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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 116 (1994), S. 2075-2084 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 116 (2002), S. 3109-3118 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Confinement of phantom networks of Gaussian chains between parallel surfaces is simulated through the application of a harmonic potential 〈fraction SHAPE="CASE"〉12Hx2 to each chain bead at a distance x from the mean plane. We consider infinite, square (cubic) networks with a topological dimensionality of two (three), in addition to three-dimensional networks with a finite number of layers along one dimension. The partition function stays Gaussian and its integration reduces to the search of the eigenvalues of cyclic, or quasicyclic matrices. As applied to an isolated chain the confinement energy is 75% the exact value obtained by Casassa's exact approach, and the accuracy is expected to improve in the network case. At strong compressions, the confinement energy per chain EH is about the same for all the networks, but smaller than for a single chain with the same contour length. Taking EH in kBT units, M=EH−1 gives the number of chains in the correlation domain. Therefore, the external potential breaks up the network into smaller and smaller correlated domains, whose statistics remain unperturbed ("blobs"). The unperturbed mean-square radius of gyration reproduces previous results on the two- and the three-dimensional networks. The enormous collapse in the three-dimensional case is evidenced once again. © 2002 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 113 (2000), S. 7554-7563 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Exploiting an electrostatic analogy, we show that the elastic forces between a set of rigid particles embedded in a phantom polymer network can be represented by a simple bead-and-spring model. The beads represent the particles and the springs the rubber matrix. The model is validated by Monte Carlo simulation of rubbers filled with hard spherical particles, at volume fractions between 0.1 and 0.3. We derive both the moduli and the full stress–strain curves, under uniaxial elongation. The model reproduces and extends previous theoretical results on the so-called hydrodynamic reinforcement effect. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 7804-7813 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The equilibrium properties and the Rouse–Zimm dynamics of polymer molecules with any architecture at temperatures T≤aitch-theta, are treated using a bead-and-spring coarse-grained description. The collapsed globule model is adopted, whereby essentially all atoms are at the same mean-square distance 〈S2〉 from the center of mass; accordingly, at a given temperature the interatomic free energy is a single-valued function of 〈S2〉 and the self-consistent free-energy minimization is greatly simplified, in the Gaussian approximation. We prove that the connectivity matrix B and the bond-vector product matrix M=[〈li⋅lj〉] possess the same eigenvectors; these are the normal modes of the chain conformation. Furthermore, we show that 〈S2〉=N−1at∑kl2α2k/λk, where Nat is the total number of atoms, λk is the general nonzero eigenvalue of B, and l2α2k is the corresponding eigenvalue of M—the expansion ratio of the normal mode. Finally, we prove that in the free-draining limit the normal mode relaxation times are proportional to l2α2k/λk. Defining αS=(square root of)〈S2〉/〈S2〉ph as the overall strain ratio with respect to the phantom state, the plots of αS vs the reduced temperature τ=(T−aitch-theta)/T≤0 indicate that polymers with more compact architectures display a prompter contraction for small ||τ||'s, although tending to larger αS's at strong undercoolings, where the average density (∝Nat⋅〈S2〉−3/2) is about the same for all architectures. Concerning the dynamical behavior, at sufficiently large ||τ||'s the longest relaxation times reach a typical plateau, as already found for the linear chain.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 107 (1997), S. 6479-6490 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We apply our previously proposed "Gaussian cluster" model [J. Chem. Phys. 104, 1626 (1996)] to the study of macromolecular association and aggregation, under poor-solvent conditions (T〈aitch-theta). The properties of the macromolecular clusters are studied as a function of the number of chains ν=2,3,4,..., of the attractive two-body excluded-volume parameter z and of the repulsive three-body parameter K1. In the temperature window between its upper stability temperature and the coil-globule transition temperature for the single chains, a cluster of 2÷10 chains can have a smaller radius of gyration than an isolated polymer chain, provided K1 is sufficiently small. We suggest that this parameter may be estimated by considering the relative separations between the aitch-theta, the critical and the collapse temperatures. We compute the equilibrium distribution of the chains in a dilute solution among all possible cluster sizes (including ν=1, the isolated chains); population of the clusters ν≥2 increases with K1, but is generally rather small. Below the coil–globule transition temperature, anywhere on the dilute side of the two-phase region of the phase diagram, there is no free-energy barrier to polymer aggregation and precipitation: a single collapsed chain is a "critical nucleus" and the spinodal practically coincides with the binodal. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 1626-1645 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We present a molecular theory of the phenomena of single-chain collapse and phase separation into a polymer-rich and a polymer-poor phase, which occur in polymer solutions below the aitch-theta temperature. The theory extends the Fourier self-consistent approach of Allegra and Ganazzoli from the study of single-chain properties to that of an ensemble of interacting chains. We derive an expression for the free energy of a "Gaussian cluster'' made up of ν chains of length N (ν=1,2,3,...; N(very-much-greater-than)1). In the limit ν→∞ this yields a mean-field expression for the solution free energy per chain as a function of the reduced temperature τ=(T−aitch-theta)/T, the polymer volume fraction cursive-phi and the mean-square radius of gyration of the chains. From this we calculate the chain dimensions in solution and several thermodynamic properties, such as the osmotic pressure and the polymer–solvent phase diagram. We find that the contraction ratio of the chain radius of gyration is a single-valued function of (τB+K1Fcursive-phi)(square root of)N, where B and K1 specify the strength of the two- and three-body interactions and F is a polymer-dependent positive constant. We provide numerical evidence for a possible universality of the binodal line for different polymer-solvent systems; the spinodals do not share this characteristic of universality. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 109 (1998), S. 3285-3292 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Within the Gaussian phantom-chain model of a polymer network, we demonstrate and apply the formal analogy between the problem of computing the force constants acting on a set of rigid filler particles and that of computing the capacity of a system of conductors in a dielectric medium. We find that a single spherical particle undergoes a mean-square displacement 〈(ΔX)2〉 from its equilibrium position which is inversely proportional to its radius R. It is thus subject to an isotropic harmonic potential with force constant [3kBT/〈(ΔX)2〉]∝R. Quantitative evaluation of the proportionality constant for typical unswollen networks shows that 〈(ΔX)2〉/R decreases from 10−1 to 10−5 as R increases from 10 nm to 1 μm. The time scale of these fluctuations is independent of R and falls in the range 10−4–101 s. The fluctuations of two neighboring particles are not additive. A distance-dependent "stiffening" of the network is demonstrated through the calculation of the appropriate response and force constant matrices. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 105 (1996), S. 8352-8361 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: This paper is devoted to the theoretical analysis of nonideality effects in stretched rubber samples. The joint effect of packing forces and topological constraints is accounted for by adopting harmonic potentials between all pairs of network atoms, in addition to fixing a suitable set of junctions at the macroscopic sample surface according to the James–Guth theory. The potential minima are set at the average, affinely deformed interatomic distances. The force constant of each interaction is proportional to the probability of interatomic contact in the undeformed state and is inversely proportional to the square strain ratio along any space direction, thus accounting for the variation of the entanglement concentration with sample stretching. The proportionality factor of the pair potential is an adjustable parameter of the theory. A periodic coarse-grained model is used and the sample free energy is evaluated through normal-mode self-consistent analysis. Both the Mooney effect and the observed radius of gyration of the chain strands projected along different directions are properly accounted for. The results are similar to those of the Ronca–Allegra theory, which is based on direct application of constraints to the junction fluctuations. However, the present approach also embodies features of the theories which adopt the tube model. Finally, the variation of the Mooney constant C2 with sample swelling is accounted for in a semiquantitative way. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    New York, NY : Wiley-Blackwell
    International Journal of Quantum Chemistry 57 (1996), S. 501-518 
    ISSN: 0020-7608
    Keywords: Computational Chemistry and Molecular Modeling ; Atomic, Molecular and Optical Physics
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: A recently proposed pair population scheme is investigated for ab initio SCF and spin-coupled wave functions. All the required expressions are rederived, in very compact form, and efficient computational schemes are presented for their evaluation. As representative examples of different types of bonding, pair populations and related quantities are examined for H2, LiH, BeH, CH4, H2O, and B2H6. Various “effective valencies” are also considered. © 1996 John Wiley & Sons, Inc.
    Additional Material: 5 Ill.
    Type of Medium: Electronic Resource
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