using lifetimes preserves information about conformational heterogeneity on the nanosecond timescale, which is lost in steady-state measurements due to the averaging process (17). Together, these capabilities make fluorescence, especially time-resolved FRET, a powerful method to connect hH_v1 structure and function (18).

A few obstacles remain to directly measuring conformational heterogeneity of hH_v1. First, a method to express and purify stable and functional protein is needed, which is challenging for membrane proteins. Second, site-specific fluorophore labeling is difficult at buried sites, resulting in low labeling efficiency. Third, traditional fluorophores are bulky and have long linkers (14), resulting in protein structure perturbation and heterogeneity dominated by the properties of the label (19). A recent method was optimized for robust expression and purification of full-length, functional hH_v1 in E. coli (20, 21). The remaining obstacles can be overcome by labeling the protein with the fluorescent noncanonical amino acid acridon-2-ylalanine (Acd) using genetic code expansion (GCE) (22–24). This technology allows site-specific labeling during translation by reassigning an amber stop codon using an orthogonal aminoacyl-tRNA synthetase (RS)/tRNA (25, 26) (Figure 1A). Acd’s small size and minimal linker reduce perturbations and heterogeneity, and its favorable photophysics support both steady-state and time-resolved measurements (27). Here, we incorporated Acd across all hH_v1 structural domains and purified 12 of 14 constructs as stable, functional proteins. We then used Acd’s environmental sensitivity and FRET from tryptophan (Trp)/tyrosine (Tyr) to Acd to validate the protein folding and report Zn²⁺-dependent conformational changes. These data establish a platform for interrogating conformational heterogeneity and dynamics in the full-length hH_v1.

Figure 1.

Results

We generated a library of hH_v1 constructs with Acd incorporated across the different structural domains

Because available H_v1 structural models were produced from either truncated or modified proteins (11, 12), we used an AlphaFold model of the full-length, dimeric hH_v1 to guide Acd site selection (28, 29) (Figure 1B and Dataset S1). The model recapitulates the expected hH_v1 architecture with high confidence: S0 as a short helix parallel to the membrane, S1-S4 transmembrane segments forming a canonical VSD, and a C-terminal helix extending from S4 that forms the CC intersubunit interface. In addition, two helices in the N-terminal domain (P1 and P2) were predicted (Figure 1C), albeit with low confidence. The dimer interface in the membrane is primarily formed by S4-S4 contacts (Figure S1A), although S1-S1 contacts have been observed experimentally (9, 13). This model appears to represent an intermediate state, with the first S4 positive charged residue R208 proximal to D112 in the selectivity filter, and the third S4 positive charged residue R211 proximal to F150 in the charge-transfer center (Figure S1B). Although the model’s accuracy and functional state are unknown, we used it as a rough starting point for selecting positions to incorporate Acd.

To test the feasibility and specificity of Acd incorporation in hH_v1, we initially selected two positions in the intracellular domains: A18 in the N-terminal domain and F247 in the CC. For each position, the wild-type codon was replaced with an amber stop codon (TAG). Bacteria co-transformed with the Acd RS/tRNA pair and hH_v1-TAG constructs expressed fluorescent full-length protein only when Acd was present in the culture medium (Figure 1D). We next generated a library of 14 constructs in which Acd was incorporated into every structural domain: the N-terminal domain, each helix of the VSD, and the CC (Figure 2A-B). Remarkably, most of the 14 hH_v1-Acd proteins expressed at levels comparable to the control (No TAG) (Figure 2C and S2). As expected, several hH_v1-Acd proteins also produced TAG-truncated products (Figure 2C). Increasing the Acd concentration in the E. coli growth medium did not reduce the fraction of truncated protein (Figure S3). One of the constructs, hH_v1-C107Acd, showed a weak in-gel fluorescence signal, although the Western blot signal was comparable to that of other constructs.

Figure 2.

We successfully purified stable and functional hH_v1 labeled with Acd at 12 of the 14 selected positions

We attempted to purify all expressed hH_v1-Acd constructs by immobilized metal affinity chromatography using the detergent Anzergent 3-12 (20, 21). For 12 of 14 constructs, purification yielded a single fluorescent band on SDS-PAGE (Figure 3A and S4). In contrast, no purified protein was detected for the V187Acd or Q233Acd constructs (Figure S4). Because hH_v1-Q233Acd was robustly expressed (Figure 2C), its loss during purification suggests reduced stability. The hH_v1-Acd yields were construct-dependent (Figure 3B), and the TAG-truncated products did not co-purify with the full-length protein (Figure 3A and S4).

Figure 3.

We then evaluated the stability and homogeneity of the hH_v1-Acd proteins using fluorescence-detection size exclusion chromatography (FSEC) (30). Similar to the control (Figure S5), most hH_v1-Acd proteins showed a main peak (∼11.5 mL) followed by a minor peak at higher elution volumes (Figure 3C and S6; Table S1). The proportion of these two peaks varied between constructs (Figure S6). To determine whether the purified hH_v1-Acd proteins were functional, we reconstituted the FSEC fractions containing both peaks in asolectin liposomes and assessed their function using a liposome proton flux assay (20, 31). All 12 reconstituted constructs produced ACMA fluorescence quenching upon valinomycin addition, indicating that our purified proteins formed functional proton-permeable channels (Figure 3D and S7). These results highlight the versatility of GCE for incorporating Acd as a fluorescent probe for structural studies of hH_v1.

Acd was relatively insensitive to the hydrophobicity of its local environment

To explore how the local environment can alter Acd’s spectral properties, we measured the emission spectra of the free amino acid in different solvents (Figure 4A and Table S2). The environmental sensitivity of Acd has been studied previously (24, 27, 32), but we expanded this work here by using the aprotic solvent ethyl acetate (EtAc) and a series of alcohols with varying alkyl chain lengths. Consistent with a general solvent effect produced by polarity (16), the emission spectrum was blue-shifted by approximately 20 nm in EtAc, the least polar solvent measured, relative to water (Figure 4A and Table S2). Alcohols produced a consistently smaller blue shift, independent of their alkyl-chain length (Figure 4A). The spectrum in Buffer-H2, our standard experimental solution containing detergent micelles, was only very slightly blue-shifted relative to water (Figure 4A), suggesting that Acd did not substantially partition into the hydrophobic core of the detergent micelles. We also tested whether solvent polarity affects the fluorescence lifetime of Acd using time-correlated single photon counting (TCSPC). The fluorescence lifetime of Acd showed a similar trend to the spectral shifts (Figure 4B): EtAc shortened the lifetime markedly, Acd exhibited shorter lifetimes in alcohols than in water, and Acd in Buffer-H2 had a lifetime similar to that measured in water.

Figure 4.

