2008
DOI: 10.1134/s0965545x08060059
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Conformational properties of rigid-chain amphiphilic macromolecules: The phase diagram

Abstract: Conformational properties of rigid-chain amphiphilic macromolecules Markov, V. A.; Vasilevskaya, V. V.; Khalatur, P. G.; ten Brinke, G.; Khokhlov, A. R. IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you wish to cite from it. Please check the document version below. Document Version Publisher's PDF, also known as Version of record Publication date: 2008Link to publication in University of Groningen/UMCG research database Citation for published version (APA): Markov, V. … Show more

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Cited by 15 publications
(7 citation statements)
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“…The discontinuous coil‐to‐globule transitions are also characteristic for some amphiphilic polymers42–47 involving both soluble (H) and insoluble (P) groups in their chains (either in distinct units in the case of amphiphilic copolymers or as parts of the same unit in amphiphilic homopolymers). Amphiphilic polymers with annealed HP structure (i.e., when each monomer unit can reversibly switch between H and P states) can undergo a first‐order coil‐to‐globule transition even in the case of completely flexible chains42: the density of the HP globule at the transition point remains finite in the limit of very long chains N → ∞ (the density is defined by the energy contrast between P and H states in the dilute regime).…”
Section: Discussionmentioning
confidence: 99%
“…The discontinuous coil‐to‐globule transitions are also characteristic for some amphiphilic polymers42–47 involving both soluble (H) and insoluble (P) groups in their chains (either in distinct units in the case of amphiphilic copolymers or as parts of the same unit in amphiphilic homopolymers). Amphiphilic polymers with annealed HP structure (i.e., when each monomer unit can reversibly switch between H and P states) can undergo a first‐order coil‐to‐globule transition even in the case of completely flexible chains42: the density of the HP globule at the transition point remains finite in the limit of very long chains N → ∞ (the density is defined by the energy contrast between P and H states in the dilute regime).…”
Section: Discussionmentioning
confidence: 99%
“…1 In modern materials engineering, the formation of micro-and nano-rings by piercing of a deflating vesicle as solvent evaporates (figure 1d). 15,19 Another phenomenon leading to the formation of molecular rings is the "coil-to-toroidal globule" transition, [20][21][22][23][24] observed previously for isolated chains of "semiflexible" polymers, such as DNA, 25 xanthan 26 among others. Chains of such polymers stay rigid at the nanometre level, but are flexible at a larger scale.…”
Section: Introductionmentioning
confidence: 81%
“…To decrease these losses, homopolymer stiff-chain macromolecules form not spherical globules but globules of complex toroidal or rod-like form. The amphiphilic stiff-chain macromolecules while collapsing are obliged form structures which have both minimal bend energy and “core-shell” organization. Our calculations show that depending on stiffness parameters amphiphilic macromolecules form cylindrical globules with a blob-like chain organization, collagen-like, and toroidal structures. Hydrophobic groups in such structures occupy the inner parts, and hydrophilic ones are arranged at the surface. The total bending stress of the chain in this case is rather high because of the high stiffness of the macromolecule.…”
Section: Introductionmentioning
confidence: 91%
“…The conformational properties of macromolecules and properties of their concentrated solutions , depend essentially on the polymeric chain stiffness. The collapse of stiff macromolecules is accompanied not only by a great reduction of the entropy of the monomeric units, but also by essential energy losses due to the bends in the polymeric chain.…”
Section: Introductionmentioning
confidence: 99%