Applied Planetary Radio Astronomy

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Jovian Radio Storms

Project Outline

Charged partical trajectory in Jupiter's magnetic field
Charged partical trajectory in Jupiter's magnetic field
Origin of the different frequency emissions in Jupiter's magnetic field
Origin of the different frequency emissions in Jupiter's magnetic field
Jupiter's A-, B- and C type radio burst
Jupiter's A-, B- and C type radio burst


The project is suitable for 1-2 practically oriented students with broad interests, who do not mind “getting their hands dirty” every now and then, in addition to the time spent in front of the PC.

  1. Contact persons – Georgi Genov, Kjetil Ullaland, Nikolai Østgaard, Kjell Aarsnes
  2. Aim - To learn basic radio astronomy, to modify an existing radio telescope amplifier (RTA), to build the telescope’s antennas and to establish observational procedures.
  3. Tasks
    • Modifying the existing RTA for automatic sweep of the frequency range;
    • Building the electronics required to establish the computer communication;
    • Building and set up of the antennas of the radio telescope;
    • Developing a simple software for data acquisition and preliminary data analysis;
    • Performing tests and developing observational procedures.
  4. Benefits – learn basic radio astronomy; get hands-on experience with applied electronics, data acquisition and data analysis, development of software for scientific purposes.
  5. Background

Two types of radio noise emitted by Jupiter have been detected – synchrotron and cyclotron. The latter is strong enough to be detected by small antennas on Earth’s surface. Charged particles spiraling around Jupiter’s magnetic field lines near both magnetic poles (top figure) produce this cyclotron radiation. These shortwave signals are often referred to as DAM, since they fall in the decameter wavelength range. At these higher latitudes, where Jupiter’s magnetic field reaches as far out as Io, its field lines sweep rapidly past the ions and electrons shed into Io’s torus. This induces DAM radiation along the surface of the cyclotron cone (given in magenta in the middle figure). Jupiter’s DAM frequency reaches a maximum of 39.5 MHz near Jupiter’s cloud tops. At twice Jupiter’s radius the frequency is 3 MHz. Intermediate frequencies are created between these two extreme distances. Jupiter radiates two distinctive types of radio signatures in the DAM frequency range:

  • L-bursts –long duration static sounding like the swoosh of the waves;
  • S-bursts – short duration static resembling the crackling of a campfire.

DAM radiation originates from at least 3 sources (A, B and C) that are fixed with respect to the planet’s rotating magnetic field. These sources are observed at around 20 MHz. They fall largely around one hemisphere (bottom figure). Source A is more than twice more likely to emit than either B or C. Jupiter’s magnetic storms depend on a combination of Io’s orbital position and the inclination of the respective radio source with respect to Earth.


Original Radio JOVE Project

  1. JOVE Receiver Documentation
  2. JOVE Antenna Documentation

Receivers - Construction and Theory

Antennae - Construction and Theory

Books

The Radio Sky and How to Observe It - by Jeff Lashley

Preface and Table of contents

Chapter 1 - The Radio Sun

Chapter 2 - Jupiter

Chapter 3 - Meteors and Meteor Streams

Chapter 4 - Beyond the Solar System

Chapter 5 - Antennae

Chapter 6 - Setting Up a Radio Astronomy Station

Chapter 7 - Radio Hardware Theory

Chapter 8 - Introduction to RF Electronics

Chapter 9 - Building a Very Low Frequency Solar Flare Monitor

Chapter 10 - Microwave Radio Telescope Projects

Chapter 11 - Building a Jupiter Radio Telescope

Chapter 12 - Building a Broad Band Solar Radio Telescope

Chapter 13 - Data Logging and Data Processing

Appendices - Formulae; Bibliography; Suppliers, Groups, and Societies; Glossary

Articles