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Biomedical subjects

H G Hansma

Publications and source records attributed to H G Hansma.

At least 37 records · Page 2Linked to original sources

Escherichia coli RNA polymerase activity observed using atomic force microscopy.

Fluid tapping-mode atomic force microscopy (AFM) was used to observe Escherichia coli RNA polymerase (RNAP) transcribing two different linear double-stranded (ds) DNA templates. The transcription process was detected by observing the translocation of the DNA template by RNAP on addition of ribonucleoside 5'-triphosphates (NTPs) in sequential AFM images. Stalled ternary complexes of RNAP, dsDNA and nascent RNA were adsorbed onto a mica surface and imaged under continuously flowing buffer. On introduction of all four NTPs, we observed some DNA molecules being pulled through the RNAP, some dissociating from the RNAP and others which did not move relative to the RNAP. The transcription rates were observed to be approximately 0.5-2 bases/s at our NTP concentrations, approximately 5 microM. The RNA transcripts were not unambiguously imaged in fluid. However, in experiments using a small single-stranded (ss) circular DNA template, known as a rolling circle, transcripts up to 1 or 2 microns long could be observed with tapping mode AFM once the samples were dried and imaged in air. This confirmed our observations of the transcriptional activity of RNAP adsorbed onto mica. This work illustrates that the development of tapping-mode in fluid has made it possible to use AFM to follow biological processes at the molecular level and get new insights about the variability of activity of individual molecules bound to a surface.

Aluminum Silicates↗

Properties of biomolecules measured from atomic force microscope images: a review.

AFM images can be used to obtain quantitative or qualitative information about the properties of biomaterials. Examples presented here are: (1) Persistence length measurements of moving and stationary DNA molecules. (2) Force mapping to measure properties such as the elasticity of cells and vesicles. (3) Phase mode imaging to detect variations in materials and properties of the sample surface. (4) Imaging of surfaces at different constant forces.

Animals↗

Changes in the elastic properties of cholinergic synaptic vesicles as measured by atomic force microscopy.

Cholinergic synaptic vesicles from Torpedo californica have been probed with the atomic force microscope in aqueous buffers to map and measure their elastic properties. Elastic properties were mapped with a new atomic force microscope technique known as force mapping. Force mapping of vesicles showed that the centers of the vesicles are harder or stiffer than the peripheral areas in the three buffers that were investigated. These were an isoosmotic buffer, a hypoosmotic buffer, and an isoosmotic buffer with 5 mM CaCl2 added. The hardness of the vesicular centers was quantified by calculation of the elastic modulus. Elastic moduli were in the range of 2-13 x 10(5) Pa. Vesicular centers were hardest in calcium-containing buffer and softest in isoosmotic buffer. Hypotheses are presented for the composition and function of the hard centers.

Acetylcholine↗

Atomic force microscopy of long and short double-stranded, single-stranded and triple-stranded nucleic acids.

Atomic force microscopy (AFM, also called scanning force microscopy) is proving to be a useful technique for imaging DNA. Thus it is important to push the limits of AFM imaging in order to explore both what types of DNA can be reliably imaged and identified and also what substrates and methods of sample preparation are suitable. The following advances in AFM of DNA are presented here. (i) DNA molecules as short as 25 bases can be seen by AFM. The short single-stranded DNAs imaged here (25 and 50 bases long) appeared globular in the AFM, perhaps because they are all capable of intramolecular base pairing and because the DNAs were in a Mg(ll) buffer, which facilitates intramolecular cross-bridging. (ii) AFM images in air of short double-stranded DNA molecules, 100-200 bp, gave lengths consistent with A-DNA. (iii) AFM images of poly (A) show both short bent lumpy molecules with an apparent persistence length of 40 nm and long straight molecules with an apparent persistence length of 600 nm. For comparison, the apparent persistence length for double-stranded DNA from phX-174 under the same conditions was 80 nm. (iv) Structures believed to be triple- stranded DNA were seen in samples of poly(dA.poly(dT) and poly (dG).poly(dC). These structures were twice as high as double-stranded DNA and the same width. (v) Entire molecules of lambda DNA, approx. 16 micron long, were imaged clearly in overlapping scans. (vi) Plasmid DNA was imaged on oxidized silicon, although less clearly than on mica.

Base Sequence↗

DNA binding to mica correlates with cationic radius: assay by atomic force microscopy.

