Nanobodies are important tools in structural biology and pose a great potential for the development of therapies. However, the selection of nanobodies with inhibitory properties can be challenging. Here we demonstrate the use of solid-supported-membrane (SSM)-based electrophysiology for the classification of inhibitory and non-inhibitory nanobodies targeting electrogenic membrane transporters.
Single domain antibodies (nanobodies) have been extensively used in mechanistic and structural studies of proteins and they pose an enormous potential as tools for developing clinical therapies, many of which depend on the inhibition of membrane proteins such as transporters. However, most of the methods used to determine the inhibition of transport activity are difficult to perform in high-throughput routines and depend on labeled substrates availability thereby complicating the screening of large nanobody libraries. Solid-supported membrane (SSM) electrophysiology is a high-throughput method, used for characterizing electrogenic transporters and measuring their transport kinetics and inhibition. Here we show the implementation of SSM-based electrophysiology to select inhibitory and non-inhibitory nanobodies targeting an electrogenic secondary transporter and to calculate nanobodies inhibitory constants. This technique may be especially useful for selecting inhibitory nanobodies targeting transporters for which labeled substrates are not available.
Antibodies are composed of two identical heavy chains and two light chains that are responsible for the antigen binding. Camelids have heavy-chain only antibodies that exhibit similar affinity for their cognate antigen compared to conventional antibodies1,2. The single variable domain (VHH) of heavy-chain only antibodies retain the full antigen-binding potential and has been shown to be very stable1,2. These isolated VHH molecules or "nanobodies" have been implemented in studies related to membrane proteins biochemistry as tools for stabilizing conformations3,4, as inhibitors5,6, as stabilization agents7, and as gadgets for structure determination8,9,10. Nanobodies can be generated by the immunization of camelids for the pre-enrichment of B-cells that encode target-specific nanobodies and subsequent isolation of B cells, followed by cloning of the nanobody library and selection by phage display11,12,13. An alternate way to generate nanobodies is based on in vitro selection methods that rely on the construction of libraries and selection by phage display, ribosome display, or yeast display14,15,16,17,18,19,20. These in vitro methods require large library sizes but benefit from avoiding animal immunization and favor the selection of nanobodies targeting proteins with relatively low stability.
The small size of nanobodies, their high stability and solubility, strong antigen affinity, low immunogenicity, and relatively easy production, make them strong candidates for the development of therapeutics21,22,23. In particular, nanobodies inhibiting the activity of multiple membrane proteins are potential assets for clinical applications5,24,25,26. In the case of membrane transporters, to evaluate whether a nanobody has inhibitory activity, it is necessary to develop an assay that allows the detection of transported substrates and/or co-substrates. Such assays usually involve labeled molecules or the design of substrate-specific detection methods, which may lack a universal application. Furthermore, the identification of inhibitory nanobodies generally requires the screening of large numbers of binders. Thus, a method that can be used in a high-throughput mode and that does not rely on labeled substrates is essential for this selection.
SSM-based electrophysiology is an extremely sensitive, highly time-resolved technique that allows the detection of movement of charges across membranes (e.g., ion binding/transport)27,28. This technique has been applied to characterize electrogenic transporters, which are difficult to study using other electrophysiology techniques due to the relative low turnover of these proteins29,30,31,32,33,34,35. SSM electrophysiology does not require the use of labeled substrates, it is suitable for high-throughput screening, and either proteoliposomes or membrane vesicles containing the transporter of interest can be used. Here, we demonstrate that SSM-based electrophysiology can be used to classify transporter-targeted nanobodies with inhibitory and non-inhibitory properties. As a proof-of-principle, we describe the reconstitution of a bacterial choline transporter into liposomes, followed by detailed steps for immobilization of proteoliposomes on the SSM sensors. We next describe how to perform SSM-based electrophysiology measurements of choline transport and how to determine the half-maximal effective concentration (EC50). We then show how to use SSM-based electrophysiology to screen multiple nanobodies and to identify inhibitors of choline transport. Finally, we describe how to determine the half maximal inhibitory concentrations (IC50) of selected inhibitory nanobodies.
