Bernice
Akpinar
ab,
Philip J.
Haynes
ab,
Nicholas A. W.
Bell
c,
Katharina
Brunner
cd,
Alice L. B.
Pyne
*ae and
Bart W.
Hoogenboom
*af
aLondon Centre for Nanotechnology, University College London, 17-19 Gordon Street, London WC1H 0AH, UK. E-mail: a.l.pyne@sheffield.ac.uk; b.hoogenboom@ucl.ac.uk
bDepartment of Chemistry, Imperial College London, SW7 2AZ, UK
cThe Francis Crick Institute, 1 Midland Road, London, NW1 1AT, UK
dDiscovery Biology, Discovery Sciences, R&D, AstraZeneca, 50F49, Mereside, Alderley Park, Macclesfield, Cheshire SK10 4TG, UK
eDepartment of Materials Science and Engineering, University of Sheffield, S1 3JD, UK
fDepartment of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UK
First published on 23rd September 2019
DNA–protein interactions are vital to cellular function, with key roles in the regulation of gene expression and genome maintenance. Atomic force microscopy (AFM) offers the ability to visualize DNA–protein interactions at nanometre resolution in near-physiological buffers, but it requires that the DNA be adhered to the surface of a solid substrate. This presents a problem when working in biologically relevant protein concentrations, where proteins may be present in large excess in solution; much of the biophysically relevant information can therefore be occluded by non-specific protein binding to the underlying substrate. Here we explore the use of PLLx-b-PEGy block copolymers to achieve selective adsorption of DNA on a mica surface for AFM studies. Through varying both the number of lysine and ethylene glycol residues in the block copolymers, we show selective adsorption of DNA on mica that is functionalized with a PLL10-b-PEG113/PLL1000–2000 mixture as viewed by AFM imaging in a solution containing high concentrations of streptavidin. We show – through the use of biotinylated DNA and streptavidin – that this selective adsorption extends to DNA–protein complexes and that DNA-bound streptavidin can be unambiguously distinguished in spite of an excess of unbound streptavidin in solution. Finally, we apply this to the nuclear enzyme PARP1, resolving the binding of individual PARP1 molecules to DNA by in-liquid AFM.
AFM has been established as a powerful single-molecule technique to probe DNA–protein interactions, due to its ability to directly image DNA at nanometre resolution under physiologically relevant conditions without the need for labelling.10–12 However, to obtain high-resolution images of biomolecules in liquids, the sample must be adhered to an underlying solid support. Muscovite mica is the substrate of choice for AFM imaging of DNA, due to the ease of preparing an atomically flat mica surface via cleavage along the basal plane, and due to the polar, hydrophilic nature of the cleaved surface, facilitating the adsorption and retention of biomolecules in aqueous solution. When mica is hydrated, K+ ions dissociate from interstitial sites within mica's aluminium phyllosilicate lattice, resulting in a net negative charge on the surface. To permit the adsorption of DNA onto its highly negatively charged phosphate backbone, the negative surface charge needs to be screened or compensated for.13,14 Many adsorption protocols have been established for the 2D confinement of DNA to pre-treated mica,15 one of the most commonly adopted being the use of transition metal cations such as Ni2+, Co2+ and Zn2+ that can substitute into vacant sites within the mica lattice, yielding positively charged patches for the adsorption of DNA.16 The strength of the electrostatic attraction can be modified by the presence of additional ions and chelating agents within the imaging buffer.17,18 Other methods to facilitate DNA absorption include the modification of surface chemistry using silanes,15 the formation of partially positively charged lipid bilayers9,19 and the electrostatic adsorption of positively charged polymers such as poly-L-lysine (PLL).20,21
The aforementioned approaches are often adopted for the study of DNA–protein binding using AFM. However, they can result in non-specific protein–surface interactions, which are non-trivial to deconvolute from specific DNA–protein interactions. The problem of non-specific adsorption can be addressed by the use of surface coatings that are protein repellent, for example polymer brushes that suppress protein binding by steric repulsion.22 One approach to suppress protein binding is to create an interfacial layer of polyethylene glycol (PEG) brushes. The high degree of hydration and flexibility of these brushes causes surface passivation when the chains are of sufficient length and grafted at high density.23 Facile preparation of PEGylated surfaces is achieved using multifunctional copolymers comprising both surface binding domains and surface passivating PEG