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Nematode locomotion in unconfined and confined fluids
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10.1063/1.4816718
/content/aip/journal/pof2/25/8/10.1063/1.4816718
http://aip.metastore.ingenta.com/content/aip/journal/pof2/25/8/10.1063/1.4816718

Figures

Image of FIG. 1.
FIG. 1.

Typical body postures of (a) crawling on agar (-shape), (b) making Ω-turn on agar, and (c) swimming in water (-shape). The corresponding right panels show PHC description of the shapes in the left panels. Circles represent the numerical skeletons of the worm images, and the lines show results of a single-mode PHC model (see Sec. II and Ref. ).

Image of FIG. 2.
FIG. 2.

Time progressions for a crawling and a swimming nematode performing the same set of body movements: (a) crawling worm (thick line) slides with velocity along a predetermined curve (thin line); (b) swimming worm undergoes translational and rotational slip superposed with the motion along the curve.

Image of FIG. 3.
FIG. 3.

Curves defined by sinusoidal curvature (5) for several values of the normalized amplitude /.

Image of FIG. 4.
FIG. 4.

Nematode body modeled as a chain of touching spheres. (a) The spheres follow the curve defined by the PHC model with wave-velocity . (b) Prescribed individual bead rotations mimic the motion of the interface of the nematode.

Image of FIG. 5.
FIG. 5.

Schematic of the flow field generated by an elongated body dragged in a transverse direction through an unconfined fluid. Overall, the scattered flow is in the same direction as the velocity of the body; the resulting resistance force is moderate.

Image of FIG. 6.
FIG. 6.

The elongated-piston effect: The motion of an elongated body dragged in the transverse direction in a parallel-wall channel produces long-range pressure-driven recirculation pattern. The corresponding pressure drop across the body results in a large resistance force. (a) Side view of the system and (b) top view.

Image of FIG. 7.
FIG. 7.

Ratio ζ between the transverse and longitudinal hydrodynamic-resistance coefficients for a linear chain of equal-size spheres vs. the chain length for unconfined system (dashed line) and parallel-wall channels (solid lines). Channel width normalized by the bead diameter, /, is as labeled. The chain moves in the midplane of the channel.

Image of FIG. 8.
FIG. 8.

Ratio ζ between transverse and longitudinal hydrodynamic-resistance coefficients vs. normalized gap width /. Solid lines represent linear chains of equal-size spheres with chain length N, as labeled. Results of a modified slender-body theory for a confined cylinder of diameter and infinite length are represented by a dotted line. Inset shows a blowup of the region of the moderate values of /.

Image of FIG. 9.
FIG. 9.

Tail trajectories and snapshots of body positions at equally spaced times for a nematode swimming in unconfined fluid (left) and in the midplane of a parallel-wall channel of normalized width / = 1.3 (right).

Image of FIG. 10.
FIG. 10.

Normalized swimming velocity γ vs. wavevector normalized by the worm length for a nematode swimming in an unconfined fluid. Normalized amplitude / is as labeled. Insets show nematode shapes for parameters corresponding to the points indicated by filled circles.

Image of FIG. 11.
FIG. 11.

Normalized swimming velocity γ vs. wavevector normalized by the worm length for a nematode swimming in a midplane of a parallel-wall channel of width (a) / = 3 and (b) / = 1.3. Normalized amplitude / is as labeled. Results obtained by using the CR method are represented by solid lines and those by the HSD approximation are represented by dashed lines.

Image of FIG. 12.
FIG. 12.

Normalized swimming velocity γ vs. normalized amplitude / for a nematode swimming in unconfined fluid (as labeled) and in the midplane of a parallel-wall channel for channel width as labeled. Results obtained by using the CR method are represented by solid lines and those by the HSD approximation are represented by dashed lines. The normalized wavevector corresponds to the maximal efficiency for the given geometry and amplitude. The dotted line represents normalized velocity for a nematode crawling without slip.

Image of FIG. 13.
FIG. 13.

Normalized swimming velocity γ vs. normalized channel width / for a nematode swimming in the midplane of a parallel-wall channel for normalized amplitudes / as labeled. Results obtained by using the CR method are represented by solid lines and those by the HSD approximation are represented by dashed lines. The normalized wavevector corresponds to the maximal efficiency for a given channel geometry and normalized amplitude.

Image of FIG. 14.
FIG. 14.

Nematodes performing turns in different geometries: (a) worm crawling without slip; (b) -shaped worm swimming in a parallel-wall channel; (c) -shaped worm swimming in unconfined fluid; (d) -shaped worm swimming in a parallel-wall channel; (e) -shaped worm swimming in unconfined fluid. Normalized channel width / = 1.3. The normalized wavevector for the -shaped worm is = 9 and for -shaped worm is = 5.5. The turning angle and mode-switching points and are marked in (a); dashed lines indicate the direction of motion.

Image of FIG. 15.
FIG. 15.

Angle of turn θ vs. the normalized point of amplitude change for the length of high-amplitude mode (a) Δ = π/2 and (b) Δ = π. Crawling without slip is represented by dotted lines. Swimming in unconfined fluid is represented by solid lines, and in parallel-wall channel of width / = 1.3 is represented by dashed lines; swimming results are presented for -shaped worms with = 5.5 (thin lines) and -shaped worms with = 9 (heavy lines). The results for a confined system are evaluated using HSD approximation.

Image of FIG. 16.
FIG. 16.

Angle of turn θ vs. normalized length of high-amplitude mode Δ for (a) = 0 and (b) = π/2; lines are the same as in Fig. 15 .

Image of FIG. 17.
FIG. 17.

Normalized swimming velocity γ vs. wavevector normalized by the worm length for a nematode swimming in unconfined fluid. The local-curvature model is represented by the dashed–dotted line, the model with smoothed angular velocity is represented by the dashed line, and the model with no interparticle slip is represented by the dotted line. Solid lines represent resistive force theory and no rotation model as labeled.

Image of FIG. 18.
FIG. 18.

A comparison of the HSD approximation (solid lines) with accurate results obtained using the CR method (dashed lines) for the transverse and longitudinal resistance coefficients of linear chains of touching spheres in the midplane of a parallel-wall channel. The (a) transverse and (b) longitudinal resistance coefficients per particle (normalized by the one-particle value) and (c) the resistance-coefficient ratio are shown vs. the chain length for the normalized channel width /, as labeled.

Tables

Generic image for table
Table I.

Coefficients , , and of the Hele–Shaw dipole approximation (B8) for active chains of touching spheres, for different values of dimensionless channel width.

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/content/aip/journal/pof2/25/8/10.1063/1.4816718
2013-08-13
2014-04-24
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Nematode locomotion in unconfined and confined fluids
http://aip.metastore.ingenta.com/content/aip/journal/pof2/25/8/10.1063/1.4816718
10.1063/1.4816718
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