In buffers containing selected transition metal salts, DNA binds to mica tightly enough to be directly imaged in the buffer in the atomic force microscope (AFM, also known as scanning force microscope). The binding of DNA to mica, as measured by AFM-imaging, is correlated with the radius of the transition metal cation. The transition metal cations that effectively bind DNA to mica are Ni(II), Co(II), and Zn(II), which have ionic radii from 0.69 to 0.74 A. In Mn(II), ionic radius 0.82 A, DNA binds weakly to mica. In Cd(II) and Hg(II), respective ionic radii of 0.97 and 1.1 A, DNA does not bind to mica well enough to be imaged with the AFM. These results may to relate to how large a cation can fit into the cavities above the recessed hydroxyl groups in the mica lattice, although hypotheses based on hydrated ionic radii cannot be ruled out. The dependence of DNA binding on the concentrations of the cations Ni(II), Co(II), or Zn(II) shows maximal DNA binding at approximately 1-mM cation. Mg(II) does not bind DNA tightly enough to mica for AFM imaging. Mg(II) is a Group 2 cation with an ionic radius similar to that of Ni(II). Ni(II), Co(II), and Zn(II) have anomalously high enthalpies of hydration that may relate to their ability to bind DNA to mica. This AFM assay for DNA binding to mica has potential applications for assaying the binding of other polymers to mica and other flat surfaces.

Adsorption↗

Applications for atomic force microscopy of DNA.

Tapping mode atomic force microscopy (AFM) of DNA in propanol, dry helium, and aqueous buffer each have specific applications. Resolution is best in propanol, which precipitates and immobilizes the DNA and provides a fluid imaging environment where adhesive forces are minimized. Resolution on exceptional images of DNA appears to be approximately 2 nm, sufficient to see helix turns in detail, but the smallest substructures typically seen on DNA in propanol are approximately 6-10 nm in size. Tapping AFM in dry helium provides a convenient way of imaging such things as conformations of DNA molecules and positions of proteins on DNA. Images of single-stranded DNA and RecA-DNA complexes are presented. In aqueous buffer DNA molecules as small as 300 bp have been imaged even when in motion. Images are presented of the changes in shape and position of circular plasmid DNA molecules.

Bacteriophage lambda↗

Following the assembly of RNA polymerase-DNA complexes in aqueous solutions with the scanning force microscope.

The capability of the scanning force microscope (SFM) to image molecules in aqueous buffers has opened the exciting possibility of following processes of molecular assembly in real time and in near-physiological environments. This capability is demonstrated in this paper by following the assembly process of RNA polymerase-DNA complexes. DNA fragments deposited on mica and imaged in Hepes/MgCl2 are shown before and after Escherichia coli RNA polymerase holoenzyme is injected in the SFM liquid chamber. The protein can recognize and bind to these DNA fragments within several seconds after injection, suggesting that the protein and the DNA retain their native configuration after deposition and during SFM imaging. A time-lapse sequence depicting the process of assembly of RNA polymerase-DNA complexes is shown. These results represent the first step for acquiring the capabilities to monitor complex biomolecular processes as they take place in ionic solutions and to characterize their spatial organization.

Bacterial Proteins↗

Direct observation of enzyme activity with the atomic force microscope.

The height fluctuations on top of the protein lysozyme adsorbed on mica were measured locally with an atomic force microscope operated in tapping mode in liquid. Height fluctuations of an apparent size of 1 nanometer that lasted for about 50 milliseconds were observed over lysozyme molecules when a substrate (oligoglycoside) was present. In the presence of the inhibitor chitobiose, these height fluctuations decreased to the level without the oligoglycoside. The most straightforward interpretation of these results is that the height fluctuations correspond to the conformational changes of lysozyme during hydrolysis. It is also possible, however, that the height fluctuations are, at least in part, the result of a different height or elasticity of the transient complex of lysozyme plus the substrate.

Adsorption↗

Bending and straightening of DNA induced by the same ligand: characterization with the atomic force microscope.

A new ligand, MGT-6b, binds to DNA with two linked parts: a polyamine that binds to the phosphate backbone and a tripyrrole peptide that binds to the minor groove. This ligand decreases the curvature of bent kinetoplast DNA (kDNA) and also increases the curvature of a 400-bp DNA that is used as a molecular weight standard (M400), as characterized with the atomic force microscope (AFM). MGT-6b is more effective than distamycin at straightening kDNA. MGT-6b retards the electrophoretic mobility of M400 DNA, although neither of its two component parts alters the mobility of M400 or its curvature as seen in the AFM. Thus, both parts of the ligand are needed for the "vise grip" mode of binding that affects DNA bending. the ability of MGT-6b to both bend and straighten DNA is probably related to the very different DNA sequences and, hence, structures of kDNA and M400 DNA.

Bacteriophage phi X 174↗

Motion and enzymatic degradation of DNA in the atomic force microscope.