domains. Graft-copolymers with a cationic PLL backbone and PEG side chains (PLL-g-PEG) have proven particularly effective at self-assembling into densely packed polymeric brushes to form non-fouling surfaces.23–28 In addition, bio-recognition sites, such as RGD-peptides, have been incorporated into these films to promote cell adhesion whilst suppressing the non-specific adsorption of serum proteins.29,30 Similarly, the incorporation of biotin-terminated PEG chains has been used to form small molecule biosensors that selectively bind streptavidin, neutravidin and avidin.31 Unmodified PLL-g-PEG films have also shown the ability to selectively adsorb DNA polyelectrolytes onto the underlying positively charged PLL layer, whilst the PEG layer remains impervious to other proteins, as confirmed by fluorescence imaging.28
The well-studied graft copolymer (PLL-g-PEG) adopts a comb-like conformation in solution comprising a long PLL backbone with randomly distributed PEG side chains, whilst the block copolymer (PLL-b-PEG) exhibits a linear worm-like conformation comprising regions of lysine repeats followed by regions of ethylene glycol repeats. Both copolymers can form protein repellent PEG brushes on a variety of substrates through the spontaneous electrostatic attachment of their lysine residues. In the case of the graft copolymer, the length of the PEG block and the grafting ratio affect the density and hence the efficacy of the anti-fouling brushes.26 The diblock copolymer has been less widely employed for surface passivation but has been shown to be effective at inhibiting cell adhesion on glass surfaces micro-patterned with PLL100-b-PEG22.32 The passivation properties of the diblock copolymer (PLLx-b-PEGy) can be tuned by varying the degree of polymerization of both the PLL ( x) and PEG ( y) chains which would affect the packing density onto the underlying substrate, although as of yet variations of these have not been explored. We here set out to determine whether linear PLLx-b-PEGy diblock copolymers can be used in the functionalization of mica to yield a surface that selectively adsorbs DNA and allows the characterization of DNA–protein complexes by AFM. Through the optimization of the composition of the diblock copolymer, we have developed biphasic films which promote the adsorption of negatively charged DNA, whilst passivating against non-specific protein adsorption. Specifically, we perform mica surface functionalization that allows high-resolution AFM imaging of DNA and of DNA–protein complexes in solution whilst resisting non-specific protein adsorption.
Monovalent streptavidin was produced by the Howarth lab.33 Block copolymers methoxy-poly(ethylene glycol)-block-poly(L-lysine hydrochloride) with varying degrees of polymerization of the poly-L-lysine and polyethylene glycol blocks were purchased as lyophilized powders from Alamanda Polymers. The polymers used for this study were PLL10–PEG22, PLL10–PEG113, PLL100–PEG113 and PLL10–PEG454 where the subscript refers to the degree of polymerization, i.e., the number of monomer repeats. ESI Table 1† details the corresponding molecular weights for each of the polymers used. A 0.01% w/v solution of poly-L-lysine (PLL1000–2000) with approximately one HBr molecule per lysine residue, along with all other reagents, were purchased from Sigma-Aldrich.
Fig. 2 Ordering of poly-L-lysine chains on a mica substrate. (a) AFM image taken in solution with tip sampling every ∼0.5 nm showing a DNA plasmid adsorbed onto PLL1000–2000-functionalized mica. (b and c) At higher magnification, PLL chains are unambiguously resolved. Height profiles underneath provide an indication of the respective protrusions of the PLL chains and of the DNA. (d) The axis of alignment observed in (b) is highlighted; (e) the mica lattice geometry36 is here aligned and overlaid with the resolved lysine chains, and their corresponding overlap with vacancies is observed. Inset colour scale for (a) is 8 nm and inset colour scales for (b) and (c) 4 nm, for (d) and (e) 0.8 nm. Scale bar for (a) is 100 nm, 10 nm for (b–d) and 5 nm for (e). |
For prior adsorption of DNA on the mica, the cleaved mica was incubated with in total 20 μl of the 1:1 PLL10-b-PEG113/PLL1000–2000 mixture and left to incubate in a humidified Petri dish for 45 minutes. This was then washed 5 times with double-deionised water and a further 5 times with imaging buffer (12.5 mM NaCl, 12.5 mM HEPES, 0.5 mM TCEP, pH 7.8, filtered by passage through a 0.2 μm syringe followed by a 10 kDa cutoff centrifugal filter (Amicon Ultra, Millipore)). 20 μL of 496 bp linear DNA with an ss break (1.5 ng μL−1, 7.8 nM) was then added to the disk and gently mixed. After a 30 minute adsorption, the sample was then washed 5 times and made up to 30 μL with imaging buffer.
