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Int. J. Mol. Sci., Volume 2, Issue 2 (June 2001) – 8 articles , Pages 40-132

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196 KiB  
Article
Maximum Topological Distances Based Indices as Molecular Descriptors for QSPR. 4. Modeling the Enthalpy of Formation of Hydrocarbons from Elements
by Andrés Mercader, Eduardo A. Castro and Andrey A. Toropov
Int. J. Mol. Sci. 2001, 2(2), 121-132; https://doi.org/10.3390/i2020121 - 28 Jun 2001
Cited by 36 | Viewed by 8602
Abstract
The enthalpy of formation of a set of 60 hydroarbons is calculated on the basis of topological descriptors defined from the distance and detour matrices within the realm of the QSAR/QSPR theory. Linear and non-linear polynomials fittings are made and results show the [...] Read more.
The enthalpy of formation of a set of 60 hydroarbons is calculated on the basis of topological descriptors defined from the distance and detour matrices within the realm of the QSAR/QSPR theory. Linear and non-linear polynomials fittings are made and results show the need to resort to higher-order regression equations in order to get better concordances between theoretical results and experimental available data. Besides, topological indices computed from maximum order distances seems to yield rather satisfactory predictions of heats of formation for hydrocarbons. Full article
415 KiB  
Article
Glycerol-Induced Aggregation of the Oligomeric L-Asparaginase II from E. coli Monitored with ATR-FTIR
by Koba Adeishvili
Int. J. Mol. Sci. 2001, 2(2), 109-120; https://doi.org/10.3390/i2020109 - 28 Jun 2001
Cited by 9 | Viewed by 9162
Abstract
In this paper attenuated total reflectance Fourier transform infrared spectroscopy has been employed for the study of the structural composition of aggregates of the oligomeric L-asparaginase II from E.coli formed in the presence of glycerol after the induction of refolding of the protein. [...] Read more.
In this paper attenuated total reflectance Fourier transform infrared spectroscopy has been employed for the study of the structural composition of aggregates of the oligomeric L-asparaginase II from E.coli formed in the presence of glycerol after the induction of refolding of the protein. Apart from the perfect coincidence of the secondary structure composition of EcA2 as determined by FTIR and crystallography [1], it has also been shown that secondary structure of protein in asparaginase deposits is similar to that of the native conformation: 20.7% extended, 22.3% disordered, 31.4% helix and 25.6% turn/bend/β sheet. Certain structural similarities in the range of experimental error was observed for all three protein deposits presented in this paper, indicating a common structural basis for the composition of this types of aggregates. It is concluded that in the constitution of such precipitates, a partially folded (molten globule like) state(s) is involved, and its stabilisation is a key factor leading to the aggregation. The results presented in this paper might serve to be a good explanation and an excellent basis for the fundamental theory of protein (oligomers) precipitation by osmotic substances. Full article
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Figure 1

Figure 1
<p>Comparison of the amide I and II regions of the ATR-FTIR spectrum of L-asparaginase II from <span class="html-italic">E.coli</span> in its native state ( wide connected) , refolded and aggregated from 1M GuHCl (dashed), from 2M GuHCl ( connected) and from 3M GuHCl (dotted). FSD resolution enhancement of raw amide I spectra has not been performed.</p>
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<p>The second derivative specra of the amide I region of the ATR-FTIR spectrum of L-asparaginase II from <span class="html-italic">E.coli</span> in its native state (wide connected) , refolded and aggregated from 1M GuHCl (dashed) ,from 2M GuHCl (connected) and from 3M GuHCl (dotted). FSD resolution enhancement of raw amide I spectra has been performed. The best coincidence between all aggregated forms is evident.</p>
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<p>Presentation of curve-fit spectra of amide I region of the ATR-FTIR spectrum after FSD resolution enhancement. A: Native state, b: Refolded and aggregated from 1M GuHCl, c and d:from 2M GuHCl and from 3M GuHCl, respectively. Clear similarities in aggregated forms can aslo be seen. Notice that the peak positions are slightly shifted and a number of fitted peaks have also changed.</p>