The spectral blue-shift and short lifetime of Acd in EtAc suggest that Acd may be able to report on the local environment at different sites in hH_v1, especially those that are surface-exposed versus those that face the lipid core. The emission spectra of the hH_v1-Acd proteins showed small, site-specific shifts (Figure 4C and Table S3). The local environment of Acd in hH_v1 spanned the range between those observed for free Acd in Buffer-H2 and in alcohols, with Q56Acd in the N-terminal intracellular domain and C107Acd in S1 showing the most red-shifted and blue-shifted spectra, respectively (Figure 4C). Consistent with the spectra, the fluorescence lifetimes of the hH_v1-Acd proteins fell between those measured for free Acd in Buffer-H2 and in alcohols, with Q56Acd exhibiting the slowest, and C107Acd the fastest, lifetimes (Figure 4D). While small, the differences in spectral properties of Acd in hH_v1 agree with their predicted location in the structural model, with C107 being the site closest to the detergent micelles’ hydrophobic core. The low sensitivity to polarity changes of Acd in different hH_v1 local environments makes it well suited for measuring FRET (27, 33).

FRET between Trp/Tyr and Acd in hH_v1 suggested that the proteins are properly folded

Trp and Tyr have fluorescence emission spectra that overlap with the Acd absorption spectrum and therefore can act as FRET donors to Acd, with relatively short R₀values (23.5 Å for Trp; 20.9 Å for Tyr) (22) (Figure 5A). Each hH_v1 monomer contains four Trp and four Tyr residues (yellow spheres in Figure 5B). In this structural model, the Trp residues are located in the N-terminal domain (W4, W38, and W45) and midway along transmembrane segment S4 in the VSD (W207). The Tyr residues are located in the N-terminal domain (Y35 and Y42) and near the extracellular end of transmembrane segment S2 (Y134 and Y141).

Figure 5.

To quantify Trp/Tyr to Acd FRET, we used spectral FRET analysis (34). The total emission spectrum from Trp/Tyr and Acd was collected (Figure 5C). The Acd emission spectrum was extracted by subtracting a scaled Trp/Tyr spectrum collected from control wild-type protein (F_280,NoTAG) (Figure 5D and S8). For each Acd-containing construct, the ratio of the extracted spectrum (F₂₈₀ – F_280,NoTAG) to the Acd spectrum with direct excitation (F₃₇₀) was calculated as Ratio A (Figure 5D and 5E). Because Ratio A is not wavelength-dependent, it reports the linearity of the detectors and the absence of significant contamination from other sources of fluorescence. The Ratio A component caused by the direct excitation of Acd (termed Ratio A₀) was measured with free Acd (35) (Figure 5E and S9). The difference between Ratio A and Ratio A₀ is directly proportional to the FRET efficiency.

As expected, the Ratio A values for our hH_v1-Acd proteins were largely flat across emission wavelengths for our hH_v1-Acd proteins (Figure 5E). For all Acd sites, Ratio A was greater than Ratio A₀ (dashed line in Figure 5E), reflecting FRET between Trp/Tyr and Acd at every site in hH_v1. Most Ratio A values were distributed between 0.60 and 0.80, with two clear exceptions: A18Acd (blue) and F247Acd (magenta) (Figure 5E). A18Acd showed the highest Ratio A, consistent with the multiple Trp/Tyr residues in the N-terminal domain. Conversely, F247Acd showed the lowest Ratio A, consistent with its location in the CC, far from most Trp/Tyr residues (Figure 5B).

We next compared Ratio A – Ratio A₀ values with FRET efficiencies predicted by the AlphaFold structural model. We modeled rotamer ensembles for Trp, Tyr, and our Acd sites in the hH_v1 structural model using chiLife (36) and calculated donor-acceptor distance distributions. These distributions were then used to calculate FRET efficiencies (details in SI Text). The experimentally determined Ratio A – Ratio A₀ values showed a moderate correlation (Pearson’s r = 0.48) with the calculated efficiencies (Figure 5F).

There were two spatially clustered deviations between experiment and model. Positions at the extracellular ends of the VSD helices (Y134 in S2, K125 in S1, and F195 in S4) showed higher experimental FRET than predicted, indicating shorter effective donor-acceptor distances relative to the model. Conversely, positions on the intracellular side of the VSD (K169 in S3 and I217 in S4) showed lower experimental FRET than predicted, implying longer effective donor-acceptor distances. Together, the spatial clustering of residues with similar deviations indicates specific deficits in the AlphaFold model or the failure to quantify the protein dynamics, which can guide future improvements.

Zinc binding changed the conformation of hH_v1

We next asked whether FRET from Trp/Tyr to Acd could report conformational changes upon addition of Zn²⁺, the classical inhibitor of H_v1 proton currents in cells (7). The two experimental structures of H_v1 were resolved with this cation bound to the extracellular side of the VSD (11, 12). We observed site-specific spectral changes in the hH_v1-Acd proteins in the presence of Zn²⁺ (Figure 6 and S10). The largest changes occurred for hH_v1-K169Acd, where 1 mM Zn²⁺ caused a decrease in the Trp/Tyr emission and an increase in the Acd emission (Figure 6A). This decrease in donor fluorescence, paired with increased acceptor fluorescence, is the hallmark of increased FRET and was corroborated by spectral analysis (Figure 6B). Additionally, a slight blue shift of the Trp/Tyr fluorescence was observed for all hH_v1-Acd proteins in the presence of Zn²⁺ (Figure S11). These changes were completely reversed by the addition of EDTA, confirming that the changes arise from a reversible conformational change upon Zn²⁺ binding (Figure 6A and 6B). Large changes in effective FRET efficiency were observed with Acd incorporated at Q56 in the N-terminal domain and C107, F159, and K169 in the VSD (Figure 6C). Notably, these positions are intracellular, even though H_v1 currents are inhibited by extracellular Zn²⁺ (7, 37). These data demonstrate that Zn²⁺ binds to hH_v1 and alters its conformation in detergent micelles, consistent with a nuclear magnetic resonance study of the VSD of hH_v1 (12).

Figure 6.

Discussion

Incorporating Acd into hH_v1 by GCE opens new possibilities for studying the structure and function of this channel. We systematically incorporated Acd at multiple positions in hH_v1 and confirmed protein stability and function after purification. 12 of 14 hH_v1-Acd proteins produced acceptable yields upon purification and were functional, despite being a human membrane protein expressed in E. coli. Two factors likely underlie the robustness of our system: (i) an optimized purification protocol for hH_v1 (20, 21) that offsets the expected reduction in yield associated with GCE (22, 25), and (ii) the high efficiency and specificity of the evolved aminoacyl-tRNA synthetase for incorporating Acd (17, 27).

Fluorescence spectroscopy has been used to detect conformational changes in H_v1. Sites at the extracellular portion of S4 (38) and S1 (39) in the VSD of Ciona intestinalis H_v1 have been labeled with the fluorophores Alexa488 and tetramethylrhodamine (TAMRA) through cysteine-selective reagents to capture conformational changes during activation using voltage-clamp fluorometry. Similarly, the fluorescent noncanonical amino acid 3-(6-acetylnaphthalen-2-ylamino)-2-aminopropanoic acid (Anap) has been incorporated at several sites in the S4 in hH_v1 (40) to study conformational changes in response to voltage and pH. In these cases, the fluorophore’s environmental sensitivity has been used as a readout of conformational changes. By contrast, FRET provides richer structural information due to its distance dependence. Single-molecule FRET has been measured in purified hH_v1 labeled with Cy3 and Cy5 to track the VSD movements in response to voltage, pH, cholesterol, and zinc (14, 41). The small size and minimal linker of Acd, along with its low environmental sensitivity and high photostability, are advantageous for measuring FRET in hH_v1 compared with previously used fluorophores.

