Self-organized mechano-chemical dynamics in amoeboid locomotion of Physarum fragments
- PMID: 30906070
- PMCID: PMC6430145
- DOI: 10.1088/1361-6463/aa68be
Self-organized mechano-chemical dynamics in amoeboid locomotion of Physarum fragments
Abstract
The aim of this work is to quantify the spatio-temporal dynamics of flow-driven amoeboid locomotion in small (~100 µm) fragments of the true slime mold Physarum polycephalum. In this model organism, cellular contraction drives intracellular flows, and these flows transport the chemical signals that regulate contraction in the first place. As a consequence of these non-linear interactions, a diversity of migratory behaviors can be observed in migrating Physarum fragments. To study these dynamics, we measure the spatio-temporal distributions of the velocities of the endoplasm and ectoplasm of each migrating fragment, the traction stresses it generates on the substratum, and the concentration of free intracellular calcium. Using these unprecedented experimental data, we classify migrating Physarum fragments according to their dynamics, finding that they often exhibit spontaneously coordinated waves of flow, contractility and chemical signaling. We show that Physarum fragments exhibiting symmetric spatio-temporal patterns of endoplasmic flow migrate significantly slower than fragments with asymmetric patterns. In addition, our joint measurements of ectoplasm velocity and traction stress at the substratum suggest that forward motion of the ectoplasm is enabled by a succession of stick-slip transitions, which we conjecture are also organized in the form of waves. Combining our experiments with a simplified convection-diffusion model, we show that the convective transport of calcium ions may be key for establishing and maintaining the spatiotemporal patterns of calcium concentration that regulate the generation of contractile forces.
Keywords: amoeboid motility; cell migration; mechano-chemical interactions; particle image velocimetry; physarum; traction force microscopy.
Figures
, peristaltic fragments;
, amphistaltic fragments. The dashed line is Δxcent = Δxflow.
) and longitudinal traction stresses (
) at two specific locations in the front (panel a) and the back (panel b) of the peristaltic Physarum fragment shown in Figure 7. The tiled bars at the top of the plots represent the time-dependent phase differences (in radians) between the ectoplasm velocity and the traction stresses. Blue and orange tiles represent phase differences near −π/2 (cell and substrate stick) and zero (cell and substrate slip) respectively, as indicated by the color scale at the top of the figure.
) and ratiometric measurement of [Ca2+]i (
), averaged along the width of a peristaltic fragment (panels a and c) and an amphistaltic fragment (panels e and g). Bottom row (b, d, f, h): Time histories of endoplasmic flow velocity (
) and peripheral traction stress (
), averaged along the width of a peristaltic fragment (panels b and d) and an amphistaltic fragment (panels f and h). Panels (a, b, e, f): Fragment front. Panels (c, d, g, h): Fragment rear.References
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