The Heating facility is situated next to the UHF and VHF incoherent scatter radars. See the list of publications that have come out of this facility since its construction in 1979.
EISCAT's ionospheric Heating facility including Dynasonde
HEATING campaign plans and relevant meetings
Latest Heating Results
Here are some results from the UK campaign in May 1995.
We also recently did a test experiment whereby Heating induced scintillations were observed on signals received at Tromso from a Russian satellite.
Other recent scientific results and events:
API technique (Artificial Periodic Irregularities)
ELF/VLF wave generation
The programme and abstracts for the 4th European Heating Seminar held in Tromso in May 1995 is here
12 linear class AB tetrode valve (or tube for you Americans) power amplifiers of 100 kW continuous rating each, driven by a 1.5 kW solid state wideband exciter. Minimum pulse length is about 20uS. Any frequency in the range 3.85-8 MHz can be tuned, but we have been allocated the following: 4.04, 4.544, 4.9128, 5.423, 6.77, 6.96, 7.1, 7.953 MHz. The transmitters can be tuned up either uniformly or to different frequencies in 2 groups of
6, 3 groups of 4, 6 groups of 2, or 12 different frequencies.
There is a choice of 3 arrays. Two of the arrays (numbers 2 and 3) have 6x6 crossed dipoles, resulting in 36 antennas. They cover the frequency range 3.85-5.65 MHz and 5.5-8 MHz. The gain of these is 24 dBi giving a half power beamwidth of 14.5 deg and a maximum effective radiated power of 300 MW. A pair of transmitters is fed to orthogonal antennas on a row of antennas. A third array (array 1), covering 5.5-8 MHz, has a gain of 30 dBi giving 1200 MW of effective rad
iated power. A pair of transmitters in this array feeds two rows of antennas. Each row has 12 crossed dipoles giving a total of 144 antennas. A particular transmitter can be connected to only one particular row (or pair of rows in array 1), but in any array independent of the other transmitters. The transmitters feed the antennas through about 50 km of aluminium co-axial transmission lines.
Tuning to a new frequency is done by a small microcomputer and can take a few minutes. Tilting of the beam in the north-south plane up to about +/- 30 deg is possible. Power can be chosen in 2.5% steps of the maximum tuned power, which itself can be less than the maximum possible. Complicated amplitude modulation formats are possible under computer or other sources of control. For example a so-called "SOUSY-switch" is used for ON/OFF modulation by about 70dB. Modulati
on frequencies in the range 15-200 Hz with duty cyles near 50% can not be used due to power supply resonance problems.
The radiated wave can be linearly or circularly polarized with either sense of rotation. Polarization reversal can be achieved on a pulse to pulse basis. Accurate timing to within microseconds is possible. Frequency stability is as good as the EISCAT cesium beam reference.
A digital HF sounder covering ca. 1-30 MHz is also available. This can be run like an ionosonde or in other modes such as fixed frequency soundings. Spaced receiving antennas are used. A sample ionogram shows a "clean" ionospheric trace. The latest soundings may also be available, but this is still experimental as yet. The Dynasonde does not run continuously so do not be surprised if the latest is not so recent.
There is a list of all soundings recorded since November 1992 when the computer was upgraded to a PC.
Since 14 Dec 1995 there have been 8,024 accesses to this page.
Document date: 17/02/93
Document name: ht-specs.doc
Author Mike Rietveld
HTML edits done 01/08-95 by Bjørge; Brekke