Cristina Gutiérrez
Sánchez‡
,
Qiang
Su‡
,
Sabine
Wenderhold-Reeb
and
Gilbert
Nöll
*
Nöll Junior Research Group, Organic Chemistry, Chem. Biol. Dept., Faculty IV, Siegen University, Adolf-Reichwein-Str. 2, 57068 Siegen, Germany. E-mail: noell@chemie.uni-siegen.de
First published on 6th June 2016
The multi-ligand binding flavoprotein dodecin is reconstituted on top of flavin-terminated oligonucleotide monolayers. A detailed quartz crystal microbalance with a dissipation monitoring (QCM-D) study showing how the length and flexibility of the oligonucleotide tethers influence the stability and the viscoelastic properties of the resulting DNA–protein layers is presented. Relatively dense protein layers can be obtained, if the length of the tethers is in the same range as the diameter of dodecin. When significantly longer tethers are used, less dense layers are formed. When rather short tethers are used, the reaching area of individual tethers is too low to capture single apododecin molecules cooperatively, and the formation of stable and dense protein layers is not possible. On top of the DNA–dodecin layers additional flavin–DNA ligands may be captured to form sandwich-type DNA–protein–DNA layers. Differences in the binding and unbinding behavior of flavin-dsDNA and flavin-ssDNA ligands are measured by QCM-D and surface plasmon fluorescence spectroscopy (SPFS). Both type of ligands show relatively low kon values, which might be explained by the structural rigidity of the binding pockets allowing a ligand to enter only when it approaches precisely in the right orientation. Apparently apododecin–flavin binding follows Fischer's classic lock-and-key binding model.
While in previous studies regarding the reconstitution of dodecin on surfaces always dsDNA tethers comprising 20 base pairs (bp) were used,1,2,5 here a detailed QCM-D study is presented showing how the length and flexibility of the surface grafted and flavin-terminated oligonucleotide tethers influence the stability and the viscoelastic properties of the resulting DNA–protein layers, which may then be used to bind additional bi- or multidentate ligands. In addition differences in the binding and unbinding behavior of flavin-dsDNA and flavin-ssDNA ligands are measured by QCM-D and surface plasmon fluorescence spectroscopy (SPFS). Both type of ligands show relatively low kon values for apdodecin–flavin complex formation in comparison to the streptavidin–biotin system, which follows almost diffusion-controlled kinetics. The different kinetics might be explained by differences in the ligand binding mechanism of both proteins. The apododecin–flavin ligand binding kinetics are discussed in the context of the lock and key model, which has been introduced in 1894 by Emil Fischer.15
For the QCM-D measurements standard sensor chips (QSX301, Q-Sense, Västra Frölunda, Sweden) with the following specifications were used: frequency 4.95 MHz ± 50 kHz, diameter 14 mm, thickness 0.3 mm, RMS surface roughness of electrode <3 nm. Before modification, the sensors were cleaned with an UV cleaner for 10 min, thereafter with basic Piranha (1:
1
:
5 of H2O2, 25% ammonia solution, pure water) at 75 °C for 5 min, and again with UV treatment for 10 min.
On the surface modified with flavin-dsDNA ligands dodecin forms a rigid layer with a typical overlap of the frequency overtones (see Fig. 1A and 2B in ref. 1). Initially there is an increase of the dissipation signal caused by rocking and sliding motions of apododecin adsorbed mainly by single flavin ligands before the dissipation factor decreases with proceeding formation of multi-ligand binding leading to a stiff layer with restricted lateral motion of the adsorbed apoprotein molecules.1 The fact that dissipation-factor values for lower overtones decrease below the initial level prior to apododecin adsorption indicates that the lateral motion of the dsDNA tethers is also being restricted upon binding with apododecin.21–24 Considerable spreading of the dissipation overtones indicates strong viscoelastic dispersion, which may originate from relaxation processes at rates comparable to the oscillation frequency of the resonator.23,25
Adsorption of apododecin on the surface modified with flavin-ssDNA tethers also results in the formation of a rigid layer (see Fig. 1B and S1B†). The somewhat lower shift in frequency in comparison to the dsDNA tethers can be explained by a lower amount of water molecules and possibly also cations being trapped in the ssDNA sublayer than in the dsDNA sublayer.23 In contrast to the flavin-dsDNA tethers, for the flavin-ssDNA tethers the bandwidth shift of the 5th through 13th overtones shows little difference during apododecin adsorption.
