Official web site of Takeuchi Lab, Univ. Tokyo

Actively propelled objects span a broad variety of actual realizations, from self-propelled bacteria, via vibrated hoppers, to animals and humans. Besides being equipped with a propulsion mechanism, all of these entities share a common feature. There is, ad hoc, no outside mechanism that rigidly dictates their propulsion direction. Instead, they have the freedom to select this direction, even if only through rotational stochastic processes. We here address different scenarios of corresponding systems. First, we address chiral objects that show bent trajectories, move in discrete steps, and tend to head towards a remote target, which leads to pronounced nonlinear dynamics [1]. Next, we consider self-propelling units organized in regular lattice structures, which leads to the onset of collective motion beyond a threshold active drive, while chirality can make collective motion break down [2]. Third, we address nematic actively propelled entities that stochastically reverse their propagation direction, where a formal analogy to a basic quantum mechanical problem is revealed during the analysis of the associated statistics [3]. Overall, we hope to stimulate experimental realizations and investigations of such systems.

[1] A. M. Menzel, Phys. Rev. E 106, 064603 (2022).
[2] Z.-F. Huang, A. M. Menzel, H. Löwen, Phys. Rev. Lett. 125, 218002 (2020).
[3] A. M. Menzel, J. Chem. Phys. 157, 011102 (2022) – Featured Communication.

Through the magic of ‘active matter,’ which converts chemical energy into mechanical work to drive emergent properties, biology solves a myriad of seemingly impossible physical challenges. I will present my lab's efforts to develop new fluid mechanics models to direct the flow of matter enabled by the use of “active” molecules found within living systems. We design 2D composite materials with tunable inclusions of lipid domains embedded within an active elastic network. These lipid inclusions enable exquisite control over the phase separation and material properties (like failure resistance) of 2D composite materials. If time permits, I will also present our recent work on model predictive control and learning of many-body colloidal interactions driven by active and hydrodynamic forces.

Chiral active fluids with broken time-reversal and parity symmetries are prevalent at various scales in nonequilibrium systems, ranging from electron fluids to biological and geophysical flows. In such fluids, a peculiar transport coefficient called odd viscosity arises. This viscosity, which does not contribute to the fluid energy dissipation, leads to novel dynamics, such as nonreciprocal (transverse) transports, free-surface dynamics, or chiral edge currents characterized by topological protection, akin to quantum Hall systems. The lack of time-reversal symmetry leads to an asymmetric response and, thus, to an asymmetric mobility tensor. This suggests that the Lorentz reciprocal theorem, a powerful and versatile principle in low-Reynolds-number fluid dynamics, is violated in chiral active systems.

In this talk, I will present my recent work on the dynamics of microswimmers in chiral active fluids. First, we analyze the behavior of a single linear swimmer in a 2D compressible fluid with odd viscosity [1]. It is found that a microswimmer undergoes circular trajectories whose radius is set by the inverse of the odd viscosity. Moreover, a pair of swimmers exhibits a wealth of two-body dynamics that depends on the initial relative orientation angles as well as on the propulsion mechanism adopted by each swimmer. We then discuss the generalization of the Lorentz reciprocal theorem in fluids with odd viscosity [2]. To demonstrate its applicability, we use the theorem to determine the swimming velocity of two categories of microswimmers in a Stokes flow with odd viscosity. We show that a surface-driven microswimmer, which we call a “twister”, can exhibit vertical dynamics induced by nonreciprocal responses due to the odd viscosity.

[1] Y. Hosaka, R. Golestanian, and A. Daddi-Moussa-Ider, New J. Phys. 25, 083046 (2023).
[2] Y. Hosaka, R. Golestanian, and A. Vilfan, Phys. Rev. Lett. 131, 178303 (2023).

The research on swimming micro-organisms and the design of swimming micro-robots is at the crossing between many fields, from theoretical fluid dynamics to biomechanics and medical applications. At the microscopic scale, locomotion through a fluid follows specific laws, due to the predominance of the viscous effects . One of the fundamental principles of locomotion in this regime, famously termed as the scallop theorem, states that non-reciprocal deformation is required to produce a net motion. I would like to elaborate on this simple concept of non-reciprocity and its many forms in microswimming studies, by presenting some of my works on modelling and control of microswimmers.

