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#12
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#13
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#14
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#16
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#17
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Avery Fineman ) writes:
Stirling's description isn't quite good enough in the '74 article covering the included "reciprocating detector." The principle is that of simply filtering out the carrier, amplifying it, and mixing it back with the incoming carrier-plus-sidebands. At the output the carrier, mixed with itself, becomes a DC level. The sidebands mix with the amplified-and- limited/filtered carrier to result in the original audio. Motorola used the same principle in the MC1330P video detector chip introduced in the early 1970s (1972?). The 1330 had what amounted to a limiter ahead of the mixing stage. The so-called "capture effect" of the limiter will output the stronger signal which, in this case, is the AM carrier. For the "filtering" (as Olberg called it), the 1330 used a simple resonant circuit tuned to the carrier frequency. While the MC1330 internal schematic is not well layed out for clear understanding, it is different from the reciprocal detector. Unique to the RD design is the fact that the filter is at the output of the differential amplifier, what it sees at it's input is not just the incoming signal, but the incoming signal modified by the output of the filter. That seems to be a key to the design. The MC1330 splits the incoming signal, with one path going to a mixer, and the other path going throught a limiter and filter which then feeds the other input of the mixer. It's behaviour is obvious, ie limit the incoming signal so it's you get a constant amplitude carrier and mix it with the incoming signal to beat it down to baseband, and shows up in plenty of designs, both before and after the Badessa patent. There was an article in Ham Radio for September 1970 about the MC1496 double balanced modulator, and Roy Hejhall specifically mentions it's use as an AM detector in a similar scheme. He said that a limiter wasn't even needed since the 1496 will limit with enough signal. The same thing is stated in the MC1496 datasheet though you have to dig a bit to find it since it's under the "product detector" heading. The filter in this scheme is optional, because not only is there the 1496 example but I've seen similar schemes with no filter. The same scheme shows up in that fairly recent QST article about a synchronous detector (it's been in the Handbook too), though there it's labelled as "quasi-synchronous" and it's merely a side circuit to the main part using a PLL. But if you look in old literature it gets the "synchronous detector" label. What is a puzzle is why Olberg did not reference such articles, because they were halfway there to explaining the reciprocal detector, and what is vague in his articles is what makes the RD different. One thing is certain. That "amplify the carrier, limit it and use it as a locally generated carrier" scheme will not work with SSB, unless the original carrier is not well suppressed. And it's not going to work with CW either, since beating a carrier, as you say, against itself will result in DC and double the carrier. There'll be no beatnote. Since the RD is claimed to work on these modes, something else has to be going on. Michael VE2BVW |
#18
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Avery Fineman ) writes:
Stirling's description isn't quite good enough in the '74 article covering the included "reciprocating detector." The principle is that of simply filtering out the carrier, amplifying it, and mixing it back with the incoming carrier-plus-sidebands. At the output the carrier, mixed with itself, becomes a DC level. The sidebands mix with the amplified-and- limited/filtered carrier to result in the original audio. Motorola used the same principle in the MC1330P video detector chip introduced in the early 1970s (1972?). The 1330 had what amounted to a limiter ahead of the mixing stage. The so-called "capture effect" of the limiter will output the stronger signal which, in this case, is the AM carrier. For the "filtering" (as Olberg called it), the 1330 used a simple resonant circuit tuned to the carrier frequency. While the MC1330 internal schematic is not well layed out for clear understanding, it is different from the reciprocal detector. Unique to the RD design is the fact that the filter is at the output of the differential amplifier, what it sees at it's input is not just the incoming signal, but the incoming signal modified by the output of the filter. That seems to be a key to the design. The