Equivalence of chain conformations in the surface region of a polymer melt and a single Gaussian chain under critical conditions
In the melt polymer conformations are nearly ideal according to Flory's ideality hypothesis. Silberberg generalized this statement for chains in the interfacial region. We check the Silberberg argument by analyzing the conformations of a probe chain end-grafted at a solid surface in a sea of fl...
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Published in | The Journal of chemical physics Vol. 139; no. 5; p. 054907 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
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United States
07.08.2013
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Abstract | In the melt polymer conformations are nearly ideal according to Flory's ideality hypothesis. Silberberg generalized this statement for chains in the interfacial region. We check the Silberberg argument by analyzing the conformations of a probe chain end-grafted at a solid surface in a sea of floating free chains of concentration φ by the self-consistent field (SCF) method. Apart from the grafting, probe chain and floating chains are identical. Most of the results were obtained for a standard SCF model with freely jointed chains on a six-choice lattice, where immediate step reversals are allowed. A few data were generated for a five-choice lattice, where such step reversals are forbidden. These coarse-grained models describe the equilibrium properties of flexible atactic polymer chains at the scale of the segment length. The concentration was varied over the whole range from φ = 0 (single grafted chain) to φ = 1 (probe chain in the melt). The number of contacts with the surface, average height of the free end and its dispersion, average loop and train length, tail size distribution, end-point and overall segment distributions were calculated for a grafted probe chain as a function of φ, for several chain lengths and substrate/polymer interactions, which were varied from strong repulsion to strong adsorption. The computations show that the conformations of the probe chain in the melt do not depend on substrate/polymer interactions and are very similar to the conformations of a single end-grafted chain under critical conditions, and can thus be described analytically. When the substrate/polymer interaction is fixed at the value corresponding to critical conditions, all equilibrium properties of a probe chain are independent of φ, over the whole range from a dilute solution to the melt. We believe that the conformations of all flexible chains in the surface region of the melt are close to those of an appropriate single chain in critical conditions, provided that one end of the single chain is fixed at the same point as a chain in the melt. |
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AbstractList | In the melt polymer conformations are nearly ideal according to Flory's ideality hypothesis. Silberberg generalized this statement for chains in the interfacial region. We check the Silberberg argument by analyzing the conformations of a probe chain end-grafted at a solid surface in a sea of floating free chains of concentration φ by the self-consistent field (SCF) method. Apart from the grafting, probe chain and floating chains are identical. Most of the results were obtained for a standard SCF model with freely jointed chains on a six-choice lattice, where immediate step reversals are allowed. A few data were generated for a five-choice lattice, where such step reversals are forbidden. These coarse-grained models describe the equilibrium properties of flexible atactic polymer chains at the scale of the segment length. The concentration was varied over the whole range from φ = 0 (single grafted chain) to φ = 1 (probe chain in the melt). The number of contacts with the surface, average height of the free end and its dispersion, average loop and train length, tail size distribution, end-point and overall segment distributions were calculated for a grafted probe chain as a function of φ, for several chain lengths and substrate∕polymer interactions, which were varied from strong repulsion to strong adsorption. The computations show that the conformations of the probe chain in the melt do not depend on substrate∕polymer interactions and are very similar to the conformations of a single end-grafted chain under critical conditions, and can thus be described analytically. When the substrate∕polymer interaction is fixed at the value corresponding to critical conditions, all equilibrium properties of a probe chain are independent of φ, over the whole range from a dilute solution to the melt. We believe that the conformations of all