Origin of overstretching transitions in single-stranded nucleic acids.

We combined single-molecule force spectroscopy with nuclear magnetic resonance measurements and molecular mechanics simulations to examine overstretching transitions in single-stranded nucleic acids. In single-stranded DNA and single-stranded RNA there is a low-force transition that involves unwinding of the helical structure, along with base unstacking. We determined that the high-force transition that occurs in polydeoxyadenylic acid single-stranded DNA is caused by the cooperative forced flipping of the dihedral angle formed between four atoms, O5'-C5'-C4'-C3' (γ torsion), in the nucleic acid backbone within the canonical B-type helix. The γ torsion also flips under force in A-type helices, where the helix is shorter and wider as compared to the B-type helix, but this transition is less cooperative than in the B type and does not generate a high-force plateau in the force spectrums of A-type helices. We find that a similar high-force transition can be induced in polyadenylic acid single-stranded RNA by urea, presumably due to disrupting the intramolecular hydrogen bonding in the backbone. We hypothesize that a pronounced high-force transition observed for B-type helices of double stranded DNA also involves a cooperative flip of the γ torsion. These observations suggest new fundamental relationships between the canonical structures of single-and double-stranded DNA and the mechanism of their molecular elasticity.

Nanomechanics of streptavidin hubs for molecular materials.

A new strategy is reported for creating protein-based nanomaterials by genetically fusing large polypeptides to monomeric streptavidin and exploiting the propensity of streptavidin monomers(SM) to self-assemble into stable tetramers. We have characterized the mechanical properties of streptavidin-linked structures and measured, for the first time, the mechanical strength of streptavidin tetramers themselves. Using streptavidin tetramers as molecular hubs offers a unique opportunity to create a variety of well-defined, self-assembled protein-based (nano)materials with unusual mechanical properties.

Separating DNA with different topologies by atomic force microscopy in comparison with gel electrophoresis.

Atomic force microscopy, which is normally used for DNA imaging to gain qualitative results, can also be used for quantitative DNA research, at a single-molecular level. Here, we evaluate the performance of AFM imaging specifically for quantifying supercoiled and relaxed plasmid DNA fractions within a mixture, and compare the results with the bulk material analysis method, gel electrophoresis. The advantages and shortcomings of both methods are discussed in detail. Gel electrophoresis is a quick and well-established quantification method. However, it requires a large amount of DNA, and needs to be carefully calibrated for even slightly different experimental conditions for accurate quantification. AFM imaging is accurate, in that single DNA molecules in different conformations can be seen and counted. When used carefully with necessary correction, both methods provide consistent results. Thus, AFM imaging can be used for DNA quantification, as an alternative to gel electrophoresis.

Fast and forceful refolding of stretched alpha-helical solenoid proteins.

Anfinsen's thermodynamic hypothesis implies that proteins can encode for stretching through reversible loss of structure. However, large in vitro extensions of proteins that occur through a progressive unfolding of their domains typically dissipate a significant amount of energy, and therefore are not thermodynamically reversible. Some coiled-coil proteins have been found to stretch nearly reversibly, although their extension is typically limited to 2.5 times their folded length. Here, we report investigations on the mechanical properties of individual molecules of ankyrin-R, beta-catenin, and clathrin, which are representative examples of over 800 predicted human proteins composed of tightly packed alpha-helical repeats (termed ANK, ARM, or HEAT repeats, respectively) that form spiral-shaped protein domains. Using atomic force spectroscopy, we find that these polypeptides possess unprecedented stretch ratios on the order of 10-15, exceeding that of other proteins studied so far, and their extension and relaxation occurs with minimal energy dissipation. Their sequence-encoded elasticity is governed by stepwise unfolding of small repeats, which upon relaxation of the stretching force rapidly and forcefully refold, minimizing the hysteresis between the stretching and relaxing parts of the cycle. Thus, we identify a new class of proteins that behave as highly reversible nanosprings that have the potential to function as mechanosensors in cells and as building blocks in springy nanostructures. Our physical view of the protein component of cells as being comprised of predominantly inextensible structural elements under tension may need revision to incorporate springs.

Detecting solvent-driven transitions of poly(A) to double-stranded conformations by atomic force microscopy.

