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Frank Dresser wrote: "Paul Sherwin" wrote in message ... [snip] Modern AM transmitters have a very sharp rolloff above a certain frequency. Broadcasting above this would just waste transmitter power, since (almost all) radios wouldn't be able to receive it because of their IF selectivity characteristics. The 9kHz or 10kHz AM channel width is just a convention, but once it has been adopted there's no point in trying to receive a wider bandwidth - you'll just get interference from adjacent stations. If the received signal is very strong, the tuner's gain will have to be very low. This will supress the adjacent channel interference quite well. In the US and Canada, AM stations are allocated 10kHz bandwidth, giving a theoretical 5kHz treble cutoff. In most other place that's 9kHz/4.5kHz. Stations transmit a more restricted frequency range than this though, for a number of technical reasons. That's where my rough and ready 3.5kHz figure came from. RDH4 says most AM BCB radio makers tried for a final IF bandwidth response of 3.5 kHz That was in 1955/ Since then, the BW has shrunk in many sets to even less than 2 kHz, especially in solid state gear, giving horrid state AM listening. No good turning up the treble control knob, there is no treble there to boost. Best regards, Paul -- Paul Sherwin Consulting http://paulsherwin.co.uk The FCC requires US AM radio stations to have an audio bandwidth between 4 and 10 kHz or a total bandwidth from 8 to 20 kHz. Typical radios with IF transformers, rather than crystal or ceramic IF filters, don't have very sharp skirt selectivity. Few radios will be able to block out a strong adjecent channel 10 kHz off channel. Many can't block out a strong adjacent 20 kHz away. Some can't even block out a strong adjacent channel 30 kHz away. Oz local stations are rarely closer than 45 kHz, which is 5 x 9 kHz spaces. In Canberra, we used to have 2XX community station of 300 watts on 1,008 kHz, with 2CA of 5 Kw at 1,053 kHz, and it was a good test of any AM radio if 2CA couldn't be heard when tuned to 2XX. My own radio allows me to pick up a weak signal at 27 kHz away from 2CA without 2CA being heard. Most simple transistor based tuners fail this test. They have high Q single tuned IF coils. 7AD on 1008 kHz sometimes drifted in late at night all the way from Tasmania, if conditions were freaky. Antenna type and location/direction minimised this effect. The FCC limits interference only partly by bandwidth restrictions. Mostly, it uses geographic seperation and power restrictions. By ear, I think most stations go to about 7 or 8 kHz audio. Many of the AM stations are talkers, but the ads can really sparkle. There's one I hear which sounds like it goes to the 10 kHz audio max. Much AM is talkback from mobile telephones, and its pretty dreadful.... Patrick Turner. |
"Patrick Turner" wrote in message ... But how does one know how to apply an expander to exactly match the inverse of the compressor characteristic? I doubt two wrongs will make a right. I had a book which described a very simple expander which was just a light bulb in parallel with the speaker, if I recall. Loud passages would heat the filament (probably not to incandesence) reduce the load of the bulb and increase the volume even more. Quiet passages would let the bulb cool, load the circuit and reduce the volume. It sounds goofy to me, and it's a circuit which wasn't popular. There were probably more sophicated expander circuits back then. A modern sophicated decompressor circuit could match the curve of the compressor, just as the dolby system does. Anyhow, in Oz there isn't to much evidence of compression or emphasis of audio HF on the stations worth listening to; I find the better the receiver, the more like FM reception the AM signal becomes. Patrick Turner. Here's some of what's been happening in radio audio processing over the years in the US: http://www.bext.com/histproc.htm Frank Dresser |
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Jon Noring wrote: Well, being the "OP", I want a high-audio performance, modern design AM tuner to integrate into my audio system -- and I believe a lot of tube-o-philes likewise want that -- but not everyone obviously. There are several reasons why most higher-grade audio systems use separate components, the reasons of which are obvious to most everyone. The AM tuner is no different than other audio components in this regard. Maybe what you want is the old JW Miller passive AM tuner. No active devices at all, just a bunch of tuned circuits and a detector diode. Mark Zenier Washington State resident |
In article ,
