2013
DOI: 10.1021/ma4020824
|View full text |Cite
|
Sign up to set email alerts
|

Free Energy and Extension of a Wormlike Chain in Tube Confinement

Abstract: The partial differential equation that yields the free energy and conformational properties of a long wormlike polymer in confinement is discussed and analyzed. In the strong confinement limit, the confinement free energy and polymer extension display the Odijk power laws; numerical solutions of the differential equations are obtained and analyzed to produce these power-law coefficients for tubes with square and circular cross sections; the result verifies recent determination of the coefficients, one of them … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

6
59
0

Year Published

2015
2015
2020
2020

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 50 publications
(65 citation statements)
references
References 26 publications
6
59
0
Order By: Relevance
“…18 The scaling of static properties in this ‘classic Odijk regime’ has been extensively studied, so much so that the prefactors in these scaling relations are known to multiple decimal places. 19,20 Our recent work confirmed the existence of a universal backfolded Odijk regime, wherein the deflection segments can form hairpins inside the channel. 10,13 Indeed, our calculations of the static properties in the backfolded Odijk regime 13 showed excellent agreement with Odijk’s theory.…”
Section: Introductionsupporting
confidence: 61%
“…18 The scaling of static properties in this ‘classic Odijk regime’ has been extensively studied, so much so that the prefactors in these scaling relations are known to multiple decimal places. 19,20 Our recent work confirmed the existence of a universal backfolded Odijk regime, wherein the deflection segments can form hairpins inside the channel. 10,13 Indeed, our calculations of the static properties in the backfolded Odijk regime 13 showed excellent agreement with Odijk’s theory.…”
Section: Introductionsupporting
confidence: 61%
“…Since the average projection of each bond along the cylinder axis is ℓ b cos θ ≈ ℓ b (1 − θ 2 /2), the reduction of the mean-squared end-to-end distance becomes 1 − R 2 e 1/2 /L ≈ θ 2 /2 = r ef f ℓp 2/3 /2. These scaling arguments can be made more precise to yield, [25][26][27] for L/ℓ p ≫ 1, [12] and typical experiments [43,44]. The shaded stripe indicates the I-N coexistence region, ρi < ρ < ρn, as predicted by Chen [12].…”
mentioning
confidence: 99%
“…It would be very interesting to study the corresponding static and dynamic collective structure factors, but this is beyond our scope here. It remains a challenge to extend the analytic theories [8][9][10][11][12]26] to self-consistently predict the length scales λ and r ef f from the molecular parameters ℓ p , d and L and the polymer density.…”
mentioning
confidence: 99%
“…1). Little is known about this phase diagram for rectangular channels, except in the limit of very strong confinement [11,24,25]. To interpret a given experiment it is necessary to determine which regime in the phase diagram it corresponds to, and what the resulting scaling relations for the extension statistics are.…”
mentioning
confidence: 99%