A solvable model of axisymmetric and non-axisymmetric droplet bouncing
Soft Matter Royal Society of Chemistry 13:5 (2017) 985-994
Abstract:
We introduce a solvable Lagrangian model for droplet bouncing. The model predicts that, for an axisymmetric drop, the contact time decreases to a constant value with increasing Weber number, in qualitative agreement with experiments, because the system is well approximated as a simple harmonic oscillator. We introduce asymmetries in the velocity, initial droplet shape, and contact line drag acting on the droplet and show that asymmetry can often lead to a reduced contact time and lift-off in an elongated shape. The model allows us to explain the mechanisms behind non-axisymmetric bouncing in terms of surface tension forces. Once the drop has an elliptical footprint the surface tension force acting on the longer sides is greater. Therefore the shorter axis retracts faster and, due to the incompressibility constraints, pumps fluid along the more extended droplet axis. This leads to a positive feedback, allowing the drop to jump in an elongated configuration, and more quickly.A solvable model of axisymmetric and non-axisymmetric droplet bouncing
(2017)
Coarse-Grained Modeling of RNA for Biology and Nanotechnology
BIOPHYSICAL JOURNAL 112:3 (2017) 369A-369A
Approximate light cone effects in a nonrelativistic quantum field theory after a local quench
Physical Review B American Physical Society (APS) 95:7 (2017) 075153
On truncated generalized Gibbs ensembles in the Ising field theory
Journal of Statistical Mechanics: Theory and Experiment IOP Publishing 2017:1 (2017) 013103
Abstract:
We discuss the implementation of two dierent truncated Generalized Gibbs Ensembles (GGE) describing the stationary state after a mass quench process in the Ising Field Theory. One truncated GGE is based on the semi-local charges of the model, the other on regularized versions of its ultra-local charges. We test the efficiency of the two different ensembles by comparing their predictions for the stationary state values of the single-particle Green's function G(x) = ⟨Ψ†(x)Ψ(0)⟩ of the complex fermion field Ψ(x). We find that both truncated GGEs are able to recover G(x), but for a given number of charges the semi-local version performs better.