1. Membrane protein reconstitution
2. Chip preparation
3. Measuring the solute transportation: determination of saturation conditions
NOTE: As proof-of-principle, these experiments were performed using a bacterial choline transporter reconstituted in liposomes following the protocol described above. The step-by-step process of determining saturating conditions of the substrate choline prior to the measurement of inhibition by nanobodies is shown here.
4. Serial classification of inhibitory and non-inhibitory nanobodies
NOTE: This section shows how to measure choline transport in the presence of nanobodies that bind specifically to the bacterial choline transporter. Smaller peak currents in the presence of nanobodies indicate transport inhibition. Non-inhibitory nanobodies will not impact substrate transport, i.e., no decrease of the peak current signal.
5. IC50 measurement with inhibitory nanobodies
NOTE: After identifying inhibitory nanobodies, it is possible to determine their half maximal inhibitory concentration (IC50). This is done by measuring the transport of choline at constant concentration, while varying concentrations of the inhibitory nanobody.
6. Cleaning of sensors
SSM-based electrophysiology has been extensively used for the characterization of electrogenic transporters. In the protocol presented here, we show how to use SSM-based electrophysiology to classify nanobodies targeting a secondary transporter (here a bacterial choline symporter) based on their inhibitory and non-inhibitory properties. One of the most useful features of this technique is that it allows for the high-throughput screening of multiple buffer conditions. This particular characteristic is beneficial for the analysis of nanobody libraries, which after the selection of binders can be constituted from a few to dozens of nanobodies. In a standard experiment, a stable lipid monolayer is assembled on a sensor chip. After applying the proteoliposomes preparation containing the choline transporter, a check for good conductivity and capacitance is performed as this is essential for the success of the experiment. In case that the integrity of the membrane is compromised during an experiment, which is easily observed due to the high noise background currents, changing to a new chip is recommended as recovering low noise conditions is rather difficult. In general, we have observed very good reproducibility among measurements of transport and inhibition by nanobodies when using different chips.
To decide about the substrate concentration to be used during a screening of nanobodies, electrogenic transport was first measured under different substrate concentrations to determine EC50 (Figure 1B,C). A substrate concentration that corresponds to saturating conditions was selected (Figure 1C). This substrate concentration was then kept constant in all activating buffers. For this particular example, we selected 5 mM choline.
For the screening of nanobodies, the nanobody must be added to both non-activating and activating buffers. When nanobodies were added to only the activating buffer, it was not possible to observe inhibition of the electrogenic transport. We speculate that this is due to an incomplete occupation of all nanobody binding sites in the transporter population on the chip, thereby revealing the importance of pre-incubation with nanobodies in non-activating conditions. To ensure that all sites are likely to be occupied, a time delay step was included during the application of the first non-activating buffer step to allow the saturation of nanobody binding sites on the transporter population. Incubation times ranging from 2-60 min have been tested with reproducible results. Keep in mind that optimal times of incubation depend on the nature of the nanobody binder and its concentration during the experiment (as well as the concentration of transporter in proteoliposomes on the chip). Therefore, it is recommended to try different incubation times. In any case, as a rule of thumb, the lower the nanobody concentration, the longer the incubation time required. We tested incubation times of 2 min, 20 min, 30 min, and 60 min for different nanobodies but did not detect further transport inhibition.
The effect of inhibitory nanobodies on electrogenic transport is visualized from the decrease of peak currents amplitudes (Figure 2A,C,D). Non-inhibitory nanobodies, on the other hand, do not affect peak currents. After running the washing protocol to allow nanobodies unbinding, a recovery of 80 to 95% of the initial peak current amplitude was observed (Figure 2A,C,D). We have performed a similar experiment but in the presence of liposomes without the transporter protein. When changing from non-activating to activating conditions, no significant artifact currents was introduced by nanobodies present in these buffers (Figure 2B). Running this control experiment is recommended as it is important to know whether changes in peak currents arise from artifacts or not.
