scholarly journals Charge–mass ratio bound and optimization in the Parikh–Wilczek tunneling model of Hawking radiation

2014 ◽  
Vol 731 ◽  
pp. 307-310 ◽  
Author(s):  
Kyung Kiu Kim ◽  
Wen-Yu Wen
Keyword(s):  
Hawking Radiation ◽  
Mass Ratio ◽  
Tunneling Model ◽  
Charge Mass

scholarly journals Hawking radiation as irreversible tunneling through self-interaction

2014 ◽  
Vol 29 (13) ◽  
pp. 1450065
Author(s):  
Wen-Yu Wen
Keyword(s):  
Black Holes ◽  
Upper Bound ◽  
Hawking Radiation ◽  
Irreversible Process ◽  
The Self ◽  
Mass Ratio ◽  
Tunneling Model ◽  
Charge Mass ◽  
Self Force

In this paper, we study the self-force in the Parikh–Wilczek tunneling model of Hawking radiation for Reissner–Nordström (RN) black holes. We conclude that the repulsive self-force speeds up the emission and the radiation becomes an irreversible process. We also find an upper bound of charge–mass ratio for emitted particles.

A 16-parts-per-trillion measurement of the antiproton-to-proton charge–mass ratio

Nature ◽  
2022 ◽  
Vol 601 (7891) ◽  
pp. 53-57
Author(s):  
M. J. Borchert ◽  
J. A. Devlin ◽  
S. R. Erlewein ◽  
M. Fleck ◽  
J. A. Harrington ◽  
...  
Keyword(s):  
Mass Ratio ◽  
Charge Mass ◽  
Proton Charge

Particle Segregation at Contact Lines of Evaporating Colloidal Drops: Influence of the Substrate Wettability and Particle Charge–Mass Ratio

Langmuir ◽  
2015 ◽  
Vol 31 (24) ◽  
pp. 6632-6638 ◽  
Author(s):  
Diego Noguera-Marín ◽  
Carmen L. Moraila-Martínez ◽  
Miguel A. Cabrerizo-Vílchez ◽  
Miguel A. Rodríguez-Valverde
Keyword(s):  
Particle Charge ◽  
Mass Ratio ◽  
Contact Lines ◽  
Particle Segregation ◽  
Charge Mass

A Discussion on solar studies with special reference to space observations - Solar cosmic rays

1971 ◽  
Vol 270 (1202) ◽  
pp. 167-174 ◽  
Keyword(s):  
Cosmic Rays ◽  
Special Reference ◽  
Source Region ◽  
Mass Ratio ◽  
Solar Cosmic Rays ◽  
Charge Mass ◽  
Relative Abundances ◽  
Solar Particles ◽  
Precise Interpretation ◽  
Space Observations

A wealth of data on many aspects of solar cosmic rays has been collected over the last decade. One of the most striking features of these events has been the tremendous variation in many of their characteristics and the related difficulty of precise interpretation. However, one feature of the solar cosmic rays which does seem to be constant from event to event and within an event is the relative abundances of the multicharged nuclei with the same charge: mass ratio. This paper will concentrate on observations of the composition of solar particles and their interpretation. A brief discussion on the propagation of the energetic solar particles including a few comments on the source region will also be given.

scholarly journals Parameters of electrostatic spraying and its influence on the application efficiency

Revista CERES ◽  
2013 ◽  
Vol 60 (4) ◽  
pp. 474-479 ◽  
Author(s):  
Robson Shigueaki Sasaki ◽  
Mauri Martins Teixeira ◽  
Haroldo Carlos Fernandes ◽  
Paulo Marcos de Barros Monteiro ◽  
Denílson Eduardo Rodrigues ◽  
...  
Keyword(s):  
Deposition Efficiency ◽  
System Efficiency ◽  
Mass Ratio ◽  
Target Orientation ◽  
Faraday Cage ◽  
Charge Mass ◽  
Electrostatic Spraying ◽  
Conventional Systems ◽  
Liquid Deposition ◽  
Electrostatic System

When the electrostatic spraying is used correctly, it provides advantages over conventional systems, however many factors can affect the system efficiency. Therefore, the objective of this study was to evaluate the charge/mass ratio (Q/M) at different spraying distances (0, 1, 2, 3, 4 and 5 m), and the liquid deposition efficiency on the target. Evaluating the Q/M ratio the Faraday cage method was used and to evaluate the liquid deposition efficiency the artificial targets were positioned longitudinally and transversely to the spray jet. It was found that the spraying distance affects the Q/M ratio, consequently, the liquid deposition efficiency. For the closest distance to the target the Q/M ratio was 4.11 mC kg-1, and at distances of 1, 2, 3, 4 and 5 m, the ratio decreased to 1.38, 0.64, 0.31, 0.17 and 0.005 mC kg-1, respectively. For the liquid deposition, the electrostatic system was affected by the target orientation and spraying distance. The target transversely to the jet of liquid did not improve the liquid deposition, but longitudinally increased the deposition up to 3 meters of distance.

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