The dynamics and enzymatic degradation of single DNA molecules can now be observed with the atomic force microscope. A combination of two advances has made this possible. Tapping in fluid has reduced lateral forces, which permits the imaging of loosely adsorbed molecules; and the presence of nickel ions appears to form a relatively stable bridge between the negatively charged mica and the negatively charged DNA phosphate backbone. Continuous imaging shows DNA motion and the process of DNA degradation by the nuclease DNase I. It is possible to see DNase degradation of both loosely adsorbed and tightly adsorbed DNA molecules. This method gives images in aqueous buffer of bare, uncoated DNA molecules with lengths of only a few hundred base pairs, or approximately 100 nm in length.

Adsorption↗

Structures of large T antigen at the origin of SV40 DNA replication by atomic force microscopy.

For inorganic crystals such as calcite (CaCO3), Atomic Force Microscopy (AFM) has provided surface structure at atomic resolution (Ohnesorge and Binnig, 1993). As part of a broad effort to obtain high resolution for an individual protein or protein assembly (Binnig et al., 1986; Rugar and Hansma, 1990; Radmacher et al., 1992), we applied AFM to study the ATP-dependent double hexamer of SV40 large T antigen, which assembles around the viral origin of DNA replication. Multimeric mass has been determined in two-dimensional projected images by Scanning Transmission Electron Microscopy (STEM) (Mastrangelo et al., 1989). By AFM, if the DNA-protein preparation has been stained positively by uranyl acetate, the contour at the junction between hexamers is visible as a cleft, 2-4 nm deep. The cleft, whether determined as a fraction of height by AFM or as a fraction of mass thickness by STEM, is of comparable magnitude. On either side of the cleft, hexamers attain a maximum height of 13-16 nm. Monomers found in the absence of ATP show heights of 5-7 nm. Taken together, the z coordinates provide a surface profile of complete and partial replication assemblies consistent with the spatial distribution of recognition pentanucleotides on the DNA, and they contribute direct geometrical evidence for a ring-like hexamer structure.

Antigens, Viral, Tumor↗

Mapping interaction forces with the atomic force microscope.

Force curves were recorded as the sample was raster-scanned under the tip. This opens new opportunities for imaging with the atomic force microscope: several characteristics of the samples can be measured simultaneously, for example, topography, adhesion forces, elasticity, van der Waals, and electrostatic interactions. The new opportunities are illustrated by images of several characteristics of thin metal films, aggregates of lysozyme, and single molecules of DNA.

Adsorption↗

Atomic force microscopy of biochemically tagged DNA.

Small fragments of DNA of known length were made with the polymerase chain reaction. These fragments had biotin molecules covalently attached at their ends. They were subsequently labeled with a chimeric protein fusion between streptavidin and two immunoglobulin G-binding domains of staphylococcal protein A. This tetrameric species was expected to bind up to four DNA molecules via their attached biotin moieties. The DNA-protein complex was deposited on mica and imaged with an atomic force microscope. The images revealed the protein chimera at the expected location at the ends of the strands of DNA as well as the expected dimers, trimers, and tetramers of DNA bound to a single protein.

Bacterial Proteins↗

Atomic force microscopy of DNA in aqueous solutions.

DNA on mica can be imaged in the atomic force microscope (AFM) in water or in some buffers if the sample has first been dehydrated thoroughly with propanol or by baking in vacuum and if the sample is imaged with a tip that has been deposited in the scanning electron microscope (SEM). Without adequate dehydration or with an unmodified tip, the DNA is scraped off the substrate by AFM-imaging in aqueous solutions. The measured heights and widths of DNA are larger in aqueous solutions than in propanol. The measured lengths of DNA molecules are the same in propanol and in aqueous solutions and correspond to the base spacing for B-DNA, the hydrated form of DNA; when the DNA is again imaged in propanol after buffer, however, it shortens to the length expected for dehydrated A-DNA. Other results include the imaging of E. coli RNA polymerase bound to DNA in a propanol-water mixture and the observation that washing samples in the AFM is an effective way of disaggregating salt-DNA complexes. The ability to image DNA in aqueous solutions has potential applications for observing processes involving DNA in the AFM.

1-Propanol↗

Atomic force microscopy of single- and double-stranded DNA.

A method has been developed for imaging single-stranded DNA with the atomic force microscope (AFM). phi X174 single-stranded DNA in formaldehyde on mica can be imaged in the AFM under propanol or butanol or in air. Measured lengths of most molecules are on the order of 1 mu, although occasionally more extended molecules with lengths of 1.7 to 1.9 mu are seen. Single-stranded DNA in the AFM generally appears lumpier than double-stranded DNA, even when extended. Images of double-stranded lambda DNA in the AFM show more sharp kinks and bends than are typically observed in the electron microscope. Dense, aggregated fields of double-stranded plasmids can be converted by gentle rinsing with hot water to well spread fields.

Bacteriophage lambda↗