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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 88 (1984), S. 6649-6654 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 88 (1984), S. 861-866 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , 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 97 (1992), S. 9267-9275 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We compare the predictions of various density functional approximation schemes as applied to the restricted-orientation, hard, rectangular-parallelepiped model of liquid crystals. These calculations illustrate some features of density functional calculations which may aid in understanding other approximate, mean-field theories of orientational ordering phase transitions and their interfaces. The isotropic–nematic coexistence curve of this model is apparently well described by the so-called third-order y expansion, and the analytical expression for the nonideal free energy derived from the simple y expansion thus provides a benchmark against which to compare the density functional approximation schemes. Using standard relations applicable to inhomogeneous fluids, we show how expansions about the bulk isotropic phase compare more favorably with the "exact'' y-expansion results when truncated at third order than do second-order truncations. Thus this model behaves somewhat differently than other hard-particle models of fluids, notably the hard-sphere one. We also examine the possibility of expanding the free energy about the ordered phase to obtain the properties of a disordered phase. An expansion about local values of the density leads to the widely used smoothed-density approximation and a hierarchy of systematic extensions. The latter appear more stable than conventional Taylor expansions about bulk disordered phases.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 8507-8520 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We derive several recent approximation schemes for the thermodynamics of inhomogeneous homopolymer solutions by functionally expanding the nonideal part of the free energy about the local density. The functional expansion contains all orders in the gradients of the monomer density even when truncated at low order. When applied to systems with slowly varying densities, it reduces to a widely used square-gradient theory of homopolymers and blends. We also recover the so-called Roe functional by considering infinitely long Gaussian chains. However, this result only applies to a small region near the center of the interface. We employ a one-parameter, exponential decay trial function and the variational theorem to obtain estimates of the surface tension between two coexisting homopolymer-solvent phases. This particular trial function facilitates a comparison of the numerically evaluated nonlocal free energy functional, the analytic summation of the full gradient expansion, the square-gradient approximation, and the Roe functional. Within the scope of a Gaussian-chain model and a Flory–Huggins local free energy, we compare the various approximations with regards to their predictions for the surface tension, the nonlocal free energy density, and the interfacial profiles. The full gradient expansion does not converge to a useful result near the center of the interface of moderately segregated phases or when the interface becomes narrow as for strongly segregated homopolymer solutions. The square-gradient theory overestimates the free energy density in the wings of the interface but underestimates this quantity near the interface's center. These two errors partially cancel, and the square-gradient theory provides an accurate estimate of the surface tension of moderately segregated homopolymer solutions. Unlike many other theories of interfaces which derive from considerations of two-body correlations in a homogeneous reference phase, the lowest nontrivial contribution of the functional expansion for Gaussian chains derives from three-body correlations. This feature is in qualitative accord with recent lattice theories of interfaces that treat chain biases in the interfacial region and thus implicitly contain three-body correlations.
    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 92 (1990), S. 1413-1426 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We employ density functional methods to derive the free energy and grand potential functionals appropriate to homopolymers and blends. The grand potential functionals are minimized by the single-monomer densities of the blends or homopolymers, and the nonideal portions of the free energies possess functional Taylor expansions whose coefficients are related to monomer–monomer direct correlation functions. In the limit that the polymerization indices become unity, the formalism reduces to that of atomic systems. By absorbing parts of the ideal free energy functionals into the nonideal contribution to the free energies, we demonstrate the formal equivalence of the theory of polymers to that of nonuniform atomic systems. The polymer formalism also reproduces the stability analyses of polymer phase transitions deduced by regarding dense polymeric liquids as atomic fluids. Nevertheless, for homogeneous polymeric fluids, the ideal free energy functionals become the well-known Flory–Huggins expressions for the entropy of mixing different homopolymers and the entropy of dissolving homopolymers in solvent. This suggests that numerical calculations, based on the correct ideal free energy functionals, will prove superior to calculations for polymers that derive from theories of atomic systems. We discuss extensions to block copolymers and mention numerous applications to polymer phase transitions and interfacial phenomena.
