1967
DOI: 10.1002/polc.5070160644
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The models of the denaturation of globular proteins. I. Theory of globula–coil transitions in macromolecules

Abstract: SynopsisThe theory of long-range interactions in macromolecules is proposed for the region where the attraction forces predominate (that is below 8-point). In an approximate analytical variant of the theory the free energy of segment-segment interactions is calculated without taking into account their bonding in the single chain, that is, by means of strict and approximate equation for the free energy of interaction of real gas molecules. The theory predicts that under some conditions the macromolecule undergo… Show more

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Cited by 104 publications
(70 citation statements)
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“…In principle, for a description of the globular state one should also include the n-body interactions with n A 3. The number density of these interactions is in general negligible if the chain is viewed as a gas of disconnected monomers 33) . Their number is increased by chain connectivity that brings together clusters of topologically close monomers.…”
Section: X9mentioning
confidence: 99%
“…In principle, for a description of the globular state one should also include the n-body interactions with n A 3. The number density of these interactions is in general negligible if the chain is viewed as a gas of disconnected monomers 33) . Their number is increased by chain connectivity that brings together clusters of topologically close monomers.…”
Section: X9mentioning
confidence: 99%
“…[1][2][3] Below the LCST, the polymer is soluble due to the hydrogen bonds formed between the water molecules and the amide groups. The coil-globule transition at the LCST arises from breaking of the hydrogen bonds and from the expelling of water molecules, leading to polymer precipitation into particles and to a two-phase system.…”
Section: Introductionmentioning
confidence: 99%
“…This has been a matter of contention (Ptitsyn et al, 1968;de Gennes, 1975;Post & Zimm, 1979;Sanchez, 1979;Grosberg & Khokhlov, 1987). Although Ptitsyn et al (1968) argued that homopolymer collapse should be two-state in the limit of infinite chain length, it now appears that the collapse of a flexible homopolymer chain of finite length is a onestate transition (Sun et al, 1980;Tiktopulo et al, 1994), unless chain stiffness is high, as in DNA (de Gennes, 1975;Post & Zimm, 1979;reviewed by Chan & Dill, 1991a. In this regard the collapse of flexible homopolymers is less cooperative than the two-state folding attributed to small globular proteins.…”
Section: Protein Folding Cooperativity: a Simplest Hypothesismentioning
confidence: 99%
“…Homopolymers are predicted to collapse when they are put into "poor" solvents (i.e., solvents that prefer phase separation to mixing with monomers of the type that comprise the homopolymer) (Anufrieva et al, 1968;Ptitsyn et al, 1968;de Gennes, 1975;Post & Zimm, 1979;Sanchez, 1979;Williams et al, 1981). It is observed experimentally that polystyrene, a chain of nonpolar monomers, collapses to a compact globule in a poor organic solvent (Sun et al, 1980) and poly-(Nisopropylacrylamide) (PNIPAM) collapses very sharply (with increasing temperature) in water (Fujishige et al, 1989;RiEka et al, 1990;Meewes et al, 1991;Tiktopulo et al, 1994), resembling the renaturation of cold-denatured proteins (Privalov & Gill, 1988;see Fig.…”
Section: Nonlocal Interactions Drive Collapse Transitions Whereas Lomentioning
confidence: 99%