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#1
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S-W model R-1822 has a "reactance dimmer" (item 2) with a 6.3 v lamp that
illuminates the band indicators. The bandswitch physically moves the nameplates over the lamp. The transformer primary appears to be open, and a 10K resistor across it does provide a little signal to the speaker. C21 & C14 are listed as 10 mfd, 25 v and 0.1 mfd, 150 v, and both are absent. I am suspicious that C21 of that value doesn't belong, since the schematic has misidentified a C22 elsewhere. Schematic is from Nostalgia Air. This radio had been severely hacked, but the beautiful cabinet has kept me picking away at it for a long time. I've found a little about reactance dimmers but nothing about use in a tube radio, mostly fluorescent dimmers. I'd really appreciate any explanation of the function here and especially thoughts about the caps that parallel the primary. Thanks, Dave Burson |
#2
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Dave Burson wrote:
S-W model R-1822 has a "reactance dimmer" (item 2) with a 6.3 v lamp that illuminates the band indicators. The bandswitch physically moves the nameplates over the lamp. The transformer primary appears to be open, and a 10K resistor across it does provide a little signal to the speaker. C21 & C14 are listed as 10 mfd, 25 v and 0.1 mfd, 150 v, and both are absent. I am suspicious that C21 of that value doesn't belong, since the schematic has misidentified a C22 elsewhere. Schematic is from Nostalgia Air. This radio had been severely hacked, but the beautiful cabinet has kept me picking away at it for a long time. I've found a little about reactance dimmers but nothing about use in a tube radio, mostly fluorescent dimmers. I'd really appreciate any explanation of the function here and especially thoughts about the caps that parallel the primary. What this appears to be is a saturable reactor who's input is the B+ current to the RF/IF stages - which means the less signal strength - the higher the B+ current - due to AGC bias action. This is the same idea that "drives" the Philco shadow meter. Low signal - high current - since the AGC is low - and biases the tube more "on". Signal strength comes up (as a station is tuned in) AGC goes negative, turning the RF & IF tubes "down" (less current). As the current through the primary rises and falls - so does the saturation - effecting the transformer's coupling. Now notice the two secondary windings- If the transformer's "coupling" is working well - the two windings "buck" - the lamp is dim. However - if the transformer's coupling isn't - the two windings "interaction" is reduced - and the lamp is brighter. Oh, the two caps - well the last thing you want is for the AC signal on the secondary to be "coupled" through to the B+ - so the two caps act as bypasses to keep the 60 cycle out of the B+. (shooting from the hip - again - (sigh) - OK guys - what'd I miss? best regards... -- randy guttery A Tender Tale - a page dedicated to those Ships and Crews so vital to the United States Silent Service: http://tendertale.com |
#3
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Randy or Sherry Guttery wrote:
Dave Burson wrote: S-W model R-1822 has a "reactance dimmer" (item 2) with a 6.3 v lamp that illuminates the band indicators. The bandswitch physically moves the nameplates over the lamp. The transformer primary appears to be open, and a 10K resistor across it does provide a little signal to the speaker. C21 & C14 are listed as 10 mfd, 25 v and 0.1 mfd, 150 v, and both are absent. I am suspicious that C21 of that value doesn't belong, since the schematic has misidentified a C22 elsewhere. Schematic is from Nostalgia Air. This radio had been severely hacked, but the beautiful cabinet has kept me picking away at it for a long time. I've found a little about reactance dimmers but nothing about use in a tube radio, mostly fluorescent dimmers. I'd really appreciate any explanation of the function here and especially thoughts about the caps that parallel the primary. What this appears to be is a saturable reactor who's input is the B+ current to the RF/IF stages - which means the less signal strength - the higher the B+ current - due to AGC bias action. This is the same idea that "drives" the Philco shadow meter. Low signal - high current - since the AGC is low - and biases the tube more "on". Signal strength comes up (as a station is tuned in) AGC goes negative, turning the RF & IF tubes "down" (less current). As the current through the primary rises and falls - so does the saturation - effecting the transformer's coupling. Now notice the two secondary windings- If the transformer's "coupling" is working well - the two windings "buck" - the lamp is dim. However - if the transformer's coupling isn't - the two windings "interaction" is reduced - and the lamp is brighter. Oh, the two caps - well the last thing you want is for the AC signal on the secondary to be "coupled" through to the B+ - so the two caps act as bypasses to keep the 60 cycle out of the B+. (shooting from the hip - again - (sigh) - OK guys - what'd I miss? best regards... So with high B+ current, the xfmr is saturated, less bucking, lamp is bright? That means the bulb dims when on station? Ken |