After the selection of nanobodies with inhibitory properties, we determined IC50 values for individual nanobodies (Figure 3A,B). For this particular experiment, it is recommended to start with a low concentration of nanobodies and then move towards high concentration during the assay. The calculation of the inhibition for each concentration was then performed by comparing peak currents measured before and after the application of nanobody. To avoid unspecific binding of nanobodies to surfaces, which can be particularly problematic when using low nanobody concentrations, it is advised to follow a similar protocol to that described by Kermani et al.37, where 50 µg/mL of bovine serum albumin was added to the buffers, preventing this deleterious effect. Adding detergents such as Tween or Triton for this purpose should be avoided as these would dissolve lipid membranes.
Figure 1: SSM-based electrophysiology. (A) Protocol for transient currents measurement. A non-activating solution is replaced by an activating solution followed by the flow of non-activating solution to restore initial conditions. During the first step, nanobodies bind to the transporter. When switching to the activating solution, the substrate gradient drives the electrogenic transport (orange curve). In the presence of an inhibitory nanobody, the peak current shows a smaller amplitude (blue curve). After finishing the protocol and running solutions without nanobody (wash), unbinding of nanobodies occurs. In the schematic, proteoliposomes with reconstituted protein (blue) are immobilized on the SSM sensor. Triangles and red circles represent nanobodies and substrate, respectively. (B) Electrogenic choline transport in the absence of nanobodies. Peak currents measured during activating conditions are shown for different substrate concentrations. (C) Representative measurement of currents during activating conditions in the absence of transporter protein at different substrate concentrations. (D) Plot of substrate concentration versus peak currents amplitude. The EC50 determined was 95 ± 11 µM choline. Error bars indicate standard deviation (n=3 biological replicates, n=3 technical replicates). Please click here to view a larger version of this figure.
Figure 2: Screening and classification of inhibitory and non-inhibitory nanobodies. (A) Electrogenic choline transport in the presence of a nanobody. Peak currents measured during activating conditions are shown in the absence of nanobody (blue), in the presence of an inhibitory nanobody (red), and after nanobody unbinding (green). (B) Measurement of currents during activating conditions in the absence of transporter protein. Traces show recordings in the absence of nanobody (blue), in the presence of an inhibitory nanobody (green), and in the presence of a non-inhibitory nanobody (red). (C,D). Histograms showing peak currents measured during activating conditions in the presence of nanobodies and after nanobody unbinding (recovery). Panel C shows the results of measurements using individual chips per nanobody. Panel D shows the results from a serial measurement using one chip. Nanobodies are indicated as Nb. Error bars indicate the standard deviation (n=3 biological replicates, n=2 technical replicates). Please click here to view a larger version of this figure.
Figure 3: Determination of IC50 of an inhibitory nanobody. (A) Electrogenic choline transport and inhibition by a nanobody. Peak currents measured during activating conditions are shown for different nanobody concentrations. (B) Plot of peak currents amplitude vs nanobody concentration from a serial measurement with an inhibitory nanobody. The IC50 determined was 18 ± 2 nM. Error bars indicate the standard deviation (n=3 biological replicates, n=3 technical replicates). Please click here to view a larger version of this figure.
