Hi all,

I believe I am also being affected by this. I regret that I did not investigate more deeply early in testing of the new modes to see why my amplifier often goes into some anomalous condition at the start of a FST4/W transmission and does not always recover. I have also been seeing evidence of significant RF output waveform anomalies at the end of all FST4/W transmissions. I did not realize these modes apparently use amplitude shaping at the start and end of a transmission until others brought it up. If I had realized this early on I would have immediately raised a red flag. Although I routinely monitor my RF output with an oscilloscope (that's how I know there are anomalies), I unfortunately don't have a storage scope to capture and examine the events in detail.

The class D and E amplifiers widely used on LF and MF cannot reproduce amplitude variations. The FETs are run as switches with two valid states: on and off. Many of the FET driver chips can improperly clock the FETs when the amplitude of the input waveform is below a certain design level. This can cause several issues, including damaged FETs. Also note that in some cases these amplifiers will produce output spectra that is not clean when in these abnormal drive states. If the shaped waveform was intended to produce a cleaner signal, it is likely having the opposite effect in some cases (almost certainly including my signal based on the anomalies I am seeing).

I realize we are in a late stage of development of these modes now, possibly about to see a GA release. But is there any way this shaped envelope can be changed (perhaps as a user option) such that the waveform will start and stop instantly (or nearly so, as other nodes do) without amplitude shaping?

73 and Happy New Year,
Paul N1BUG



On 1/4/2021 9:59 PM, Peter Hall wrote:
Hi WSJT Developers,

I’ve not submitted a bug report before and hope that this email find its way to the appropriate team members.

Recently, in the RSGB low frequency and WSJT-X user groups I’ve raised the issue of the slow envelope rise times on FST4 and FST4W causing problems with the non-linear power amplifier designs (Class D or E) common among LF/MF users.  For your information, I’ve reproduced the original post in the WSJT-X group below, but note that the thread has developed as other users have injected their own experiences.  The thread is at: https://wsjtx.groups.io/g/main/topic/79269122?p=Created,,,20,2,0,0 <https://wsjtx.groups.io/g/main/topic/79269122?p=Created,,,20,2,0,0>  In particular, please note that ON7YD has retracted his first measurements (referenced in my original post, below) and has supplied an update which agrees well with my own and other envelope risetime characterizations.

If you’d like any additional information or assistance, I’d be very happy to help.

73, and thanks for your assistance, Peter (VK6HP)

Original WSJT-X user group post containing details of issue and configuration:

Hello everyone,

I've just joined this group and would be interested to know if anyone can shed some light on an issue I'm experiencing.  I do quite a bit of work on 630 m using a TS-890S exciter and a homebrew 300 W Class D amplifier.  The 0 dBm drive for the PA is taken from the Kenwood "DRV" output.  For those interested, the transmit antenna is a ZS6BKW HF doublet loaded as a Marconi T and the most usual receive antenna is a 1 m diameter active loop.  I'm running Windows 10 on a Microsoft SurfaceBook and a USB connection between the PC and the radio's internal audio interface ("sound card").  The software version is WSJT-X v2.3.0-rc2, although the -rc1 version behaves identically. I use PTT/CAT control but have experimented with VOX with no resolution of the central issue.

I've had no problems running any JT modes on any bands until I began trying out the FST4 and 4W modes on 630 m a few months ago.  Both WSPR and JT9 work very well on 630 m and the new modes also work, but with a small twist: the risetime of the FST4 envelope is so slow that it upsets the clocking arrangement in the push-pull PA.  This causes the PA protection to activate, with a consequent small loss of signal at the start of the transmission.  It's not a particularly serious problem, but is annoying.  I do have a hardware fix in the form of what is essentially a noise gate circuit between the radio and PA; the drive signal has to be above a set level (chosen to reliably clock the PA) before it is passed to the amplifier.  However, after some recent investigation I can quite clearly see a difference in the transmit delays and transceiver waveforms when doing nothing else but changing from e.g. WSPR to FST4W-120.

In brief, the WSPR envelope rise time is of order a few milliseconds and the delays are well-behaved, with a zero transmit delay actually corresponding to a few ms delay in seeing the TS-890S drive waveform. With FST4W, the RF envelope rise time is very slow indeed, with many tens of ms observed.  The transceiver delay is also much longer - typically more than 100 ms.

I should add that I've successfully sent and received FST4W signals, including some 4-300 and 4-900 contacts.

I'm unable to spot any transceiver setting differences between old and new modes and have not yet experimented with other transceivers. However one fellow member of the RSGB LF Group was kind enough to show that, using a simple sound card, he was unable to see any difference between the envelope characteristics of various modes.  It does look like a software issue to me and I'd appreciate comments from anyone running a similar setup, or with relevant suggestions.

73, Peter (VK6HP)

Peter J Hall

Emeritus Professor of Radio Astronomy Engineering, Curtin University

ICRAR/CIRA,
Building 610,
1 Turner Avenue
Bentley Technology Park, WA 6102.

Ph: + 61 400 801 531
Post: GPO Box U1987, Perth WA 6845, Australia.
www.icrar.org <http://www.icrar.org/>



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