Experimental observation of pinned solitons in a flowing dusty plasma

TL;DR

This study reports the first experimental observation of pinned solitons in a flowing dusty plasma, demonstrating their formation, characteristics, and dependence on flow velocity, and comparing results with a theoretical model.

Contribution

First experimental demonstration of pinned solitons in a dusty plasma flowing over a charged obstacle, validating numerical predictions.

Findings

Pinned solitons observed in laboratory dusty plasma.

Soliton shape changes from single to multi-humped with increased flow velocity.

Amplitude of solitons increases with flow velocity.

Abstract

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 {\Pi} 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 multi-humped 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.