"Frank Dresser" wrote: "Patrick Turner" wrote in message ... But how does one know how to apply an expander to exactly match the inverse of the compressor characteristic? I doubt two wrongs will make a right. I had a book which described a very simple expander which was just a light bulb in parallel with the speaker, if I recall. Loud passages would heat the filament (probably not to incandesence) reduce the load of the bulb and increase the volume even more. Quiet passages would let the bulb cool, load the circuit and reduce the volume. It sounds goofy to me, and it's a circuit which wasn't popular. There were probably more sophicated expander circuits back then. A modern sophicated decompressor circuit could match the curve of the compressor, just as the dolby system does. I am surprised at the size of this thread and how it has taken off, but many of the comments seem to be either misleading as a result of wrong facts or limited understanding of the technology involved. I have several comments that I will lump together. 1. It has been variously stated that the audio bandwidth of AM broadcasting is either 3.5 kHz, 5 kHz, or 10 kHz. In the US AM broadcast channels are 20 kHz wide, so audio is effectively limited to a maximum of 10 kHz by law/regulation. It is my impression that most AM stations transmit audio out to this legal maximum. Of course as HD-radio takes hold this will change with the analog signal cutting off somewhere around 5 kHz. I know there are at least 2 active broadcast engineers that read this group, perhaps they could fill us in on what the stations they are involved with are actually doing as far as audio bandwidth goes? 2. The idea expressed above that a "modern sophicated decompressor circuit could match the curve of the compressor" seems far fetched to me. In the days of yore when audio processing consisted of a single broad band compressor, and a broad band "peak limiter" one might have contemplated this, at least as far as the compression part went, but today's audio processing is much more complex. Processing today involves broad band AGC, multiband compressors, plus multiband and broadband clippers in place of the old "peak limiter". It isn't clear to me that this would be easy to undo, or even possible. I don't know if the multiband aspect creates problems for reversing the process or not, but how do you undo clipping, and if there are any feed forward compressors involved it is possible that the output isn't even a single valued function of the input, making recovery mathematically impossible. 3. TRF receivers have been mentioned, and everyone seems to assume that a TRF receiver would consist of cascaded single tuned resonators with RF amplifier stages between. There is no reason why double tuned circuits, similar to those used in the IF transformers of a superhetrodyne can't be used in a TRF receiver, with all the selectivity/bandwidth benefits that brings to the party. For examples see the Western Electric No. 10A receiver, the J.W. Miller TRF receiver, the early Altec AM receiver, as well as others. 4. It has been stated that constructing the various RF and IF coils, especially IF transformers with variable bandwidth, that are required, is one reason why people aren't doing this type of project. I would suggest that a variable bandwidth double tuned IF filter can be built using standard two terminal inductors, by using low side capacitive coupling. I have a British Acoustical AM tuner that uses this approach in place of the first IF transformer to provide variable bandwidth. Rather than using an IF transformer with a tertiary winding to provide variable bandwidth, two separate coils are used which are coupled by low side capacitive coupling, where the amount of coupling can be switched to change the bandwidth just the same as with the tertiary approach. 5. The thinking here seems to be limited to single tuned circuits for TRF receivers, and double tuned IF transformers for superhetrodyne receivers. There is no reason why one can't build more complex filters that will provide better performance than an equivalent number of poles in ordinary double tuned IFTs. Quad tuned filters are relatively easy to do, and it is possible to go to even more poles in a single filter module, providing an improved selectivity vs. bandwidth trade off. 6. It has been suggested that adding resistors across an ordinary IF transformer will widen the audio bandwidth. This is not always true as the Heath company illustrated in the manual for their BC-1A High Fidelity AM tuner. They suggested adding a resistor to the first IFT to narrow the bandwidth if interference from adjacent stations was encountered, and IIRC they provide audio response graphs with and without the added resistor showing how the resistor narrows the bandwidth. Actually I think that in this case it is only the nose bandwidth that gets narrower, the bandwidth further out beyond the audio range does increase as you would expect. I think this effect is probably due to the fact that the first IFT in the Heath, and other quality tuners, is overcoupled, and adding the resistor eliminates the overcoupling effect narrowing the nose bandwidth. It pays to be careful and make sure you know the theory and what you are doing, as things don't always work as you might expect. 