flexible chains in the surface region of the melt are close to those of an appropriate single chain in critical conditions, provided that one end of the single chain is fixed at the same point as a chain in the melt. In the melt polymer conformations are nearly ideal according to Flory's ideality hypothesis. Silberberg generalized this statement for chains in the interfacial region. We check the Silberberg argument by analyzing the conformations of a probe chain end-grafted at a solid surface in a sea of floating free chains of concentration φ by the self-consistent field (SCF) method. Apart from the grafting, probe chain and floating chains are identical. Most of the results were obtained for a standard SCF model with freely jointed chains on a six-choice lattice, where immediate step reversals are allowed. A few data were generated for a five-choice lattice, where such step reversals are forbidden. These coarse-grained models describe the equilibrium properties of flexible atactic polymer chains at the scale of the segment length. The concentration was varied over the whole range from φ = 0 (single grafted chain) to φ = 1 (probe chain in the melt). The number of contacts with the surface, average height of the free end and its dispersion, average loop and train length, tail size distribution, end-point and overall segment distributions were calculated for a grafted probe chain as a function of φ, for several chain lengths and substrate∕polymer interactions, which were varied from strong repulsion to strong adsorption. The computations show that the conformations of the probe chain in the melt do not depend on substrate∕polymer interactions and are very similar to the conformations of a single end-grafted chain under critical conditions, and can thus be described analytically. When the substrate∕polymer interaction is fixed at the value corresponding to critical conditions, all equilibrium properties of a probe chain are independent of φ, over the whole range from a dilute solution to the melt. We believe that the conformations of all flexible chains in the surface region of the melt are close to those of an appropriate single chain in critical conditions, provided that one end of the single chain is fixed at the same point as a chain in the melt.In the melt polymer conformations are nearly ideal according to Flory's ideality hypothesis. Silberberg generalized this statement for chains in the interfacial region. We check the Silberberg argument by analyzing the conformations of a probe chain end-grafted at a solid surface in a sea of floating free chains of concentration φ by the self-consistent field (SCF) method. Apart from the grafting, probe chain and floating chains are identical. Most of the results were obtained for a standard SCF model with freely jointed chains on a six-choice lattice, where immediate step reversals are allowed. A few data were generated for a five-choice lattice, where such step reversals are forbidden. These coarse-grained models describe the equilibrium properties of flexible atactic polymer chains at the scale of the segment length. The concentration was varied over the whole range from φ = 0 (single grafted chain) to φ = 1 (probe chain in the melt). The number of contacts with the surface, average height of the free end and its dispersion, average loop and train length, tail size distribution, end-point and overall segment distributions were calculated for a grafted probe chain as a function of φ, for several chain lengths and substrate∕polymer interactions, which were varied from strong repulsion to strong adsorption. The computations show that the conformations of the probe chain in the melt do not depend on substrate∕polymer interactions and are very similar to the conformations of a single end-grafted chain under critical conditions, and can thus be described analytically. When the substrate∕polymer interaction is fixed at the value corresponding to critical conditions, all equilibrium properties of a probe chain are independent of φ, over the whole range from a dilute solution to the melt. We believe that the conformations of all flexible chains in the surface region of the melt are close to those of an appropriate single chain in critical conditions, provided that one end of the single chain is fixed at the same point as a chain in the melt. In the melt polymer conformations are nearly ideal according to Flory's ideality hypothesis. Silberberg generalized this statement for chains in the interfacial region. We check the Silberberg argument by analyzing the conformations of a probe chain end-grafted at a solid surface in a sea of floating free chains of concentration phi by the self-consistent field (SCF) method. Apart