Quantitative determination of size and shape of surface-bound DNA using an acoustic wave sensor

DNA bending plays a significant role in many biological processes, such as gene regulation, DNA replication, and chromosomal packing. Understanding how such processes take place and how they can, in turn, be regulated by artificial agents for individual oriented therapies is of importance to both biology and medicine. In this work, we describe the application of an acoustic wave device for characterizing the conformation of DNA molecules tethered to the device surface via a biotin-neutravidin interaction. The acoustic energy dissipation per unit mass observed upon DNA binding is directly related to DNA intrinsic viscosity, providing quantitative information on the size and shape of the tethered molecules. The validity of the above approach was verified by showing that the predesigned geometries of model double-stranded and triple-helix DNA molecules could be quantitatively distinguished: the resolution of the acoustic measurements is sufficient to allow discrimination between same size DNA carrying a bent at different positions along the chain. Furthermore, the significance of this analysis to the study of biologically relevant systems is shown during the evaluation of DNA conformational change upon protein (histone) binding.     

Visualizing ion relaxation in the transport of short DNA fragments

Ion relaxation plays an important role in a wide range of phenomena involving the transport of charged biomolecules. Ion relaxation is responsible for reducing sedimentation and diffusion constants, reducing electrophoretic mobilities, increasing intrinsic viscosities, and, for biomolecules that lack a permanent electric dipole moment, provides a mechanism for orienting them in an external electric field. Recently, a numerical boundary element method was developed to solve the coupled Navier-Stokes, Poisson, and ion transport equations for a polyion modeled as a rigid body of arbitrary size, shape, and charge distribution. This method has subsequently been used to compute the electrophoretic mobilities and intrinsic viscosities of a number of model proteins and DNA fragments. The primary purpose of the present work is to examine the effect of ion relaxation on the ion density and fluid velocity fields around short DNA fragments (20 and 40 bp). Contour density as well as vector field diagrams of the various scalar and vector fields are presented and discussed at monovalent salt concentrations of 0.03 and 0.11 M. In addition, the net charge current fluxes in the vicinity of the DNA fragments at low and high salt concentrations are briefly examined and discussed.     

Contribution of the intrinsic curvature to measured DNA persistence length

The persistence length of DNA, a, depends both on the intrinsic curvature of the double helix and on the thermal fluctuations of the angles between adjacent base-pairs. We have evaluated two contributions to the value of a by comparing measured values of a for DNA containing a generic sequence and for an "intrinsically straight" DNA. In each 10 bp segment of the intrinsically straight DNA an initial sequence of five bases is repeated in the sequence of the second five bases, so any bends in the first half of the segment are compensated by bends in the opposite direction in the second half. The value of a for the latter DNA depends, to a good approximation, on thermal fluctuations only; there is no intrinsic curvature. The values of a were obtained from measurements of the cyclization efficiency for short DNA fragments, about 200 bp in length. This method determines the persistence length of DNA with exceptional accuracy, due to the very strong dependence of the cyclization efficiency of short fragments on the value of a. We find that the values of a for the two types of DNA fragment are very close and conclude that the contribution of the intrinsic curvature to a is at least 20 times smaller than the contribution of thermal fluctuations. The relationship between this result and the angles between adjacent base-pairs, which specify the intrinsic curvature, is analyzed.     

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.     

Special factors in biological strings

Biological macromolecules such as DNA, RNA, and proteins can be regarded as finite sequences of symbols (or words) over a finite alphabet. In this paper, we refer to DNA (RNA) sequences which are words on a four-letter alphabet. A comparison is made between some "genes", or fragments of them, with random sequences or random reshuffled sequences on the same alphabet and having the same length. Some combinatorial techniques of analysis of finite words are developed. A crucial role in the comparison is played by the so-called special factors of a given word. In all the analysed DNA (RNA) fragments the distribution on the length of the number of right (left) special factors differs, in a very typical way, from the corresponding distribution in a string on the same alphabet and having the same length generated by a random source or obtained by making a random alteration (=shuffling) of the original string. This kind of change is irrespective of the length in the range that we have considered <2650 bp and of the phylogenetic origin of the fragment.     

