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Some theoretical considerations regarding the effects of steric hindrance and intrinsic global coupling on the flexibility of Fc-anchored immunoglobulins.

Nanosecond fluorescence depolarization studies reported in the accompanying companion paper showed that the long rotational correlation time, phi L, increased somewhat when rabbit IgG anti-dansyl antibodies were anchored in staphylococcal protein A (SpA) soluble complexes. The increases in phi L upon anchoring IgG probably resulted from "global coupling" effects caused by: increased steric hindrance of the antibody segments in the SpA complexes and intrinsic structural constraints already present in the monomeric IgG. Global coupling results from a restriction in the angular range of a flexible segment and is manifest when flexible motions alone cannot depolarize all of the fluorescence, so that the slower global tumbling of the entire particle is also required. Such effects cannot be resolved directly from experimental anisotropy data, however, because only a single long correlation time, phi L, is well defined over the limited time range of most fluorophores. In this paper, estimates of the anisotropy contributions from flexible and global motions of the IgG-SpA complexes are determined by contrasting theoretical and measured decays. For this analysis it was assumed that each of the experimental phi L-values is a weighted composite of the rotational correlation time associated with the less restricted flexible motions of the Fab arms, phi F, and the correlation time associated with global tumbling of the entire particle, phi G. A general two-exponential expression was used to relate phi F and phi G to phi L. This approach was meaningful because phi G-values of the various SpA complexes had been calculated from hydrodynamic measurements. The theoretical decays clearly show that, even if phi G is much longer than phi F, these two rotational motions still cannot be resolved over the experimentally accessible time range. Families of emission anisotropy decay curves for IgG antibodies with different amounts of intrinsic global coupling and for anchored antibodies with different amounts of steric hindrance were simulated by varying the preexponential weighting factors of the flexible and global terms. By comparing the calculated curves with the measured decays, it is evident that the rabbit IgG anti-dansyl antibodies do not have much intrinsic global coupling, but rather they are highly flexible. The curves also indicate that even for the exceptionally compact IgG4-SpA2 17-S complex, which showed the most steric hindrance in electron micrographs, the appropriate phi G weighting factor is only 0.28. Thus, as supposed earlier, the anchored antibodies exhibit considerable segmental flexibility. In closing, the above concepts are used to examine the results of

Antigen-Antibody Complex↗

Colloidal aggregation induced by long range attractions.

The structure of colloidal clusters formed by long-range attractive interactions under diluted conditions is studied by means of Monte Carlo simulations. For a not-too-long attraction range, clusters show self-similar internal structure with lower density than that typical for diffusive aggregation. For long-range interactions, low kappa, nonfractal clusters are formed (dense at short scales but open at long ones). The dependence on the volume fraction shows that more-compact clusters are grown the higher the colloidal density for diffusive aggregation and attraction-driven aggregation in the fractal regime. The whole trend is explained in terms of the interpenetration among aggregates. In attraction-driven aggregations, the interpenetration of clusters competes with aggregation in the tips of the clusters, causing low-density clusters.

Journal Article↗

Comparison of the dynamics of substrate access channels in three cytochrome P450s reveals different opening mechanisms and a novel functional role for a buried arginine.

Understanding the mechanism and specificity of substrate binding in the cytochrome P450 (P450) superfamily is an important step toward explaining its key role in drug metabolism, toxicity, xenobiotic degradation, and several biosynthetic pathways. Here we investigate the ligand exit pathways and mechanisms of P450cam (CYP101), P450BM-3 (CYP102), and P450eryF (CYP107A1) by using random expulsion molecular dynamics and classical molecular dynamics simulations. Although several different pathways are found for each protein, one pathway is common to all three. The mechanism of ligand exit along this pathway is, however, quite different in the three different proteins. For P450cam, small backbone conformational changes, in combination with aromatic side chain rotation, allow for the passage of the rather rigid, compact, and hydrophobic substrate, camphor. In P450BM-3, larger transient backbone changes are observed on ligand exit. R47, situated at the entrance to the channel, appears important in guiding negatively charged fatty acid substrates in and out of the active site. In P450eryF, an isolated buried arginine, R185, stabilized by four hydrogen bonds to backbone carbonyl oxygen atoms, is located in the exit channel and is identified as having a particularly unusual functionality, dynamically gating channel opening. The results for these three P450s suggest that the channel opening mechanisms are adjusted to the physico-chemical properties of the substrate and can kinetically modulate protein-substrate specificity.