The resulting flavin-dsDNA (100 bp) tether contains two nicks in the DNA backbone, which may introduce additional flexibility. As before, a solution of apododecin in buffer was incubated on the flavin-terminated dsDNA layer for a few minutes before the surface was rinsed with buffer solution. In Fig. 2 and S2† the corresponding QCM-D binding and unbinding curves are shown. On the surface with flavin-dsDNA (100 bp) tethers the adsorption of the apododecin considerably increases the dissipation-factor. Mechanical compliance of the extended DNA linkers results in the formation of a viscous layer, also indicated by spreading of the frequency overtones. The decrease in frequency upon apododecin adsorption is 2–3 times lower than for the 20 bp dsDNA tethers, which could be explained by a somewhat lower amount of flavin ligands at the surface, since the efficiencies of the individual hybridization steps leading to the formation of the flavin-dsDNA (100 bp) tethers are expected to be less than 100%. Additionally the formation of a less regular and less dense dodecin layer is expected, since with increasing tether length the reaching area of individual flavin-DNA tethers increases and for a single apododecin molecule more flavin ligands attached to the surface at different sites are available. To minimize the tether length, a double-stranded locked nucleic acid (dsLNA) tether formed by hybridization of flavin and 1,2-dithiane modified LNA was employed (see Fig. 3).
In contrast to the typical B-type DNA/DNA helix, A-type conformation in DNA/LNA and LNA/LNA with a shorter base stacking distance and rigid duplex structure is expected to increase the thermal stability.26,27 Using LNA 7 bp were sufficient for strong hybridization at the surface leading to a long-term stable monolayer (the length of dsLNA with 7 bp is about 2 nm).28 Again a solution of apododecin in buffer was incubated for a few minutes before the surface was rinsed with buffer solution. Similar to the flavin-dsDNA tethers with 20 bp (see Fig. 1A) there is not much splitting of the frequency overtones in Fig. 3 and S3.† The fact that this time the overtones do not completely overlap can be explained by the formation of a less dense layer allowing some lateral motion of the adsorbed apododecin molecules. This assumption is supported by the decrease in frequency, which is 2–3 times less intense than for the flavin-terminated dsDNA layer with 20 bp. As the reaching area of the short flavin-LNA tethers is strongly decreased, less apododecin molecules can be captured.
As a consequence of the decreased reaching area of the tethers the probability for multi-ligand binding is less pronounced. This can also be deduced from the unbinding curve showing that by rinsing with buffer solution for a few minutes almost 80% of the apododecin molecules are being released. Again the spreading of the dissipation overtones indicates viscoelastic dispersion, which may originate from relaxation processes at rates comparable to the oscillation frequency of the resonator.
For the different tethers used in this study also the average distance between individual flavin-terminated oligonucleotide tethers is of interest. Due to the contribution of surface entrapped solvent molecules a determination of the increase in surface bound mass from the QCM-D data would not allow an accurate calculation of the surface coverage.23 Nevertheless the experimental data show that for the dsDNA and the ssDNA tethers used in Fig. 1 (with a length of about 7 nm) the distance between individual tethers is sufficiently short to allow the vast majority of the apododecin molecules to be captured by multi-ligand binding. As for the stepwise formation of the long flavin-dsDNA (100 bp) tethers (including three hybridization steps) the same type of capture probe layer as in Fig. 1A was used, but the hybridization efficiency for each step is expected to be less than 100%, the flavin surface coverage is expected to be somewhat lower than in Fig. 1A, but still sufficiently high to capture most apododecin molecules by multi-ligand binding. As for the flavin-dsLNA tethers with an overall length of 2–3 nm still about 20% of the adsorbed apododecin molecules are captured by multi-ligand binding, also here a rather dense layer was formed.
In Fig. 4 and S4† three times the adsorption of apododecin followed by rinsing with buffer solution and subsequent chemical flavin reduction resulting in the release of the remaining apododecin molecules is shown. In contrast to layers formed from flavin-terminated dsDNA of 20 bp the multiple binding and quantitative release of apododecin could only be achieved on the thin flavin-terminated dsLNA monolayer, if a fresh QCM crystal was applied (usually after a QCM experimental run the crystal can be cleaned and reused a few times). Apparently the quality of a monolayer formed by chemisorption of short LNA tethers is extremely sensitive against surface roughness, whereas minor inhomogeneities in the gold surface can be compensated by longer dsDNA tethers.