Interaction of aminoacridines with deoxyribonucleic acid: viscosity of the complexes

The intrinsic, viscosities at zero shear rate of defined complexes of proflavine, 9-aminoacridine, and 9-amino-l,2,3,4-tetrahydroaeridine with calf thymus DNA have been determined at, various ionic strengths by means of rotating cylinder viscometers. By controlled adjustment, of the composition of the mixtures, the amount of bound acridine (r moles/g.-atom DNA phosphorus) was maintained constant at different dilutions. The intrinsic viscosities of the complexes increased with r up to r values (ca. 0.16–0.20) corresponding to the end of the process of strong binding of the acridinium cations. However, complex formation between the acridines and thermally denatured DNA caused either a marked decrease in viscosity (at the low ionic strengths of 0.0015 and 0.005) or no change at all (ionic strength 0.1). These results are discussed in the light of presently available hydrodynamic theories relating the intrinsic, viscosity of DNA to its molecular extension.     

Function and assembly of the bacteriophage T4 DNA replication complex: interactions of the T4 polymerase with various model DNA constructs

Complexes formed between DNA polymerase and genomic DNA at the replication fork are key elements of the replication machinery. We used sedimentation velocity, fluorescence anisotropy, and surface plasmon resonance to measure the binding interactions between bacteriophage T4 DNA polymerase (gp43) and various model DNA constructs. These results provide quantitative insight into how this replication polymerase performs template-directed 5' --> 3' DNA synthesis and how this function is coordinated with the activities of the other proteins of the replication complex. We find that short (single- and double-stranded) DNA molecules bind a single gp43 polymerase in a nonspecific (overlap) binding mode with moderate affinity (Kd approximately 150 nm) and a binding site size of approximately 10 nucleotides for single-stranded DNA and approximately 13 bp for double-stranded DNA. In contrast, gp43 binds in a site-specific (nonoverlap) mode and significantly more tightly (Kd approximately 5 nm) to DNA constructs carrying a primer-template junction, with the polymerase covering approximately 5 nucleotides downstream and approximately 6-7 bp upstream of the 3'-primer terminus. The rate of this specific binding interaction is close to diffusion-controlled. The affinity of gp43 for the primer-template junction is modulated specifically by dNTP substrates, with the next "correct" dNTP strengthening the interaction and an incorrect dNTP weakening the observed binding. These results are discussed in terms of the individual steps of the polymerase-catalyzed single nucleotide addition cycle and the replication complex assembly process. We suggest that changes in the kinetics and thermodynamics of these steps by auxiliary replication proteins constitute a basic mechanism for protein coupling within the replication complex.     

Optical model studies of the salt-induced 10-30-nm fiber transition in chromatin

Fractionated chicken erythrocyte chromatin fibers consisting of 10-mer and 75-mer polynucleosomes have been studied by flow birefringence and viscosity over a range of Na+ and Mg2+ ion concentrations sufficient to span the 10-30-nm fiber transition. Negative intrinsic flow bifringence was observed under all solvent conditions investigated. The intrinsic birefringence, obtained from the reduced birefringence to intrinsic viscosity ratio, was used to evaluate various optical models for the DNA conformation in the fiber. Results are consistent with an extended chromatosome-linker "necklace" model for the unfolded, low-salt fiber and with a solenoidal model of edge-stacked chromatosomes for the condensed fiber at high salts. These results are consistent with and independently corroborative of similar models based upon electric dichroism and neutron scattering reported by others.     

A comparison of five methods for obtaining the intrinsic viscosity of bovine serum albumin

