Experimental direct spatial damping identification by the Stabilised Layers Method

2018 ◽  
Vol 437 ◽  
pp. 325-339 ◽  
Author(s):  
Domenico Lisitano ◽  
Elvio Bonisoli ◽  
John E. Mottershead
Keyword(s):  
1975 ◽  
Vol 38 (6) ◽  
pp. 1793-1793 ◽  
Author(s):  
Yasuyoshi Yasaka ◽  
Yasuhide Sudoh ◽  
Ryohei Itatani

2015 ◽  
Vol 581 ◽  
pp. A130 ◽  
Author(s):  
Ming-Zhe Guo ◽  
Shao-Xia Chen ◽  
Bo Li ◽  
Li-Dong Xia ◽  
Hui Yu
Keyword(s):  

2021 ◽  
Vol 8 ◽  
Author(s):  
Pallabi Pathak

The effect of enhanced Landau damping on the evolution of ion acoustic Peregrine soliton in multicomponent plasma with negative ions has been investigated. The experiment is performed in a multidipole double plasma device. To enhance the ion Landau damping, the temperature of the ions is increased by applying a continuous sinusoidal signal of frequency close to the ion plasma frequency ∼1 MHz to the separation grid. The spatial damping rate of the ion acoustic wave is measured by interferometry. The damping rate of ion acoustic wave increases with the increase in voltage of the applied signal. At a higher damping rate, the Peregrine soliton ceases to show its characteristics leaving behind a continuous envelope.


2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Muhammad Sarfraz ◽  
Gohar Abbas ◽  
Hashim Farooq ◽  
I. Zeba

Abstract A sequence of in situ measurements points the presence of non-thermal species in the profile of particle distributions. This study highlights the role of such energetic electrons on the wave-spectrum. Using Vlasov–Maxwell’s model, the dispersion relations of the parallel propagating modes along with the space scale of damping are discussed using non-relativistic bi-Maxwellian and bi-Kappa distribution functions under the weak field approximation, i.e., ω − k . v > Ω 0 $\left\vert \omega -\mathbf{k}.\mathbf{v}\right\vert { >}{{\Omega}}_{0}$ . Power series and asymptotic expansions of plasma dispersion functions are performed to derive the modes and spatial damping of waves, respectively. The role of these highly energetic electrons is illustrated on real frequency and anomalous damping of R and L-modes which is in fact controlled by the parameter κ in the dispersion. Further, we uncovered the effect of external magnetic field and thermal anisotropy on such spatial attenuation. In global perspective of the kinetic model, it may be another step.


2010 ◽  
Vol 515 ◽  
pp. A80 ◽  
Author(s):  
M. Carbonell ◽  
P. Forteza ◽  
R. Oliver ◽  
J. L. Ballester

1970 ◽  
Vol 13 (10) ◽  
pp. 2546 ◽  
Author(s):  
A. Lee

1987 ◽  
Vol 30 (1) ◽  
pp. 115 ◽  
Author(s):  
Amnon Fruchtman ◽  
Kurt Riedel ◽  
H. Weitzner ◽  
D. B. Batchelor

2012 ◽  
Vol 69 (12) ◽  
pp. 3715-3731 ◽  
Author(s):  
Dustin F. P. Grogan ◽  
Terrence R. Nathan ◽  
Robert S. Echols ◽  
Eugene C. Cordero

An equatorial β-plane model of the tropical stratosphere is used to examine the effects of ozone on Kelvin, Rossby–gravity, equatorial Rossby, inertia–gravity, and smaller-scale gravity waves. The model is composed of coupled equations for wind, temperature, and ozone volume mixing ratio, which are linearized about a zonally averaged background state. Using the Wentzel–Kramers–Brillouin (WKB) formalism, equations are obtained for the vertical spatial scale, spatial damping rate, and amplitude of the waves. These equations yield an analytical expression for the ozone-modified wave driving of the zonal-mean circulation. The expression for the wave driving provides an efficient parameterization that can be implemented into models that are unable to spontaneously generate the ozone-modified, convectively coupled waves that drive the quasi-biennial and semiannual oscillations of the tropical stratosphere. The effects of ozone on the wave driving, which are strongly modulated by the Doppler-shifted frequency, are maximized in the upper stratosphere, where ozone photochemistry and vertical ozone advection combine to augment Newtonian cooling. The ozone causes a contraction in spatial scale and an increase in the spatial damping rate. In the midstratosphere to lower mesosphere, the ozone-induced increase in wave driving is about 10%–30% for all wave types, but it can be as large as about 80% over narrow altitude regions and for specific wave types. In the dynamically controlled lower stratosphere, vertical ozone advection dominates over meridional ozone advection and opposes Newtonian cooling, causing, on average, a 10%–15% reduction in the damping rate.


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