7. It has been suggested that using a 2 MHz IF frequency would allow wider bandwidth than the standard 455 kHz IF frequency. I fail to see why this should be true. Within reason, for bandwidths typical of audio receivers, you should be able to build a filter at 455 kHz that has effectively the same response as a 2 MHz filter. There is no need to throw out the 455 kHz IF just to get wide bandwidth. Regards, John Byrns Surf my web pages at, http://users.rcn.com/jbyrns/ |
Jon Noring schrieb: In the last couple of years I've posted various inquiries to this and related newsgroups regarding high-performance, tube-based AM (MW/BCB) tuners, both "classic" and modern. Have a look into the "Collins" S-series. These are state-of-the-art tube sets 'til now. At least it's not the tubes alone but the fabulous mechanical IF-filters giving outstanding results for a tube set. Manuals with layout diagrams should be available on the web.... |
John Byrns wrote:
3. TRF receivers have been mentioned, and everyone seems to assume that a TRF receiver would consist of cascaded single tuned resonators with RF amplifier stages between. There is no reason why double tuned circuits, similar to those used in the IF transformers of a superhetrodyne can't be used in a TRF receiver, with all the selectivity/bandwidth benefits that brings to the party. For examples see the Western Electric No. 10A receiver, the J.W. Miller TRF receiver, the early Altec AM receiver, as well as others. I did a cursory check on the Internet, but did not yet find any schematics for the mentioned receivers. Are they online somewhere? Anyone? I also found the following article from John posted back in 2000, where he talks about the double tuned TRFs, such as WE-10A, J.W. Miller, Collins (which I assume is the same one Volker Tonn mentioned today), Meissner, and the Weeden (the last of which John noted to be the best designed of all of them): http://groups.google.com/groups?selm...&output=gplain Unfortunately the URLs to the TRF schematics at John's site are not working. John, how exactly do these double tuned circuits work in TRF circuits compared to using single tuned resonators, as depicted on slide 7 of: http://www.technology.niagarac.on.ca...531unit6rx.ppt John, I also recall you mentioning a while back about "modernizing" one of these TRF receivers. What is the current state of your research on these circuit designs? Have you advanced to the point that a detailed schematic is right around the corner? Thanks for posting your thoughts. Jon Noring |
Patrick Turner wrote:
I won't budge from the idea that its possible to digitise the signal from the antenna and simply apply suitable algorithms, and get digital decoding, without all the phase shift caused by consecutive tuned circuits. And I agree with Patrick. Despite my desire to have a nice, kit-made, high-performance AM tube tuner, ultimately I think the best radio tuner for sound quality and overall performance (whether AM, ASM, FM, digital broadcast, etc.) is the pure digital system as described by Patrick. But do the necessary low-level A-D converters already exist? Is anyone actually building radios on this principle, or are we still a few years off? Jon Noring [p.s., pure Class D digital amps are continuing to improve, with better switching and so on, so ultimately the only analog streams we'll be dealing with will be radio signals captured by the antenna (which will promptly be digitized), and the output to the speakers from the last-stage PWM of the digital amplifier. Everything inbetween will totally be digital, using advanced and inexpensive DSP to do things not possible in the analog processing realm. The only realm left for the audiophiles to play in will be speakers.) |
