SkyPipe Calibration
at the

NJ3B Radio Observatory

Jim Brown, NJ3B

Last modified 12/31/2009

Why calibrate?

Data collected in the Radio JOVE program can be submitted to the JOVE data archive.  This data is freely available to students and researches alike. 

Uncalibrated data is useful in that it shows the Jupiter or Solar burst relative to the background noise but it doesn't convey the true intensity of the burst.  Uncalibrated data between, for example, two JOVE sites can't be compared. The lack of comparability between these uncalibrated sites reduces the true value of  information contained in the data sets.

Calibrated data sets show a true value of the intensity of the burst at your location.   With calibrated data, values of bursts can then be used in research.  With known values to work with, a researcher can then use YOUR data in their research programs.   Just think about that for a second.  With the calibrated data sets we submit to the JOVE Archive, we are making a REAL contribution to radio astronomy!

Such studies include, but are not limited to:

  • The study of decametric radio emission from the planet Jupiter.
  • Studying very-fine structure in the dynamic spectra of the Jovian decametric emission.
  • Developing models explaining certain types of lane features present in the decametric radiation from Jupiter.
  • Determining a more precise value of the Jovian rotation period.
  • Determining the shape of the emission beams from Jupiter by studying how the declination of Earth affects the observations.
  • Earth ionospheric study; the propagation of radio emissions at several locations based on ionospheric transparency or translucency.

 


Calibration

SkyPipe software allows the user to take data from a receiver and manipulate it so that the data plotted is the true value of the intensity of the burst.  This value is, by convention, is displayed in "Degrees Kelvin".  This is also called the "Equivalent Antenna Temperature".  A more detailed description of antenna temperature can be found at: http://en.wikipedia.org/wiki/Noise_temperature.

 

The Procedure

The following steps can be made with either a sound source going through your sound card in the computer, or, as in my case, an A/D converter and a sound source from the receiver straight to the A/D converter that is then connected to my computer via a printer port.  Systems can vary and it's not in the scope of this tutorial to cover them all.   A more complete description and information can be found at: http://www.radiosky.com/skypipehelp/skypipehelpindex.html.

In order to calibrate your data, you need a known value, or a series of known values displayed on SkyPipe so that you can compare the known value to what is actually being displayed on your SkyPipe chart.

One such known value noise source is the RF2020 noise source generator manufactured by Richard Flagg (rf_at_hawaii_dot_rr_dot_com).

 

rf2020.jpg (302063 bytes)

 

 

IcomCal.jpg (122858 bytes)

 

 

zoom1.jpg (37873 bytes)

 

 

zoom3.jpg (69491 bytes)

 

 

zoom2.jpg (72306 bytes)

 


The values produced for this demonstration are as follows (your values will differ):

 

Noise Source Switch Setting Noise Source
Temperature
1000 deg. K
SkyPipe Plotted Value
1 25 42.11
2 51 84.89
3 102 154.12
4 204 254.03
5 407 385.52
6 814 568.14

 

 

image002.jpg (15976 bytes)

 

20 MHz = 8.5948+.35016*X+.0015232*X^2+.000000627X^3

For Channel 1 (20 MHz), A=X;B=X^2,C=X^3;8.5848+(.35016*A)+(.0015232*B)+(.000000627*C)

 

Noise Source Switch Setting Calibrated Noise Source
Temp. 1000 K
SkyPipe values without
calculations
SkyPipe plot
with calculation
Temp 1000 K
1 25 42.11 26.08
2 51 84.89 49.67
3 102 154.12 101.03
4 204 254.03 206.11
5 407 385.52 405.89
6 814 568.14 814.17

 

As you can see from the table, with the calculations applied, the results are very close to the actual values and the difference is negligible.

Accounting for loss

Example:

For argument sake, let's say that I've accounted for all the loss in my system:

100 feet coax......   .9 db loss
Filter ............  1.4 db loss
Arrestor............ 1.0 db loss
Phase cable.........  .2 db loss
Coax to both dipoles  .57 db loss

Total loss in system = 4.07 db
Total loss without phase cable  = 3.87 db

 

A=X;B=X^2,C=X^3;((-8.5116)+(.91888*A)+(.0041002*B)+(.0000024432*C))*(Log(4.07).    (Remember this is a log scale, hence the Log(4.07)

 

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