Koutilya
Buchapudi
a,
Xiaohe
Xu
a,
Yeganeh
Ataian
b,
Hai-Feng
Ji
*a and
Marvin
Schulte
*b
aDepartment of Chemistry, Drexel University, Philadelphia, PA, USA 19104. E-mail: hj56@drexel.edu
bDepartment of Pharmacy, University of Alaska at Fairbanks, Fairbanks, AK, USA 99775. E-mail: mkschulte@alaska.edu
First published on 2nd November 2011
A potential binding assay based on binding-driven micromechanical motion is described. Acetylcholine binding protein (AChBP) was used to modify a microcantilever. The modified microcantilever was found to bend on application of the naturally occurring agonist (acetylcholine) or the antagonist (nicotine and d-tubocurarine). Control experiments show that microcantilevers modified without AChBP do not respond to acetylcholine, nicotine, and d-tubocurarine. Kd values obtained for acetylcholine, nicotine, and d-tubocurarine are similar to those obtained from radio-ligand binding assays. These results suggest that the microcantilever system has potential for use in label free, drug screening applications.
Current high throughput analyses commonly utilize membrane bound receptor proteins or cell lines that express cloned receptor subtypes. These assays typically provide high throughput using either radioligand or fluorescent binding assays in combination with low to moderate throughput functional assays. Functional assays for LGIC receptors often use either automated patch clamp,12 automated Xenopusoocyte two electrode voltage clamp,13 or a system using a fluorescent calcium or voltage sensing dye.14 While these assays provide reasonably high throughput for evaluation of drug candidates, they have significant limitations. Chief among these are the need to prepare isolated membrane preparations and/or maintain cell cultures for each receptor type being evaluated. Receptor proteins are not particularly stable and cannot be easily stored for long periods of time. Cellular assays require continually maintained cell cultures. The assays themselves must be designed so that as many potential cross-reactions with other receptors are identified as possible. While these assays are reasonably high throughput, it is still time consuming to evaluate interactions on large numbers of receptors. In addition, commonly used assays do not identify all interactions with a receptor but only interactions that produce effects observable in the assay system used. As the technology for the rapid production of new chemical entities is extended, so the analytical characterization efforts must increase to support these programs. Such drug screening technologies will need to provide rapid evaluation of drug molecules, multiple receptor analysis, and must be cost efficient. One such technology involves the use of microcantilevers.
Advances in the field of micro-electro-mechanical systems (MEMS) and their uses offer unique opportunities in the design of small-size and cost-effective analytical methods. Microcantilevers are the simplest MEMS device that can be micromachined and mass-produced.15 The unique characteristic of microcantilevers is that they can be made to undergo bending due to molecular adsorption by confining the adsorption to one side of the microcantilever.16–23 Microcantilever sensors hold a position as a cost-effective and highly sensitive sensor platform for medical diagnostics, and environmental and high throughput analysis. Since the microcantilever's deflection is derived from molecular binding, no labeled compound is needed, and this technology could undoubtedly be used to study the interaction of small molecules with drug targets for drug screening. Microcantilevers can also be incorporated into multichannel microcantilever chips that offer improved dynamic response, greatly reduced size, high precision, increased reliability and integration of micromechanical components with on-chip electronic circuitry.19,20 The low cost of the microcantilever technology would be more accessible to smaller laboratories than current high throughput systems, thus providing an added advantage over existing technology.
In our previous work, we have studied interactions of small molecules with the 5-HT3R receptor embedded membrane by using the microcantilever method.24 This membrane immobilized microcantilever and its binding with the naturally occurring agonist serotonin (5-hydroxytryptamine) and the antagonist MDL-72222 were determined. However, although hydrophobic chip surfaces have been created for coupling membrane receptors, these receptors produce much less stable and reliable surfaces than covalently linked proteins. On the other hand, receptor proteins, such as AChBP, could be produced in large quantities and distributed for use in a variety of assay systems, since they are soluble receptor proteins they are relatively easily attached to chip based biosensors and they are stable. In this work, microcantilever bending is used for an AChBP-analytes binding study, which has applications in drug screening and drug development.
Purity and assembly of AChBP were determined using native and denaturing PAGE as shown in Fig. 1. The left hand gel shows the results of PAGE (non-denaturing conditions) and the right hand gel shows the result of separation under denaturing conditions (SDS-PAGE). Gels were stained with Coomassie Blue stain (BioRad). The protein sample lane is indicated by S and the BioRad Kaleidoscope standard is indicated by Std. Under non-denaturing conditions, a distinct band is shown to migrate similar to the 150 kDa standard. Under denaturing conditions, the dominant band shifts to slightly less than 37 kDa. The molecular weight of the native protein of about 150 kDa is consistent with the predicted molecular weight of the pentameric AChBP. The 37 kDa single band in the denaturing gel is as expected for the monomeric protein. In the non-denatured protein, a smaller band is evident at around 37 kDa as well suggesting some unassembled monomers are present.