Jon Noring wrote: Patrick Turner wrote: I won't budge from the idea that its possible to digitise the signal from the antenna and simply apply suitable algorithms, and get digital decoding, without all the phase shift caused by consecutive tuned circuits. And I agree with Patrick. Despite my desire to have a nice, kit-made, high-performance AM tube tuner, ultimately I think the best radio tuner for sound quality and overall performance (whether AM, ASM, FM, digital broadcast, etc.) is the pure digital system as described by Patrick. But do the necessary low-level A-D converters already exist? Is anyone actually building radios on this principle, or are we still a few years off? Jon Noring There are virtual radios which can be installed in a PC. Been around for years. They involve a suitable antenna interface and sound card, and program on a disc, and were advertised for sale on the back of Electronics, the british magazine. The front plate of a radio communications receiver appears on the screen and I guess you tune and select receiver functions by dabbing items on the screen with a mouse. [p.s., pure Class D digital amps are continuing to improve, with better switching and so on, so ultimately the only analog streams we'll be dealing with will be radio signals captured by the antenna (which will promptly be digitized), and the output to the speakers from the last-stage PWM of the digital amplifier. Everything inbetween will totally be digital, using advanced and inexpensive DSP to do things not possible in the analog processing realm. The only realm left for the audiophiles to play in will be speakers.) I think the world of totally digital is still some way off. And while things like good vinyl replay still beats all digital disc formats, there will always be a following for analog. I will be dead in 25 years, or deaf by then, so I won't give a hoot what the human race does after that. Patrick Turner. |
Volker Tonn wrote: Jon Noring schrieb: In the last couple of years I've posted various inquiries to this and related newsgroups regarding high-performance, tube-based AM (MW/BCB) tuners, both "classic" and modern. Have a look into the "Collins" S-series. These are state-of-the-art tube sets 'til now. At least it's not the tubes alone but the fabulous mechanical IF-filters giving outstanding results for a tube set. Manuals with layout diagrams should be available on the web.... The mechanical filters are only good for reducing the BW of an existing IF strip to make the receiver extremenly selective, so a much reduced bandwidth is possible which isn't capable of wide AF BW. Crystal filters are also used for the same purpose. Since Mr Noring says he has regularly trawled the Net for everyone else's expertise on AM reception, but got nowhere, because he's still doin it, why doesn't he gird his loins and put his shoulder to the task of learning all about AM and radio engineering as spelled out so clearly in all the old text books, and then damn well build his own perfect AM radio??? Patrick Turner. |
John Byrns wrote: In article , "Frank Dresser" wrote: "Patrick Turner" wrote in message ... But how does one know how to apply an expander to exactly match the inverse of the compressor characteristic? I doubt two wrongs will make a right. I had a book which described a very simple expander which was just a light bulb in parallel with the speaker, if I recall. Loud passages would heat the filament (probably not to incandesence) reduce the load of the bulb and increase the volume even more. Quiet passages would let the bulb cool, load the circuit and reduce the volume. It sounds goofy to me, and it's a circuit which wasn't popular. There were probably more sophicated expander circuits back then. A modern sophicated decompressor circuit could match the curve of the compressor, just as the dolby system does. I am surprised at the size of this thread and how it has taken off, but many of the comments seem to be either misleading as a result of wrong facts or limited understanding of the technology involved. I have several comments that I will lump together. 1. It has been variously stated that the audio bandwidth of AM broadcasting is either 3.5 kHz, 5 kHz, or 10 kHz. In the US AM broadcast channels are 20 kHz wide, so audio is effectively limited to a maximum of 10 kHz by law/regulation. It is my impression that most AM stations transmit audio out to this legal maximum. Of course as HD-radio takes hold this will change with the analog signal cutting off somewhere around 5 kHz. I know there are at least 2 active broadcast engineers that read this group, perhaps they could fill us in on what the stations they are involved with are actually doing as far as audio bandwidth goes? The Oz situation is different to the US, as I and PA have indicated. If two stations are 10 kHz apart on carrier F, and the both use 10 kHz modulation, then the sidebands of one station will interfere and be heard when tuned to the other, if the signal strengths are the same. 10 kHz notch filters won't stop the monkey chatter. 