Arginine↗

Ultrasound phase-contrast transmission imaging of localized thermal variation and the identification of fat/tissue boundaries.

We present a new ultrasound technique for registering localized temperature changes in soft tissues. Conversely, small temperature changes may be induced in order to image tissue layers. The concept is motivated by the search for a compact, low cost method for guiding noninvasive thermal therapies; however its utility may extend to a wide range of imaging problems such as tumour imaging in the breast. This method combines ultrasound transmission imaging, planar projection techniques and phase-contrast theory. After outlining the theoretical foundation of the technique, its feasibility is tested by simulating localized heating within homogeneous tissue layers. Success of this imaging method is evaluated as a function of the ultrasound-imaging wavelength for a Gaussian-shaped heated region over the frequency range from 0.1 to 2 MHz. Furthermore we simulate two-dimensional image reconstruction from a receiving array. We conclude that thermal phase-contrast imaging in tissues is plausible for detecting the treatment spot in thermal therapies while operating at frequencies below 1 MHz. Additionally, it may also be possible to use the method for noninvasive thermometry. However, thermometry would require operation at higher frequencies at the tradeoff of increased attenuation and higher sensitivity to scattering, which needs to be further explored.

Body Temperature↗

Approaching the Ocean Color problem using fuzzy rules.

In this paper, we propose a fuzzy logic-based approach which exploits remotely sensed multispectral measurements of the reflected sunlight to estimate the concentration of optically active constituents of the sea water. The relation between the concentrations of interest and the subsurface reflectances is modeled by a set of fuzzy rules extracted automatically from the data through a two-step procedure. First, a compact initial rule base is generated by projecting onto the input variables the clusters produced by a fuzzy clustering algorithm. Then, a genetic algorithm is applied to optimize the rules. Appropriate constraints maintain the semantic properties of the initial model during the genetic evolution. Results of the application of the fuzzy model obtained from data simulated with an ocean color model over the channels of the Medium Resolution Imaging Spectrometer are shown and discussed.

Algorithms↗

Ammonia detection by using quantum-cascade laser photoacoustic spectroscopy.

A pulsed quantum-cascade distributed-feedback laser, temperature tunable from -41 degrees C to +31.6 degrees C, and a resonant differential photoacoustic detector are used to measure trace-gas concentrations to as low as 66 parts per 10(9) by volume (ppbv) ammonia at a low laser power of 2 mW. Good agreement between the experimental spectrum and the simulated HITRAN spectrum of NH3 is found in the spectral range between 1046 and 1052 cm(-1). A detection limit of 30 ppbv ammonia at a signal-to-noise ratio of 1 was obtained with the quantum-cascade laser (QCL) photoacoustic (PA) setup. Concentration changes of approximately 50 ppbv were detectable with this compact and versatile QCL-based PA detection system. The performance of the PA detector, characterized by the product of the incident laser power and the minimum detectable absorption coefficient, was 4.7 x 10-9 W cm(-1).

Journal Article↗

Parallel implementation of the biorthogonal multiresolution time-domain method.

The three-dimensional biorthogonal multiresolution time-domain (Bi-MRTD) method is presented for both free-space and half-space scattering problems. The perfectly matched layer (PML) is used as an absorbing boundary condition. It has been shown that improved numerical-dispersion properties can be obtained with the use of smooth, compactly supported wavelet functions as the basis, whereas we employ the Cohen-Daubechies-Fouveau (CDF) biorthogonal wavelets. When a CDF-wavelet expansion is used, the spatial-sampling rate can be reduced considerably compared with that of the conventional finite-difference time-domain (FDTD) method, implying that larger targets can be simulated without sacrificing accuracy. We implement the Bi-MRTD on a cluster of allocated-memory machines, using the message-passing interface (MPI), such that very large targets can be modeled. Numerical results are compared with analytical ones and with those obtained by use of the traditional FDTD method.

Journal Article↗

Recognition of cyclooxygenase-2 (COX-2) active site by NSAIDs: a computer modelling study.

