Thursday, 27 December 2018

Quiet Baseline for Longwave - Part 1

Ionospheric propagation is probably my number one radio interest, particularly the idea of prediction so that I can choose the best frequency or time or, ideally, the best date for a particular path.

We have these general rules about moving up and down the bands according to how high the sun is above the horizon and where we are in the sunspot cycle and propagation software that incorporates these factors has been around for years but I would like to do better than that, especially since I am interested in low power communications.

One problem with programs like VOACAP is that almost all of the work has gone into the HF part of the spectrum from 3 MHz to 30 MHz but these days I am mostly interested in the lower frequencies, partly because we are at the bottom of the sunspot cycle and partly because of the new 630 m and 2200 m allocations.

After almost a year and a half of renovating the home I moved into in 2017, I finally have a couple of descent wire aerials installed. My first project is to evaluate my local noise level under quiet solar and geomagnetic conditions and to get some quantified baseline of what to expect as "normal" propagation so that I can recognize unusual conditions when they occur.

Aircraft NDBs are wonderful for studying frequencies below 3 MHz because, unlike medium wave broadcasters, they transmit 24/7 without changing power or their antenna patterns and they constantly identify in slow Morse.

I spent much of this month collecting longwave data by recording NDBs with a Perseus SDR. My original idea was to record from 135 kHz to 535 kHz for two minutes every hour for at least three consecutive days with quiet solar and geomagnetic indices and then chart the carrier strength for each signal I found. Since this is winter, QRN from northern hemisphere storms should be low enough to give me a good chance at capturing some of the weaker signals.

Unfortunately, the human element of this did not go well. The best I could do was get through three hours of data in one hour. Manually estimating and recording signal strengths just took too long, especially for weak signals where I sometimes had to spend 10 minutes replaying a file to pull a single ID out of the noise. For 72 files it would have taken me about 50 hours just to do the data entry.

Then I remembered that the Perseus has the ability to place markers on up to eight frequencies and record the corresponding signal strengths to a text file at regular intervals along with a timestamp.

Eight was not ideal because a typical evening file had 15 identifiable signals. Still, about 10 of those were nearby “daytime regulars” of little interest for studying ionospheric propagation so eight markers should be enough for the more variable distant signals.

One weird thing I discovered is that, even when automatically logging markers from a previously recorded file, the timestamps were for the current UTC of when I was playing back the file, rather than when the file was recorded. That was a nuisance but I was able to work around it. The marker signal strength file is always named markers.log and old versions get overwritten by new ones so I included the timestamp of the original recording when renaming the file. That made it available for use when analyzing the data.

The above graph shows my result from a single 24-hour period (2018-12-06 UT). The vertical scale is in dBm but I only care about the shapes of the curves. The following graph is the result of averaging the respective ToH values over 4 consecutive UT days (2018-12-06 to 2018-12-09). Correction to both charts: The ID for 284 should be QD.

Q: What can I conclude from this?
A: Not much, other than "Distant signals are stronger at night." but this is nothing new.

That's why this post is Part 1.

Before this line of enquiry can be of any use to me, more work will be required:

  1. The 284-MB signal from The Pas, Manitoba indicates a problem. It's one of the weakest regular nightly signals here but both graphs show it as being surprisingly strong during the day and not changing much at night. That's because that part of the spectrum was consistently noisy and the marker's bandwidth was between 200 and 300 Hz with the settings I had to use to span all eight frequencies. A future attempt at this should record only four stations and use the other four markers to record only the adjacent noise so that it can be subtracted.
  2. Recording only the markers, as opposed to recording raw spectrum, generates very little data so next time I will sample the carriers much more often. I should not have chosen smoothed curves when producing these graphs because they are misleading considering the hourly sampling windows.
  3. The eight stations were chosen for geographic diversity. I was hoping to see trends like a peak moving from east to west but that was too ambitious for only eight signal sources. Next time I should do something like comparing a group of four Manitoba stations to a group of four Alberta stations averaged over several consecutive nights of similar quiet solar and geomagnetic conditions.

The work to this point has not been a waste of time because it has served as a "shake out" to see what is realistic. I hope to come away from subsequent experiments with a general idea of how a typical night of longwave behaves. A bonus would be to come up with a credible strategy for targeting the states and provinces that are still missing from my log, especially since I decided to reset it to zero at this new QTH.

Once I get that sorted out I would like to compare propagation on nights of quiet solar and geomagnetic conditions to nights of more active or disturbed conditions as we claw our way out from the bottom of the sunspot cycle. Even if nothing meaningful comes of it I should at least have good data from which to draw that conclusion.

Saturday, 3 November 2018

Wildlife and the DXer


The deer around here have no idea how much effort I have put into keeping them from trampling my feedlines or getting tangled in my aerials.

