banner image
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Effects of tube persistence length on dynamics of mildly entangled polymers
Rent this article for
View: Figures


Image of FIG. 1.
FIG. 1.

Cloud points show bead positions of a test chain from 28 MD trajectories spanning the time . The center thick line is the average of bead positions, called the mean path. The confining tube surrounding the primitive path is easily visualized.

Image of FIG. 2.
FIG. 2.

Primitive paths approximated with trajectory mean paths, for a single chain in the C400 system. (a) Results for different average times , for , , and . (b) Results for the same average time (), but at different elapsed times.

Image of FIG. 3.
FIG. 3.

Equilibrium tangent–tangent correlation functions of primitive paths for , 20, 40, 100, and 200, for C400 system. The apparent spikes right off the maximum are associated with the immediate neighboring bonds. The averages have been taken over primitive paths at different snapshots, and over different chains. Inset: same data plotted on log-linear scale.

Image of FIG. 4.
FIG. 4.

Data points: integrated tangent–tangent correlation functions, , for , at times , 6, 12, 36, and , respectively, which corresponding to 0, 0.01, 0.02, 0.06, and . (a) Solid curves are prediction of dynamics theory of flexible tube. (b) Solid curves are prediction of dynamics theory of semiflexible tube (see Sec. III).

Image of FIG. 5.
FIG. 5.

Normalized autocorrelation function of six independent stress components for C400 system, computed using multi- correlator. Inset: time dependence of .

Image of FIG. 6.
FIG. 6.

Average of the autocorrelation functions of independent stress components (solid curve with circles), and tube EOM predictions (solid and dashed curves; see Sec. III).

Image of FIG. 7.
FIG. 7.

Early time bead MSD of a semiflexible tube. Solid line: numerical results from Eq. (7). Thin lines: asymptotic limits by integrating Eq. (7) using the (slope = 1/2) and the (slope = 3/4) modes alone.

Image of FIG. 8.
FIG. 8.

Solution of EOM with only reptation and CR mechanisms () for . Initial condition: exponential decay. Time: , , , and . Number of mesh points: 40.


Article metrics loading...


Full text loading...

This is a required field
Please enter a valid email address
752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Effects of tube persistence length on dynamics of mildly entangled polymers