Intrinsic viscosity [η] is a characteristic of proteins and other molecules related directly to their ability to disturb flow and indirectly to their size and shape. It is usually determined by extrapolating reduced viscosity to zero concentration. Four other methods for deriving [η] have been utilized by previous investigators. Studies of the intrinsic viscosity of bovine serum albumin had been carried out two years apart as a test of viscometry technique; the data obtained were used to compare the five methods. Four of the five produced [η] values ranging from 3.92 to 4.21 ml/g. Agreement was good between the two studies. The five methods were compared to each other using linearity of regression, statistical error of determination, effect of varying solvent time, and result obtained in different concentration ranges. By these four criteria, use of the regression of specific fluidity (1 ? 1/η_rel) with concentration was found superior to other methods. Its only deficiency was a requirement that solution density be corrected for at each concentration studied rather than applying a single correction for density after using kinematic viscosity data. All methods for deriving intrinsic viscosity are based on one of three equations; flow is expressed either in terms of reduced viscosity (Huggins), inherent viscosity (Kraemer), or specific fluidity. Of these three equations, specific fluidity is the most closely related both to theoretical analyses and to experimental studies of rigid spheres. There is abundant evidence in past reports that in contrast to rigid spheres, flexible polymers do not produce a linear rise in specific fluidity as their concentration increases, strongly suggesting that their molecular conformation is changing with concentration. A linear relation between fluidity and concentration has been observed for almost all proteins and protein mixtures studied. When this linear relation is present it indicates both that molecular conformation during flow is independent of concentration in the range studied and that the specific fluidity method for deriving intrinsic viscosity is the most appropriate.     

Effect of Bending Strain on the Torsion Elastic Constant of DNA

The torsion constants of both circular and linear forms of the same 181 bp DNA were investigated by time-resolved fluorescence polarization anisotropy (FPA) of intercalated ethidium. The ratio of intrinsic ethidium binding constants of the circular and linear species was determined from the relative fluorescence intensities of intercalated and non-intercalated dye in each case. Possible changes in secondary structure were also probed by circular dichroism (CD) spectroscopy. Upon circularization, the torsion constant increased by a factor of 1.42, the intrinsic binding constant for ethidium increased by about fourfold, and the CD spectrum underwent a significant change. These effects are attributed to an altered secondary structure induced by the bending strain. Quantitative agreement between torsion constants obtained from the present FPA studies and previous topoisomer distribution measurements on circular DNAs containing 205 to 217 bp removes a long-standing apparent discrepancy between those two methods. After storage at 4°C for eight months, the torsion constant of the circular DNA increased by about 1.25-fold, whereas that of the linear DNA remained unchanged. For these aged circles, both the torsion constant and intrinsic binding constant ratio lie close to the corresponding values obtained previously for a 247 bp DNA by analyzing topoisomer distributions created in the presence of various amounts of ethidium. The available evidence strongly implies that torsion constants measured for small circular DNAs with less than 250 bp are specific to the altered secondary structure(s) therein, and are not applicable to linear and much larger circular DNAs with lower mean bending strains.     

Nucleotide sequences and expression in Escherichia coli of the in-phase overlapping Pseudomonas aeruginosa plcR genes.

The translation products of chromosomal DNAs of Pseudomonas aeruginosa encoding phospholipase C (heat-labile hemolysin) have been examined in T7 promoter plasmid vectors and expressed in Escherichia coli cells. A plasmid carrying a 4.7-kilobase (kb) DNA fragment was found to encode the 80-kilodalton (kDa) phospholipase C as well as two more proteins with an apparent molecular mass of 26 and 19 kDa. Expression directed by this DNA fragment with various deletions suggested that the coding region for the two smaller proteins was contained in a 1-kb DNA region. Moreover, the size of both proteins was reduced by the same amount by an internal BglII-BglII DNA deletion, suggesting that they were translated from overlapping genes. Similar results were obtained with another independently cloned 6.1-kb Pseudomonas DNA, which in addition coded for a 31-kDa protein of opposite orientation. The nucleotide sequence of the 1-kb region above revealed an open reading frame with a signal sequence typical of secretory proteins and a potential in-phase internal translation initiation site. Pulse-chase and localization studies in E. coli showed that the 26-kDa protein was a precursor of a secreted periplasmic 23-kDa protein (PlcR1) while the 19-kDa protein (PlcR2) was mostly cytoplasmic. These results indicate the expression of Pseudomonas in-phase overlapping genes in E. coli.     