Fig. 1 Polyacrylamide gel electrophoresis of AChBP purified by IMAC. |
We used commercially available silicon microcantilevers (Veeco Instrument, CA, http://store.veeco.com/) in these experiments. The dimensions of the V-shaped microcantilever are 200 μm in length, 20 μm in width, and 1 μm in thickness. One side of the cantilever had a thin film of chromium (3 nm) followed by a 20 nm layer of gold deposited by e-beam evaporation. The deflection experiments were performed in a flow-through glass cell (Veeco, CA) similar to those used in atomic force microscopy (AFM). For continuous flow-through experiments, initially, the electrolyte solution was driven through the cell using a syringe pump. A constant flow rate at 10 ml h−1 was maintained during each experiment. The cantilever was immersed in the electrolyte solution until a baseline was obtained and the voltage of the position-sensitive detector was set as background corresponding to 0 nm.
Experimental solutions containing different concentrations of analytes were injected directly into the flowing fluid stream via a low-pressure injection port sample loop arrangement with a loop volume of 0.5 ml. This arrangement allows for continuous exposure of the cantilever to the desired solution without disturbing the flow cell or changing the flow rate. Since the volume of the glass cell, including the tubing, was only 0.3 ml, a relatively fast replacement of the liquid in contact with the cantilever was achieved. Deflection measurements were determined using the optical beam deflection method. The bending of the cantilever was measured by monitoring the position of a laser beam reflected from the gold-coated side of the cantilever onto a four-quadrant AFM photodiode. We define bending toward the gold side as “bending up”; “bending down” refers to bending toward the silicon side. In case the adsorption occurs on the gold surface, in general, the downward bending is caused by repulsion or expansion of molecules on the gold surface, which is the so-called compressive stress; vice versa, the upward bending is caused by attraction or contraction of molecules on the gold surface, which is called tensile surface stress. Three cantilevers were prepared for each of the individual experiments to allow statistical comparison of repeatability and efficiency between devices. To eliminate thermomechanical motion of the silicon cantilever caused by temperature fluctuations, we mounted the fluid cell on thermoelectric coolers so that the temperature of the fluid cell could be controlled to 20 ± 0.2 °C.
The Kd, Hill coefficient and Bmax were calculated by fitting the data to the following equation: B/Bmax = 1/(1 + (Kd/[L])n), where B is the microcantilever bending, Bmax is the maximum bending at equilibrium, L is the free ligand (acetylcholine) concentration and n is the Hill coefficient.
Scheme 1 Immobilization of AChBP on the gold surface of microcantilevers by EDC/NHS crosslinker. |
In our experiments, clean microcantilevers were stored for 48 hours in a 1 mM ethanolic solution of 11-mercaptoundecanoic acid. These microcantilevers were then thoroughly rinsed with distilled water before being immersed in a solution of 0.5 M NHS and 0.2 M EDC in distilled water for a time period of 12–72 hours. This was followed by thorough rinsing of cantilevers in DI water to remove excess chemicals. The final step was the immobilization of the AChBP on the microcantilever. 5 μl of the AChBP was dissolved in 1 ml of phosphate buffer solution. The microcantilevers were incubated in this solution for a period of 12–48 hours. The microcantilevers were then rinsed to remove any excess AChBP. The chemically modified microcantilevers were stored in buffer solution before use.
Table 1 shows the effect of conjugation time of the EDC/NHS methods on the deflection of the AChBP-modified microcantilever surfaces. It shows that the conjugation time of EDC/NHS is more important than that of the following conjugation time of AChBP. It also showed that a protocol of EDC/NHS reaction time 48 hours and the following cross-linking for 48 hours provided the maximum deflection upon exposure to the same concentration of analytes and the standard error was within 7%. We used this protocol in our entire sensor test in this work.
EDC/NHS reaction time/h | AChBP conjugation time/h | Deflection amplitude/nm |
---|---|---|
12 | 12 | 69.0 ± 20.4 |
12 | 24 | 75.2 ± 15.9 |
12 | 48 | 75.2 ± 17.7 |
24 | 12 | 81.4 ± 17.7 |
24 | 24 | 83.2 ± 16.8 |
24 | 48 | 83.2 ± 17.8 |
48 | 12 | 88.5 ± 9.73 |
48 | 24 | 86.7 ± 10.6 |
48 | 48 | 90.2 ± 6.20 |
72 | 12 | 77.0 ± 13.3 |
72 | 24 | 83.2 ± 17.7 |
72 | 48 | 85.8 ± 11.5 |
Fig. 2 Bending response as a function of time, t, for a silicon microcantilever coated with AChBP on the gold surface after injection of a 10−4 M solution of acetylcholine in 0.01 M phosphate buffer at pH = 7.0. The microcantilever was pre-equilibrated in the 0.01 M phosphate buffer solution before injection of the acetylcholine solution. |
The bending amplitudes of the microcantilevers at equilibrium vs. the log of the concentration of acetylcholine are shown in Fig. 3. Each point shown on the curve represents the mean ± SE of three experiments. The standard deviation induced by variation in the cross-linked AChBP on different cantilevers and the position of the focused laser spot at the end of the cantilever was found to be within ±25%. The data in Fig. 3 were used to determine dissociate constants (Kd) of the AChBP to acetylcholine. A Kd value of 1.83 × 10−6 M was calculated from these data using non-linear curve fitting techniques and Graphpad Prism software, which is close to 4.3 × 10−6 M from Smit et al.28 for radioligand binding. A Bmax value of 107 ± 1.7 nm was also determined.