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<p>The spectra of the amide III region from the ATR-FTIR spectrum of L-asparaginase II in the native state (wide connected) , refolded and aggregated from 1M GuHCl (dashed) ,from 2M GuHCl (connected) and from 3M GuHCl (dotted). All three deposits of protein exhibit a nearly identical shape, suggesting a similar structural composition.</p>
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<p>The second derivative of amide III region of FTIR spectra of L-asparaginase II in ist native state (wide connected) , refolded and aggregated from 1M GuHCl (dashed) ,from 2M GuHCl (connected) and from 3M GuHCl (dotted). A substantial difference from the native spectra of all protein aggregates can easily be noticed.</p>
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<p>Kinetics of L-asparaginase refolding monitored with circular dichroism at 225 nm and 22°C in Tris/HCl buffer pH=8.0. The protein concentration was 2 mg/ml. The enzyme was unfolded in 3M GuHCl solution and refolding was inititated by diluting into refolding buffer. The upper bar indicates kinetic traces measured on stopped-flow device. The lower bar theoretical double-exponential curve fit the stopped flow data. The kinetic parameters are as follow: A<sub>1</sub>= -0.67 deg cm<sup>2</sup> dmol<sup>-1</sup> , A<sub>2</sub>= -2.09 deg cm<sup>2</sup> dmol<sup>-1</sup>, A<sub>infinity</sub>= -1.89 deg cm<sup>2</sup> dmol<sup>-1</sup>, k<sub>1</sub>=0.15, k<sub>2</sub>=0.0041.</p>
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38 KiB  
Article
Variational Perturbation Theory of the Confined Hydrogen Atom
by H. E. Montgomery, Jr.
Int. J. Mol. Sci. 2001, 2(2), 103-108; https://doi.org/10.3390/i2020103 - 16 Jun 2001
Cited by 11 | Viewed by 5516
Abstract
Variational perturbation theory was used to solve the Schrödinger equation for a hydrogen atom confined at the center of an impenetrable cavity. Ground state and excited state energies and expectation values calculated from the perturbation wavefunction are comparable in accuracy to results from [...] Read more.
Variational perturbation theory was used to solve the Schrödinger equation for a hydrogen atom confined at the center of an impenetrable cavity. Ground state and excited state energies and expectation values calculated from the perturbation wavefunction are comparable in accuracy to results from direct numerical solution. Full article
174 KiB  
Article
Extended Coupled Cluster Approach for Molecular Properties: Study of H2O and HF Complexes
by Nayana Vaval, Aparna Basu Kumar and Sourav Pal
Int. J. Mol. Sci. 2001, 2(2), 89-102; https://doi.org/10.3390/i2020089 - 16 Jun 2001
Cited by 17 | Viewed by 7357
Abstract
In this paper, we study stationary variant of extended coupled-cluster response approach for properties. This has been studied at the singles and doubles approximation using cubic-truncated functional. This approximation has been studied earlier around equilibrium for small molecules. In this paper, efficacy of [...] Read more.
In this paper, we study stationary variant of extended coupled-cluster response approach for properties. This has been studied at the singles and doubles approximation using cubic-truncated functional. This approximation has been studied earlier around equilibrium for small molecules. In this paper, efficacy of this approximation has been shown using perturbative arguments. Further we have calculated dipole moments and polarizabilities of weakly interacting dimers of HF, H2O and H2O - HF complex. Results of HF and H2O monomers have been presented at the same level for comparison. The results have been compared with experimental results, wherever available and other theoretical results. Full article
160 KiB  
Article
Characterizing Cavities in Model Inclusion Fullerenes: A Comparative Study
by Francisco Torrens
Int. J. Mol. Sci. 2001, 2(2), 72-88; https://doi.org/10.3390/i2020072 - 2 Jun 2001
Cited by 6 | Viewed by 8575
Abstract
The fullerene-82 cavity is selected as a model system in order to test several methods for characterizing inclusion molecules. The methods are based on different technical foundations such as a square and triangular tessellation of the molecular surface, spherical tessellation of the molecular [...] Read more.