For adsorption using PLL, 10 μL of PLL (0.01%) was added to a freshly cleaved mica surface and left to incubate for 1 minute. The disk was then held at an angle and thoroughly rinsed under a stream of double-deionised water. The disk was then blotted and 20 μL 494 bp linear DNA with an ss break (0.3 ng μL−1, 1.6 nM) was added. After incubating for 10 minutes, the sample was washed 5 times with imaging buffer. For adsorption using NiCl2, the freshly cleaved mica was incubated for 20 minutes with the DNA sample (0.3 ng μL−1, 1.6 nM) and 4 mM NiCl2. The sample was then washed 5 times with imaging buffer (the same as above but containing 3 mM NiCl2). For the PARP exchange assays, a buffer exchange for PARP1 in imaging buffer was carried out. Imaging was resumed after 5 minutes of incubation.
PLL surface functionalization is obtained by the incubation of a cleaved mica surface in PLL solution. Deposition at low concentrations (0.001% w/v) allows relaxation of the lysine chains and adsorption in flattened, stretched out conformations where individual poly-L-lysine molecules are resolved (Fig. 2).34 High resolution on the individual lysine chains was achieved in 10 mM phosphate buffer, a relatively poor solvent for poly-L-lysine, reducing the repulsion of the AFM tip which can then come into contact with the collapsed chains (Fig. 2(b)).35 The PLL chains are seen to preferentially align along three orientations, with an angular difference of about 60° (Fig. 2(d)). PLL chains appear to be better resolved when aligned at larger angles with respect to the fast scan axis (left to right in these images). When aligned along the fast scan axis itself, PLL chains are more difficult to resolve as their width is approximately equal to the width of one scan line (0.5 nm) and therefore more sensitive to the precise position of consecutive lines. While the underlying atomic lattice of the mica substrate cannot be resolved in these images, the observed orientations are consistent with a molecular arrangement in which the lysine residues occupy interstitial sites on the mica lattice vacated by K+ ions (Fig. 2(e)).36
When deposited from the stock solution at high PLL concentration (0.01% w/v), the lysine chains adopt more globular forms, resulting in an apparently more homogeneous surface functionalization (Fig. 3(a), see Fig. S3† for comparison of PLL deposition at low (a) and high concentrations (b)). PLL functionalized mica enhances the adsorption of DNA, but also of other biomolecules that may be present in solution, including those of reduced charge. This is demonstrated by the immobilization of both the highly negatively charged plasmid DNA and the slightly negatively charged streptavidin (pKa ∼5.0–6.0, at pH 7.4) (Fig. 3(a)).37 We show that the surface can be modified to achieve a more preferential, selective adsorption of DNA by functionalization with PLL10-b-PEG22 alone or by a combination of PLL10-b-PEG22 and long-chain PLL1000–2000. In the presence of the block copolymer streptavidin adheres as sparse clusters (Fig. 3(b) and (c)), perhaps due to the heterogeneous surface coverage of the protein-repellent PEG. In both cases, large areas of functionalized mica are visible without the protein adsorbed. This can be explained by the effective repulsion that arises when the polyethylene-glycol chains form a sufficiently dense steric barrier.
To achieve a homogeneous surface that resists protein adsorption across the entire sample, the PEG molecules should be grafted at a density that is large enough to facilitate the overlap between different chains, resulting in the formation of a dense polymer brush.38 This requires the radius of gyration RG for the polymer to be comparable or larger than the mean distance between grafting sites. It follows that longer PEG chains are more effective in passivating a surface against protein binding, provided that they are grafted at sufficient densities.39 By increasing the PEG block length (y) in the PLLx-b-PEGy diblock copolymer, we generated an optimized surface functionalization which resisted non-specific protein adsorption in 160 nM streptavidin (Fig. 4). PLL10-b-PEG113 constructs were more effective than PLL10-b-PEG22 in preventing streptavidin binding, however co-functionalization with PLL1000–2000 was required to facilitate the adsorption and imaging of DNA; functionalization with the block copolymer alone yielded a densely packed surface that did not appear to bind DNA (data not shown). Finally, for even longer PEG chains (PLL10-b-PEG454), DNA adsorption appeared to be prevented altogether, even in the additional presence of PLL1000–2000 chains (Fig. S4†). This comes with the caveat that we cannot fully exclude that DNA absorption onto the underlying PLL layer is obscured by the PEG layer: the hydrodynamic radius of PEG454 is ∼13.7 nm and therefore the film thickness is expected to be much greater than the height of the DNA.