from the grafting, probe chain and floating chains are identical. Most of the results were obtained for a standard SCF model with freely jointed chains on a six-choice lattice, where immediate step reversals are allowed. A few data were generated for a five-choice lattice, where such step reversals are forbidden. These coarse-grained models describe the equilibrium properties of flexible atactic polymer chains at the scale of the segment length. The concentration was varied over the whole range from phi = 0 (single grafted chain) to phi = 1 (probe chain in the melt). The number of contacts with the surface, average height of the free end and its dispersion, average loop and train length, tail size distribution, end-point and overall segment distributions were calculated for a grafted probe chain as a function of phi , for several chain lengths and substrate/polymer interactions, which were varied from strong repulsion to strong adsorption. The computations show that the conformations of the probe chain in the melt do not depend on substrate/polymer interactions and are very similar to the conformations of a single end-grafted chain under critical conditions, and can thus be described analytically. When the substrate/polymer interaction is fixed at the value corresponding to critical conditions, all equilibrium properties of a probe chain are independent of phi , over the whole range from a dilute solution to the melt. We believe that the conformations of all flexible chains in the surface region of the melt are close to those of an appropriate single chain in critical conditions, provided that one end of the single chain is fixed at the same point as a chain in the melt. In the melt polymer conformations are nearly ideal according to Flory's ideality hypothesis. Silberberg generalized this statement for chains in the interfacial region. We check the Silberberg argument by analyzing the conformations of a probe chain end-grafted at a solid surface in a sea of floating free chains of concentration φ by the self-consistent field (SCF) method. Apart from the grafting, probe chain and floating chains are identical. Most of the results were obtained for a standard SCF model with freely jointed chains on a six-choice lattice, where immediate step reversals are allowed. A few data were generated for a five-choice lattice, where such step reversals are forbidden. These coarse-grained models describe the equilibrium properties of flexible atactic polymer chains at the scale of the segment length. The concentration was varied over the whole range from φ = 0 (single grafted chain) to φ = 1 (probe chain in the melt). The number of contacts with the surface, average height of the free end and its dispersion, average loop and train length, tail size distribution, end-point and overall segment distributions were calculated for a grafted probe chain as a function of φ, for several chain lengths and substrate/polymer interactions, which were varied from strong repulsion to strong adsorption. The computations show that the conformations of the probe chain in the melt do not depend on substrate/polymer interactions and are very similar to the conformations of a single end-grafted chain under critical conditions, and can thus be described analytically. When the substrate/polymer interaction is fixed at the value corresponding to critical conditions, all equilibrium properties of a probe chain are independent of φ, over the whole range from a dilute solution to the melt. We believe that the conformations of all flexible chains in the surface region of the melt are close to those of an appropriate single chain in critical conditions, provided that one end of the single chain is fixed at the same point as a chain in the melt. |
Author | Leermakers, F. A. M. Fleer, G. J. Skvortsov, A. M. |
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BackLink | https://www.ncbi.nlm.nih.gov/pubmed/23927284$$D View this record in MEDLINE/PubMed |
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Cites_doi | 10.1021/la7023154 10.1063/1.1676755 10.1007/s10955-011-0354-0 10.1016/0927-7757(94)02846-X 10.1021/ma020416s 10.1063/1.443835 10.1021/ma00015a011 10.1103/PhysRevE.87.022604 10.1021/ma00183a036 10.1016/0021-9797(82)90400-3 10.1088/0953-8984/17/20/004 10.1063/1.462612 10.1063/1.457840 10.1021/j100475a012 10.1021/ma00197a042 10.1103/PhysRevE.79.030802 10.1016/j.polymer.2010.06.043 10.1088/0370-1328/85/4/301 10.1063/1.1696332 10.1039/c0cp02868a 10.1140/epje/i2012-12097-6 10.1103/PhysRevE.82.050801 10.1063/1.465163 10.1063/1.1346686 10.1039/fd9949800111 10.1063/1.3689316 10.1021/ma980793y 10.1021/ma0345145 10.1016/0021-9797(88)90049-5 10.1063/1.443257 10.1103/PhysRevLett.90.226103 10.1021/ma0474731 10.1140/epje/i2008-10392-5 10.1021/ma00222a016 10.1063/1.3693515 10.1021/ma00051a044 10.1021/ma0015370 10.1016/0001-8686(95)00270-Z 10.1021/ma050176r 10.1088/0370-1328/88/2/301 10.1021/ma00202a033 10.1002/polb.1995.090331709 10.1021/ma0626113 10.1021/ma00023a034 10.1021/ma00202a034 10.1140/epje/i2009-10454-2 |