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Fig. 4 Frequency (blue) and dissipation factor (red) shifts (overtones 5-13) observed in situ by QCM-D measurements. Three times the adsorption of apododecin DtE on monolayers of flavin-terminated dsLNA with 7 base pairs, followed by rinsing with buffer solution, and subsequently by rinsing with an oxygen-free buffered sodium dithionite solution for flavin reduction in order to release remaining DtE molecules captured by multi-ligand binding was measured. For the second and third chemical reduction step the period for rinsing with sodium dithionite had to be subsequently expanded. Prior to the first incubation of DtE a non-binding apododecin variant, W36A, was incubated as negative control at a concentration of 5 μM and subsequently rinsed with buffer to ensure that there was no unspecific binding.2,5 |
After addition of the non-binding ligand (A) the fluorescence signal decreases as soon as the ligand containing solution is removed from the cell. During incubation of the dsDNA ligand (B) the increase in the fluorescence signal is only little larger than for the negative control, and the vast majority of this ligand could be removed after less than one hour of rinsing with buffer. In contrast for the ssDNA ligand (C) the increase in fluorescence is much larger indicating that a lot more ligand molecules are bound. The difference in fluorescence increase is so large that binding seems to follow faster kinetics and cannot only be explained by a larger amount of bound ligand molecules. In addition the unbinding kinetics of the ssDNA ligand are slower, since after rinsing for one hour still a significant amount of ligand is captured. For a detailed analysis of the unbinding kinetics the experimental curves were fitted exponentially as presented in the ESI, Fig. S6.† If the signal increase by fluorophores, which are present in the cell without being bound to the surface, is neglected, the unbinding kinetics of the dsDNA ligand can be fitted mono-exponentially, whereas two exponential functions are necessary in order to fit the unbinding kinetics of the ssDNA ligand. The latter finding can be explained by the fact that in principle each dodecin binding pocket can capture up to two ligands, and the second binding/unbinding event may follow different kinetics than the first. If this holds true for the ssDNA ligand, it can further be assumed that in the case of the dsDNA ligand only a single ligand is bound to each binding pocket. Probably the rather large and stiff dsDNA substructure acts as a stopper and prevents a second ligand from entering the binding pocket for steric reasons. Individual values of kon and koff obtained by fitting the SPFS unbinding kinetics exponentially are presented the ESI.† Since the accuracy of the analysis of the SPFS data is limited due to additional contribution of non-bound molecules to the fluorescence signal (as shown by the negative control), the corresponding experiments were carried out in the QCM-D cell as well, shown in Fig. 6 and S5.† Also these measurements show that a lot more molecules of the flavin-ssDNA can be captured than of the flavin-dsDNA (assuming there is not much difference in the number of trapped solvent molecules, which also contribute to the overall shift in frequency).23 A detailed analysis of the kinetic QCM binding/unbinding curves revealed that binding and unbinding of the flavin-dsDNA ligand can be fitted by a single exponential curve as presented in the ESI, Fig. S7.† Apparently only one flavin-dsDNA ligand can be captured in each binding pocket. Average values of kon = 1.3 × 103 M−1 s−1, koff = 3.5 × 10−3 s−1, and Kd = 2.7 × 10−6 M were determined from three experimental runs.
In accordance with the analysis of the SPFS unbinding curve, two exponential functions were required to fit the binding/unbinding curve of the flavin-ssDNA ligand in Fig. S7.† For the first binding/unbinding event, i.e. binding of the ligand to an empty and release from a singly occupied pocket average values of kon = 1.6 × 104 M−1 s−1, koff = 2.2 × 10−3 s−1, and Kd = 1.4 × 10−7 M were obtained. Apparently for binding to an empty binding pocket the flavin-ssDNA ligand binds with a kon value that is about one order of magnitude larger than for the flavin-dsDNA ligand, whereas both ligands follow nearly the same unbinding kinetics. While after binding a single flavin-dsDNA ligand the entrance to the pocket seems to be blocked, after binding a first flavin-ssDNA ligand a second flavin-ssDNA ligand may enter the same pocket following slower kinetics. For the second binding event a mean value of kon = 7.0 × 102 M−1 s−1 has been determined. The binding of the second ligand is expected to be stabilized by aromatic tetrade formation inside the binding pocket i.e. by π-stacking interaction between the two isoalloxazine moieties of the flavins and the two tryptophans W36 belonging to the apoprotein.2,5 This results in a relatively low value of koff = 1.9 × 10−4 s−1. Since for the second binding event not only kon but also koff is smaller than for the first, the value of Kd for the second binding/unbinding event (Kd = 2.7 × 10−7 M) is similar to that of the first (Kd = 1.4 × 10−7 M).