The high number of FRET donors, 4 tryptophans and 4 tyrosines per subunit, limits the utility of the Trp/Tyr-Acd FRET pair as a strategy to measure conformational rearrangements in hH_v1. Our library of a dozen single Acd-incorporating constructs, with sites distributed across the entire primary sequence of the protein, opens the door to using Acd as a FRET donor. We have previously used time-resolved transition metal ion FRET (tmFRET), which utilizes a transition metal ion as a FRET acceptor (27, 33), to measure conformational energetics in the bacterial cyclic nucleotide-gated ion channel SthK (42). However, in that work, we incorporated Acd at a single position in the intracellular C-terminal domain of SthK. With Acd incorporated at multiple sites in full-length hH_v1, we can interrogate its gating mechanisms in unprecedented detail.

Materials and Methods

Protein expression and purification

hH_v1 was expressed and purified according to the published protocol with minor modifications (20, 21). Briefly, fresh competent BL21-Gold(DE3) cells (Agilent) were co-transformed with the His-EK-hH_v1-C107A-C249A.pET15-b (hH_v1-Cysless, referred to as No TAG) and MjA9Acd-RS.pDule2 (22, 23) plasmids (sequences in SI Text) using the heat shock method. For expressing hH_v1-Acd proteins, the codon corresponding to the selected position was changed to the amber stop codon (TAG) by site-directed mutagenesis. All plasmids were sequenced before use. Pre-cultures were grown overnight in LB medium supplemented with 0.2% glucose, 0.4 mg/mL ampicillin, and 0.1 mg/mL spectinomycin at 37 °C and 250 rpm. The next day, cultures were diluted 1:100 in complete autoinduction medium (43) supplemented with 0.4 mg/mL ampicillin and 0.1 mg/mL spectinomycin, and then grown at 37 °C and 250 rpm until an OD₆₀₀ of 1.5 was reached. The protein expression level was proportional to the Acd concentration in the culture medium (Figure S11). We chose 0.6 mM Acd in the culture medium as optimal for hH_v1 expression, as higher concentrations only slightly increased the final biomass (Figure S11B). Cultures supplemented with 0.6 mM Acd were grown overnight at 20 °C and 250 rpm. Cells were then harvested, resuspended in Buffer-H1 (50 mM Tris, 150 mM NaCl, 1 mM benzamidine, 0.17 mg/mL PMSF, pH 8.0) supplemented with 0.5 mg/mL lysozyme, and incubated for 30 min at 4 °C before being flash-frozen. After thawing, the extracts were supplemented with 5 mM MgCl₂, fresh protease inhibitors, and 12.5 μg/mL DNase I, incubated for 1 h at 4 °C, sonicated, and centrifuged at 100,000g at 4 °C for 1 h. The membrane pellet was resuspended in Buffer-H1 and stored at -80 °C until further use. After thawing, the membranes were solubilized with 1.5% Anzergent 3-12 (Anatrace) (Anz3-12) at room temperature for 1 hour. Insoluble material was removed by centrifuging at 100,000g and 4 °C for 1 h, and the solubilized membrane extract was incubated with His-Pur Ni-NTA (Thermo Scientific) resin equilibrated with Buffer-H2 (50 mM Tris, 150 mM NaCl, 12 mM Anz3-12, pH 8.0) for 1 hour at room temperature. Resin was collected in a gravity column and washed with 20 column volumes (CV) of Buffer-H2, followed by 16 CV of Buffer-H2 with 90 mM imidazole. The hH_v1 protein was eluted with 20 CV of Buffer-H2 with 0.5 M imidazole, was concentrated with 50kDa cut-off centrifugal filters, and imidazole was removed by FSEC (Ex/Em = 385/450 nm) in an ENrich SEC 650 (Bio-Rad) column with Buffer-H2. The hH_v1-containing fractions were concentrated to 0.5-1.5 mg/mL, depending on the amount of purified protein, and then aliquoted, flash-frozen, and stored at -80 °C until use.

Reconstitution and fluorescence proton flux assays

The hH_v1-Acd samples were reconstituted and assayed using a liposome proton flux assay, as described previously, with minor modifications (20). Briefly, soy polar lipid extract (Avati) in chloroform was dried overnight at room temperature in a rotary evaporator under vacuum and then hydrated in Buffer-K (20 mM HEPES, 150 mM KCl, and 1 mM EDTA, pH 7.0) to a concentration of 10 mg/mL. The vesicles were sonicated in a water bath until the solution became translucent, aliquoted, flash-frozen, and stored at -80 °C until further use. Reconstitutions were performed at a 1:100 (protein:lipid, by mass) ratio by mixing 12.5 μg of purified hH_v1-Acd with 1.25 mg of liposomes in a final volume of 330 μL Buffer-K containing 8 mM Anz3-12. The mixture was incubated at room temperature for 1 h, then diluted with 5 mL of Buffer-K and incubated for 30 min. The mixture was further incubated with three cumulative pulses of 100 mg Bio-Beads SM2 (Bio-Rad), each for 1 h at room temperature. After the final Bio-Beads pulse, the mixture was incubated overnight at 4 °C. The next day, two successive 100 mg additions of Bio-Beads were performed, with a 1-hour incubation at room temperature following each addition. Bio-Beads were removed in a gravity column, the mixture was diluted with 10 mL of Buffer-K, and then centrifuged at 150,000g for 2 hours at 4 °C. The proteoliposome pellets were resuspended in 250 μL of Buffer-K, aliquoted, flash-frozen, and stored at -80 °C until further use. On the day of the liposome proton flux assays, samples were thawed at 37 °C and then placed on ice. The sample (40 μL) was diluted in Buffer-Na (20 mM HEPES, 150 mM NaCl, 1 mM EDTA, pH 7.0). 9-Amino-6-chloro-2-methoxyacridine (ACMA; Sigma) was added to a final concentration of 2 μM from a 2 mM stock solution in DMSO, and the mixture was incubated at room temperature for 5 minutes before the fluorescence measurement began. The baseline was recorded for 3 min (F_max). Subsequently, 10 nM of valinomycin (Cell Signaling) was added from a 10 μM stock solution in DMSO, followed by 1 μM carbonyl cyanide m-chlorophenyl hydrazone (CCCP; Sigma) from a 1 mM stock solution in DMSO to record F_min. The final volume was 2 mL. The fluorescence signal (F(t)) was normalized according to the equation (F(t)-F_min)/(F_max-F_min). Fluorescence measurements were performed at 5-second intervals with a 2-second integration time using a Fluorolog-3 spectrometer (Horiba) configured to an excitation wavelength of 410 nm (5 nm bandpass) and an emission wavelength of 490 nm (1 nm bandpass) at room temperature.