The energetics and models of COX-2 complexed with nonsteroidal anti-inflammatory drugs (NSAIDs) having different degrees of selectivity for two isoforms of COX (COX-2 and COX-1) have been studied using computer modelling approach. The models are obtained for complexes of NS398 (NS), a selective COX-2 inhibitor; indoprofen (Ind), a non-selective inhibitor; di-tert-butylbenzofurans (DHDMBFs) with substituents at the 5th position: CONH(CH2)2OMe (BF1), CONH-c-Pr (BF2), 3-methylene-gamma-butyrolactonyl (BF3) and oxicams namely, meloxicam (Mel), piroxicam (Pir) and tenoxicam (Ten). These were optimized using molecular mechanics (MM) and molecular dynamics (MD) techniques. The binding energies and structures were compared with pharmacological parameters and available results with COX-1. In case of NS a larger difference in the binding energies between COX-2 and COX-1 was noticed as compared to that of Ind. It also had stronger interaction with His90 and Tyr355 which is considered important for COX-2 selectivity. There was a difference in the compactness at the channel entrance between COX-2 selective and non-selective ligands. Models with DHDMBFs and oxicams showed a similar correlation. The results were used to design a peptide inhibitor, Tyr-Arg-Cys-Ala-delta Phe-Cys (Pept) which could fit better in the COX-2 cavity. As per our MD simulation results this peptide inhibitor showed both higher activity and COX-2 selectivity.

Anti-Inflammatory Agents, Non-Steroidal↗

Towards understanding the interaction between oligosaccharides and water molecules.

Complex carbohydrates are implicated in many important biological processes, and have a strong interaction with water. This close interplay with molecular water through multiple hydroxyls may be an integral part of their emergent structure and dynamics, as selected during evolution. Using molecular dynamics simulations with explicit water the interactions at the linkages within a variety of oligosaccharides are investigated and contrasted, in order to establish correlations between linkage orientation, sugar epimerization, and water interaction. In particular, interactions at alpha linkages, and between mannose and glucose residues, that are common in oligosaccharides are considered. Sugars joined by alpha linkages at the 2-, 3-, and 6-position were found to interact via a combination of weak hydrogen-bonds and water-bridges, which is dependent on the epimerization state of the sugars. Due to their three-dimensional structure, they are also likely to interact with noncontiguous sugar residues in an oligosaccharide, which can lead to ordered structures through the exclusion of water. On the other hand, beta linkages (to 3- and 4-position) maintain strong hydrogen-bonds, have a limited ability to be involved in water-bridges, and predominantly interact with the directly attached sugars. Therefore, sequences of alpha-linked sugars form compact, branched structures that have conformational flexibility, and beta linkages form extended, relatively rigid structures, suitable for structural molecules, and at the termini of protein bound oligosaccharides. These results provide further tentative ties between chemical structure, water interactions, and the emergent form and function of specific sugars and linkages in oligosaccharides.

Carbohydrate Conformation↗

Conformational characterization of DnaK and its complexes by small-angle X-ray scattering.

DnaK, a member of the 70 kDa heat shock protein (hsp70) family, and its complexes with substrate proteins and nucleotides were characterized by small-angle X-ray scattering (SAXS) and size-exclusion chromatography (SEC) techniques. The SAXS data indicated that DnaK has a dumbbell-shaped structure with a maximum dimension (dmax) of 112 angstrom, which is consistent with the reported two major functional domains [Chappell et al. (1987) J. Biol. Chem. 268, 12730-12735; Flaherty et al. (1990) Nature 346, 623-628]. The data were best fit by a model in which the two domains either are connected by a short hinge region or are just in contact with each other. The radius of gyration (Rg) of DnaK was determined as 37.5 +/- 1.0 angstrom in the absence of nucleotide. Binding of ATP induces a conformational change in DnaK as reflected by the changes in its P(r) function and Kratky plot, the increases (1-2 angstrom) in both its radius of gyration (Rg) and its Stokes radius (Rs), and the increase in its dmax (5-10 angstrom ). SAXS and SEC-HPLC results indicate that the association state of DnaK is very sensitive to the buffer concentration and the presence of substrates, as well as the protein concentration. At high buffer and protein concentrations, DnaK dimerizes, resulting in an increase in its apparent Rg and dmax values. The addition of substrate (unfolded protein or ATP) results in a return to the Rg value of monomeric DnaK, due to the dissociation of DnaK multimers induced by the substrate binding and resultant conformational changes. The DnaK-substrate protein complex gives a smaller Rg than expected, suggesting that the substrate protein binds to a cavity or cleft on DnaK rather than the exterior of the chaperone. The Kratky plot of the Gdn.HCl-induced unfolding intermediate state of DnaK is consistent with a compact, molten globule-like conformation, as previously suggested based on CD, fluorescence, and SEC-HPLC results [Palleros et al. (I 993) Biochemistry 32, 4314-4321].