Fig. 3 Maximum deflection of a silicon cantilever coated with AChBP on the gold surface as a function of the concentration of acetylcholine in 0.01 M phosphate buffer at pH = 7.0. The Kd and Bmax were calculated by fitting the data to the following equation: B/Bmax = 1/(1 + (Kd/[L])n), where B is the microcantilever bending, Bmax is the maximum bending at equilibrium, L is the free ligand (acetylcholine) concentration and n is the Hill coefficient. |
Competitive antagonists were also tested to verify the specificity of microcantilever bending resulting from binding of ligands to the AChBP receptor and to identify any variation in binding kinetics for agonistsversusantagonists. Nicotine and d-tubocurarine were chosen due to their availability and they were well studied for ready comparison.
Similar to application of acetylcholine, 10−6 M nicotine or d-tubocurarine produced a deflection of the microcantilever coated with the AChBP (Fig. 4). The time to plateau is much faster for d-tubocurarine and nicotine compared to that for acetylcholine, indicating a high binding constant between AChBP with nicotine or d-tubocurarine. In the absence of AChBP no bending was observed on application of 10−6 M nicotine or d-tubocurarine indicating that nicotine or d-tubocurarine by itself does not produce a deflection of the microcantilever. The deflection amplitude at equilibrium of the microcantilever vs. the concentration of nicotine in the buffer solutions is shown in Fig. 5. Kd values of 1.92 × 10−8 M and 7.1 × 10−9 M−1 for nicotine and d-tubocurarine, respectively, were calculated from these data as described above. The Bmax values are 13 ± 0.47 nm and 32 ± 0.67 nm for nicotine and d-tubocurarine, respectively.
Fig. 4 Bending response as a function of time, t, for a silicon microcantilever coated with AChBP after injection of a 10−6 M solution of nicotine (■) and d-tubocurarine (◆) in 0.01 M phosphate buffer at pH = 7.0. The microcantilever was pre-equilibrated in the 0.01 M phosphate buffer solution before injection of the analyte solution. Control experiments were done by introducing 10−6 M solution of nicotine (●) and d-tubocurarine (line not shown) to a microcantilever without AChBP in 0.01 M phosphate buffer at pH = 7.0. |
Fig. 5 Maximum deflection of a silicon cantilever coated with AChBP as a function of the concentration of nicotine (left) and d-tubocurarine (right) in 0.01 M phosphate buffer at pH = 7.0. The Kd and Bmax were calculated as described in Fig. 2 for acetylcholine. |
The data presented here demonstrate that the deflections we observed are the result of binding of acetylcholine, nicotine, and d-tubocurarine with AChBP. From a molecular point of view, binding can result in electrostatic repulsion, attraction, steric effects, intermolecular interactions or a combination of effects that alter the surface stresses on the cantilever.29 The mechanism responsible for producing deflections of the AChBP-modified microcantilever in response to ligand binding may be due to a slight conformational change of the AChBP on the microcantilever derived from the binding of the ligand to AChBP. The conformational change of the AChBP upon binding to agonists and antagonists has been demonstrated by using a fluorescent probe.30 The surface stress resulting from protein conformation change has been a recent focus of MCL research.31 Conformational changes are capable of altering immobilization of molecules on the surface, distances between molecules, relative orientations and surface interactions; thus it is reasonable that conformational changes will alter MCL bending. The Bmax for nicotine and d-tubocurarine is much less than that for acetylcholine, which reflects a difference in conformational change of the AChBP on the surface. Partial agonists and antagonists, such as nicotine and d-tubocurarine, would likely produce smaller conformational changes compared to a full agonist like acetylcholine.
The bending approach based on adsorption-induced surface stress is of particular interest in the study of conformational change in proteins. Surface stress changes due to protein conformational change on interaction with analytes could act as transducers of chemical information. The AChBP is an example of a protein that undergoes conformational change on ligand binding. Microcantilevers responding to these stresses would be ideal for high sensitivity detection of the small dimensional changes expected. These microcantilevers could also be used to investigate conformational changes that do not involve analyte interactions.
While the use of the AChBP in high throughput applications may be limited, the similarity of this protein to the LGIC family makes it likely that other similar proteins might be developed with similar functionality on microcantilevers. Kostelidou et al. have reported the expression of multiple nicotinic subunits in a soluble form similar to the AChBP. Further advance in this direction could provide a wide array of human LGICs for use in microcantilever arrays.32 The development of microchip arrays makes it possible to evaluate a single drug candidate on a wide variety of receptors simultaneously. In addition to the development of large arrays containing multiple receptor subtypes, it would also be possible to develop arrays designed to identify the specific binding site on a receptor at which a drug candidate binds. This array would be composed of fully functional receptor proteins along with receptors mutated at different known binding sites on the protein. An inkjet printing technique can be used to modify the cantilever array, each cantilever modified by specific AChBP mutants or references.
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