Absorption and fluorescence spectra recordings

The absorption and fluorescence spectra were recorded in the indicated solvents or fresh Buffer-H2 at room temperature. Absorption spectra were recorded in a DU 800 Spectrometer (Beckman Coulter) with a wavelength interval of 0.5 nm and a scan speed of 600 nm/min. Fluorescence emission spectra were measured using a Fluorolog-3 spectrometer (Horiba) with an integration time of 0.1 s, 1 nm increments, and excitation and emission slits of 5 nm. For solubilizing Acd in different solvents, a saturated solution of the amino acid was prepared by dissolving 0.5 mg of Acd powder in the respective solvent. Acd spectra were corrected by subtracting a blank of the solvent. hH_v1-Acd proteins were measured at concentrations ranging from 180 to 240 nM in Buffer-H2. Each spectrum was corrected by subtracting a blank with the solvent or Buffer-H2 before adding the protein sample to the cuvette.

Spectral FRET analysis

We used our previously established spectral FRET analysis to remove contamination caused by direct excitation of Acd by 280 nm light (35). This method had the added benefit of eliminating errors arising from the recording system’s transfer function, variations in the acceptor’s quantum yield, or variations in the total concentration of fluorescent molecules. A Trp/Tyr spectrum was collected from control protein without any TAG codons (no Acd incorporation). This was used to subtract the Trp/Tyr emission spectra collected at 280 nm for each Acd-incorporating protein. This yielded the extracted Acd spectrum, F₂₈₀, that had two components: the component due to direct excitation of Acd, and the component due to FRET, . F₂₈₀was normalized by the total Acd emission with 370 nm excitation, F₃₇₀. The resulting ratio, termed Ratio A, can be expressed as: The direct excitation component, termed Ratio A₀, was measured using free Acd amino acid in Buffer-H2. We then quantified the relative FRET efficiency as This quantity is directly proportional to FRET efficiency. An average Ratio A value was calculated between 410 and 480 nm.

Time-resolved fluorescence measurements

TCSPC measurements were performed in a FluoTime 300 spectrometer equipped with a PMA Hybrid 40 detector and LDH-P-C-375 laser diode head (PicoQuant) at room temperature. Emitted photons were detected at 446 nm with the emission polarizer at the magic angle. The TCSPC measurements were performed in the indicated solvent or fresh Buffer-H2. The hH_v1-Acd samples were measured at a concentration of 1 μM and the Acd amino acid at 500 nM. The count rate was always less than 1% of the excitation repetition rate to avoid pile-up distortions of the fluorescence decay. The IRF was measured using a dilute Ludox solution in water.

Supplementary Text

Calculation of the FRET efficiency from the structural model

We calculated the FRET efficiency using the AlphaFold model of the full-length hH_v1 (Dataset S1). For each Acd position, the measured steady-state FRET would correspond to the mean FRET efficiency (E_FRET), which will be proportional to the Ratio A – Ratio A₀ value obtained from the spectral FRET analysis.

For n number of donors and two acceptors in the hH_v1 dimer:

where P_Ex,i is the probability of excitation and E_iis the FRET efficiency of the ith donor. P_Ex,i is the number of photons absorbed by the ith donor divided by the total number of photons absorbed by the total number n of donors, which is quantified by the donor’s extinction coefficient. Supposing the same extinction coefficient for each of the Trp (e_W = 5,501 M^-1 cm^-1) and Tyr (e_Y = 1,209 M^-1 cm^{- 1})(44), equation 1 can be written as:

where the sum of the total number of Trp (n_W) and Tyr (n_Y) is equal to n. The efficiency of FRET for the ith donor can be expressed as the sum of rates of energy transfer to each of the j = 2 Acd acceptors, k_ij, divided by the total rates of photon emission. Therefore, the right terms of equation 2 can be expressed as:

where the Trp lifetime (t_W = 3.1 ns) and tyrosine lifetime (t_Y= 3.6 ns) in the absence of donors are considered constant(1). Finally, each energy transfer rate k_ij is a function of the distance r_ij between the ith donor and the jth acceptor:

where the donor lifetime t_D and R₀ would be t_Wand 23.5 Å or t_Y and 20.9 Å for Trp or Tyr residues, respectively. Calculating E_FRET using the above equations considers a fixed distance between donors and acceptors. A better approach is to consider the distance distributions P_ij(r) produced by the different rotameric states of the FRET pair, which can be modeled easily using chiLife(45). Then, equation 4 will be replaced by equation 5:

DNA plasmid sequences in FASTA format

>His-EK-hHv1-C107A-C249A.pET15-b TTGAGATCCTTTTTTTCTGCGCGTAATCTGCTGCTTGCAAACAAAAAAACCAC CGCTACCAGCGGTGGTTTGTTTGCCGGATCAAGAGCTACCAACTCTTTTTCC GAAGGTAACTGGCTTCAGCAGAGCGCAGATACCAAATACTGTCCTTCTAGT GTAGCCGTAGTTAGGCCACCACTTCAAGAACTCTGTAGCACCGCCTACATA CCTCGCTCTGCTAATCCTGTTACCAGTGGCTGCTGCCAGTGGCGATAAGTC GTGTCTTACCGGGTTGGACTCAAGACGATAGTTACCGGATAAGGCGCAGCG GTCGGGCTGAACGGGGGGTTCGTGCACACAGCCCAGCTTGGAGCGAACGA CCTACACCGAACTGAGATACCTACAGCGTGAGCTATGAGAAAGCGCCACGC TTCCCGAAGGGAGAAAGGCGGACAGGTATCCGGTAAGCGGCAGGGTCGGA ACAGGAGAGCGCACGAGGGAGCTTCCAGGGGGAAACGCCTGGTATCTTTA TAGTCCTGTCGGGTTTCGCCACCTCTGACTTGAGCGTCGATTTTTGTGATGC TCGTCAGGGGGGCGGAGCCTATGGAAAAACGCCAGCAACGCGGCCTTTTT ACGGTTCCTGGCCTTTTGCTGGCCTTTTGCTCACATGTTCTTTCCTGCGTTA TCCCCTGATTCTGTGGATAACCGTATTACCGCCTTTGAGTGAGCTGATACCG CTCGCCGCAGCCGAACGACCGAGCGCAGCGAGTCAGTGAGCGAGGAAGC GGAAGAGCGCCTGATGCGGTATTTTCTCCTTACGCATCTGTGCGGTATTTCA CACCGCATATATGGTGCACTCTCAGTACAATCTGCTCTGATGCCGCATAGTT AAGCCAGTATACACTCCGCTATCGCTACGTGACTGGGTCATGGCTGCGCCC CGACACCCGCCAACACCCGCTGACGCGCCCTGACGGGCTTGTCTGCTCCC GGCATCCGCTTACAGACAAGCTGTGACCGTCTCCGGGAGCTGCATGTGTCA GAGGTTTTCACCGTCATCACCGAAACGCGCGAGGCAGCTGCGGTAAAGCT CATCAGCGTGGTCGTGAAGCGATTCACAGATGTCTGCCTGTTCATCCGCGT CCAGCTCGTTGAGTTTCTCCAGAAGCGTTAATGTCTGGCTTCTGATAAAGCG GGCCATGTTAAGGGCGGTTTTTTCCTGTTTGGTCACTGATGCCTCCGTGTAA GGGGGATTTCTGTTCATGGGGGTAATGATACCGATGAAACGAGAGAGGATG CTCACGATACGGGTTACTGATGATGAACATGCCCGGTTACTGGAACGTTGT GAGGGTAAACAACTGGCGGTATGGATGCGGCGGGACCAGAGAAAAATCAC TCAGGGTCAATGCCAGCGCTTCGTTAATACAGATGTAGGTGTTCCACAGGG TAGCCAGCAGCATCCTGCGATGCAGATCCGGAACATAATGGTGCAGGGCG CTGACTTCCGCGTTTCCAGACTTTACGAAACACGGAAACCGAAGACCATTCA TGTTGTTGCTCAGGTCGCAGACGTTTTGCAGCAGCAGTCGCTTCACGTTCG CTCGCGTATCGGTGATTCATTCTGCTAACCAGTAAGGCAACCCCGCCAGCC TAGCCGGGTCCTCAACGACAGGAGCACGATCATGCGCACCCGTGGCCAGG ACCCAACGCTGCCCGAGATGCGCCGCGTGCGGCTGCTGGAGATGGCGGA CGCGATGGATATGTTCTGCCAAGGGTTGGTTTGCGCATTCACAGTTCTCCG CAAGAATTGATTGGCTCCAATTCTTGGAGTGGTGAATCCGTTAGCGAGGTG CCGCCGGCTTCCATTCAGGTCGAGGTGGCCCGGCTCCATGCACCGCGACG CAACGCGGGGAGGCAGACAAGGTATAGGGCGGCGCCTACAATCCATGCCA ACCCGTTCCATGTGCTCGCCGAGGCGGCATAAATCGCCGTGACGATCAGC GGTCCAGTGATCGAAGTTAGGCTGGTAAGAGCCGCGAGCGATCCTTGAAG CTGTCCCTGATGGTCGTCATCTACCTGCCTGGACAGCATGGCCTGCAACGC GGGCATCCCGATGCCGCCGGAAGCGAGAAGAATCATAATGGGGAAGGCCA TCCAGCCTCGCGTCGCGAACGCCAGCAAGACGTAGCCCAGCGCGTCGGCC GCCATGCCGGCGATAATGGCCTGCTTCTCGCCGAAACGTTTGGTGGCGGG ACCAGTGACGAAGGCTTGAGCGAGGGCGTGCAAGATTCCGAATACCGCAA GCGACAGGCCGATCATCGTCGCGCTCCAGCGAAAGCGGTCCTCGCCGAAA ATGACCCAGAGCGCTGCCGGCACCTGTCCTACGAGTTGCATGATAAAGAAG ACAGTCATAAGTGCGGCGACGATAGTCATGCCCCGCGCCCACCGGAAGGA GCTGACTGGGTTGAAGGCTCTCAAGGGCATCGGTCGAGATCCCGGTGCCT AATGAGTGAGCTAACTTACATTAATTGCGTTGCGCTCACTGCCCGCTTTCCA GTCGGGAAACCTGTCGTGCCAGCTGCATTAATGAATCGGCCAACGCGCGG GGAGAGGCGGTTTGCGTATTGGGCGCCAGGGTGGTTTTTCTTTTCACCAGT GAGACGGGCAACAGCTGATTGCCCTTCACCGCCTGGCCCTGAGAGAGTTG CAGCAAGCGGTCCACGCTGGTTTGCCCCAGCAGGCGAAAATCCTGTTTGAT GGTGGTTAACGGCGGGATATAACATGAGCTGTCTTCGGTATCGTCGTATCC CACTACCGAGATATCCGCACCAACGCGCAGCCCGGACTCGGTAATGGCGC GCATTGCGCCCAGCGCCATCTGATCGTTGGCAACCAGCATCGCAGTGGGA ACGATGCCCTCATTCAGCATTTGCATGGTTTGTTGAAAACCGGACATGGCAC TCCAGTCGCCTTCCCGTTCCGCTATCGGCTGAATTTGATTGCGAGTGAGATA TTTATGCCAGCCAGCCAGACGCAGACGCGCCGAGACAGAACTTAATGGGC CCGCTAACAGCGCGATTTGCTGGTGACCCAATGCGACCAGATGCTCCACGC CCAGTCGCGTACCGTCTTCATGGGAGAAAATAATACTGTTGATGGGTGTCT GGTCAGAGACATCAAGAAATAACGCCGGAACATTAGTGCAGGCAGCTTCCA CAGCAATGGCATCCTGGTCATCCAGCGGATAGTTAATGATCAGCCCACTGA CGCGTTGCGCGAGAAGATTGTGCACCGCCGCTTTACAGGCTTCGACGCCG CTTCGTTCTACCATCGACACCACCACGCTGGCACCCAGTTGATCGGCGCGA GATTTAATCGCCGCGACAATTTGCGACGGCGCGTGCAGGGCCAGACTGGA GGTGGCAACGCCAATCAGCAACGACTGTTTGCCCGCCAGTTGTTGTGCCAC GCGGTTGGGAATGTAATTCAGCTCCGCCATCGCCGCTTCCACTTTTTCCCG CGTTTTCGCAGAAACGTGGCTGGCCTGGTTCACCACGCGGGAAACGGTCT GATAAGAGACACCGGCATACTCTGCGACATCGTATAACGTTACTGGTTTCAC ATTCACCACCCTGAATTGACTCTCTTCCGGGCGCTATCATGCCATACCGCGA AAGGTTTTGCGCCATTCGATGGTGTCCGGGATCTCGACGCTCTCCCTTATG CGACTCCTGCATTAGGAAGCAGCCCAGTAGTAGGTTGAGGCCGTTGAGCAC CGCCGCCGCAAGGAATGGTGCATGCAAGGAGATGGCGCCCAACAGTCCCC CGGCCACGGGGCCTGCCACCATACCCACGCCGAAACAAGCGCTCATGAGC CCGAAGTGGCGAGCCCGATCTTCCCCATCGGTGATGTCGGCGATATAGGC GCCAGCAACCGCACCTGTGGCGCCGGTGATGCCGGCCACGATGCGTCCG GCGTAGAGGATCGAGATCTCGATCCCGCGAAATTAATACGACTCACTATAG GGGAATTGTGAGCGGATAACAATTCCCCTCTAGAAATAATTTTGTTTAACTTT AAGAAGGAGATATACCATGGGCAGCAGCCATCATCATCATCATCACAGCAG CGGCGATGATGATGATAAAATGGCGACCTGGGACGAAAAGGCGGTGACCC GTCGTGCGAAAGTTGCGCCGGCGGAGCGTATGAGCAAGTTCCTGCGTCAC TTTACCGTGGTTGGTGACGATTACCACGCGTGGAACATCAACTATAAGAAAT GGGAGAACGAGGAAGAGGAAGAGGAAGAGGAACAGCCGCCGCCGACCCC GGTTAGCGGCGAGGAAGGCCGTGCGGCGGCGCCGGATGTGGCGCCGGC GCCGGGTCCGGCGCCGCGTGCGCCGCTGGATTTCCGTGGCATGCTGCGTA AACTGTTCAGCAGCCACCGTTTTCAAGTTATCATTATCGCGCTGGTGGTTCT GGATGCGCTGCTGGTGCTGGCGGAGCTGATCCTGGACCTGAAGATTATCCA GCCGGATAAAAACAACTACGCGGCGATGGTTTTCCACTATATGAGCATCAC CATTCTGGTGTTCTTTATGATGGAAATCATCTTCAAGCTGTTCGTTTTCCGTC TGGAGTTCTTTCACCACAAATTCGAAATCCTGGACGCGGTGGTTGTGGTTGT GAGCTTTATCCTGGATATTGTGCTGCTGTTCCAGGAGCACCAATTTGAAGCG CTGGGTCTGCTGATTCTGCTGCGTCTGTGGCGTGTTGCGCGTATTATCAAC GGCATTATCATTAGCGTGAAGACCCGTAGCGAGCGTCAGCTGCTGCGTCTG AAGCAGATGAACGTTCAACTGGCGGCGAAAATCCAGCACCTGGAATTTAGC GCGAGCGAGAAGGAACAAGAGATTGAACGTCTGAACAAACTGCTGCGTCAG CACGGTCTGCTGGGCGAAGTGAACTAAGGATCCGGCTGCTAACAAAGCCC GAAAGGAAGCTGAGTTGGCTGCTGCCACCGCTGAGCAATAACTAGCATAAC CCCCTTGGGGCCTCTAAACGGGTCTTGAGGGGTTTTTTGCTGAAAGGAGGA ACTATATCCGGATATCCCGCAAGAGGCCCGGCAGTACCGGCATAACCAAGC CTATGCCTACAGCATCCAGGGTGACGGTGCCGAGGATGACGATGAGCGCA TTGTTAGATTTCATACACGGTGCCTGACTGCGTTAGCAATTTAACTGTGATAA ACTACCGCATTAAAGCTTATCGATGATAAGCTGTCAAACATGAGAATTCTTG AAGACGAAAGGGCCTCGTGATACGCCTATTTTTATAGGTTAATGTCATGATA ATAATGGTTTCTTAGACGTCAGGTGGCACTTTTCGGGGAAATGTGCGCGGA ACCCCTATTTGTTTATTTTTCTAAATACATTCAAATATGTATCCGCTCATGAGA CAATAACCCTGATAAATGCTTCAATAATATTGAAAAAGGAAGAGTATGAGTAT TCAACATTTCCGTGTCGCCCTTATTCCCTTTTTTGCGGCATTTTGCCTTCCTG TTTTTGCTCACCCAGAAACGCTGGTGAAAGTAAAAGATGCTGAAGATCAGTT GGGTGCACGAGTGGGTTACATCGAACTGGATCTCAACAGCGGTAAGATCCT TGAGAGTTTTCGCCCCGAAGAACGTTTTCCAATGATGAGCACTTTTAAAGTT CTGCTATGTGGCGCGGTATTATCCCGTGTTGACGCCGGGCAAGAGCAACTC GGTCGCCGCATACACTATTCTCAGAATGACTTGGTTGAGTACTCACCAGTCA CAGAAAAGCATCTTACGGATGGCATGACAGTAAGAGAATTATGCAGTGCTG CCATAACCATGAGTGATAACACTGCGGCCAACTTACTTCTGACAACGATCG GAGGACCGAAGGAGCTAACCGCTTTTTTGCACAACATGGGGGATCATGTAA CTCGCCTTGATCGTTGGGAACCGGAGCTGAATGAAGCCATACCAAACGACG AGCGTGACACCACGATGCCTGCAGCAATGGCAACAACGTTGCGCAAACTAT TAACTGGCGAACTACTTACTCTAGCTTCCCGGCAACAATTAATAGACTGGAT GGAGGCGGATAAAGTTGCAGGACCACTTCTGCGCTCGGCCCTTCCGGCTG GCTGGTTTATTGCTGATAAATCTGGAGCCGGTGAGCGTGGGTCTCGCGGTA TCATTGCAGCACTGGGGCCAGATGGTAAGCCCTCCCGTATCGTAGTTATCT ACACGACGGGGAGTCAGGCAACTATGGATGAACGAAATAGACAGATCGCTG AGATAGGTGCCTCACTGATTAAGCATTGGTAACTGTCAGACCAAGTTTACTC ATATATACTTTAGATTGATTTAAAACTTCATTTTTAATTTAAAAGGATCTAGGT GAAGATCCTTTTTGATAATCTCATGACCAAAATCCCTTAACGTGAGTTTTCGT TCCACTGAGCGTCAGACCCCGTAGAAAAGATCAAAGGATCTTC