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 9130-9144 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We extend our previous density functional theory of homopolymers to block copolymers. The constraints on the relative number densities of the different types of monomers comprising the block copolymers alter the ideal free energy compared to that of homopolymers and of polymer blends. As in our previous work, the second-order functional derivatives of the nonideal free energy with respect to monomer densities are simply related to monomer–monomer direct correlation functions. When applied to incompressible diblock copolymers, this formalism reduces to quasi-one-component form and reproduces the Landau theory of near symmetric diblock copolymers. For homogeneous liquids, we recover the Flory–Huggins ideal free energy of mixing of block copolymers. The present theory, however, permits the treatment of compressible systems and therefore of more strongly first-order microphase separations. It also provides a rigorous formulation for developing improved density functional models for block copolymer systems.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 105 (1996), S. 4798-4811 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The segmental concentration profile ρ of end-tethered flexible polymer chains is calculated for comparison with recent measurements on polymer layers having a low surface grafting density σ. Moments of ρ are also calculated as these quantities, rather than the full concentration profiles, are usually measured experimentally. Exact calculations of ρ are summarized for ideal flexible chains with an arbitrary short-range polymer–surface interaction. Though technical difficulties restrict our renormalization group (RG) calculations for swollen chains to limiting values of the polymer–surface interaction, our analysis indicates that the relatively simple, closed-form, Gaussian-chain expression for ρ provides a good approximation to the RG results if the average size of the Gaussian chain is replaced by its swollen-chain analog. This approximate concentration profile for chains with excluded volume and variable polymer–surface interaction should prove useful when interpreting experimental results for low-grafting-density polymer layers formed in good solvents. Recent measurements [Kent et al., J. Chem. Phys. 103, 2320 (1995)] of the second moment of ρ in the limit σ→0 agree well with our RG calculations, and the measured concentration profile ρ, whose determination by neutron reflection is somewhat uncertain, agrees qualitatively with our theoretical predictions. © 1996 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 102 (1995), S. 1449-1460 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We derive a gradient expansion for the external field necessary to weakly perturb the density profile of noninteracting polymer chains near a surface. This result can be used as part of a more general methodology for analyzing the long-wavelength adsorptive properties of polymer solutions and melts. The coefficients appearing in the expansion are determined from the solutions of a hierarchy of linear, Fredholm integral equations that contain information about the reference (unperturbed) state. We illustrate the calculation of the two lowest-order coefficients for reflecting and absorbing reference boundary conditions. A similar gradient expansion of the intrinsic free energy functional suggests the need to exercise care in obtaining variational forms for the grand free energy from the Legendre transform of the grand partition function. Extremely simple symmetry arguments show that a proper application of gradient expansion techniques leads to a vanishing of the linear gradient contributions to the free energy. © 1995 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 103 (1995), S. 8257-8272 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We analyze the long-wavelength features of near-surface composition profiles of monomers in a binary, symmetric blend using a recently developed density functional formalism for polymers in nonuniform environments. Relative to simpler theories of polymer–surface adsorption, our theory predicts a small increase of the interfacial width. We illustrate a derivation of a surface–boundary condition on the composition profile directly from the monomer–surface Hamiltonian. This boundary condition, when combined with our density functional analysis, leads to first-order wetting transitions. © 1995 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 5372-5387 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We analyze the weak-segregation, thermodynamic predictions of a simple mean-field model of diblock copolymer melts sandwiched between surfaces that interact weakly with melts. Under many conditions, these films do not exhibit a phase transition although the segregation that develops within them resembles ordering in the bulk. When transitions occur, they result from a competition between surface and bulk effects and have no bulk analog. Thin films confined by identical surfaces and films bounded by surfaces having equal in magnitude, but opposite affinities for the monomers may exhibit first- as well as second-order intrafilm transitions when the melt–surface interactions are small. The model predicts that second-order transitions do not occur in films with large surface affinities and that films bounded by different surfaces undergo only first-order intrafilm transitions. The instabilities that lead to the second-order transitions in films with symmetry-breaking affinities disappear with increases in the film thickness.
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