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Originally posted by simonbaker View PostOk, sounds like your talking about minimizing noise, different topic from "on-resonant" design phase-shift problems.
I'm guessing that you are comparing these two configurations for noise?
-SB
True differential amplifier is neither Zin>>infinity nor Zin>>0 like the solutions in your picture, but Zin = Zin (inv) + Zin (noninv) where Zin (inv) = Zin (noninv)
Picking correct resistor values to set up an opamp to be a true differential is not trivial, but reasonable choice is possible. So instead of R1=R3=6k8 and R2=R4=330k you may use R1 and R2 as they are (inverting branch) while in noninverting branch use 68ohm and 3k3. This combination provides less than 2% Zin (inv) against Zin (noninv).
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Originally posted by Davor View PostActually somewhere in between. Noise is not my primary concern. Typical solution nowadays uses an opamp amplifier with moderate to high input impedance, connected as a typical LF radio frontend with resonant frame antenna, and to avoid phase problems it is detuned. My idea is using lower Zin that would get close to the coil reactance and squeeze as much juice there. So instead of impedance transformation by means of a resonant tank, I'd go directly where juice is produced - at low Z. Also to avoid E field problems I think the best choice would be a true differential amplifier, a low Zin brother of an instrumentation amplifier.
True differential amplifier is neither Zin>>infinity nor Zin>>0 like the solutions in your picture, but Zin = Zin (inv) + Zin (noninv) where Zin (inv) = Zin (noninv)
Picking correct resistor values to set up an opamp to be a true differential is not trivial, but reasonable choice is possible. So instead of R1=R3=6k8 and R2=R4=330k you may use R1 and R2 as they are (inverting branch) while in noninverting branch use 68ohm and 3k3. This combination provides less than 2% Zin (inv) against Zin (noninv).
Also, the appeal of the tuned RX is the potentially high-Q which should boost S/N -- but maybe the SD is so narrow band it doesn't matter (except for the aliased stuff). Have to think on that.
Is your idea basically impedance-matching the amp to the coil for optimum power xfer?
-SB
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I don't expect to see much of aliases, at least not compared to normal IBOC noise. Sinc. detectors pick very narrow band stripe in VLF, so any additional noise will be of the same nature: not related to Tx or target. Besides, I can rely on feedback capacitor to take care of that. Anyway, I did not decide on optimum configuration yet. Maybe I'll keep a somewhat smaller capacitor in parallel to take care of the Tx harmonics and noise, with resonance at 1.5 Tx or something.
I'll experiment with this setup a bit. I have everything ready for ~6k8 true differential input impedance, and when I put a 10k trimmer in parallel I'll have it ready for testing. My goal will be the lowest impedance that works right, and I'll extrapolate from there. I expect to see some influence on GB, so when I hit the position where GB does not work right - I overdid it.
Optimum power transfer is a kind of goal here because it already happens with standard solution using a semi-resonant tank. Using low impedance is just a way to mimic it by non-resonant means. Real goal will be a bullet-proof solution for multiple frequencies.
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Originally posted by Davor View PostI don't expect to see much of aliases, at least not compared to normal IBOC noise. Sinc. detectors pick very narrow band stripe in VLF, so any additional noise will be of the same nature: not related to Tx or target. Besides, I can rely on feedback capacitor to take care of that. Anyway, I did not decide on optimum configuration yet. Maybe I'll keep a somewhat smaller capacitor in parallel to take care of the Tx harmonics and noise, with resonance at 1.5 Tx or something.
I'll experiment with this setup a bit. I have everything ready for ~6k8 true differential input impedance, and when I put a 10k trimmer in parallel I'll have it ready for testing. My goal will be the lowest impedance that works right, and I'll extrapolate from there. I expect to see some influence on GB, so when I hit the position where GB does not work right - I overdid it.
Optimum power transfer is a kind of goal here because it already happens with standard solution using a semi-resonant tank. Using low impedance is just a way to mimic it by non-resonant means. Real goal will be a bullet-proof solution for multiple frequencies.
What is IBOC?
-SB
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IBOC= in band on channel, as different from all aliases. RF jargon.
I think I know the goal, sort of. It is "normal" to seek for some angle between Tx and Rx with semi-resonant Rx, and it is usually between 10° and 20°. If I use input impedance ~15 times lower than in a case of a resonant tank I obtain ~20° shift. Well, it is not too low. So instead of common base I can go with a common emitter or a somewhat better opamp instead.
In case I use an Rx coil with more inductance, like for example a Musketeer coil, I'm well within an opamp ball game, and I SHOULD go with higher resonance just to stay within the 20° shift goal.
A short summary: If I connect a coil to a low impedance amplifier input, I'll obtain the same S/N as if I use some kind of impedance transformation and a high input impedance amplifier. Resonant tank IS a way of impedance transformation, and in case of poor component choice it provides you with more pain than joy. Hence, a low impedance method will provide more joy because it will be much easier to set up, and it will tolerate great margins of error in winding of Rx coils.
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Originally posted by simonbaker View PostOk - I don't completely understand your design goals, but maybe your final circuit will make it clearer. Look forward to what you discover.
What is IBOC?
-SB
http://www.ibiquity.com/hd_radio/iboc_white_papers
Jerry
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Ah, you'd be surprised. It was introduced with digital receivers because of their sampling nature and aliases all over the place. True, there is not much in common with them and MDs, but there is a common behaviour regarding aliases and sampling nature of synchronous detectors. It was on my mind at that moment. I'll try not to use such abbreviations any more.
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Hi all,
we don't need impedance matching here. We aren't transferring energy, we are just picking up a RX voltage with very low bias current (ultra tiny energy transfer only).
For best noise performance, just use a low impedance bipolar input front-end. A lot of the bipolar low noise op-amps are doing well.
BTW, the coil will pickup more noise.
My 2 cents
Aziz
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Originally posted by Aziz View PostHi all,
we don't need impedance matching here. We aren't transferring energy, we are just picking up a RX voltage with very low bias current (ultra tiny energy transfer only).
For best noise performance, just use a low impedance bipolar input front-end. A lot of the bipolar low noise op-amps are doing well.
BTW, the coil will pickup more noise.
My 2 cents
Aziz
On the other hand, hi-Q resonant tanks seem to make a high voltage on their own (as Davor says, a kind of impedance matcher), so they seem a good fit for a low-noise JFet front end.
-SB
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Originally posted by Davor View PostAh, you'd be surprised. It was introduced with digital receivers because of their sampling nature and aliases all over the place. True, there is not much in common with them and MDs, but there is a common behaviour regarding aliases and sampling nature of synchronous detectors. It was on my mind at that moment. I'll try not to use such abbreviations any more.
It seems more secure to have a tuned RX coil, but certainly we should be open to other ideas. I've always wondered about the off-resonant designs which receive maximum power (noise) off to the side -- but they seem to work quite well I must say.
Anyway, we'll be interested in your designs and how they compare.
-SB
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