#4
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![]() "Ken" wrote in message ... Randy or Sherry Guttery wrote: Dave Burson wrote: best regards... So with high B+ current, the xfmr is saturated, less bucking, lamp is bright? That means the bulb dims when on station? Ken Core saturates, and windings lose their inductance, basically becoming purely resistive (only the wire winding DC resistance with no reactance), the light would be brighter. Pee |
#5
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In article ,
Randy or Sherry Guttery wrote: Dave Burson wrote: S-W model R-1822 has a "reactance dimmer" (item 2) with a 6.3 v lamp that illuminates the band indicators. The bandswitch physically moves the nameplates over the lamp. The transformer primary appears to be open, and a 10K resistor across it does provide a little signal to the speaker. C21 & C14 are listed as 10 mfd, 25 v and 0.1 mfd, 150 v, and both are absent. I am suspicious that C21 of that value doesn't belong, since the schematic has misidentified a C22 elsewhere. Schematic is from Nostalgia Air. This radio had been severely hacked, but the beautiful cabinet has kept me picking away at it for a long time. I've found a little about reactance dimmers but nothing about use in a tube radio, mostly fluorescent dimmers. I'd really appreciate any explanation of the function here and especially thoughts about the caps that parallel the primary. What this appears to be is a saturable reactor who's input is the B+ current to the RF/IF stages - which means the less signal strength - the higher the B+ current - due to AGC bias action. This is the same idea that "drives" the Philco shadow meter. Low signal - high current - since the AGC is low - and biases the tube more "on". Signal strength comes up (as a station is tuned in) AGC goes negative, turning the RF & IF tubes "down" (less current). As the current through the primary rises and falls - so does the saturation - effecting the transformer's coupling. Now notice the two secondary windings- If the transformer's "coupling" is working well - the two windings "buck" - the lamp is dim. However - if the transformer's coupling isn't - the two windings "interaction" is reduced - and the lamp is brighter. Oh, the two caps - well the last thing you want is for the AC signal on the secondary to be "coupled" through to the B+ - so the two caps act as bypasses to keep the 60 cycle out of the B+. (shooting from the hip - again - (sigh) - OK guys - what'd I miss? This circuit is very confusing to me, I don't understand how it is supposed to work. There seem to be two opposing forces at work in the saturable transformer. The first is what you point out, that the two secondary windings are connected so they "buck", so that when the transformer is saturated by the DC in the primary, the coupling decreases and the light dims. But at the same time when the transformer is saturated the inductance also goes down, so even though the two secondary windings might be not coupled as tightly, their reactance is also lower which would tend to cause the light to become brighter. If this is all there is to it the question would be which one of the two effects is stronger than the other? But maybe the windings aren't arranged as on an ordinary transformer. What if we had E-core style laminations with the primary wound on the center leg and one of the two secondaries wound on each outer leg. The presence of the center leg would act as a magnetic short and greatly reduce the coupling between the two secondaries even when the transformer isn't saturated. When the transformer isn't saturated the light would be dim because of the high reactance of the two secondaries in series with the light. When the transformer becomes saturated at low signal levels the lights would become brighter because of the lowered reactance of the two secondary halves. Just another shot from the hip, it would be interesting to know what the actual disposition of the primary and secondary windings on the the transformer core is? Regards, John Byrns -- Surf my web pages at, http://fmamradios.com/ |
#6
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In article ,