The fullerene-82 cavity is selected as a model system in order to test several methods for characterizing inclusion molecules. The methods are based on different technical foundations such as a square and triangular tessellation of the molecular surface, spherical tessellation of the molecular surface, numerical integration of the atomic volumes and surfaces, triangular tessellation of the molecular surface, and cubic lattice approach to the molecular volume. Accurate measures of the molecular volume and surface area have been performed with the pseudorandom Monte Carlo (MCVS) and uniform Monte Carlo (UMCVS) methods. These calculations serve as a reference for the rest of the methods. The SURMO2 method does not recognize the cavity and may not be convenient for intercalation compounds. The programs that detect the cavities never exceed 1% deviation relative to the reference value for molecular volume and 5% for surface area. The GEPOL algorithm, alone or combined with TOPO, shows results in good agreement with those of the UMCVS reference. The uniform random number generator provides the fastest convergence for UMCVS and a correct estimate of the standard deviations. The effect of the internal cavity on the solvent-accessible surfaces has been calculated. Fullerene-82 is compared with fullerene-60 and -70. Full article
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<p>Molecular image of fullerene-82.</p>
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<p><b>2a.</b> Molecular volumes and surfaces of fullerene-82: Molecular volume <span class="html-italic">V<sub>m</sub></span>, cavity volume <span class="html-italic">V<sub>c</sub></span>, and total volume <span class="html-italic">V<sub>t</sub></span>, <b>2b.</b> Molecular volumes and surfaces of fullerene-82: External surface <span class="html-italic">S<sub>e</sub></span>, cavity surface <span class="html-italic">S<sub>c</sub></span>, and molecular surface <span class="html-italic">S<sub>m</sub></span>.</p>
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32 KiB  
Article
A Quantum Theory of Thermodynamic Relaxation
by Roumen Tsekov
Int. J. Mol. Sci. 2001, 2(2), 66-71; https://doi.org/10.3390/i2020066 - 23 May 2001
Cited by 6 | Viewed by 8776
Abstract
A new approach to quantum Markov processes is developed and the corresponding Fokker-Planck-like equation is derived. The latter was examined to reproduce known results from classical and quantum physics. It was also applied to the phase-space description of a mechanical system thus leading [...] Read more.
A new approach to quantum Markov processes is developed and the corresponding Fokker-Planck-like equation is derived. The latter was examined to reproduce known results from classical and quantum physics. It was also applied to the phase-space description of a mechanical system thus leading to a new treatment of this problem different from the Wigner presentation. The equilibrium probability density obtained in the mixed coordinate-momentum space is a reasonable extension of the Gibbs canonical distribution. Full article
56 KiB  
Article
Improved Molecular Descriptors Based on the Optimization of Correlation Weights of Local Graph Invariants
by Germán Krenkel, Eduardo A. Castro and Andrey A. Toropov
Int. J. Mol. Sci. 2001, 2(2), 57-65; https://doi.org/10.3390/i2020057 - 7 May 2001
Cited by 27 | Viewed by 11011
Abstract
We report the calculation of boiling points for several alkyl alcohols through the use of improved molecular descriptors based on the optimization of correlation weights of local invariants of graphs. As local invariants we have used the presence of different chemical elements (i.e. [...] Read more.
We report the calculation of boiling points for several alkyl alcohols through the use of improved molecular descriptors based on the optimization of correlation weights of local invariants of graphs. As local invariants we have used the presence of different chemical elements (i.e. C, H, and O) and the existence of different vertex degree values (i.e. 1, 2, 3 and 4). The inherent flexibility of the chosen molecular descriptor seems to be rather suitable to obtain satisfactory enough predictions of the property under study. Comparison with other similar approximation reveals a very good behavior of the present method. The use of higher order polynomials do not seem to be necessary to improve results regarding the simple linear fitting equations. Some possible future extensions are pointed out in order to achieve a more definitive conclusion about this approximation. Full article
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<p>Experimental versus theoretical boiling points of alkyl alcohols.</p>
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396 KiB  
Article
Structural And Energetic Changes of Si (100) Surface With Fluorine in Presence of Water – A Density Functional Study
by Abhijit Chatterjee, Takashi Iwasaki and Takeo Ebina
Int. J. Mol. Sci. 2001, 2(2), 40-56; https://doi.org/10.3390/i2020040 - 1 May 2001
Cited by 4 | Viewed by 11698
Abstract
We report density functional electronic structure calculations to monitor the change in the surface characteristics of the Si (100)-2x1 surface after fluorination followed by interaction with water. Embedded finite silicon clusters are used to model an extended Si (100)-2x1 surface. Two high symmetry [...] Read more.