We report the results of direct measurements by atomic force microscopy of solvent-driven structural transitions within polyadenylic acid (poly(A)). Both atomic force microscopy imaging and pulling measurements reveal complex strand arrangements within poly(A) induced by acidic pH conditions, with a clear fraction of double-stranded molecules that increases as pH decreases. Among these complex structures, force spectroscopy identified molecules that, upon stretching, displayed two distinct plateau features in the force-extension curves. These plateaus exhibit transition forces similar to those previously observed in native double-stranded DNA (dsDNA). However, the width of the first plateau in the force-extension curves of poly(A) varies significantly, and on average is shorter than the canonical 70% of initial length corresponding to the B-S transition of dsDNA. Also, similar to findings in dsDNA, stretching and relaxing elasticity profiles of dspoly(A) at forces below the mechanical melting transition overlap but reveal hysteresis when the molecules are stretched above the mechanical melting transition. These results strongly suggest that under acidic pH conditions, poly(A) can form duplexes that are mechanically stable. We hypothesize that under acidic conditions, similar structures may be formed by the cellular poly(A) tails on mRNA.

UVA generates pyrimidine dimers in DNA directly.

There is increasing evidence that UVA radiation, which makes up approximately 95% of the solar UV light reaching the Earth's surface and is also commonly used for cosmetic purposes, is genotoxic. However, in contrast to UVC and UVB, the mechanisms by which UVA produces various DNA lesions are still unclear. In addition, the relative amounts of various types of UVA lesions and their mutagenic significance are also a subject of debate. Here, we exploit atomic force microscopy (AFM) imaging of individual DNA molecules, alone and in complexes with a suite of DNA repair enzymes and antibodies, to directly quantify UVA damage and reexamine its basic mechanisms at a single-molecule level. By combining the activity of endonuclease IV and T4 endonuclease V on highly purified and UVA-irradiated pUC18 plasmids, we show by direct AFM imaging that UVA produces a significant amount of abasic sites and cyclobutane pyrimidine dimers (CPDs). However, we find that only approximately 60% of the T4 endonuclease V-sensitive sites, which are commonly counted as CPDs, are true CPDs; the other 40% are abasic sites. Most importantly, our results obtained by AFM imaging of highly purified native and synthetic DNA using T4 endonuclease V, photolyase, and anti-CPD antibodies strongly suggest that CPDs are produced by UVA directly. Thus, our observations contradict the predominant view that as-yet-unidentified photosensitizers are required to transfer the energy of UVA to DNA to produce CPDs. Our results may help to resolve the long-standing controversy about the origin of UVA-produced CPDs in DNA.

Construction of a single-axis molecular puller for measuring polysaccharide and protein mechanics by atomic force microscopy.

INTRODUCTIONPolysaccharides and proteins are frequently subjected to mechanical forces in vivo. Because these forces affect a wide range of biological activities, it is important to develop methods that directly investigate the mechanical properties of these molecules. Recent progress in techniques that allow the mechanical manipulation of biopolymers at a single-molecule level has revealed the complex nature of the elasticity of proteins and polysaccharides. The atomic force microscope (AFM) is an excellent force spectrometer for probing the mechanical properties (e.g., length and tension) of individual polysaccharides and proteins. The following protocol describes the basic design and construction of an AFM (a single-axis molecular puller) that has four parts: a head, a base, electronics, and software. Those with a background in mechanical engineering, basic knowledge of electronics and data acquisition techniques, and some computer programming skills (e.g., with LabView, Matlab, or Igor) should be able to construct this instrument. It is advisable to inspect commercial AFMs before constructing one from scratch.

Measuring polysaccharide mechanics by atomic force microscopy.

INTRODUCTIONPolysaccharides are frequently subjected to mechanical forces in vivo. Because these forces affect a wide range of biological activities, it is important to develop methods that directly investigate the mechanical properties of these molecules. Recent progress in techniques that allow the mechanical manipulation of biopolymers at a single-molecule level has revealed the complex nature of the elasticity of polysaccharides. The atomic force microscope (AFM) is an excellent force spectrometer for probing the mechanical properties (e.g., length and tension) of individual polysaccharides. The following protocol describes the use of AFM for stretch-release measurements of polysaccharide chains.

Measuring protein mechanics by atomic force microscopy.

INTRODUCTIONProteins are frequently subjected to mechanical forces in vivo. Because these forces affect a wide range of biological activities, it is important to develop methods that directly investigate the mechanical properties of these molecules. Force spectroscopy of individual proteins (modular or single-domain) allows one to characterize their entropic elasticity under low stretching forces and to determine their persistence length by fitting the worm-like chain (WLC) model to the force-extension curve. At higher stretching forces, it is possible to mechanically unravel these proteins, study their mechanical strength, and examine their unfolding and refolding properties. This provides data on their rates of mechanical unfolding and refolding, as well as on the position of the transition state along the unfolding reaction coordinate, which is defined as the extension of the protein module along the direction of the applied force. Thus, single-protein force spectroscopy may generate a plethora of interesting data that cannot be obtained using traditional biophysical methods. The atomic force microscope (AFM) is an excellent force spectrometer for probing the mechanical properties (e.g., length and tension) of individual proteins. The following protocol describes the use of AFM for measurements of protein mechanics under the constant extension rate regime.