>MjA9Acd-RS.pDule2 TTGAGATCGTTTTGGTCTGCGCGTAATCTCTTGCTCTGAAAACGAAAAAACC GCCTTGCAGGGCGGTTTTTCGAAGGTTCTCTGAGCTACCAACTCTTTGAACC GAGGTAACTGGCTTGGAGGAGCGCAGTCACCAAAACTTGTCCTTTCAGTTT AGCCTTAACCGGCGCATGACTTCAAGACTAACTCCTCTAAATCAATTACCAG TGGCTGCTGCCAGTGGTGCTTTTGCATGTCTTTCCGGGTTGGACTCAAGAC GATAGTTACCGGATAAGGCGCAGCGGTCGGACTGAACGGGGGGTTCGTGC ATACAGTCCAGCTTGGAGCGAACTGCCTACCCGGAACTGAGTGTCAGGCGT GGAATGAGACAAACGCGGCCATAACAGCGGAATGACACCGGTAAACCGAA AGGCAGGAACAGGAGAGCGCACGAGGGAGCCGCCAGGGGGAAACGCCTG GTATCTTTATAGTCCTGTCGGGTTTCGCCACCACTGATTTGAGCGTCAGATT TCGTGATGCTTGTCAGGGGGGCGGAGCCTATGGAAAAACGGCTTTGCCGC GGCCCTCTCACTTCCCTGTTAAGTATCTTCCTGGCATCTTCCAGGAAATCTC CGCCCCGTTCGTAAGCCATTTCCGCTCGCCGCAGTCGAACGACCGAGCGT AGCGAGTCAGTGAGCGAGGAAGCGGAATATATCCTGTATCACATATTCTGC TGACGCACCGGTGCAGCCTTTTTTCTCCTGCCACATGAAGCACTTCACTGAC ACCCTCATCAGTGCCAACATAGTAAGCCAGTATACACTCCGCTAGCGCTGA TGTCCGGCGGTGCTTTTGCCGTTACGCACCACCCCGTCAGTAGCTGAACAG GAGGGACAGCTCCCGGCGGATTTGTCCTACTCAGGAGAGCGTTCACCGAC AAACAACAGATAAAACGAAAGGCCCAGTCTTTCGACTGAGCCTTTCGTTTTA TTTGATGCCTGGCAGTTCCCTACTCTCGCATGGGGAGACCCCACACTACCA TCGGCGCTACGGCGTTTCACTTCTGAGTTCGGCATGGGGTCAGGTGGGAC CACCGCGCTACTGCCGCCAGGCAAATTCTGTTTTATCAGACCGCTTCTGCG TTCTGATTTAATCTGTATCAGGCTGAAAATCTTCTCTCATCCGCCAAAACAGC CAAGCTGGAGACCGTTTAAACTCAATGATGATGATGATGATGGTCGACGGC GCTATTCAGATCCTCTTCTGAGATGAGTTTTTGTTCGGGCCCAAGCTTCGAA TTCCCATATGGTACCCGTTTGAAACTGCAGTTATAATCTCTTTCTAATTGGCT CTAAAATCTTTATAAGTTCTTCAGCTACAGCATTTTTTAAATCCATTGGATGC AATTCCTTATTTTTAAATAAACTCTCTAACTCCTCATAGCTATTAACTGTCAAA TCTCCACCAAATTTTTCTGGCCTTTTTATGGTTAAAGGATATTCAAGGAAGTA TTTAGCTATCTCCATTATTGGATTTCCTTCAACAACTCCAGCTGGGCAGTATG CTTTCTTTATCTTAGCCCTAATCTCTTCTGGAGAGTCATCAACAGCTATAAAA TTCCCTTTTGAAGAACTCATCTTTCCTTCTCCATCCAAACCCGTTAAGACAGG GTTGTGAATACAAACAACCTTTTTTGGTAAAAGCTCCCTTGCTAACATGTTTA TTTTTCTCTGCTCCATCCCTCCAACTGCAACATCAACGCCAGTATAATGAATA GAATTAACCTGCATTATTGGATAGATAACTTCAGCAACCTTTGGATTTTCATC CTCTCTTGCTATAAGTTCCATACTCCTTCTTGCTCTTTTTAAGGTAGTTTTTAA AGCCAATCTATAGACATTCAGTGTATAATCCTTATCAAGCTCCAGTTCACTTC CATAAACATATTTTGCCTTTAACCCCATTGCTTCAAAAACTTTTTTGTTATAAT CTCCTATTTTTCTAATCTCATCCAACTCTCCTTTCTGGTTTAAATAGGCGTGT AAATCAGCCAAATCTATAATTATATCAAATCCAGCATTTTGTAAATCAATCAT CTTTTTTATTTGGAGATAATGCCCTAAATGTATTTTACCACTTGGTTCAAAAC CTATCGCAGCAGATTTTTCATCTTTTTTTAAAACCTCTCTTAACTCTTCCTCG CTGATAATTTCAGATGTGTTTCTCTTTATCATTTCAAATTCGTCCATGGGGGA TTCCTCAAAGCGTAAACTCAGCGTTACAAGTATTACACAAAGTTTTTTATGTT GAGAATATTTTTTTGATGGGGCGCCACTTATTTTTGATCGTTCGCTCAAAGAA GCGGCGCCAGGGTTGTTTTTCTTTTCACCGGTGAGACGGGCAACAGAACGC CATGAGCGGCCTCATTTCTTATTCTGAGTTACAACAGTCCGCACCGCTGTCC GTATATATGAGTAAACTTGGTCCCGGGTTACCGGTTTGGTTAGCGAGAAGA GCCAGTAAAAGACGCAGTGACGGCAATGTCTGATGCAATATGGACAATTGG TTTCTTCTCTGAATGGCGGGAGTATGAAAAGTATGGCTGAAGCGCAAAATGA TCCCCTGCTGCCGGGATACTCGTTTAATGCCCATCTGGTGGCGGGTTTAAC GCCGATTGAGGCCAACGGTTATCTCGATTTTTTTATCGACCGACCGCTGGG AATGAAAGGTTATATTCTCAATCTCACCATTCGCGGTCAGGGGGTGGTGAAA AATCAGGGACGAGAATTTGTTTGCCGACCGGGTGATATTTTGCTGTTCCCG CCAGGAGAGATTCATCACTACGGTCGTCATCCGGAGGCTCGCGAATGGTAT CACCAGTGGGTTTACTTTCGTCCGCGCGCCTACTGGCATGAATGGCTTAAC TGGCCGTCAATATTTGCCAATACGGGGTTCTTTCGCCCGGATGAAGCGCAC CAGCCGCATTTCAGCGACCTGTTTGGGCAAATCATTAACGCCGGGCAAGGG GAAGGGCGCTATTCGGAGCTGCTGGCGATAAATCTGCTTGAGCAATTGTTA CTGCGGCGCATGGAAGCGATTAACGAGTCGCTCCATCCACCGATGGATAAT CGGGTACGCGAGGCTTGTCAGTACATCAGCGATCACCTGGCAGACAGCAAT TTTGATATCGCCAGCGTCGCACAGCATGTTTGCTTGTCGCCGTCGCGTCTG TCACATCTTTTCCGCCAGCAGTTAGGGATTAGCGTCTTAAGCTGGCGCGAG GACCAACGTATCAGCCAGGCGAAGCTGCTTTTGAGCACCACCCGGATGCCT ATCGCCACCGTCGGTCGCAATGTTGGTTTTGACGATCAACTCTATTTCTCGC GGGTATTTAAAAAATGCACCGGGGCCAGCCCGAGCGAGTTCCGTGCCGGT TGTGAAGAAAAAGTGAATGATGTAGCCGTCAAGTTGTCATAATTGGTAACGA ATCAGACAATTGACGGCTTGACGGAGTAGCATAGGGTTTGCAGAATCCCTG