We report density functional electronic structure calculations to monitor the change in the surface characteristics of the Si (100)-2x1 surface after fluorination followed by interaction with water. Embedded finite silicon clusters are used to model an extended Si (100)-2x1 surface. Two high symmetry pathways and subsequent adsorption sites were examined: (i) adsorption of an fluorine atom directing onto a silicon dangling bond to form a monocoordinated fluorine atom (ii) adsorption of a fluorine atom directing on top of silicon dimer to form a bridging dicoordinated fluorine atom. However, in the later case we find that no barrier exists for the bridging fluorine atom to slide towards silicon dimer dangling bond to form more stable mono coordinated Si-F bond. We calculated activation barriers and equilibrium surface configuration as a function of fluorine coverage upto 2.0 ML. We compared the stability of the fluorinated surface. The results were compared with existing experimental and theoretical results. The reaction of water with HF treated Si surface is monitored. It produces, as a first step, the exchange of Si-F with water to form Si-OH groups reducing the concentration of the fluorine on the surface, followed by a rapture of Si-Si bonds and finally the Si-O-Si bridge formation in the lattice. Full article
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Figure 1
<p>Schematic pictures of silicon clusters used in this calculation with formula: (a) Si<sub>9</sub>H<sub>16</sub> cluster representing unreconstructed surface (b) Si<sub>9</sub>H<sub>14</sub> cluster representing reconstructed Si (100)-2x1 surface.</p>
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<p>The pathways of fluorine adsorption: (a) Directly onto a Si dangling bond (b) on top of a Si dimer.</p>
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<p>The optimized structure of (a) Si<sub>9</sub>H<sub>15</sub>F, (b) Si<sub>9</sub>H<sub>13</sub>F (c) Si<sub>9</sub>H<sub>12</sub>F and (d) Si<sub>9</sub>H<sub>12</sub>F<sub>2</sub> following the pathways of <a href="#ijms-02-00040-f002" class="html-fig">figure 2</a>.</p>
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<p>Potential curve for F atom approaching a Si dimer along the dangling bond direction as a function of Si-F distance.</p>
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<p>Potential curve for F atom diffusion from the twofold bridge-bonded position (R|| = 0 Å) to the onefold dangling-bond site of a silicon dimer (R|| = 1.6 Å), as a function of the parallel distance (R||) between the F atom and the original twofold bridge-bonded position. The vertical distance between the F atom and the surface was kept fixed. At R⊥ = 1.6 Å.</p>
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<p>Comparison of relative stabilization energy for different clusters representing both recon-structed and unreconstructed Si (100) surface for different fluorine coverage. The nomenclatures are the following with two groups 1-4 clusters are for unreconstructed surface and 5-6 is for reconstructed surface. The cluster formulas and detail ordering are mentioned in the text.</p>
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<p>MESP for water interaction with all hydrogen on Si (100) surface dimer. The +ve (+0.05 to 0.00 au.) and –ve (-0.05 to 0.00 au.) potential contours are shown as green and red shades respectively. The color code is as follows: Si (yellow), H (black), and O (red).</p>
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<p>MESP for water interaction with alternate hydrogen and fluorine on Si (100) surface dimer. The +ve (+0.05 to 0.00 au.) and –ve (-0.05 to 0.00 au.) potential contours are shown as green and red shades respectively. The color code is as follows: Si (yellow), H (black), F (Blue) and O (red).</p>
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<p>MESP for water interaction with all fluorine on Si (100) surface dimer. The +ve (+0.05 to 0.00 au.) and –ve (-0.05 to 0.00 au.) potential contours are shown as green and red shades respectively. The color code is as follows: Si (yellow), H (black), F (Blue) and O (red).</p>
Full article ">Figure 10
<p>The reaction mechanism to show the interaction of water with Si (100) surface. The color code is as follows: Si (yellow), H (black), F (Blue) and O (red).</p>
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