The technique presented here classifies nanobodies with inhibitory and non-inhibitory properties targeting electrogenic transporters. Assessing the substrate transport is possible due to the detection of the movement of charges through the transporter embedded in the membrane of proteoliposomes. Some of the critical steps during the setup of an experiment are reconstitution of active protein in liposomes, preparation of stable monolayers on SSM chips, and recovering of initial conditions after the application of the wash protocol to remove bound nanobody molecules. Once the membrane protein is reconstituted at an appropriate lipid-to-protein ratio, a general SSM protocol can be established using the native substrate. It is crucial to perform control experiments using protein-free liposomes to reveal noise currents that would need to be subtracted from the currents measured using proteoliposomes. However, if noise currents are too large, we recommend trying protein reconstitution using different lipids, or screen for buffer conditions that minimize these deleterious signals. After successfully establishing conditions for an SSM assay, screening of nanobodies can be performed. A very useful option that may help in faster screening of nanobodies is to perform high-throughput assays using a single SSM sensor chip. This reduces the time of manipulation of chips and buffers and reduces the costs. However, because during this type of assay multiple nanobodies are applied sequentially, it is important to ensure that the applied nanobody can be washed away after the measurement. A stringent washing cycle may need to be implemented to unbind some nanobodies in case that reduced peak current amplitudes are detected in the absence of nanobody. We recommend using, as the starting point, the washing conditions described here. If increasing the washing volume or the number of cycles does not help, individual chips would need to be used to screen each nanobody separately. In all the cases examined here, the binding of nanobodies was reversible and a high-throughput protocol could be applied. In our experimental setup, we could not recover the full amplitude of the initial peak current after measurements with nanobodies (Figure 1A; Figure 2C,D). However, in most cases, the magnitude of the peak currents recovered ranged between 80 and 95% of the amplitude measured before applying nanobodies (Fig. 2C,D). We speculate that this could be a consequence of washing away a fraction of the proteoliposomes adhered to the chip, or due to slow kinetics of unbinding of some inhibitory nanobodies, or a combination of both. In either case, it was still possible to continue assaying further nanobodies as electrogenic transport was measurable. This is shown in Figure 2D, where we screened six nanobodies using a single chip preparation.
The high-throughput characteristic is one of the most significant advances of the method presented. In addition, in contrast to other approaches, this method allows for the selection of inhibitory nanobodies targeting electrogenic transporters for which labeled substrates are not available. A fast identification of inhibitory nanobodies can help to speed up the research aiming to identify novel applications of nanobodies as drugs. Their apparent advantages compared to similar therapies such as antibody treatments are numerous, starting with a smaller size which helps them propagate further into tissues or cells, to their low production costs and high stability.
SSM-based electrophysiology has been used in the past for the characterization of electrogenic transporters in membrane vesicles29,38. These types of experiments are advantageous as they do not depend on the protein purification and reconstitution protocols. We speculate that performing the selection of inhibitory nanobodies using membrane vesicles is feasible. This would help to reduce costs and avoid manipulations of purified proteins.
SSM-based electrophysiology is a strong technique to screen for nanobody inhibitors of multiple membrane proteins that exhibit electrogenic transport. We envision that SSM-based electrophysiology will become an important tool for the selection of inhibitory nanobodies and other antibodies with potential clinical applications.
The authors have nothing to disclose.
We thank Cedric A. J. Hutter and Markus A. Seeger from the Institute of Medical Microbiology at the University of Zurich, and Gonzalo Cebrero from Biozentrum of the University of Basel for collaboration in the generation of synthetic nanobodies (sybodies). We thank Maria Barthmes and Andre Bazzone from NANION Technologies for technical assistance. This work was supported by the Swiss National Science Foundation (SNSF) (PP00P3_170607 and NANION Research Grant Initiative to C.P.).
1-octadecanethiol solution | Sigma Aldrich | O1858-25ML | |
1,2-diphytanoyl-sn-glycero-3-phosphocholine | Avanti Polar Lipids | 850356C-25mg | |
Bio-Beads SM-2 Adsorbent (Polystyrene adsorbent beads) | BioRad | #152-3920 | |
PD 10 Desalting Columns | GE Healthcare | GE17-0851-01 | |
Filter 200 nm membrane | Whatman Nucleopore | WHA800282 | |
2-Propanol | Merck | 33539-1L-R | |
n-Decane | Sigma Aldrich | 8034051000 | |
n-dodecyl-ß-D-maltoside (DDM) | Avanti Polar Lipids | 850520P-25g | |
Sodium Chloride | AppliChem | 131659.1211 | |
(SSM setup) SURFE2R N1 | Nanion | —– | |
SURFE2R N1 Single Sensor Chips | Nanion | # 161001 | |
Trizma Base | Sigma Aldrich | T1503 | |
E. coli Polar Lipid Extract | Avanti Polar Lipids | 100600C | |
Egg PC L-α-phosphatidylcholine | Avanti Polar Lipids | 840051C |