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References | (2023070322380946800_c10b) 1989; 22 (2023070322380946800_c40) 2005; 17 (2023070322380946800_c33) 2009; 79 (2023070322380946800_c5) 2005; 38 (2023070322380946800_c36) 2008; 24 (2023070322380946800_c27) 1979 (2023070322380946800_c6) 2012; 136 (2023070322380946800_c3c) 1991; 24 (2023070322380946800_c32) 2001; 114 (2023070322380946800_c11) 1990; 92 (2023070322380946800_c28) 2003; 36 (2023070322380946800_c13) 2003; 90 (2023070322380946800_c9) 2011; 13 (2023070322380946800_c34) 2013; 87 (2023070322380946800_c37) 1971; 55 (2023070322380946800_c26) 1994; 86 (2023070322380946800_c35) 1965; 42 (2023070322380946800_c12) 1993; 99 (2023070322380946800_c24) 1986 (2023070322380946800_c3d) 1991; 24 (2023070322380946800_c23a) 1965; 85 (2023070322380946800_c30) 2011 (2023070322380946800_c7) 1979; 83 (2023070322380946800_c20b) 1988; 125 (2023070322380946800_c31) 1995; 62 (2023070322380946800_c42) 2008; 27 (2023070322380946800_c17) 2012; 35 (2023070322380946800_c19) 1994; 98 (2023070322380946800_c39) 2007; 40 (2023070322380946800_c14) 2005; 38 (2023070322380946800_c20a) 1982; 90 (2023070322380946800_c2) 1992; 96 (2023070322380946800_c3b) 1990; 23 (2023070322380946800_c16) 2010; 51 (2023070322380946800_c10a) 1988; 21 (2023070322380946800_c41) 2011; 145 (2023070322380946800_c10c) 1989; 22 (2023070322380946800_c1) 2010; 82 (2023070322380946800_c38) 1982; 76 (2023070322380946800_c23b) 1966; 88 (2023070322380946800_c25) 2012; 136 (2023070322380946800_c4) 1992; 25 (2023070322380946800_c8) 1993 (2023070322380946800_c15b) 2001; 34 (2023070322380946800_c3a) 1989; 22 (2023070322380946800_c22) 1953 (2023070322380946800_c29) 1999; 32 (2023070322380946800_c21) 1982; 77 (2023070322380946800_c18) 1995; 33 (2023070322380946800_c43) 2009; 29 (2023070322380946800_c15a) 2002; 35 |
References_xml | – volume: 24 start-page: 1930 year: 2008 ident: 2023070322380946800_c36 publication-title: Langmuir doi: 10.1021/la7023154 – volume: 55 start-page: 4318 year: 1971 ident: 2023070322380946800_c37 publication-title: J. Chem. Phys. doi: 10.1063/1.1676755 – volume: 145 start-page: 1017 year: 2011 ident: 2023070322380946800_c41 publication-title: J. Stat. Phys. doi: 10.1007/s10955-011-0354-0 – volume: 86 start-page: 61 year: 1994 ident: 2023070322380946800_c26 publication-title: Colloids Surf., A Physicochemical and Engineering Aspects doi: 10.1016/0927-7757(94)02846-X – volume: 35 start-page: 8191 year: 2002 ident: 2023070322380946800_c15a publication-title: Macromolecules doi: 10.1021/ma020416s – volume: 77 start-page: 6296 year: 1982 ident: 2023070322380946800_c21 publication-title: J. Chem. Phys. doi: 10.1063/1.443835 – volume: 24 start-page: 4295 year: 1991 ident: 2023070322380946800_c3c publication-title: Macromolecules doi: 10.1021/ma00015a011 – volume: 87 start-page: 022604 year: 2013 ident: 2023070322380946800_c34 publication-title: Phys. Rev. E doi: 10.1103/PhysRevE.87.022604 – volume: 21 start-page: 1400 year: 1988 ident: 2023070322380946800_c10a publication-title: Macromolecules doi: 10.1021/ma00183a036 – volume: 90 start-page: 86 year: 1982 ident: 2023070322380946800_c20a publication-title: J. Colloid Interface Sci. doi: 10.1016/0021-9797(82)90400-3 – volume-title: The Theory of Polymer Dynamics year: 1986 ident: 2023070322380946800_c24 – volume: 17 start-page: S1697 year: 2005 ident: 2023070322380946800_c40 publication-title: J. Phys. Condens. Matter doi: 10.1088/0953-8984/17/20/004 – volume: 96 start-page: 6213 year: 1992 ident: 2023070322380946800_c2 publication-title: J. Chem. Phys. doi: 10.1063/1.462612 – volume: 92 start-page: 3827 year: 1990 ident: 2023070322380946800_c11 publication-title: J. Chem. Phys. doi: 10.1063/1.457840 – volume: 83 start-page: 1619 year: 1979 ident: 2023070322380946800_c7 publication-title: J. Phys. Chem. doi: 10.1021/j100475a012 – volume: 22 start-page: 3143 year: 1989 ident: 2023070322380946800_c3a publication-title: Macromolecules doi: 10.1021/ma00197a042 – volume: 79 start-page: 030802 year: 2009 ident: 2023070322380946800_c33 publication-title: Phys. Rev. E doi: 10.1103/PhysRevE.79.030802 – volume: 51 start-page: 4259 year: 2010 ident: 2023070322380946800_c16 publication-title: Polymer doi: 10.1016/j.polymer.2010.06.043 – volume: 85 start-page: 613 year: 1965 ident: 2023070322380946800_c23a publication-title: Proc. Phys. Soc. doi: 10.1088/0370-1328/85/4/301 – volume: 42 start-page: 