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#21
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Phil Hobbs wrote...
Tom Bruhns wrote: So the right way to do this is to lower the _effective_ minimum capacitance. You can do that by adding an inductor, to cancel out capacitance. You can end up making the tuning range as wide as you want, but at the expense of the crystal (ceramic resonator in your case) being less of the overall frequency determination. In other words, there comes a point where you'd be as well off to just do an LC oscillator. But to double, say, the range, it's a good way to go. I guess I re-discovered what was already well known, but a few years ago I designed such a VCXO, and was amazed how linear the freq-vs-controlvoltage curve was (a good thing for use in a PLL). Don't know what range you're trying to achieve, but I had no trouble getting a bit more than 0.1% (~20kHz at 14MHz) that way, with a crystal. An inductor in series with the varactors, then another one in parallel with the series combo can get you a very wide range of impedance from a decent varactor. Sounds good. How about a specific example? Thanks, - Win whill_at_picovolt-dot-com |
#22
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On Wed, 10 Dec 2003 14:39:22 +0000, Phil Hobbs
wrote: Tom Bruhns wrote: So the right way to do this is to lower the _effective_ minimum capacitance. You can do that by adding an inductor, to cancel out capacitance. You can end up making the tuning range as wide as you want, but at the expense of the crystal (ceramic resonator in your case) being less of the overall frequency determination. In other words, there comes a point where you'd be as well off to just do an LC oscillator. But to double, say, the range, it's a good way to go. I guess I re-discovered what was already well known, but a few years ago I designed such a VCXO, and was amazed how linear the freq-vs-controlvoltage curve was (a good thing for use in a PLL). Don't know what range you're trying to achieve, but I had no trouble getting a bit more than 0.1% (~20kHz at 14MHz) that way, with a crystal. An inductor in series with the varactors, then another one in parallel with the series combo can get you a very wide range of impedance from a decent varactor. Thanks, is this the kind of thing you mean? +-------+ | | | | | | C| | L1 C| | C| | | | | | V | D1 - | | C| Applied DC control voltage | C| L2 Line --------------------+ C| | | | | D2 - | ^ | | | | | | | +-------+ View in FP font. created by Andy´s ASCII-Circuit v1.24.140803 Beta www.tech-chat.de -- "I expect history will be kind to me, since I intend to write it." - Winston Churchill |
#23
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On Wed, 10 Dec 2003 14:39:22 +0000, Phil Hobbs
wrote: Tom Bruhns wrote: So the right way to do this is to lower the _effective_ minimum capacitance. You can do that by adding an inductor, to cancel out capacitance. You can end up making the tuning range as wide as you want, but at the expense of the crystal (ceramic resonator in your case) being less of the overall frequency determination. In other words, there comes a point where you'd be as well off to just do an LC oscillator. But to double, say, the range, it's a good way to go. I guess I re-discovered what was already well known, but a few years ago I designed such a VCXO, and was amazed how linear the freq-vs-controlvoltage curve was (a good thing for use in a PLL). Don't know what range you're trying to achieve, but I had no trouble getting a bit more than 0.1% (~20kHz at 14MHz) that way, with a crystal. An inductor in series with the varactors, then another one in parallel with the series combo can get you a very wide range of impedance from a decent varactor. Thanks, is this the kind of thing you mean? +-------+ | | | | | | C| | L1 C| | C| | | | | | V | D1 - | | C| Applied DC control voltage | C| L2 Line --------------------+ C| | | | | D2 - | ^ | | | | | | | +-------+ View in FP font. created by Andy´s ASCII-Circuit v1.24.140803 Beta www.tech-chat.de -- "I expect history will be kind to me, since I intend to write it." - Winston Churchill |
#24
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On Wed, 10 Dec 2003 19:53:30 +0000, Paul Burridge
wrote: On Tue, 09 Dec 2003 17:28:22 -0700, Jim Thompson wrote: I'm using a 555 timer to generate a sawtooth waveform to feed the diodes, so I get a constant frequency sweep at the vcxo's output. Main problem is the limited voltage output range; starts above zero volts and peaks well before supply rail. So not much of a ramp; just around 4 or 5 volts, I guess. I could try changing the diodes for more The 555 thresholds are set to charge and discharge the timing cap at 1/3 and 2/3rds the supply voltage. If you using that directly the easiest way to get more "swing" is : Use an opamp to translate the voltage lower and add some gain (use at least 12v on the opamp). That can get you a Tuning voltage that is near 0 to near 12V (that should help). OR use a higher Vcc on the 555, say 12v. That will get your total swing to about 4V and the low will be 4v and the peak will be 8v. There are tricks that can be used to "offset" that 1/3 and 2/3 point but the total swing is usually the same. That can help as operating the Varicap closer to 0V will allow you to use more of it's capacitance range though it's usualy less linear at the bottom. Myself I'd use an opamp to create a saw generator and then I can control the swings. Allison |