First, I will talk about our recent research on modelling the internal activity of living matter by non-reciprocal interactions. I will present the framework of ‘odd elasticity’ on which this analysis is based, and how it successfully applies to microscale locomotion, illustrating this on flagellar swimmer models.

Then, I will discuss controllability of microswimming models, which aims at determining whether a given swimmer may or may not reach a given target. To mathematically characterize controllability, one relies on Lie brackets, which are, in this context, a sort of measure of the non-reciprocity of a sequence of moves. Using these, we determined conditions to ensure controllability of magnetically-driven elastic swimmers.

Artificial micro-swimmers have recently become a central field of research in soft-matter. A very promising and original type of swimmer developed in our team, consists in pure water droplet swimming in an oil phase containing micelles of surfactant. The droplet’s activity comes from the formation of swollen micelles at its interface which induces Marangoni stresses and then motion of the droplets.

We investigate experimentally the behavior of such self-propelled water-in-oil droplets, confined in capillaries of different square and circular cross-sections. Stretched circular capillaries have been used to explore even stronger confinement. Within the most constricted regions, droplets elongate very strongly. These extremely long droplets reveal unexpected behaviors during their motion, in particular regarding their stability.

We build up on the Bretherthon formalism to rationalize this new kind of self-motion of confined droplets in a tube, not anymore driven by pressure or flow rate but rather by locally-induced interfacial stresses.

We are active matter. From molecular motors noisily walking in living cells to the mesmerizing swirls in a starling flock, systems driven far from equilibrium by a sustained flux of energy through its constituents routinely exhibit stunning emergent phenomena that pose fundamental challenges to our understanding of the natural world. Much is known about what patterns and dynamics active systems can exhibit, but the inverse problem of controlling active matter is less explored. I will discuss our current work on searching for design principles to control localized excitations, drops etc., in active materials using ideas from control theory, optimal transport and symmetry-based approaches. I will conclude by highlighting future directions for embodying function, programmable response and computation in biological and synthetic active systems.

The rapid and universal emergence of antibiotic resistance in bacterial populations poses a worldwide health care challenge, but also serves as a paradigm of microbial evolution. In many cases the evolution of high levels of resistance requires multiple mutational steps, which can be conceptualized as pathways in the microbial fitness landscape. The talk will use the evolution of a specific antibiotic resistance enzyme to explain the theoretical framework within which this process can be described, and report on recent results on the predictability of pathways that were obtained in a collaborative effort between experiment and theory.

Obligately hydrocarbonoclastic bacteria (OHCB) are cosmopolitan marine bacteria that can survive by consuming hydrocarbons as a sole energy and carbon source. In the ocean, these bacteria are typically found at very low densities but bloom to become the dominant bacteria at the site of oil spills. These organisms have likely evolved to directly utilize the abundant hydrocarbons in the marine environment as part of the cryptic carbon cycle and around natural oil-seeps on the sea floor. They are thought to degrade a significant amount of the worldwide spilled oil, which is why they have been organisms of interest for use as agents of bioremediation.

Alcanivorax borkumensis was the first OHCB sequenced in the mid-2000s. Like most bacteria, it is thought to transition between planktonic and biofilm states. Biofilms are 3D communities of densely packed bacteria encased in a self-secreted matrix of extracellular polymeric substances (EPS) that both protect and help the community remain attached to a surface. However, unlike most environmental bacteria, which typically absorb their carbon (and energy) directly from nutrients in the surrounding water, A. borkumensis biofilms must form on the oil-water interface. Although formation of a biofilm at fluid-fluid interface is not unique and, in some ways, shares some similarity to pellicle formation at the air-liquid interface, the similarities diverge there. Biofilms can generate gradients in the nutrients between the internal and external environments. In the case of an A. borkumensis biofilm surrounding an oil droplet, only the cells at the interface have access to the carbon/energy, while the outward facing cells have access to micronutrients. It is not clear how the obvious nutrient gradients and the fluid interface affects A. borkumensis biofilm formation.