MC1330 splits the incoming signal, with one path going to a mixer, and the other path going throught a limiter and filter which then feeds the other input of the mixer. It's behaviour is obvious, ie limit the incoming signal so it's you get a constant amplitude carrier and mix it with the incoming signal to beat it down to baseband, and shows up in plenty of designs, both before and after the Badessa patent. There was an article in Ham Radio for September 1970 about the MC1496 double balanced modulator, and Roy Hejhall specifically mentions it's use as an AM detector in a similar scheme. He said that a limiter wasn't even needed since the 1496 will limit with enough signal. The same thing is stated in the MC1496 datasheet though you have to dig a bit to find it since it's under the "product detector" heading. The filter in this scheme is optional, because not only is there the 1496 example but I've seen similar schemes with no filter. The same scheme shows up in that fairly recent QST article about a synchronous detector (it's been in the Handbook too), though there it's labelled as "quasi-synchronous" and it's merely a side circuit to the main part using a PLL. But if you look in old literature it gets the "synchronous detector" label. What is a puzzle is why Olberg did not reference such articles, because they were halfway there to explaining the reciprocal detector, and what is vague in his articles is what makes the RD different. One thing is certain. That "amplify the carrier, limit it and use it as a locally generated carrier" scheme will not work with SSB, unless the original carrier is not well suppressed. And it's not going to work with CW either, since beating a carrier, as you say, against itself will result in DC and double the carrier. There'll be no beatnote. Since the RD is claimed to work on these modes, something else has to be going on. Michael VE2BVW |
#19
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"David J. Windisch" wrote in message
news:3f13ee31_1@newsfeed... Hmmmm. Been a long time since I thought about the r-d. IIRC #1: It (the reciprocating detector) would detect SSB and c-w, and it was silent between SSB bursts and c-w characters. Hmmmmmm. My RD implementation behaves like a BFO, no silence like you recall. Heterodynes 5kHz and higher with a wide IF. Olberg's hr 74/09 article says "Through regenerative feedback Q1 and Q2 form a simple oscillator operating at the filter centre frequency". When not locked onto a carrier ("nonsynchronous mode") he said, "the reference level is no longer completely amplitue controlled by the input signal". That seems to suggest that as a locked on signal becomes weak, the amplitude of the reference signal will diminish until lock is lost and rise when it becomes unlocked. He went on "but it does have signal-induced phase fluctuations", whatever that means. I do notice a tendency for the reference signal (BFO) to pull on signal strength and also on keyed carrier or bass speech energy close to the lock-in range. The latter can sound like a lf resonant belch. The narrower the lock-in range, the less susceptible it would seem, but then with no better than 50Hz tuning steps and some drift to contend with, we can't be too narrow. IIRC #2: It was best preceded by mode-suited, steeply-sloped filtering. I recall speculating, back then, that its operating principle was to generate the bfo signal by ringing a bfo tank, offset from the incoming signal, with the bursts of incoming signal. When the tank ceased oscillating, the r-d output was silent. A mode-suited, steeply-sloped filter ahead of the r-d would help keep its bfo tank from being rung by unwanted (off-frequency) signals. It would certainly prevent them beating against the product detector's self oscillation. The filtering of the reference signal inside the RD is supposed to be fairly narrow but not so narrow as to make lock difficult. The narrower the filter, purportedly the greater the immunity to impulse noise. In my current implementation, I use a ceramic resonator paralleled by a white top 455kHz IF L-C resonator. Olberg showed just an inductor in parallel with a quartz crystal, the inductor apparently chosen to resonate with the crystal's interelectrode capacitance at the crystal's frequency. My LC ratio is much lower and is perhaps not as effective at suppressing wideband noise but I can tune for a tighter lock range than Olberg recommended. The bfo offset required for these modes, and thus non-synchronousness of the bfo with the incoming signals, I think, might help to support, to some degree, the speculation above, as well as to explain the use of "reciprocating", rather than "synchronous", as part of the name. The "reciprocating" nomenclature seems to be related