#25
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On Wed, 10 Dec 2003 19:53:30 +0000, Paul Burridge
wrote: On Tue, 09 Dec 2003 17:28:22 -0700, Jim Thompson wrote: I'm using a 555 timer to generate a sawtooth waveform to feed the diodes, so I get a constant frequency sweep at the vcxo's output. Main problem is the limited voltage output range; starts above zero volts and peaks well before supply rail. So not much of a ramp; just around 4 or 5 volts, I guess. I could try changing the diodes for more The 555 thresholds are set to charge and discharge the timing cap at 1/3 and 2/3rds the supply voltage. If you using that directly the easiest way to get more "swing" is : Use an opamp to translate the voltage lower and add some gain (use at least 12v on the opamp). That can get you a Tuning voltage that is near 0 to near 12V (that should help). OR use a higher Vcc on the 555, say 12v. That will get your total swing to about 4V and the low will be 4v and the peak will be 8v. There are tricks that can be used to "offset" that 1/3 and 2/3 point but the total swing is usually the same. That can help as operating the Varicap closer to 0V will allow you to use more of it's capacitance range though it's usualy less linear at the bottom. Myself I'd use an opamp to create a saw generator and then I can control the swings. Allison |
#26
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Winfield Hill wrote:
Phil Hobbs wrote... Tom Bruhns wrote: So the right way to do this is to lower the _effective_ minimum capacitance. You can do that by adding an inductor, to cancel out capacitance. You can end up making the tuning range as wide as you want, but at the expense of the crystal (ceramic resonator in your case) being less of the overall frequency determination. In other words, there comes a point where you'd be as well off to just do an LC oscillator. But to double, say, the range, it's a good way to go. I guess I re-discovered what was already well known, but a few years ago I designed such a VCXO, and was amazed how linear the freq-vs-controlvoltage curve was (a good thing for use in a PLL). Don't know what range you're trying to achieve, but I had no trouble getting a bit more than 0.1% (~20kHz at 14MHz) that way, with a crystal. An inductor in series with the varactors, then another one in parallel with the series combo can get you a very wide range of impedance from a decent varactor. Sounds good. How about a specific example? Thanks, - Win whill_at_picovolt-dot-com Last time I used this was with an MV104 common-cathode dual hyperabrupt, to make a 110-MHz phase shifter. It used a Mini-Circuits quadrature hybrid in the usual way, coming in the 0 degree port, coming out the 180 degree port, and hanging matched reactances on the 90 degree ports. Each section had its own inductors, and the cathodes were bypassed heavily (1000 pF) to ground so that the two sides didn't interact too much. The component values were 45 nH in series and 43 nH in parallel. It was linear to within +-4 degrees, and the one section gave phase shifts from 12 to 164 degrees, both dramatically better than I could get with a bare varactor. The idea is to have the varactor resonate with the series inductor just off the low-voltage end of the range, and have the series combination resonate with the parallel L just off the high-voltage end of the range. Since the series-resonance doesn't even notice the parallel L, the design equations decouple nicely, too. You adjust the placement of the resonances to get the range and linearity desired. Cheers, Phil Hobbs |
#27
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Winfield Hill wrote:
Phil Hobbs wrote... Tom Bruhns wrote: So the right way to do this is to lower the _effective_ minimum capacitance. You can do that by adding an inductor, to cancel out capacitance. You can end up making the tuning range as wide as you want, but at the expense of the crystal (ceramic resonator in your case) being less of the overall frequency determination. In other words, there comes a point where you'd be as well off to just do an LC oscillator. But to double, say, the range, it's a good way to go. I guess I re-discovered what was already well known, but a few years ago I designed such a VCXO, and was amazed how linear the freq-vs-controlvoltage curve was (a good thing for use in a PLL). Don't know what range you're trying to achieve, but I had no trouble getting a bit more than 0.1% (~20kHz at 14MHz) that way, with a crystal. An inductor in series with the varactors, then another one in parallel with the series combo can get you a very wide range of impedance from a decent varactor. Sounds good. How about a specific example? Thanks, - Win whill_at_picovolt-dot-com Last time I used this was with an MV104 common-cathode dual hyperabrupt, to make a 110-MHz phase shifter. It used a Mini-Circuits quadrature hybrid in the usual way, coming in the 0 degree port, coming out the 180 degree port, and hanging matched reactances on the 90 degree ports. Each section had its own inductors, and the cathodes were bypassed heavily (1000 pF) to ground so that the two sides didn't interact too much. The component values were 45 nH in series and 43 nH in parallel. It was linear to within +-4 degrees, and the one section gave phase shifts from 12 to 164 degrees, both dramatically better than I could get with a bare varactor. The idea is to have the varactor resonate with the series inductor just off the low-voltage end of the range, and have the series combination resonate with the parallel L just off the high-voltage end of the range. Since the series-resonance doesn't even notice the parallel L, the design equations decouple nicely, too. You adjust the placement of the resonances to get the range and linearity desired. Cheers, Phil Hobbs |
