2004
DOI: 10.1002/bip.10584
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Excluded volume effect in unzipping DNA with a force

Abstract: A double stranded DNA molecule when pulled with a force acting on one end of the molecule can become either partially or completely unzipped depending on the magnitude of the force F. For a random DNA sequence, the number M of unzipped base pairs goes as M approximately (F - Fc)(-2) and diverges at the critical force Fc with an exponent chi = 2. We find that when excluded volume effect is taken into account for the unzipped part of the DNA, the exponent chi = 2 is not changed but the critical force Fc is chang… Show more

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Cited by 15 publications
(22 citation statements)
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“…The prediction of unzipping transition based on interacting Gaussian chains [10] raised a lot interest and now results are available from dynamical approach [11], exact solutions of lattice models [12, 13], simple models of quenched-averaged DNA [14, 15], numerical simulations and scaling analysis [16, 17]. Recently for a model of interacting polymers where any monomer of one chain can interact with any monomer of the other chain (we call it model A), the role of an intermediate entropy-stabilized phase was recognized and a force-induced triple point [18] in a force-temperature plane was established.In most of the models studied for dsDNA [12,13,14,15,16,19], a monomer i of one strand can only interact with the i-th monomer of the other strand, which is similar to the models of DNA (we call it model B) proposed earlier by Poland and Scheraga [20]. These models do not take into account the directional nature of the hydrogen bond and underestimate the entropy by restricting the formation of hydrogen bonds.…”
mentioning
confidence: 63%
“…The prediction of unzipping transition based on interacting Gaussian chains [10] raised a lot interest and now results are available from dynamical approach [11], exact solutions of lattice models [12, 13], simple models of quenched-averaged DNA [14, 15], numerical simulations and scaling analysis [16, 17]. Recently for a model of interacting polymers where any monomer of one chain can interact with any monomer of the other chain (we call it model A), the role of an intermediate entropy-stabilized phase was recognized and a force-induced triple point [18] in a force-temperature plane was established.In most of the models studied for dsDNA [12,13,14,15,16,19], a monomer i of one strand can only interact with the i-th monomer of the other strand, which is similar to the models of DNA (we call it model B) proposed earlier by Poland and Scheraga [20]. These models do not take into account the directional nature of the hydrogen bond and underestimate the entropy by restricting the formation of hydrogen bonds.…”
mentioning
confidence: 63%
“…This curve (for B ′ ) represents the jump from one coexistence region to another with a sudden, detectable change in force (Eqs. (11) and (12)). Point B ′ corresponds to the separation X(s, T ) of Eq.…”
Section: Closed Loops In the Phase Diagrammentioning
confidence: 94%
“…Serious progress in the analysis of statistics of single polymer chains and membranes with excluded-volume interactions was reached by using the renormalization group technique [3,4,5,6]. These methods, however, have been employed for the analysis of the distribution functions only and have not yet been applied to determine the strain energy of a network, despite the importance of the latter problem for applications, see [7,8] and the references therein, as well as recent publications [9,10,11,12].…”
Section: Introductionmentioning
confidence: 99%