Difference between revisions of "Team:Freiburg/Results/Surface"

Optimizing cell-free expression as such is already a challenging task. But it becomes increasingly more complicated when the expressed proteins should be immobilized on a glass surface directly after expression: Cell-free mix is a complex system mainly consisting of proteins not that different to the target proteins to be immobilized. To overcome this hurdle we decided on fusing a tag to the proteins of interest that specifically binds on a catcher on the surface. But even with such a system, the surface has to be optimized in order to minimize unspecific binding.

Effective - The Unspecific Surface

Figure 1: Comparison of fluorescence intensity of bound GFP on GOPTS and PDITC surfaces

As we needed a glass surface for measuring in iRIf, we used silanes to introduce reactive groups on the surface. Silanes integrate into the chemical structure of glass after being activated using oxygen plasma. Adding either the silane GOPTS (3-Glycidyloxypropyltrimethoxysilane) or APTES (3-Aminopropyltriethoxysilane) allowed us to couple certain chemical groups to the surface. The epoxy-group of GOPTS reacts covalently with amino-, hydroxy- and thiol-groups so that a large spectrum of molecules can be coupled. APTES on the other hand is not reactive itself but can be coupled to amino-groups with the homobifunctional cross-linker PDITC (p-Phenyldiisothiocyanate). For further information on chemistry and methods see surface chemistry methods . To evaluate these two coupling chemistries, we compared the binding capacities of the respective surfaces on simple microscope glass slides. Self-purified GFP in different concentrations was spotted on both surfaces and the resulting fluroescence intensity was compared (Figure 1). Especially for low concentrations it is clearly visible that APTES/PDITC outcompetes the GOPTS surface. Therefore, we continued our experiments using the APTES-chemistry. With these results we decided to switch on special glass slides, suitable for iRIf. With this method we were able to detect the interaction of anti-GFP antibodies with spotted GFP of different concentrations. To check for variations in different GFP-purification protocols, we compared GFP obtained from different groups (GFP1 to GFP3).

Surface bound GFP was first washed mutliple times in the iRIf device. Anti-GFP in buffer solution was flushed over the slide and changes in surface layer thickness due to GFP-binding were detected in real-time. Figure 2 shows a quotient picture from this step, thus the increase in surface thickness due to antibody binding. The signal can further be amplified by a second binding step. As the anti-GFP antibody was biotinylated it could easily be attached to streptavidin flushed through the microfluidic chamber (Figure 3). This step also confirms the binding of anti-GFP to the spots and therefore the specificity of the interaction. Biotinylated BSA (bBSA, bottom middle) spotted on the slide, additionally served as positive control.

Figure 2: iRIf quotient picture of spotted proteins after anti-GFP bindingstrong>

Figure 3: iRIf quotient picture of spotted proteins after additional Strep-Cy5 binding

Getting Selective - The Specific Surface

Figure 4: Comparison of specific Ni-NTA with unspecific PDITC surfaces>

All the surfaces presented above show, that a detection of antigen-antibody interaction is possible using a surface chemistry. But as we need a specific surface to purify antigens out of cell-free expression mix, we fused a 10x Histidin tag to our proteins and optimized a Ni-NTA (Nickel-Nitrolotriacetic acid) surface derivatization. To determine the specificity of this Ni-NTA surface we compared it to the PDITC surface. To asses the purifcation properties we used complete E. coli lysate transformed with either a tagged or an untagged GFP-construct. Additionally purified GFP-His as used in previous experiments was spotted and fluorescence intensity was measured. Figure 4 shows the intensities obtained for all spots: the intensity for the His-GFP lysate on the Ni-NTA surface is about four times higher than on the PDITC surface, while the values for the purified His-GFP are in a comparable range. The mean intensity for the untagged GFP-lysate spot is in the range of the background for the Ni-NTA surface and just slightly higher for the PDITC surface, which shows, that the GFP cannot bind to Ni-NTA without a His-tag. The low fluorescence intensities for lysate on PDITC may be due to the fact, that non-fluorescent proteins in the lysate are bound as efficient as GFP. This way the surface is blocked for further GFP molecules and overall fluorescence decreases compared to the specific Ni-NTA surface.

After we showed that we were able to bind his-tagged proteins specifically, we attempted to immobilize our cell-free expressed His-GFP-Lysate on our Ni-NTA surface. You can find the results for this crucial part of our project at the main results page.

Diverse - Other Surface Systems

Besides Ni-NTA we worked with the Promega Halo-Tag system, to find the system best suited to our needs. The Halo-Tag that can be fused to target proteins binds covalently to chloralkanes which are immobilized on the surface. We tested several ligands, which differed in length of the alkane chain and surface attachment method. The ligand that worked best for us, was a 3-chloropropylsilane, which we directly immobilized on plasma activated iRIf slides. To test the surface we spotted our self-expressed Halo-GFP and Halo-mCherry as well as purified Halo-GFP as a positive control and purified untagged GFP as a negative control, which we both got from a research group from Osnabrück. As an additional negative control we spotted bBSA. The iRIf measurement showed that the Halo-tagged GFPs were successfully immobilized on the surface. Unfortunately there was a lot of unspecific binding, so that the negative control nearly bound as much to the surface as the positive control. The needed optimizations that would be necessary for a specific surface could not be performed due to time limitations. We decided to work with the Ni-NTA surface we established for future experiments.

Figure 7: quotient picture Halo-surface

Figure 8: binding curve Halo-surface

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