CTTCGTCCATTTGACAGGCACATTATGCATGCCGCTTCGCCTTCGCGCGCG AATTGATCTGCTGCCTCGCGCGTTTCGGTGATGACGGTGAAAACCTCTGAC ACATGCAGCTCCCGGAGACGGTCACAGCTTGTCTGTAAGCGGATGCCGGG AGCAGACAAGCCCGTCAGGGCGCGTCAGCGGGTGTTGGCGGGTGTCGGG GCGCAGCCATGACCCAGTCAACTGCGATGAGTGGCAGGGCGGGGCGTAAT TTTTTTAAGGCAGTTATTGGTGCCCTTAAACGCCTGGTTGCTACGCCTGAAT AAGTGATAATAAGCGGATGAATGGCAGAAATTCGAAAGCAAATTCGACCCG GTCGTCGGTTCAGGGCAGGGTCGTTAAATAGCCGCTTATGTCTATTGCTGG TTTACCGGTTTATTGACTACCGGAAGCAGTGTGACCGTGTGCTTCTCAAATG CCTGAGGCCAGTTTGCTCAGGCTCTCCCCGTGGAGGTAATAATTGACGATA TGATCATTTATTCTGCCTCCCAGAGCATGATAAAAACGGTTAGCGCTTCGTT AATACAGATGTAGGTGTTCCACAGGGTAGCCAGCAGCATCCTGCGATGCAG ATCCGGAACATAATGGTGCAGGGCGCTTGTTTCGGCGTGGGTATGGTGGCA GGCCCCGTGGCCGGGGGACTGTTGGGCGCTGCCGGCACCTGTCCTACGA GTTGCATGATAAAGAAGACAGTCATAAGTGCGGCGACGATAGTCATGCCCC GCGCCCACCGGAAGGAGCTACCGGCAGCGGTGCGGACTGTTGTAACTCAG AATAAGAAATGAGGCCGCTCATGGCGTTCTGTTGCCCGTCTCACTGGTGAA AAGAAAAACAACCCTGGCGCCGCTTCTTTGAGCGAACGATCAAAAATAAGT GGCGCCCCATCAAAAAAATATTCTCAACATAAAAAACTTTGTGTAATACTTGT AACGCTGAATTCCCGGCGGTAGTTCAGCAGGGCAGAACGGCGGACTCTAA ATCCGCATGGCGCTGGTTCAAATCCGGCCCGCCGGACCACTGCAGATCCTT AGCGAAAGCTAAGGATTTTTTTTAAGCTTGGCACTGGCCGTCGTTTTACAAC GTCGTGACTGGGAAAACCCTGGCGTTACCCAACTTAATCGCCTTGCAGCAC ATCCCCCTTTCGCCAGACGCTCTCCCTTATGCGACTCCTGCATTAGGAAGC AGCCCAGTAGTAGGTTGAGGCCGTTGAGCACCGCCGCCGCAAGGAATGGT GCATGCAAGGAGCCCGAGATGCGCCGCGTGCGGCTGCTGGAGATGGCGG ACGCGATGGATATGTTCTGCCAAGGGTTGGTTTGCGCATTCACAGTTCTCC GCAAGAATTGATTGGCTCCAATTCTTGGAGTGGTGAATCCGTTAGCGAGGT GCCGCCGGCTTCCATTCAGGTCGAGGTGGCCCGGCTCCATGCACCGCGAC GCAACGCGGGGAGGCAGACAAGGTATAGGGCGGCGCCTACAATCCATGCC AACCCGTTCCATGTGCTCGCCGAGGCGGCATAAATCGCCGTGACGATCAG CGGTCCAATGATCGAAGTTAGGCTGGTAAGAGCCGCGAGCGATCCTTGAAG CTGTCCCTGATGGTCGTCATCTACCTGCCTGGACAGCATGGCCTGCAACGC GGGCATCCCGATGCCGCCGGAAGCGAGAAGAATCATAATGGGGAAGGCCA TCCAGCCTCGCGTCGCGAACGCCAGCAAGACGTAGCCCAGCGCGTCGGCC GCCATGCCGGCGATAATGGCCTGCTTCTCGCCGAAACGTTTGGTGGCGGG ACCAGTGACGAAGGCTTGAGCGAGGGCGTGCAAGATTCCGAATACCGCAA GCGACAGGCCGATCATCGTCGCGCTCCAGCGAAAGCGGTCCTCGCCGAAA ATGACCCAGAGCGCTGCCGGCACCTGTCCTACGAGTTGCATGATAAAGAAG ACAGTCATAAGTGCGGCGACGATAGTCATGCCCCGCGCCCACCGGAAGGA GCTGACTGGGTTGAAGGCTCTCAAGGGCATCGGTCGACGCTCTCCCTTATG CGACTCCTGCATTAGGAAGCAGCCCAGTAGTAGGTTGAGGCCGTTGAGCAC CGCCGCCGCAAGGAATGGTGCATGCAAGGAGATGGCGCCCAACAGTCCCC CGGCCACGGGGCCTGCCACCATACCCACGCCGAAACAAGCGCTCATGAGC CCGAAGTGGCGAGCCCGATCTTCCCCATCGGTGATGTCGGCGATATAGGC GCCAGCAACCGCACCTGTGGCGCCGGTGATGCCGGCCACGATGCGTCCG GCGTAGAGGATCCCGGTAAACCAGCAATAGACATAAGCGGCTATTTAACGA CCCTGCCCTGAACCGACGACCGGGTCATCGTGGCCGGATCTTGCGGCCCC TCGGCTTGAACGAATTGTTAGACATTATTTGCCGACTACCTTGGTGATCTCG CCTTTCACGTAGTGGACAAATTCTTCCAACTGATCTGCGCGCGAGGCCAAG CGATCTTCTTCTTGTCCAAGATAAGCCTGTCTAGCTTCAAGTATGACGGGCT GATACTGGGCCGGCAGGCGCTCCATTGCCCAGTCGGCAGCGACATCCTTC GGCGCGATTTTGCCGGTTACTGCGCTGTACCAAATGCGGGACAACGTAAGC ACTACATTTCGCTCATCGCCAGCCCAGTCGGGCGGCGAGTTCCATAGCGTT AAGGTTTCATTTAGCGCCTCAAATAGATCCTGTTCAGGAACCGGATCAAAGA GTTCCTCCGCCGCTGGACCTACCAAGGCAACGCTATGTTCTCTTGCTTTTGT CAGCAAGATAGCCAGATCAATGTCGATCGTGGCTGGCTCGAAGATACCTGC AAGAATGTCATTGCGCTGCCATTCTCCAAATTGCAGTTCGCGCTTAGCTGGA TAACGCCACGGAATGATGTCGTCGTGCACAACAATGGTGACTTCTACAGCG CGGAGAATCTCGCTCTCTCCAGGGGAAGCCGAAGTTTCCAAAAGGTCGTTG ATCAAAGCTCGCCGCGTTGTTTCATCAAGCCTTACGGTCACCGTAACCAGC AAATCAATATCACTGTGTGGCTTCAGGCCGCCATCCACTGCGGAGCCGTAC AAATGTACGGCCAGCAACGTCGGTTCGAGATGGCGCTCGATGACGCCAACT ACCTCTGATAGTTGAGTCGATACTTCGGCGATCACCGCTTCCCTCATACTCT TCCTTTTTCAATATTATTGAAGCATTTATCAGGGTTATTGTCTCATGAGCGGA TACATATTTGAATGTATTTAGAAAAATAAACAAATAGCTAGCTCACTCGGTCG CATCGATGATAAGCTGTCAAACATGAGAATTACAACTTATATCGTATGGGGC TGACTTCAGGTGCTACATTTGAAGAGATAAATTGCACTGAAATCTAGAAATAT TTTATCTGATTAATAAGATGATCTTC