to switching the path between opposite phase legs of the product detector on the carrier phase reversals that occur with zero crossings of the modulation envelope of a suppressed carrier AM signal. Perhaps he borrowed it from "reciprocating engine" metaphor. The inventor, Badessa, did not use the term in his patent. Thinking about it now, I simply can't recall any attraction other than novelty ;o) It does seem to me to be an inexpensive synchronous/nonsynchronous detector for all AM modes (and possibly NBFM) that can be easily constructed for low frequencies, eg 455kHz. I'm sure my parts cost is only about $10 compared to $150 for a kit that uses the Sony ICF2010 parts. I'd like to try a 2010 as many extol the virtues of its SD and see how they compare. My main complaint with the RD (or, at least, with my RD) is the audio null that occurs at one point in the lock range. 73, Dave, N3HE and 73 to you. Tom VE3MEO |
#20
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"David J. Windisch" wrote in message
news:3f13ee31_1@newsfeed... Hmmmm. Been a long time since I thought about the r-d. IIRC #1: It (the reciprocating detector) would detect SSB and c-w, and it was silent between SSB bursts and c-w characters. Hmmmmmm. My RD implementation behaves like a BFO, no silence like you recall. Heterodynes 5kHz and higher with a wide IF. Olberg's hr 74/09 article says "Through regenerative feedback Q1 and Q2 form a simple oscillator operating at the filter centre frequency". When not locked onto a carrier ("nonsynchronous mode") he said, "the reference level is no longer completely amplitue controlled by the input signal". That seems to suggest that as a locked on signal becomes weak, the amplitude of the reference signal will diminish until lock is lost and rise when it becomes unlocked. He went on "but it does have signal-induced phase fluctuations", whatever that means. I do notice a tendency for the reference signal (BFO) to pull on signal strength and also on keyed carrier or bass speech energy close to the lock-in range. The latter can sound like a lf resonant belch. The narrower the lock-in range, the less susceptible it would seem, but then with no better than 50Hz tuning steps and some drift to contend with, we can't be too narrow. IIRC #2: It was best preceded by mode-suited, steeply-sloped filtering. I recall speculating, back then, that its operating principle was to generate the bfo signal by ringing a bfo tank, offset from the incoming signal, with the bursts of incoming signal. When the tank ceased oscillating, the r-d output was silent. A mode-suited, steeply-sloped filter ahead of the r-d would help keep its bfo tank from being rung by unwanted (off-frequency) signals. It would certainly prevent them beating against the product detector's self oscillation. The filtering of the reference signal inside the RD is supposed to be fairly narrow but not so narrow as to make lock difficult. The narrower the filter, purportedly the greater the immunity to impulse noise. In my current implementation, I use a ceramic resonator paralleled by a white top 455kHz IF L-C resonator. Olberg showed just an inductor in parallel with a quartz crystal, the inductor apparently chosen to resonate with the crystal's interelectrode capacitance at the crystal's frequency. My LC ratio is much lower and is perhaps not as effective at suppressing wideband noise but I can tune for a tighter lock range than Olberg recommended. The bfo offset required for these modes, and thus non-synchronousness of the bfo with the incoming signals, I think, might help to support, to some degree, the speculation above, as well as to explain the use of "reciprocating", rather than "synchronous", as part of the name. The "reciprocating" nomenclature seems to be related to switching the path between opposite phase legs of the product detector on the carrier phase reversals that occur with zero crossings of the modulation envelope of a suppressed carrier AM signal. Perhaps he borrowed it from "reciprocating engine" metaphor. The inventor, Badessa, did not use the term in his patent. Thinking about it now, I simply can't recall any attraction other than novelty ;o) It does seem to me to be an inexpensive synchronous/nonsynchronous detector for all AM modes (and possibly NBFM) that can be easily constructed for low frequencies, eg 455kHz. I'm sure my parts cost is only about $10 compared to $150 for a kit that uses the Sony ICF2010 parts. I'd like to try a 2010 as many extol the virtues of its SD and see how they compare. My main complaint with the RD (or, at least, with my RD) is the audio null that occurs at one point in the lock range. 73, Dave, N3HE and 73 to you. Tom VE3MEO |
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