z-logo
open-access-imgOpen Access
Modelling the Io‐related DAM emission by modifying the beaming angle
Author(s) -
Ray L. C.,
Hess S.
Publication year - 2008
Publication title -
journal of geophysical research: space physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/2008ja013669
Subject(s) - physics , jovian , astrophysics , polarization (electrochemistry) , computational physics , viewing angle , relativistic beaming , range (aeronautics) , magnetic field , solid angle , optics , active galactic nucleus , galaxy , chemistry , materials science , quantum mechanics , liquid crystal display , planet , saturn , composite material , detector
The Io–Jupiter interaction generates strong decametric radio emissions (DAM), which appear as arcs in the time–frequency plane. These emissions are beamed at an angle from the magnetic field lines, which may vary with frequency and longitude amongst other properties. Empirical models of this beaming angle describe the shape of the DAM arcs and offer insight into the emission mechanism for DAM. Several studies have investigated the variation in the emission beaming angle. The studies span a range of frequencies which depend on the observational means (spacecraft, ground‐based radio telescopes) used to obtain data. Subsequently, because of the varying assumptions made (e.g. relativistic vs. non‐relativistic electrons for the wave polarization), methods used (e.g. prescribing a beaming angle function vs. determining a beaming angle function from observational geometry) and frequency ranges observed, different results have been found in each study. In the present paper, we model the shape of the emission with an empirical beaming angle function and adjust the parameters to best fit the emission arcs. However, our model builds on previous models by taking into account the location of Io in the Jovian magnetic field. We also look at a broader frequency range than many of the intermediate studies. We find that a simple empirical beaming angle function describes the shape of the A, B, and D arcs and that the beaming angle function must decrease at high and low frequencies. We then propose a simple explanation for the beaming angle profile, deduced from cyclotron maser theory.

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here