Supplementary Figures

Figure S1.

Figure S2.

Figure S3.

Figure S4.

Figure S5.

Figure S6.

Figure S7.

Fig. S8.

Figure S9.

Fig. S10.

Figure S11.

Supplementary Tables

Table S1.

Table S2.

Table S3.

Acknowledgements

We thank the Oregon State University GCE4ALL (Center for Genetic Code Expansion for All) for their long-standing collaboration. We also appreciate the excellent technical support provided by Dr. James Petersson and Kyle D. Shaffer (University of Pennsylvania) with the Acd synthesis. This work was supported by the National Institutes of Health under award numbers R01EY037223 and R35GM145225 to S.E.G., and R01EY010329 and R35GM148137 to W.N.Z. E.M.C. is a Pew Latin American Fellow.

Additional information

Data availability

All data generated or analyzed during this study are included in the manuscript and supporting files; source data files have been provided for all figures.

Author Contributions:

All the authors conceived the study and designed the experiments. E.M.C. performed the experiments and analyzed the data. All the authors interpreted the data. E.M.C. wrote the first version of the manuscript. All the authors critically revised the article.

Funding

National Institutes of Health (R01EY037223)

• Sharona E Gordon

HHS | National Institutes of Health (NIH) (R35GM145225)

• Sharona E Gordon

HHS | National Institutes of Health (NIH) (R01EY010329)

• William N Zagotta

HHS | National Institutes of Health (NIH) (R35GM148137)

• William N Zagotta

Pew Charitable Trusts (Pew)

• Emerson M Carmona

Additional files

Supplementary Dataset S1. Coordinates of the AlphaFold predicted model of the hH_v1 dimer (in PDB format).