2. The idea expressed above that a "modern sophicated decompressor circuit could match the curve of the compressor" seems far fetched to me. In the days of yore when audio processing consisted of a single broad band compressor, and a broad band "peak limiter" one might have contemplated this, at least as far as the compression part went, but today's audio processing is much more complex. Processing today involves broad band AGC, multiband compressors, plus multiband and broadband clippers in place of the old "peak limiter". It isn't clear to me that this would be easy to undo, or even possible. And two wrongs don't make a right. I don't know if the multiband aspect creates problems for reversing the process or not, but how do you undo clipping, and if there are any feed forward compressors involved it is possible that the output isn't even a single valued function of the input, making recovery mathematically impossible. Limiting stuffs audio, and it cannot be undone. 3. TRF receivers have been mentioned, and everyone seems to assume that a TRF receiver would consist of cascaded single tuned resonators with RF amplifier stages between. There is no reason why double tuned circuits, similar to those used in the IF transformers of a superhetrodyne can't be used in a TRF receiver, with all the selectivity/bandwidth benefits that brings to the party. For examples see the Western Electric No. 10A receiver, the J.W. Miller TRF receiver, the early Altec AM receiver, as well as others. With variable tuning? its hard to get right. fixed IF tuning is far easier. 4. It has been stated that constructing the various RF and IF coils, especially IF transformers with variable bandwidth, that are required, is one reason why people aren't doing this type of project. I would suggest that a variable bandwidth double tuned IF filter can be built using standard two terminal inductors, by using low side capacitive coupling. I have a British Acoustical AM tuner that uses this approach in place of the first IF transformer to provide variable bandwidth. Rather than using an IF transformer with a tertiary winding to provide variable bandwidth, two separate coils are used which are coupled by low side capacitive coupling, where the amount of coupling can be switched to change the bandwidth just the same as with the tertiary approach. Very hard to get right. I tried all that. I tried tertiaries, but mechanical variation of the distance between IF coils seemed to work best. 5. The thinking here seems to be limited to single tuned circuits for TRF receivers, and double tuned IF transformers for superhetrodyne receivers. There is no reason why one can't build more complex filters that will provide better performance than an equivalent number of poles in ordinary double tuned IFTs. Quad tuned filters are relatively easy to do, and it is possible to go to even more poles in a single filter module, providing an improved selectivity vs. bandwidth trade off. 6. It has been suggested that adding resistors across an ordinary IF transformer will widen the audio bandwidth. This is not always true as the Heath company illustrated in the manual for their BC-1A High Fidelity AM tuner. If it lowers the Q, the BW is widened, but at the expense of attenuation just outside the band. Its a bandaid measure. They suggested adding a resistor to the first IFT to narrow the bandwidth if interference from adjacent stations was encountered, and IIRC they provide audio response graphs with and without the added resistor showing how the resistor narrows the bandwidth. ?? Actually I think that in this case it is only the nose bandwidth that gets narrower, the bandwidth further out beyond the audio range does increase as you would expect. I think this effect is probably due to the fact that the first IFT in the Heath, and other quality tuners, is overcoupled, and adding the resistor eliminates the overcoupling effect narrowing the nose bandwidth. So its the rabbit eared response curve which is damped by the R, thus narrowing the BW. It pays to be careful and make sure you know the theory and what you are doing, as things don't always work as you might expect. You got it. 7. It has been suggested that using a 2 MHz IF frequency would allow wider bandwidth than the standard 455 kHz IF frequency. I fail to see why this should be true. Because for the same Q value, the pass band would be 4 times wider Within reason, for bandwidths typical of audio receivers, you should be able to build a filter at 455 kHz that has effectively the same response as a 2 MHz filter. There is no need to throw out the 455 kHz IF just to get wide bandwidth. Its difficult to make a 455kHz typical old IFT produce a nice flat topped 20 kHz wide BW. Its either pointy nosed, undecoupled, or flat topped, critical coupled, or over critical or rabbit eared. I have tried all that. Patrick Turner. Regards, John Byrns Surf my web pages at, http://users.rcn.com/jbyrns/ |
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