Viscosity study of DNA. II. The effect of simple salt concentration on the viscosity of high molecular weight DNA and application of viscometry to the study of DNA isolated from T4 and T5 bacteriophage mutants

Polyelectrolyte expansion effects on high molecular weight bacteriophage DNA have been studied by examining the influence of simple salt concentration upon the intrinsic viscosity, [η]. The viscosity–molecular weight exponent a in the expression [η] = KM^a diminishes from 0.8 in 0.005M simple salt to a limiting value of 0.6 for salt concentrations greater than 0.6M at 25°C. The ε parameter of the N^1+ε hydrodynamic representation thus varies from approximately 0.2–0.07 over this range of salt concentration. The intrinsic, viscosity of DNA decreases slightly with increasing temperature at low and moderate salt concentrations but becomes independent of temperature at high salt concentrations. The expansion of the DNA molecular domain is linear in the reciprocal square root of the simple salt concentration. Viscosity differences among DNA's isolated from several bacteriophage T5 mutants reflect small differences in molecular weight which are in agreement, with sine determination by other techniques. The DNA's isolated from various rII mutants of T4 bacteriophage including some very large deletion mutations were found to be identically the same size in accord with current genetic ideas. Details of the representation and extrapolation of viscosity data are discussed and the sensitivity of the technique is evaluated.     

Bacterial protein HU dictates the morphology of DNA condensates produced by crowding agents and polyamines

Controlling the size and shape of DNA condensates is important in vivo and for the improvement of nonviral gene delivery. Here, we demonstrate that the morphology of DNA condensates, formed under a variety of conditions, is shifted completely from toroids to rods if the bacterial protein HU is present during condensation. HU is a non-sequence-specific DNA binding protein that sharply bends DNA, but alone does not condense DNA into densely packed particles. Less than one HU dimer per 225 bp of DNA is sufficient to completely control condensate morphology when DNA is condensed by spermidine. We propose that rods are favored in the presence of HU because rods contain sharply bent DNA, whereas toroids contain only smoothly bent DNA. The results presented illustrate the utility of naturally derived proteins for controlling the shape of DNA condensates formed in vitro. HU is a highly conserved protein in bacteria that is implicated in the compaction and shaping of nucleoid structure. However, the exact role of HU in chromosome compaction is not well understood. Our demonstration that HU governs DNA condensation in vitro also suggests a mechanism by which HU could act as an architectural protein for bacterial chromosome compaction and organization in vivo.     

Analysis of alphoid DNA variation and kinetochore size in human chromosome 21: evidence against pathological significance of alphoid satellite DNA diminutions.

Centromeric alpha satellite DNA sequences are linked to the kinetochore CENP-B proteins and therefore may be involved in the centromeric function. The high heterogeneity of size of the alphoid blocks raises the question of whether small amount of alphoid DNA or "deletion" of this block may have a pathological significance in the human centromere. In the present study, we analysed the correlation between size variations of alphoid DNA and kinetochore sizes in human chromosome 21 by molecular cytogenetic and immunochemical techniques. FISH analyses of alpha satellite DNA sizes in chromosome 21 homologues correlated well with the variation of their physical size as determined by pulsed field gel electrophoresis (PFGE). By contrast, the immunostaining study of the same homologous chromosomes with antikinetochore antibodies suggested that there is no positive correlation between the alpha satellite DNA block and kinetochore sizes. FISH analysis of chromosome 21-specific alphoid DNA and immunostaining of kinetochore extended interphase chromatin fibers indicate that centromeric kinetochore-specific proteins bind to restricted areas of centromeric DNA arrays. Thus, probably, restricted regions of centromeric DNA play an important role in kinetochore formation, centromeric function and abnormal chromosome segregation leading to non-disjunction.     

Analysis of a Candida albicans gene that encodes a novel mechanism for resistance to benomyl and methotrexate

Summary The pathogenic yeast, Candida albicans, is insensitive to the anti-mitotic drug, benomyl, and to the dihydrofolate reductase inhibitor, methotrexate. Genes responsible for the intrinsic drug resistance were sought by transforming Saccharomyces cerevisiae, a yeast sensitive to both drugs, with genomic C. albicans libraries and screening on benomyl or methotrexate. Restriction analysis of plasmids isolated from benomyl- and methotrexate-resistant colonies indicated that both phenotypes were encoded by the same DNA fragment. Sequence analysis showed that the fragments were nearly identical and contained a long open reading frame of 1694 bp (ORF1) and a small ORF of 446 bp (ORF2) within ORF1 on the opposite strand. By site-directed mutagenesis, it was shown that ORF1 encoded both phenotypes. The protein had no sequence similarity to any known proteins, including -tubulin, dihydrofolate reductase, and the P-glycoprotein of the multi-drug resistance family. The resistance gene was detected in several C. albicans strains and in C. stellatoidea by DNA hybridization and by the polymerase chain reaction.     

