Swimming microorganisms often have to propel in complex, non-Newtonian
fluids. We carry out experiments with self-propelling helical swimmers driven
by an externally rotating magnetic field in shear-thinning, inelastic fluids.
Similarly to swimming in a Newtonian fluid, we obtain for each fluid a
locomotion speed which scales linearly with the rotation frequency of the
swimmer, but with a prefactor which depends on the power index of the fluid.
The fluid is seen to always increase the swimming speed of the helix, up to 50%
faster and thus the strongest of such type reported to date. The maximum
relative increase for a fluid power index of around 0.6. Using simple scalings,
we argue that the speed increase is not due to the local decrease of the flow
viscosity around the helical filament but hypothesise instead that it
originates from confinement-like effect due to viscosity stratification around
the swimmer
Viscoelastic fluids impact the locomotion of swimming microorganisms and can be harnessed to devise new types of self-propelling devices. Here we report on experiments demonstrating the use of normal stress differences for propulsion. Rigid dumbbells are rotated by an external magnetic field along their axis of symmetry in a Boger fluid. When the dumbbell is asymmetric (snowman geometry), non-Newtonian normal stress differences lead to net propulsion in the direction of the smaller sphere. The use of a simple model allows to rationalise the experimental results and to predict the dependence of the snowman swimming speed on the size ratio between the two spheres.
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Summary
In this paper, we study a supercapacitor model represented by an equivalent RC circuit considering five different types of derivatives: Caputo, Caputo‐Fabrizio, and Atangana‐Baleanu fractional derivatives and the conformable and integer‐order derivatives. A set of experimental data from six commercial supercapacitors are used to estimate the parameter values for each derivative model by applying interior point optimization. The results show that the most accurate approach is achieved with the conformable derivative followed by the Caputo fractional derivative.
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