2020/12/18 by Garima Arora, P. Bandyopadhyay, P Bandyopadhyay +4 · 2 citations
Earth and Planetary Sciences · Physics and Astronomy · #Atomic physics #Dust and Plasma Wave Phenomena #Dusty plasma #High-pressure geophysics and materials #Ionosphere and magnetosphere dynamics #Materials science #Mechanics #Physics #Plasma #Quantum mechanics #physics.plasm-ph
paper · pdf · doi:10.1103/physreve.103.013201
published as Phys. Rev. E 103, 013201 (2021) · The manuscript contains nine pages and ten figures
arxiv created 2020/12/18 · openalex publication_date 2021/01/05 · arxiv updated 2021/01/13 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
Pinned solitons are a special class of nonlinear solutions created by a supersonically moving object in a fluid. They move with the same velocity as the moving object and thereby remain pinned to the object. A well-known hydrodynamical phenomenon, they have been shown to exist in numerical simulation studies but to date have not been observed experimentally in a plasma. In this paper we report the first experimental excitation of pinned solitons in a dusty (complex) plasma flowing over a charged obstacle. The experiments are performed in a Π shaped dusty plasma experimental (DPEx) device in which a dusty plasma is created in the background of a DC glow discharge Ar plasma using micron sized kaolin dust particles. A biased copper wire creates a potential structure that acts as a stationary charged object over which the dust fluid is made to flow at a highly supersonic speed. Under appropriate conditions nonlinear stationary structures are observed in the laboratory frame that correspond to pinned structures moving with the speed of the obstacle in the frame of the moving fluid. A systematic study is made of the propagation characteristics of these solitons by carefully tuning the flow velocity of the dust fluid by changing the height of the potential structure. It is found that the nature of the pinned solitons changes from a single-humped one to a multihumped one and their amplitudes increase with an increase of the flow velocity of the dust fluid. The experimental findings are then qualitatively compared with the numerical solutions of a model forced Korteweg de Vries (fKdV) equation.