In addition to varying the PEG block length, we studied the effect of changing the PLL chain length x in the diblock copolymer PLLx-b-PEG113 (Fig. S4†). In contrast to PLL10-b-PEG113, PLL100-b-PEG113 facilitated DNA adsorption without additional long chain PLL, however this surface was less selective, binding increased streptavidin. This implies that the longer lysine block (in PLLx-b-PEG113) increases the spacing between the passivating PEG moieties. In this case the effective grafting distance between these moieties becomes larger than their extension (radius of gyration), such that they adopted collapsed coil conformations and no longer formed an effective steric barrier.22 We also note that with the increased length PLL in the block copolymer, the DNA plasmids appear more condensed than on PLL10-b-PEGy, forming toroid and rod-like structures, as seen in Fig S4(a) and (b).†40
Full quantification of streptavidin binding is complicated when considering images with complex arrangements of DNA and streptavidin on the surface. However, PLL10-b-PEG113/PLL1000–2000 functionalization emerges as the most effective in suppressing streptavidin binding whilst allowing visualization of DNA by AFM, both by qualitative comparison of the images and by tentative quantification (Fig. 4c). To determine if this functionalization is also effective at studying DNA–protein interactions, we created a 672 bp length of dsDNA with a single biotin at each end by using PCR amplification with biotinylated primers. Biotin binds to streptavidin with an extremely high affinity with Kd on the order of femtomolar. These binding partners were chosen for the strong binding affinity of their interaction and relatively low dissociation rate (less than 10% of molecules dissociated after 12 hours at 37 °C).33 Two streptavidin variants were considered: tetravalent streptavidin and monovalent streptavidin. Although both exhibit a similar binding affinity, monovalent streptavidin has only one functional biotin binding subunit compared to four in wild-type streptavidin. This prevents end-tailing of biotin labelled DNA. The binding of both proteins to the dsDNA construct was confirmed by electrophoretic band shift assay (Fig. S5†). DNA incubated with a 50× excess of monovalent streptavidin was adsorbed on the PLL10-b-PEG113/PLL1000–2000 functionalized mica surface (Fig. 5(a)). DNA molecules with streptavidin bound to both biotinylated ends were specifically adsorbed to the surface (Fig. 5(b)). The excess monovalent streptavidin in solution was not observed at high concentration on the surface, implying good non-specific protein passivation. 40% of the adsorbed streptavidin molecules were found at the ends of DNA (n = 531). The advantages of PLL10-b-PEG113/PLL1000–2000 functionalization were further demonstrated by comparison with the traditional PLL1000–2000 only functionalization which yielded increased adsorption of non-DNA-bound streptavidin on the surface (Fig. S6†).
To determine next whether this method can be used to study the binding of proteins to DNA in situ, tetravalent streptavidin was flowed over biotinylated DNA that had already been immobilized on PLL10-b-PEG113/PLL1000–2000 functionalized mica (Fig. 5(c)). Binding is observed as the formation of cyan protrusions at the ends of the immobilized biotinylated DNA substrates (magenta) which increase from 150 nM to 750 nM. A higher concentration of streptavidin is required for immobilized biotinylated DNA as compared to biotinylated DNA in solution. This suggests limited accessibility of the biotin binding site which is attached to the end of a large DNA molecule and hidden underneath the PEG layer. In this instance tetravalent streptavidin was used as opposed to monovalent streptavidin to increase the surface area for binding and thus reduce steric hindrance effects.41 High-resolution AFM imaging requires the surface immobilization of DNA, which can result in the masking of binding sites, and consequently we found it best, in this case, to pre-incubate the DNA with the streptavidin prior to depositing the DNA on the surface.
Finally, we consider the nuclear enzyme poly(ADP-ribose) polymerase-1 (PARP1) as an example of a DNA-binding protein in a biologically relevant context. Present in the nucleus at a concentration on the order of 10 μM,42,43 PARP1 plays an important role in DNA break repair and as such has also been targeted by anticancer drugs.44 Previous AFM studies on PARP-DNA binding, carried out on dried samples, have shown that the sample preparation for observing DNA-bound PARP is non-trivial, and have visualized PARP bound to DNA breaks/ends as well as to undamaged DNA.45–47 Here we use PARP1 to demonstrate the wider applicability of our method, imaging DNA before and after the addition of the enzyme in solution (Fig. 6). Importantly, we find that the added PARP predominantly binds to the solid support (Fig. 6(a and b)) when this mica support is functionalized using common protocols for AFM imaging in solution, such as the addition of Ni2+ ions48 and PLL1000–2000.20 Specifically, we observe a corrugated background of surface-bound proteins over the whole image (Fig. 6(a and b), bottom), precluding the identification of specific protein–DNA binding events. By contrast, in line with our results on streptavidin, PLL10-b-PEG113/PLL1000–2000 adequately passivates the mica substrate against protein binding while still allowing DNA adhesion, and thus facilitates the single-molecule detection of DNA-bound PARP1, here shown as white, globular structures decorating the DNA molecules (Fig. 6(c), bottom).
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c9nr07104k |
This journal is © The Royal Society of Chemistry 2019 |