By comparing ssDNA and dsDNA it turned out that each dodecin binding pocket binds only a single flavin-dsDNA ligand whereas two flavin-ssDNA ligands can be incorporated. As the dsDNA is rather bulky and stiff, the kinetics for binding the dsDNA ligand to an empty pocket are slower than for the flavin-ssDNA ligand, but the unbinding kinetics are about the same. For the flavin-ssDNA ligands a second binding event is possible comprising smaller values for kon and koff than the first. As a consequence the binding strength reflected by the Kd values are about the same for the first and second binding/unbinding event of the flavin-ssDNA ligand, whereas the flavin-dsDNA ligand binds about one order of magnitude weaker.
However, also for the first binding event of the flavin-ssDNA ligand the kon value of kon = 1.6 × 104 M−1 s−1 is much lower than expected for diffusion-limited complex formation. For a diffusion controlled process, i.e. if each collision between apododecin and flavin ligand results in complex formation a value for kon in the order of 108 M−1 s−1 or even 109 M−1 s−1 would be expected. As a possible explanation the rather low kon values might be originated from the dodecin binding mode fitting the classic lock-and-key model of protein ligand interaction quite well. This assumption is made based on crystallographic data from apododecin (with empty pockets) and dodecin complexes with different flavin ligands, which show little to no difference between Cα-atom positions.2–5 Thus the (apo)dodecin binding pockets comprise a fixed steric configuration and there is nearly no structural rearrangement of the complex upon ligand binding. Ligands can enter only if they approach the binding pocket in a precise orientation. For flavin-oligonucleotide ligands with larger flexibility there will be a (somewhat) higher probability for the isoalloxazine moiety to reach the final binding site, i.e. binding is favored, if a rather long and flexible linker in between isoalloxazine and oligonucleotide is present, and/or if the oligonucleotide as such is flexible, which is the case for ssDNA but not for dsDNA. This is in contrast to ligand binding by an induced fit mechanism that has been described e.g. for the prominent multi-ligand binding (apo)streptavidin–biotin system, which comprises nearly a diffusion-limited rate for complex formation.29,30 For streptavidin–biotin a value of kon ≈ 3.8 × 108 M−1 s−1 can be calculated from Kd ≈ 10 fM and koff = 3.8 × 10−6 s−1.29–35 Binding a biotin ligand is going along with mayor structural rearrangement, and one surface loop folds over the binding site when biotin is bound.36–39 Accordingly the rather low kon value of dodecin can be explained by its ligand binding mechanism. Taking the structural peculiarity of dodecin into account, a strategy for the formation of stable and dense protein layers with high mechanical stiffness could be the hybridization of a 20 bases capture probe strand (as used previously, e.g. as shown in Fig. 1A) with a flavin-modified complementary strand comprising 20 bases complementary to the capture probe, and an overhang of five to ten bases (e.g. thymidines) at the flavin-terminated 5′-end providing the flavin at a flexible subunit of ssDNA. In principle also flavin and thiol (or dithiane) modified ssDNA can be used (as shown in Fig. 1B), but the synthesis of ssDNA modified at both ends is synthetically more demanding. Furthermore it has been reported that the isoalloxazine moiety of flavins may absorb irreversibly at bare gold surfaces.40
This can be prevented if the gold surface is first modified with (flavin-free) ssDNA, followed by adsorption of short thiol molecules, before the flavin moiety is introduced in a hybridization step. This surface modification strategy has also the advantage that the flavin density at the surface (relative to the number of dsDNA-strands) can be varied by hybridization with mixtures of flavin-modified and flavin-free complementary ssDNA with different ratio as shown before.1
Footnotes |
† Electronic supplementary information (ESI) available: The different presentation of QCM-D readout is shown and the analysis of kinetics is presented. See DOI: 10.1039/c6ra10090b |
‡ Authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2016 |