Vibration of DNA polymer in viscous solvent

The problem of viscous damping of vibrating DNA polymer in solution is solved in the low-amplitude limit for all acoustic branches of the spectrum. The acoustic spectrum covers the microwave region of frequencies. Analytic solutions are obtained for a model describing the DNA polymer as a smooth circular cylinder. Numerical solutions are presented for a model describing the DNA polymer as a twisted cylinder of elliptical cross section. The amount of mass loading is determined for both models and the damped spectrum for the mass-loaded oscillator is calculated. The viscous damping is found to be a strong function of frequency, singular at very low frequencies for all modes except the torsional mode of the circular cylinder. All acoustic modes are overdamped, implying that the observation of well-defined resonances in DNA requires either highly structured water on the molecular level or very dry material.     

DNA rings with multiple energy minima

Within the context of DNA rings, we analyze the relationship between intrinsic shape and the existence of multiple stable equilibria, either nicked or cyclized with the same link. A simple test, based on a perturbation expansion of symmetry breaking within a continuum elastic rod model, provides good predictions of the occurrence of such multiple equilibria. The reliability of these predictions is verified by direct computation of nicked and cyclized equilibria for several thousand DNA minicircles with lengths of 200 and 900 bp. Furthermore, our computations of equilibria for nicked rings predict properties of the equilibrium distribution of link, as calculated by much more computationally intensive Monte Carlo simulations.     

Acoustic wave based MEMS devices for biosensing applications

This paper presents a review of acoustic-wave based MEMS devices that offer a promising technology platform for the development of sensitive, portable, real-time biosensors. MEMS fabrication of acoustic wave based biosensors enables device miniaturization, power consumption reduction and integration with electronic circuits. For biological applications, the biosensors are integrated in a microfluidic system and the sensing area is coated with a biospecific layer. When a bioanalyte interacts with the sensing layer, mass and viscosity variations of the biospecific layer can be detected by monitoring changes in the acoustic wave properties such as velocity, attenuation, resonant frequency and delay time. Few types of acoustic wave devices could be integrated in microfluidic systems without significant degradation of the quality factor. The acoustic wave based MEMS devices reported in the literature as biosensors and presented in this review are film bulk acoustic wave resonators (FBAR), surface acoustic waves (SAW) resonators and SAW delay lines. Different approaches to the realization of FBARs, SAW resonators and SAW delay lines for various biochemical applications are presented. Methods of integration of the acoustic wave MEMS devices in the microfluidic systems and functionalization strategies will be also discussed.     

Microscopic viscosity and rotational diffusion of proteins in a macromolecular environment

The Stokes-Einstein-Debye equation is currently used to obtain information on protein size or on local viscosity from the measurement of the rotational correlation time. However, the implicit assumptions of a continuous and homogeneous solvent do not hold either in vivo, because of the high density of macromolecules, or in vitro, where viscosity is adjusted by adding viscous cosolvents of various size. To quantify the consequence of nonhomogeneity, we have measured the rotational Brownian motion of three globular proteins with molecular mass from 66 to 4000 kD in presence of 1.5 to 2000 kD dextrans as viscous cosolvents. Our results indicate that the linear viscosity dependence of the Stokes-Einstein relation must be replaced by a power law to describe the rotational Brownian motion of proteins in a macromolecular environment. The exponent of the power law expresses the fact that the protein experiences only a fraction of the hydrodynamic interactions of macromolecular cosolvents. An explicit expression of the exponent in terms of protein size and cosolvent's mass is obtained, permitting definition of a microscopic viscosity. Experimental data suggest that a similar effective microviscosity should be introduced in Kramers' equation describing protein reaction rates.