The Role of Particle Diffusion in the Lower Transition Region: Revised Interpretation of Emission Measures

Author(s):  
Eugene H. Avrett ◽  
Juan M. Fontenla
2021 ◽  
Vol 922 (1) ◽  
pp. 48
Author(s):  
H. Saleem ◽  
Shaukat Ali Shan ◽  
A. Rehman

Abstract Theoretical models are presented to show that expansion of plasma in the radial direction from a denser solar surface to a rarefied upper atmosphere with short-scale inhomogeneous field-aligned flows and currents in the form of thin threads itself is an important source of electrostatic instabilities. Multifluid theory shows that the shear flow–driven purely growing electric fields appear in the transition region. On the other hand, plasma kinetic theory predicts that the short-scale current sheets (or filaments) produce current-driven electrostatic ion acoustic (CDEIA) waves in the hydrogen plasma of the transition region that damp out in the system through wave–particle interactions and increase the temperature. Similar processes take place in the solar corona and act positively for increasing the temperature further and maintaining it. The shear flow–driven instabilities and CDEIA waves have short perpendicular wavelengths of the order of 1 m and low frequencies of the order of 1 or several Hz when the ions’ shear flow scale length is considered to be of the order of 1 km. It is pointed out that the purely growing fluid instabilities turn into oscillatory instabilities and the growth rates of kinetic CDEIA wave instabilities are reduced when the dynamics of 10% helium ions is taken into account along with 90% hydrogen ions. Therefore, the role of helium ions should not be ignored in the study of wave dynamics in solar plasma.


1991 ◽  
Vol 99 (4) ◽  
pp. 731-740
Author(s):  
JONATHAN W. JARVIK ◽  
JOSEPH P. SUHAN

Thin-section electron microscopy of the Chlamydomonas reinhardtii mutant vfl-2 revealed striking defects in the transition region between basal body and flagellum. In place of the highly organized transition cylinders and stellate fibers characteristic of wild type, variable quantities of poorly organized electron-dense material were present. In many cases the transition region was penetrated by central pair microtubules that passed from the axoneme into the basal body. On the basis of these observations we propose that an important function of the structures present in the normal transition region is to physically exclude the central pair microtubules from the basal body. The transition region is the site of flagellar autotomy – the process by which doublet microtubules are severed and flagella are released from the cell. It has been claimed that autotomy is caused by contraction of the centrin-containing stellate fibers, resulting in the mechanical severing of the doublet microtubules and a concomitant reduction of the diameter of the axoneme adjacent to the abscission point. Our observations do not support this claim in that vfl-2 cells, which lack organized stellate fibers, display effective autotomy unaccompanied by detectable narrowing of the axoneme.


2001 ◽  
Vol 563 (1) ◽  
pp. 374-380 ◽  
Author(s):  
A. Vourlidas ◽  
J. A. Klimchuk ◽  
C. M. Korendyke ◽  
T. D. Tarbell ◽  
B. N. Handy

2015 ◽  
Vol 799 (1) ◽  
pp. L12 ◽  
Author(s):  
B. De Pontieu ◽  
S. McIntosh ◽  
J. Martinez-Sykora ◽  
H. Peter ◽  
T. M. D. Pereira

2017 ◽  
Vol 139 (11) ◽  
Author(s):  
Collin T. Burkhart ◽  
Kara L. Maki ◽  
Michael J. Schertzer

This investigation experimentally examines the role of interface capture on the transport and deposition of colloidal material in evaporating droplets. It finds that deposition patterns cannot be characterized by the ratio of interface velocity to particle diffusion rate alone when the two effects are of the same order. Instead, the ratio of radial velocity to particle diffusion rate should also be considered. Ring depositions are formed when the ratio of radial velocity to the particle diffusion rate is greater than the ratio of interface velocity to diffusion. Conversely, uniform depositions occur when the ratio of radial velocity to diffusion is smaller than the ratio of interface velocity to diffusion. Transitional depositions with a ring structure and nonuniform central deposition are observed when these ratios are similar in magnitude. Since both ratios are scaled by diffusion rate, it is possible to characterize the depositions here using a ratio of interface velocity to radial velocity. Uniform patterns form when interface velocity is greater than radial velocity and ring patterns form when radial velocity is larger. However, Marangoni effects are small and Derjaguin, Landau, Verwey, and Overbeek (DLVO) forces repel particles from the surface in these cases. Further research is required to determine if these conclusions can be extended or modified to describe deposition patterns when particles are subjected to appreciable Marangoni recirculation and attractive DLVO forces.


1997 ◽  
Vol 490 (2) ◽  
pp. L195-L198 ◽  
Author(s):  
Philip Judge ◽  
Mats Carlsson ◽  
Klaus Wilhelm

The kinetics of anodic oxygen evolution have been studied on Pd, Au and Pd + Au alloys in ultra-pure sulphuric acid and potassium hydroxide solutions and mechanisms of the processes involved are proposed. The role of barrier-layer films in determining the kinetic behaviour is demonstrated and supported by self-consistent interpretations of the Tafel slopes and the e.m.f. decay behaviour observed on open-circuit. Transient effects, characteristic of barrier-layer films, are observed when changes of the polarization current are made. At Au, and the gold-rich alloys in alkaline solution, a transition region in the currentpotential relation is observed which probably corresponds to a limiting high coverage of the electrochemically active surface with adsorbed reaction intermediates. The transition region corresponds to an onset of passive behaviour. In acid solutions, only the lower Tafel region is observed which has the same Tafel constants b and i 0 as those for the lower Tafel line in alkaline solutions indicating that the discharge process involves water rather than OH - ions, irrespective of pH. The relation of exchange currents to composition of the alloys is considered.


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