Bacterial Proteins↗

The molecular potential energy surface and vibrational energy levels of methyl fluoride. Part II.

New analytical bending and stretching, ground electronic state, potential energy surfaces for CH(3)F are reported. The surfaces are expressed in bond-length, bond-angle internal coordinates. The four-dimensional stretching surface is an accurate, least squares fit to over 2000 symmetrically unique ab initio points calculated at the CCSD(T) level. Similarly, the five-dimensional bending surface is a fit to over 1200 symmetrically unique ab initio points. This is an important first stage towards a full nine-dimensional potential energy surface for the prototype CH(3)F molecule. Using these surfaces, highly excited stretching and (separately) bending vibrational energy levels of CH(3)F are calculated variationally using a finite basis representation method. The method uses the exact vibrational kinetic energy operator derived for XY(3)Z systems by Manson and Law (preceding paper, Part I, Phys. Chem. Chem. Phys., 2006, 8, DOI: 10.1039/b603106d). We use the full C(3v) symmetry and the computer codes are designed to use an arbitrary potential energy function. Ultimately, these results will be used to design a compact basis for fully coupled stretch-bend calculations of the vibrational energy levels of the CH(3)F system.

Chemical Phenomena↗

Formulation and integration of learning differential equations on the stiefel manifold.

This letter aims at illustrating the relevance of numerical integration of learning differential equations on differential manifolds. In particular, the task of learning with orthonormality constraints is dealt with, which is naturally formulated as an optimization task with the compact Stiefel manifold as neural parameter space. Intrinsic properties of the derived learning algorithms, such as stability and constraints preservation, are illustrated through experiments on minor and independent component analysis (ICA).

Algorithms↗

Impact of propagation through an aberrating medium on the linear effective apodization of a nonlinearly generated second harmonic field.

Techniques based on the nonlinearly generated second harmonic signal (tissue harmonic imaging) have rapidly supplanted linear (fundamental) imaging methods as the standard in two-dimensional echocardiography. Enhancements to the compactness of the nonlinearly generated second harmonic (2f) field component with respect to the fundamental (1f) field component are widely considered to be among the factors contributing to the observed image quality improvements. The objective of this study was to measure the impact of phase and amplitude aberrations resulting from propagation through an inhomogeneous tissue, on the beamwidths associated with: the fundamental (1f); the nonlinearly generated second harmonic (2f); and the linearly propagated, effective apodization signal at the same (21) frequency. Modifications to the transmit characteristics of a phased-array imaging system were validated with hydrophone measurements. Results demonstrate that the characteristics of the diffraction pattern associated with the linear-propagation effective apodization transmit case were found to be in good agreement with the detailed spatial characteristics of the nonlinearly generated second harmonic field. The effects of the abdominal wall tissue aberrators are apparent for all three of the beam profiles studied. Consistent with the improved image quality associated with harmonic imaging, the aberrated nonlinearly generated second harmonic beam was shown to remain more compact than the corresponding aberrated fundamental beam patterns in the presence of the interposed aberrator.

Algorithms↗

Variations in coupled water, viscoelastic properties, and film thickness of a Mefp-1 protein film during adsorption and cross-linking: a quartz crystal microbalance with dissipation monitoring, ellipsometry, and surface plasmon resonance study.

