light particle
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2022 ◽  
Author(s):  
Andres M. Castillo ◽  
Prabhat Kumar ◽  
Kentaro Hara

2021 ◽  
Vol 11 (15) ◽  
pp. 7113
Author(s):  
Sensen Yang ◽  
Chengxu Tu ◽  
Minglu Dai ◽  
Xianfu Ge ◽  
Rongjun Xu ◽  
...  

Particle sedimentation has widely existed in nature and engineering fields, and most carrier fluids are non-Newtonian. Recently, the manipulation of a settling particle in liquid has been a topic of high interest to those involved in engineered processes such as composite materials, pharmaceutical manufacture, chemistry and the petroleum industry. Compared with Newtonian fluid, the viscosity of non-Newtonian fluid is closely related to the shear rate, leading to a single settling particle having different dynamic behaviors. In this article, the trajectories and velocities of two side-by-side particles of different densities (heavy and light) settling in a shear-thinning fluid with viscoelastic property were studied, as well as that for the corresponding single settling particle. Regardless of the difference in the particle density, the results show the two-way coupling interaction between the two side-by-side settling particles. As opposed to a single settling particle, the wake of the heavier particle can clearly attract or rebound the light particle due to the shear-thinning or viscoelastic property of the fluid. Regarding the trajectories of the light particle, three basic path types were found: (i) the light particle is first attracted and then repelled by the wake of the heavy one; (ii) the light particle approaches and then largely traces within the path of the heavy one in the limited field of view; (iii) the light particle is first slightly shifted away from its original position and then returns to this initial position. In addition to this, due to the existence of a corridor of reduced viscosity and negative wake generated by the viscoelastic property, the settling velocity of a light particle can exceed the terminal velocity of a single particle of the same density. On the other hand, the sedimentation of the light particle can induce the distinguishable transverse migration of the heavy one.


2021 ◽  
Vol 8 (1) ◽  
Author(s):  
Clemens Albrecht ◽  
Serena Barbanotti ◽  
Heiko Hintz ◽  
Kai Jensch ◽  
Ronald Klos ◽  
...  

2021 ◽  
Author(s):  
Yang Liu ◽  
Lixing Zhou

Abstract Turbulence modulations by particles of swirling gas-particle two-phase flow the axisymmetric chamber is investigated. To fully consider the preferential concentrations and anisotropic dispersions of particle, a second-order moment model coupling particle-particle collision model was improved based on the Eulerian-Eulerian two-fluid approach and the kinetic theory of granular flow. Proposed model, algorithm and in-house codes are validated and they are in good agreement with the experiment. Effects of ultralight expanded graphite and heavy Copper particles with large spans of Stokes number on gas velocity and fluctuations, Reynolds shear stress and tensor invariants, turbulence kinetic energy, and vortices structures are numerically simulated. Results show turbulent modulation exhibits strongly anisotropic characteristics and keeps in close relationship with flow structure. The disturbances of modulations, the alternations of vortex evolution are enforced by heavy-large particle with higher Stokes numbers. Preferential accumulations of light particle at shear stress regions in low vortices are weaker than those of heavy particle. For axial turbulence modulations, heavy particle plays the primary role on inhibition action due to larger inertia and light particle contributes to enhancement effect due to excellent followability.


Nanoscale ◽  
2021 ◽  
Author(s):  
Cheng Lv ◽  
Jian Ao ◽  
Ji Wang ◽  
Man Tang ◽  
An-An Liu ◽  
...  

Targeted cancer therapy has aroused broad interests of researchers due to its accuracy in specific tumor targeting and few side effects on normal cells. In the last decades, oncolytic viral...


2020 ◽  
Vol 80 (12) ◽  
Author(s):  
Chun-Hao Lee ◽  
Chrisna Setyo Nugroho ◽  
Martin Spinrath

AbstractWe present prospects for discovering dark matter scattering in gravitational wave detectors. The focus of this work is on light, particle dark matter with masses below 1 $$\hbox {GeV}/\text {c}^{2}$$ GeV / c 2 . We investigate how a potential signal compares to typical backgrounds like thermal and quantum noise, first in a simple toy model and then using KAGRA as a realistic example. That shows that for a discovery much lighter and cooler mirrors would be needed. We also give some brief comments on space-based experiments and future atomic interferometers.


2020 ◽  
Vol 188 ◽  
pp. 169-173 ◽  
Author(s):  
L.T. Belkacemi ◽  
E. Meslin ◽  
B. Décamps ◽  
J.-P. Crocombette ◽  
O. Tissot ◽  
...  

2020 ◽  
Vol 2020 (11) ◽  
Author(s):  
Eung Jin Chun ◽  
Tanmoy Mondal

Abstract We consider the two Higgs doublet model (2HDM) along with a generation of vector-like lepton doublet and singlet to explain the observed discrepancies in the electron and muon anomalous magnetic moments. The type-X (lepton-specific) 2HDM can allow a light pseudo-scalar which is known to explain the muon anomalous magnetic moment at two-loop. Such a light particle induces a sizable negative contribution to the electron anomalous magnetic moment at one-loop in the presence of vector-like leptons evading all the experimental constraints.


2020 ◽  
Vol 102 (5) ◽  
Author(s):  
Yi Liao ◽  
Hao-Lin Wang ◽  
Chang-Yuan Yao ◽  
Jian Zhang
Keyword(s):  

Author(s):  
A. M. Baldini ◽  
F. Berg ◽  
M. Biasotti ◽  
G. Boca ◽  
P. W. Cattaneo ◽  
...  

AbstractWe present the first direct search for lepton flavour violating muon decay mediated by a new light particle X, $$\upmu ^+ \rightarrow \mathrm {e}^+\mathrm {X}, \mathrm {X} \rightarrow \upgamma \upgamma \ $$ μ + → e + X , X → γ γ . This search uses a dataset resulting from $$7.5\times 10^{14}$$ 7.5 × 10 14 stopped muons collected by the MEG experiment at the Paul Scherrer Institut in the period 2009–2013. No significant excess is found in the mass region 20–45 MeV/c$$^2$$ 2 for lifetimes below 40 ps, and we set the most stringent branching ratio upper limits in the mass region of 20–40 MeV/c$$^2$$ 2 , down to $${\mathcal {O}}(10^{-11})$$ O ( 10 - 11 ) at 90% confidence level.


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