Javascript must be enabled to continue!
Radial dependence of ionization losses of protons of the Earth's radiation belts
View through CrossRef
Abstract. Coulomb losses and charge exchange of protons are considered in detail. On the basis of modern models of the plasmasphere and the exosphere, the radial dependences of the rates of ionization losses of protons, with μ from 0.3 to 10 keV nT−1, of the Earth's radiation belts near the equatorial plane are calculated for quiet periods. For calculation of Coulomb losses of protons we used data of ISEE-1 satellite (protons with energy from 24 to 2081 keV) on L from 3 to 9, data of Explorer-45 satellite (protons with energy from 78.6 to 872 keV) on L from 3 to 5 and data of CRRES satellite (protons with energy from 1 to 100 MeV) on L ≤ 3 (L is the McIlwain parameter). It is shown that with decreasing L the rate of ionization losses of protons of the radiation belts is reduced; for protons with μ > 1.2 keV nT−1 in a narrow region (ΔL ∼ 0.5) in the district of plasmapause in this dependence may form a local minimum of the rate. We found that the dependence from μ of the boundary on L between Coulomb losses and charge exchange of the trapped protons with hydrogen atoms is well approximated by the function Lb = 4.71μ0.32, where [μ] = keV nT−1. Coulomb losses dominate at L < Lb(μ), and at L > Lb(μ) dominates charge exchange of protons. We found the effect of subtracting the Coulomb losses from the charge exchange of protons of the radiation belts at low μ and L, which can simulate a local source of particles.
Title: Radial dependence of ionization losses of protons of the Earth's radiation belts
Description:
Abstract.
Coulomb losses and charge exchange of protons are considered in detail.
On the basis of modern models of the plasmasphere and the exosphere, the radial dependences of the rates of ionization losses of protons, with μ from 0.
3 to 10 keV nT−1, of the Earth's radiation belts near the equatorial plane are calculated for quiet periods.
For calculation of Coulomb losses of protons we used data of ISEE-1 satellite (protons with energy from 24 to 2081 keV) on L from 3 to 9, data of Explorer-45 satellite (protons with energy from 78.
6 to 872 keV) on L from 3 to 5 and data of CRRES satellite (protons with energy from 1 to 100 MeV) on L ≤ 3 (L is the McIlwain parameter).
It is shown that with decreasing L the rate of ionization losses of protons of the radiation belts is reduced; for protons with μ > 1.
2 keV nT−1 in a narrow region (ΔL ∼ 0.
5) in the district of plasmapause in this dependence may form a local minimum of the rate.
We found that the dependence from μ of the boundary on L between Coulomb losses and charge exchange of the trapped protons with hydrogen atoms is well approximated by the function Lb = 4.
71μ0.
32, where [μ] = keV nT−1.
Coulomb losses dominate at L < Lb(μ), and at L > Lb(μ) dominates charge exchange of protons.
We found the effect of subtracting the Coulomb losses from the charge exchange of protons of the radiation belts at low μ and L, which can simulate a local source of particles.
Related Results
Distribution of the Earth's radiation belts protons over the drift frequency of particles
Distribution of the Earth's radiation belts protons over the drift frequency of particles
Abstract. On the base of generalized data on the proton fluxes of the Earth's radiation belts (ERB) with energy from E ~ 0.2 MeV to 100 MeV at drift shells L from ~ 1 to 8, constru...
Distribution of Earth's radiation belts' protons over the drift frequency of particles
Distribution of Earth's radiation belts' protons over the drift frequency of particles
Abstract. Using data on the proton fluxes of the Earth's radiation belts
(ERBs) with energy ranging from 0.2 to 100 MeV on the drift L shells ranging
from 1 to 8, the quasi-station...
The in-situ exploration of Jupiter's radiation belts
The in-situ exploration of Jupiter's radiation belts
<p>Jupiter has the most energetic and complex radiation belts in our solar system. Their hazardous environment is the reason why so many spacecraft avoid rather than ...
Secret of radiation protection and anti-static clothing
Secret of radiation protection and anti-static clothing
In the current era, electromagnetic radiation is everywhere. Every day electromagnetic radiation and static electricity caused by a variety of hazards. So, anti-electromagnetic rad...
e0517 Forearm arteries with ultrasound for percutaneous coronary procedures
e0517 Forearm arteries with ultrasound for percutaneous coronary procedures
Background
The radial artery has become a widely used approach for coronary angiography and intervention in patients, and the ulnar artery is another approach for...
Research and Application of Rigless Radial Drilling Technologies in China and Middle East
Research and Application of Rigless Radial Drilling Technologies in China and Middle East
Abstract
Rigless radial drilling, or radial jet drilling involves drilling lateral holes from a vertical wellbore to enhance reservoir contact. Radial jet drilling s...
A novel radial beam smoothing scheme based on optical Kerr effect
A novel radial beam smoothing scheme based on optical Kerr effect
Laser-beam illumination uniformity is a key issue in inertial confinement fusion facilities. In order to fulfill the requirement of improving illumination uniformity, a radial smoo...
Characteristics of solar radiation at Xiaotang, in the northern marginal zone of the Taklimakan Desert
Characteristics of solar radiation at Xiaotang, in the northern marginal zone of the Taklimakan Desert
The characteristics of solar radiation and the influence of sand and dust on solar radiation in the northern margin of Taklimakan Desert were analyzed using radiation observation d...