#28
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Winfield Hill wrote:
Phil Hobbs wrote... Tom Bruhns wrote: So the right way to do this is to lower the _effective_ minimum capacitance. You can do that by adding an inductor, to cancel out capacitance. You can end up making the tuning range as wide as you want, but at the expense of the crystal (ceramic resonator in your case) being less of the overall frequency determination. In other words, there comes a point where you'd be as well off to just do an LC oscillator. But to double, say, the range, it's a good way to go. I guess I re-discovered what was already well known, but a few years ago I designed such a VCXO, and was amazed how linear the freq-vs-controlvoltage curve was (a good thing for use in a PLL). Don't know what range you're trying to achieve, but I had no trouble getting a bit more than 0.1% (~20kHz at 14MHz) that way, with a crystal. An inductor in series with the varactors, then another one in parallel with the series combo can get you a very wide range of impedance from a decent varactor. Sounds good. How about a specific example? Thanks, - Win whill_at_picovolt-dot-com Last time I used this was with an MV104 common-cathode dual hyperabrupt, to make a 110-MHz phase shifter. It used a Mini-Circuits quadrature hybrid in the usual way, coming in the 0 degree port, coming out the 180 degree port, and hanging matched reactances on the 90 degree ports. Each section had its own inductors, and the cathodes were bypassed heavily (1000 pF) to ground so that the two sides didn't interact too much. The component values were 45 nH in series and 43 nH in parallel. It was linear to within +-4 degrees, and the one section gave phase shifts from 12 to 164 degrees, both dramatically better than I could get with a bare varactor. The idea is to have the varactor resonate with the series inductor just off the low-voltage end of the range, and have the series combination resonate with the parallel L just off the high-voltage end of the range. Since the series-resonance doesn't even notice the parallel L, the design equations decouple nicely, too. You adjust the placement of the resonances to get the range and linearity desired. Cheers, Phil Hobbs |
#29
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Winfield Hill wrote:
Phil Hobbs wrote... Tom Bruhns wrote: So the right way to do this is to lower the _effective_ minimum capacitance. You can do that by adding an inductor, to cancel out capacitance. You can end up making the tuning range as wide as you want, but at the expense of the crystal (ceramic resonator in your case) being less of the overall frequency determination. In other words, there comes a point where you'd be as well off to just do an LC oscillator. But to double, say, the range, it's a good way to go. I guess I re-discovered what was already well known, but a few years ago I designed such a VCXO, and was amazed how linear the freq-vs-controlvoltage curve was (a good thing for use in a PLL). Don't know what range you're trying to achieve, but I had no trouble getting a bit more than 0.1% (~20kHz at 14MHz) that way, with a crystal. An inductor in series with the varactors, then another one in parallel with the series combo can get you a very wide range of impedance from a decent varactor. Sounds good. How about a specific example? Thanks, - Win whill_at_picovolt-dot-com Last time I used this was with an MV104 common-cathode dual hyperabrupt, to make a 110-MHz phase shifter. It used a Mini-Circuits quadrature hybrid in the usual way, coming in the 0 degree port, coming out the 180 degree port, and hanging matched reactances on the 90 degree ports. Each section had its own inductors, and the cathodes were bypassed heavily (1000 pF) to ground so that the two sides didn't interact too much. The component values were 45 nH in series and 43 nH in parallel. It was linear to within +-4 degrees, and the one section gave phase shifts from 12 to 164 degrees, both dramatically better than I could get with a bare varactor. The idea is to have the varactor resonate with the series inductor just off the low-voltage end of the range, and have the series combination resonate with the parallel L just off the high-voltage end of the range. Since the series-resonance doesn't even notice the parallel L, the design equations decouple nicely, too. You adjust the placement of the resonances to get the range and linearity desired. Cheers, Phil Hobbs |
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