Tuesday, 27 September 2016

ABSC Nostalgia

A recent comment on an earlier post got me thinking about other experiments I did with kits of parts from the American Basic Science Club so I opened up a box and extracted these items.

Tuesday, 5 January 2016

Loop Comparison

LW, MW and HF listening did not become practical at my current location until I got my first Wellbrook active loop antenna (an ALA1530). Even when I just had it sitting out on the wood-frame balcony outside my home office it was a huge improvement over the indoor random wires I had been using up to that point. The noise level was low enough that I could rely on it for reception of much more than WWV and CRI. When I moved it away from the house to be mounted NE-SW on a nearby fence the noise level dropped a further 5 dB to 10 dB on most of the frequencies I tested. I call this Loop A.

A few years later I added a second Wellbrook loop (an ALA100) with four turns of wire wound on a wood frame and mounted on a different fence panel so that it favours NW-SE. I call this Loop B. It's centre is about 5 metres away from Loop A.

The plan was for Loop A to favour Europe and the South Pacific on HF while nulling the MW broadcasters in northwest WA. To compliment that, Loop B was to favour Asia, Alaska, the Lower 48, and the Caribbean on HF while nulling the MW broadcasters in the lower mainland of BC. That has all turned out as expected and the spacing between them has also been adequate for creating a deep electronically steerable null on MW using a DX Tools RF+ Quantum Phaser (not nearly as lethal as it sounds). I also hoped that on HF either loop could serve as a reference for the other when connected to an MFJ-1025 noise canceller. Unfortunately that turned out to be a complete waste of time and money because I did not find a single signal that benefited from use of the device.

After a recent post to the Shortwave Radio Station Listening group on Facebook I was asked about how well Loop B works. Such things are difficult to quantify so the best I can add to what I have said above is to refer to the following two frequency response curves from yesterday afternoon.

Loop A

Loop B

At almost all frequencies the output of Loop B is lower than that of Loop A but this is to be expected because, even with four turns, Loop B is built with much less "capture area" than recommended by the manufacturer. What else do the two images reveal? As expected, my only local MW broadcaster is clearly weakened by being in the null of Loop A and multiple Vancouver stations are brought down by being near the axis of Loop B. Aside from that, the two curves show differences in the sizes and locations of their peaks and valleys but there is no way to know, from this experiment alone, the extent to which that is due to differences in their frequency response or to differences in their location and orientation. For example, the electromagnetically noisiest place in my house is the service panel where AC power, cable TV and ADSL internet all converge and it is almost directly in the null of Loop A while the orientation of Loop B favours reception of noise from my nearest neighbours.

Switching from Loop A to Loop B

This last image shows what happened in the vicinity of a broadband noise source when I switched from Loop A to Loop B. I am sure that the frequency shift means something but I currently have no clue about what that might be or how to use the information.

Saturday, 26 December 2015

Signal Tracer and Injector

On Christmas Eve I finished building this simple piece of test equipment from QRPkits. It's a combined signal tracer and injector. It doesn't do anything that I cannot accomplish with an oscilloscope and a function generator but it's much more convenient to use.

As with the Accuprobe described in my previous post, this device uses heat-shrink tubing as a case. At Joanna's suggestion, instead of using a hair dryer as a heat source, I simply place the unit on top of a space heater (as shown in photo) with the air flow directed vertically. This worked much more quickly and provided more uniform heating.

Tuesday, 22 December 2015

Accuprobe for Measuring RF Voltages

Today I finished building my latest piece of test equipment -- the N2CX Accuprobe Plus from Pacific Antenna. It was an easy, high-quality kit. The only odd bit was using heat-shrinkable tubing in lieu of a tubular case. Without a proper heat gun I had to improvise with a hair drier but it worked well enough.

For testing, I compared the results obtained with it against the RMS values I calculated from the peak-to-peak readings off of an old Kenwood oscilloscope when using a function generator feeding my Elecraft dummy load for weak signals and a Yaesu FT-817 as a source for QRP power levels. The accuracy was what would be expected from the specs and much better than the readings made with my old Heathkit probe. However the latter would still be the device to use for voltages over the Accuprobe's 35 V limit.

Tuesday, 15 December 2015

Elecraft DL1 Dummy Load

Around the same time that I got the ZM-2 shown in my previous post, I also bought an Elecraft dummy load kit that you can find on this page.

One nice thing about it is that it includes a diode, capacitor and two convenient test points for measuring power with any high input impedance voltmeter. The manual comes with a graph for converting the voltage readings to watts. Using an inline meter to measure forward power as a reference, I got considerably more accurate results by using an old Heathkit RF probe across the load. However he test points are convenient and for my needs would be perfectly adequate to get relative readings for peaking the output of a QRP transmitter.