We have measured the time-resolved adsorption kinetics of the mussel adhesive protein (Mefp-1) on a nonpolar, methyl-terminated (thiolated) gold surface, using three independent techniques: quartz crystal microbalance with dissipation monitoring (QCM-D), surface plasmon resonance, and ellipsometry. The QCM-D and ellipsometry data shows that, after adsorption to saturation of Mefp-1, cross-linking of the protein layer using NaIO4 transforms it from an extended (approximately 20 nm), water-rich, and hydrogel-like state to a much thinner (approximately 5 nm), compact, and less water-rich state. Furthermore, we show how quantitative data about the thickness, shear elastic modulus, and shear viscosity of the protein film can be obtained with the QCM-D technique, even beyond the Sauerbrey regime, if frequency (f) and energy dissipation (D) measurements measured at multiple harmonics are combined with theoretical simulations using a Voight-based viscoelastic model. The modeling result was confirmed by substituting H2O for D2O. As expected, the D2O substitution does not influence the actual adsorption behavior, but resulted in expected differences in the estimated effective density and shear viscosity. These results provide new insight and understanding about the adsorption kinetics and crosslinking behavior of Mefp-1. They also demonstrate how the above three techniques complement each other for biomolecule adsorption studies.

Adsorption↗

Conformational properties of adenylyl-3' leads to 5'-adenosine in aqueous solution.

A detailed 220-MHz NMR study has been made of the conformational properties for the homodinucleotide adenylyl-3' leads to 5'-adenosine, ApA, in D2O. Unambiguous signal assignments of all proton signals were made with the aid of selectively deuterated nucleotidyl units, ApA, ApA, and D-8ApA, and complete, accurate sets of NMR parameters were derived by simulation-iteration methods. Sets of limiting chemical shifts and coupling values were also obtained for ApA and constituent monomers 3'-AMP and 5'-AMP at infinite dilution and at identical ionization states for assessment of dimerization effects. Conformational properties were evaluated quantitatively for most of the conformational bonds of ApA and these are consistent with two compact folded dynamically averaged structures, a base-stacked right helical structure, I, characterized as anti, C3'-endo, g-, w,w' (320,330 degrees), g'g', gg, C3'-endo, anti, and a more loosely base-stacked loop structure, II, with anti, C3'-endo, g-, w,w' (80 degrees, 50 degrees), g'g', gg, C3'-endo, anti orientations. Dimerization produces a number of nucleotidyl conformational changes including a shift in ribose equilibrium C2'-endo (S) in equilibrium C3'-endo (N) in favor of C3'-endo in both Ap- and -pA (60:40 vs. 35:65 in monomers), a change in glycosidic torsion angle chiCN toward 0 degrees, and a greater locking-in of rotamers along bonds involved in the phosphodiester backbone. Moreover, there is clear evidence that the transitions from S leads to N forms and chiCN leads to 0 degrees are directly related to base stacking in ApA. Finally, ApA exists in solution as an equilibrium between I, II and an unstacked form(s) with as yet undetermined conformational features. Since C4'-C5', C5'-O5', and C3'-O3' bonds possess exceptional conformational stabilities, it is proposed that destacking occurs primarily by rotation about P-O5' and/or O3'-P. Predominant factors influencing the overall ApA conformation are thus base-base interaction and flexibility about P-O5' and O3'-P, with change of ribose conformation occurring in consequence of an alteration of chiCN, the latter in turn being governed by the need for maximum eta overlap of stacked adenine rings.

Adenine Nucleotides↗

The effect of conformation on membrane permeability of an acyloxyalkoxy-linked cyclic prodrug of a model hexapeptide.

PURPOSE: To determine the different conformations of the acyloxyalkoxy-linked cyclic prodrug 1 of the model hexapeptide 2 in solution and to investigate the relationship between these solution conformations and the cellular permeability characteristics of this prodrug. METHODS: Two-dimensional Homonuclear Hartmann-Hahn spectroscopy, Rotating-Frame Overhouser effect spectroscopy, circular dichroism and molecular dynamics simulations were used to find the solution conformers of cyclic prodrug 1. RESULTS: Our spectroscopic findings suggest that cyclic prodrug 1 exhibits a major and a minor conformer in solution. The major conformer appears to have a well-defined secondary structure, which involves a beta-turn and 4-->1 intramolecular hydrogen bond, creating a compact structure with a reduced average hydrodynamic radius compared to the model hexapeptide 2. CONCLUSIONS: The increased ability of cyclic prodrug 1 to permeate membranes compared to the model hexapeptide 2 could be due to reduction in the average hydrodynamic radius of the molecule facilitating paracellular flux and/or the reduction in the hydrogen bonding potential facilitating transcellular flux.