"Uncle Peter" wrote: "Ken" wrote in message ... Randy or Sherry Guttery wrote: Dave Burson wrote: best regards... So with high B+ current, the xfmr is saturated, less bucking, lamp is bright? That means the bulb dims when on station? Ken Core saturates, and windings lose their inductance, basically becoming purely resistive (only the wire winding DC resistance with no reactance), the light would be brighter. The problem with this explanation is that the two secondaries appear to be connected so that they "buck" one another. If that is the actual case then the reactance of the two series connected secondary windings wouldn't change much with transformer saturation. Regards, John Byrns -- Surf my web pages at, http://fmamradios.com/ |
#7
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John Byrns wrote:
The problem with this explanation is that the two secondaries appear to be connected so that they "buck" one another. If that is the actual case then the reactance of the two series connected secondary windings wouldn't change much with transformer saturation. Yes, I agree - I think its more of the coupling increasing and decreasing causing more or less bucking between the windings. The decrease in inductance (at 60 cycle) would not be near as influential as the loss of coupling... Then again - as you noted - physical layout could have very significant impact on both / either... hmmmm... It is an interesting application. Didn't GE have something like this in some of their consoles? I've never had one in for service - but it seems I recall reading something about them. best regards... -- randy guttery A Tender Tale - a page dedicated to those Ships and Crews so vital to the United States Silent Service: http://tendertale.com |
#8
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John Byrns wrote:
Just another shot from the hip, it would be interesting to know what the actual disposition of the primary and secondary windings on the the transformer core is? Oh good heavens, John, how reckless - shooting from the hip... I'm proud of you! ;-) We had a circuit that was similar in a piece of RADAR gear - IIRC the transformer was pretty standard looking (but then it's been 30+ years). I think the key here is the the phasing of the two secondaries - with the core approaching saturation - the mutual coupling would decrease (as would the inductance itself) and since the phasing is opposed - both tend to incease the bulb's current... Am I missing something? -- randy guttery A Tender Tale - a page dedicated to those Ships and Crews so vital to the United States Silent Service: http://tendertale.com |
#9
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![]() This circuit is very confusing to me, I don't understand how it is supposed to work. There seem to be two opposing forces at work in the saturable transformer. The first is what you point out, that the two secondary windings are connected so they "buck", so that when the transformer is saturated by the DC in the primary, the coupling decreases and the light dims. But at the same time when the transformer is saturated the inductance also goes down, so even though the two secondary windings might be not coupled as tightly, their reactance is also lower which would tend to cause the light to become brighter. If this is all there is to it the question would be which one of the two effects is stronger than the other? But maybe the windings aren't arranged as on an ordinary transformer. What if we had E-core style laminations with the primary wound on the center leg and one of the two secondaries wound on each outer leg. The presence of the center leg would act as a magnetic short and greatly reduce the coupling between the two secondaries even when the transformer isn't saturated. When the transformer isn't saturated the light would be dim because of the high reactance of the two secondaries in series with the light. When the transformer becomes saturated at low signal levels the lights would become brighter because of the lowered reactance of the two secondary halves. Just another shot from the hip, it would be interesting to know what the actual disposition of the primary and secondary windings on the the transformer core is? Regards, John Byrns -- Surf my web pages at, http://fmamradios.com/ This may not shed light, since the drawing quality is poor, but there is a connection detail for the dimmer. I still don't understand the need for 2 caps of such different values and voltage ratings. Dave Burson |
#10
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Uncle Peter wrote:
"Ken" wrote in message ... Randy or Sherry Guttery wrote: Dave Burson wrote: best regards... So with high B+ current, the xfmr is saturated, less bucking, lamp is bright? That means the bulb dims when on station? Ken Core saturates, and windings lose their inductance, basically becoming purely resistive (only the wire winding DC resistance with no reactance), the light would be brighter. Pee But the core saturates on high current, that's off station. So the light is bright off station and dim on. It would make sense to have the lamp brighten on station, but I have seen other schemes work like this. Ken |
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