Due to the difficulty in tracking individual droplets over time, biofilm dynamics of this interesting organism have largely been conducted though bulk methods. From an applied ecology perspective, clarifying the microscopic mechanisms of biofilm formation for this and similar OHCB organism may reveal features to be exploited in the management of oil spills in the natural environment. From the active-matter physics perspective, the behavior of self-driven layer at a phase-separated interface of may reveal new physics.

We introduce a microfluidic platform that can trap and store oil microdroplets for weeks. This platform greatly facilitates imaging and analysis of biofilm formation at the oil-water interface. We demonstrate unresolved biofilm dynamics by A. borkumensis, showing its ability to rapidly shred oil drops. We analyze various physical aspects of this organism and correlate them to its ability to align and cooperate at the interface to drive a rapid and large-scale remodeling of the interface. This remodeling appears to be the most egalitarian and efficient distribution of resources.

Wind is a variable energy source whose fluctuations threaten electrical grid stability and complicate dynamical load balancing. The power generated by a wind turbine fluctuates due to the variable wind speed that blows past the turbine. Indeed, the spectrum of wind power fluctuations is widely believed to reflect the Kolmogorov spectrum of atmospheric turbulence; both vary with frequency $f$ as $f^{-5/3}$. This variability decreases when aggregate power fluctuations from geographically distributed wind plants are averaged at the grid via a mechanism known as geographic smoothing. Neither the $f^{-5/3}$ wind power fluctuation spectrum nor the mechanism of geographic smoothing are understood. In this talk, I will chart out the non-equilibrium character of wind power fluctuations, and explain the wind power fluctuation spectrum from the turbine through the grid scales. The $f^{-5/3}$ wind power fluctuation spectrum results from the largest length scales of atmospheric turbulence of order 200 km influencing the small scales where individual turbines operate. This long-range influence correlates outputs from geographically distributed wind plants over a range of frequencies that decreases with increasing inter-farm distance. Consequently, aggregate grid-scale power fluctuations remain correlated, and are smoothed until they reach a limiting $f^{-7/3}$ spectrum, which is confirmed with field data. I will discuss engineering and policy implications of these results and chart out the future directions I intend to pursue in the broad area of energy research.

Microbial attachment to material surfaces is a complex phenomenon involving a complexity of electrostatic, biochemical and physical mechanisms. Despite the major problems associated with medical device-associated infection, infectious disease transmission within healthcare environments, and hospital acquired infections (HAIs), many aspects of microbial surface attachment are not well understood. Rates of HAI remain relatively high, and there is significant concern about the effects of antibiotic resistance, globally. Most approaches to antimicrobial material design still usually just rely on the release of biocidal chemical species (such as Ag ions).
We are interested in how material surface design - factors such as surface chemistry, biochemical functionalization, nano- and microtopography, and wettability – can influence microbial surface attachment and biofilm development. In particular, our work has focussed on strategies to disrupt the early stages of microbial surface attachment in antimicrobial material design, as an alternative to biocidal chemistries. In the context of medical device-associated infections, there is an important advantage to keeping bacteria in a planktonic (swimming) state, as they are much more vulnerable than in a biofilm community.
This talk will summarize several experimental research projects that explore aspects of bacterial cell attachment to material surfaces; (1) The immobilization of glycoside hydrolase enzymes to disrupt pseudomonas aeruginosa biofilms; (2) Nanotopographies in wetting contact (the ‘cicada effect’) ; (3) Nano- and microtopographies in non-wetting (superhydrophobic) contact ; (4) Microbial attraction to topographical surface defects ; and (5) ‘Slippery’ surfaces (SLIPS) in the design of non-specific, non-fouling material. Overall, the application of these various materials chemistry design tools has enabled us to learn something about microbial behaviour, through material surface design.