Cell Membrane Permeability↗

Limited internal friction in the rate-limiting step of a two-state protein folding reaction.

Small, single-domain proteins typically fold via a compact transition-state ensemble in a process well fitted by a simple, two-state model. To characterize the rate-limiting conformational changes that underlie two-state folding, we have investigated experimentally the effects of changing solvent viscosity on the refolding of the IgG binding domain of protein L. In conjunction with numerical simulations, our results indicate that the rate-limiting conformational changes of the folding of this domain are strongly coupled to solvent viscosity and lack any significant "internal friction" arising from intrachain collisions. When compared with the previously determined solvent viscosity dependencies of other, more restricted conformational changes, our results suggest that the rate-limiting folding transition involves conformational fluctuations that displace considerable amounts of solvent. Reconciling evidence that the folding transition state ensemble is comprised of highly collapsed species with these and similar, previously reported results should provide a significant constraint for theoretical models of the folding process.

Bacterial Proteins↗

Biomechanical evaluation of conventional internal contemporary spinal fixation techniques used for stabilization of complete sacroiliac joint separation: a 3-dimensional unilaterally isolated experimental stiffness study.

STUDY DESIGN: Comparative 3-dimensional biomechanical testing. OBJECTIVE: To compare 5 fixation techniques, 3 using screws or screw and plates and 2 spinal, used for stabilization of complete unilateral sacroiliac dislocation in composite models. SUMMARY OF BACKGROUND DATA: Harrington compression rods have been used for posterior iliosacral stabilization. Recently, the use of compact spinal instrumentation has been introduced for stabilization of iliosacral joint separation to achieve immediate and permanent stability, allowing early mobilization. To the authors' knowledge, no comparative mechanical studies between commonly used internal fixation techniques and contemporary spinal instrumentation have been performed. METHODS: Fifteen identical composite models of the left hemipelvis and sacrum were used to simulate consistently the "worst-case scenario" of complete unilateral sacroiliac dislocation. Subgroups of 3 models each were used to apply 5 (A-E) alternative fixation iliosacral joint fixation techniques: 1 multiaxial 7.5 mm Cotrel-Dubousset screw inserted in the posterior superior iliac spine and connected with a long Cotrel-Dubousset horizontal rod with 6.5 mm multiaxial Cotrel-Dubousset screws inserted bilaterally in the S1 pedicles (technique A); 1 multiaxial 7.5 mm Cotrel-Dubousset titanium pedicle screw inserted in the posterior superior iliac spine and connected with a short horizontal Cotrel-Dubousset-rod to a 6.5 mm multiaxial Cotrel-Dubousset-screw inserted to the ipsilateral S1 pedicle (technique B); 1, 6.5 mm cancellous AO-screw (technique C); 2, 6.5 mm cancellous AO screws (technique D); and 2 dynamic stainless steel compression plates (technique E) placed anteriorly. Constructs were biomechanically tested. The ilium was unilaterally rigidly fixed, the sacrum was put horizontal in the mediolateral direction with a forward tilt of 30 degrees (close to physiologic conditions) in the sagittal plane, and a vertical quasi-static compressive load ranging from 0 to 500 N was applied on the endplate of S1, reproducing a "worst case" loading scenario. Construct stiffness, frontal plus sagittal kinematics, and iliosacral joint gap size for all 5 techniques were measured. RESULTS: The construct stiffness (N/mm +/- standard deviation) ranged for model: A, 121 +/- 18; B, 78 +/- 10; C, 168 +/- 13; D, 193 +/- 42; and E, 145 +/- 4. All other parameters exhibited minor variations between the different techniques of fixation: at the 400 N load level, the maximum iliosacral gap globally ranged 0.9-2.8 mm, the maximum mediolateral sacral tilt ranged 1.3-2.4 degrees, and the maximum anteroposterior sacral tilt ranged 0.6-3.0 degrees. CONCLUSIONS: The iliosacral fixation with 2 6.5 mm AO-cancellous screws for complete sacroiliac dislocation demonstrated the highest stiffness and the short spinal instrumentation the poorest stiffness. All other fixation techniques could be generally considered of equivalent stability value.

Biomechanical Phenomena↗