2558 year: 1965 ident: 2023070322380946800_c35 publication-title: J. Chem. Phys. doi: 10.1063/1.1696332 – volume: 13 start-page: 10491 year: 2011 ident: 2023070322380946800_c9 publication-title: Phys. Chem. Chem. Phys. doi: 10.1039/c0cp02868a – volume-title: Polymers at Interfaces year: 1993 ident: 2023070322380946800_c8 – volume: 35 start-page: 97 year: 2012 ident: 2023070322380946800_c17 publication-title: Eur. Phys. J. E doi: 10.1140/epje/i2012-12097-6 – volume: 82 start-page: 050801 year: 2010 ident: 2023070322380946800_c1 publication-title: Phys. Rev. E doi: 10.1103/PhysRevE.82.050801 – volume: 99 start-page: 3100 year: 1993 ident: 2023070322380946800_c12 publication-title: J. Chem. Phys. doi: 10.1063/1.465163 – volume-title: Scaling Concepts in Polymer Physics year: 1979 ident: 2023070322380946800_c27 – volume: 114 start-page: 5366 year: 2001 ident: 2023070322380946800_c32 publication-title: J. Chem. Phys. doi: 10.1063/1.1346686 – volume: 98 start-page: 111 year: 1994 ident: 2023070322380946800_c19 publication-title: Faraday Discuss. doi: 10.1039/fd9949800111 – volume: 136 start-page: 094901 year: 2012 ident: 2023070322380946800_c6 publication-title: J. Chem. Phys. doi: 10.1063/1.3689316 – volume: 32 start-page: 825 year: 1999 ident: 2023070322380946800_c29 publication-title: Macromolecules doi: 10.1021/ma980793y – volume: 36 start-page: 7857 year: 2003 ident: 2023070322380946800_c28 publication-title: Macromolecules doi: 10.1021/ma0345145 – volume: 125 start-page: 14 year: 1988 ident: 2023070322380946800_c20b publication-title: J. Colloid Interface Sci. doi: 10.1016/0021-9797(88)90049-5 – volume: 76 start-page: 2720 year: 1982 ident: 2023070322380946800_c38 publication-title: J. Chem. Phys. doi: 10.1063/1.443257 – volume: 90 start-page: 226103 year: 2003 ident: 2023070322380946800_c13 publication-title: Phys. Rev. Lett. doi: 10.1103/PhysRevLett.90.226103 – volume-title: Colloids and the Depletion Interaction year: 2011 ident: 2023070322380946800_c30 – volume: 38 start-page: 4495 year: 2005 ident: 2023070322380946800_c14 publication-title: Macromolecules doi: 10.1021/ma0474731 – volume: 27 start-page: 435 year: 2008 ident: 2023070322380946800_c42 publication-title: Eur. Phys. J. E doi: 10.1140/epje/i2008-10392-5 – volume: 23 start-page: 4430 year: 1990 ident: 2023070322380946800_c3b publication-title: Macromolecules doi: 10.1021/ma00222a016 – volume: 136 start-page: 134707 year: 2012 ident: 2023070322380946800_c25 publication-title: J. Chem. Phys. doi: 10.1063/1.3693515 – volume: 25 start-page: 7011 year: 1992 ident: 2023070322380946800_c4 publication-title: Macromolecules doi: 10.1021/ma00051a044 – volume: 34 start-page: 1946 year: 2001 ident: 2023070322380946800_c15b publication-title: Macromolecules doi: 10.1021/ma0015370 – volume: 62 start-page: 31 year: 1995 ident: 2023070322380946800_c31 publication-title: Adv. Colloid Interface Sci. doi: 10.1016/0001-8686(95)00270-Z – volume: 38 start-page: 5780 year: 2005 ident: 2023070322380946800_c5 publication-title: Macromolecules doi: 10.1021/ma050176r – volume: 88 start-page: 265 year: 1966 ident: 2023070322380946800_c23b publication-title: Proc. Phys. Soc. doi: 10.1088/0370-1328/88/2/301 – volume: 22 start-page: 4578 year: 1989 ident: 2023070322380946800_c10b publication-title: Macromolecules doi: 10.1021/ma00202a033 – volume: 33 start-page: 2373 year: 1995 ident: 2023070322380946800_c18 publication-title: J. Polym. Sci. B doi: 10.1002/polb.1995.090331709 – volume-title: Principles of Polymer Chemistry year: 1953 ident: 2023070322380946800_c22 – volume: 40 start-page: 3805 year: 2007 ident: 2023070322380946800_c39 publication-title: Macromolecules doi: 10.1021/ma0626113 – volume: 24 start-page: 6283 year: 1991 ident: 2023070322380946800_c3d publication-title: Macromolecules doi: 10.1021/ma00023a034 – volume: 22 start-page: 4589 year: 1989 ident: 2023070322380946800_c10c publication-title: Macromolecules doi: 10.1021/ma00202a034 – volume: 29 start-page: 107 year: 2009 ident: 2023070322380946800_c43 publication-title: Eur. Phys. J. E doi: 10.1140/epje/i2009-10454-2 |
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Snippet | In the melt polymer conformations are nearly ideal according to Flory's ideality hypothesis. Silberberg generalized this statement for chains in the... |
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SubjectTerms | Adsorption Chains Chains (polymeric) Freezing Grafting Mathematical analysis Mathematical models Melts Molecular Conformation Polymers - chemistry Segments Surface Properties |
Title | Equivalence of chain conformations in the surface region of a polymer melt and a single Gaussian chain under critical conditions |
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