Self-organization: What robotics can learn from amoebae

Self-organization: What robotics can learn from amoebae
a Polar self-propelled particles undergo alignment in binary collisions. b A diffusible signal (green) aligns the cells’ orientation vectors. c Schematic of a Schmitt trigger with variable threshold cth. d Temporal response c(t) of the agents’ signaling system with characteristic timescale 𝜏. en Representative collective dynamic states in the agent-based (ei) and the hydrodynamic model (jn). The snapshots illustrate aggregation and vortex formation following initial ring formation (e, j), where remnant spiral wave arms induce chemical wave propagation in the ring after the spiral core vanished due to depletion in its center (‘whispering gallery’-modes); active droplets (f, k), with a collective response to external stimuli; a collective stream (g, l), where agents propagate toward the source of communication waves; a large vortex with a spiral wave (h, m), and a polar band (i, n). White scale bars indicate a length of 10 units. Colors indicate the polar orientation of particles (top panels) and the chemical concentration c (bottom panels). White and yellow arrows illustrate the direction of motion of the particles (top panels) and the propagation direction of signaling activity (bottom panels), respectively. Credit: Nature Communications (2022). DOI: 10.1038/s41467-022-34484-2″>

Self-organization: What robotics can learn from amoebaea Polar self-propelled particles undergo alignment in binary collisions. b A diffusible signal (green) aligns the cells’ orientation vectors. c Schematic of a Schmitt trigger with variable threshold cth. d Temporal response c(t) of the agents’ signaling system with characteristic timescale 𝜏. en Representative collective dynamic states in the agent-based (ei) and the hydrodynamic model (jn). The snapshots illustrate aggregation and vortex formation following initial ring formation (e, j), where remnant spiral wave arms induce chemical wave propagation in the ring after the spiral core vanished due to depletion in its center (‘whispering gallery’-modes); active droplets (f, k), with a collective response to external stimuli; a collective stream (g, l), where agents propagate toward the source of communication waves; a large vortex with a spiral wave (h, m), and a polar band (i, n). White scale bars indicate a length of 10 units. Colors indicate the polar orientation of particles (top panels) and the chemical concentration c (bottom panels). White and yellow arrows illustrate the direction of motion of the particles (top panels) and the propagation direction of signaling activity (bottom panels), respectively. Credit: Nature Communications (2022). DOI: 10.1038/s41467-022-34484-2″ width=”800″ height=”477″>
Schematics of the agent-based model for communicating active matter and summary of collective dynamic states. a Polar self-propelled particles undergo alignment in binary collisions. b A diffusible signal (green) aligns the cells’ orientation vectors. c Schematic of a Schmitt trigger with variable threshold cth. d Temporal response c(t) of the agents’ signaling system with characteristic timescale 𝜏. en Representative collective dynamic states in the agent-based (ei) and the hydrodynamic model (jn). The snapshots illustrate aggregation and vortex formation following initial ring formation (e, j), where remnant spiral wave arms induce chemical wave propagation in the ring after the spiral core vanished due to depletion in its center (‘whispering gallery’-modes); active droplets (f, k), with a collective response to external stimuli; a collective stream (g, l), where agents propagate toward the source of communication waves; a large vortex with a spiral wave (h, m), and a polar band (i, n). White scale bars indicate a length of 10 units. Colors indicate the polar orientation of particles (top panels) and the chemical concentration c (bottom panels). White and yellow arrows illustrate the direction of motion of the particles (top panels) and the propagation direction of signaling activity (bottom panels), respectively. Credit: Nature Communications (2022). DOI: 10.1038/s41467-022-34484-2

Amoebae are single-cell organisms. By means of self-organization, they can form complex structures—and do this purely through local interactions: If they have a lot of food, they disperse evenly through a culture medium. But if food becomes scarce, they emit the messenger known as cyclic adenosine monophosphate (cAMP). This chemical signal induces amoebae to gather in one place and form a multicellular aggregation. The result is a fruiting body.

“The phenomenon is well known,” says Prof. Erwin Frey from LMU’s Faculty of Physics. “Before now, however, no research group has investigated how , at a general level, affects the aggregation of systems of agents when individual agents—in our case, —are self-propelled.” More knowledge about these mechanisms would also be interesting, adds Frey, as regards translating them to artificial technical systems.

Together with other researchers, Frey describes in Nature Communications how active systems that process information in their environment can be used—for technological or biological applications. It is not about understanding all details of the communication between individual agents, but about the specific structures formed through . This applies to amoebae—and also to certain kinds of robots. The research was undertaken in collaboration with Prof. Igor Aronson during his stay at LMU as a Humboldt Research Award winner.

From biological mechanism to technological application

The term “active matter” refers to biological or technical systems from which larger structures are formed by means of self-organization. Such processes are based upon exclusively local interactions between identical, self-propelled units, such as amoebae or indeed robots.

Inspired by , Frey and his co-authors propose a new model in which self-propelled agents communicate with each other. These agents recognize chemical, biological, or physical signals at a local level and make individual decisions using their internal machinery that result in collective self-organization. This orientation gives rise to larger structures, which can span multiple length scales.

The of communicating active matter forms the basis of the study. Local decisions in response to a signal and the transmission of information, lead to collectively controlled self-organization.

Frey sees a possible application of the new model in soft robots—which is to say, robots that are made of soft materials. Such robots are suitable, for example, for performing tasks in human bodies. They can communicate with other soft robots via for purposes such as administering drugs at specific sites in the body. The new model can help nanotechnologists design such systems by describing the collective properties of robot swarms.

“It’s sufficient to roughly understand how individual agents communicate with each other; self-organization takes care of the rest,” says Frey. “This is a specifically in robotics, where researchers are attempting to do precisely the opposite—they want to obtain extremely high levels of control.” But that does not always succeed.

“Our proposal, by contrast, is to exploit the capacity for self-organization.”

More information:
Alexander Ziepke et al, Multi-scale organization in communicating active matter, Nature Communications (2022). DOI: 10.1038/s41467-022-34484-2

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Peyman Taeidi

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